diff --git a/.github/workflows/basic_checks.yml b/.github/workflows/basic_checks.yml new file mode 100644 index 000000000..4e40790b5 --- /dev/null +++ b/.github/workflows/basic_checks.yml @@ -0,0 +1,21 @@ +name: Basic checks for CCPP physics schemes + +on: [push, pull_request] + +jobs: + build: + + runs-on: macos-latest + + steps: + - name: Checkout + uses: actions/checkout@v2 + - name: Init submodules + run: git submodule update --init --recursive + #- name: Update packages + # run: | + # /usr/bin/ruby -e "$(curl -fsSL https://raw.githubusercontent.com/Homebrew/install/master/install)" + # #brew install autoconf automake coreutils gcc@9 libtool mpich gnu-sed wget + # brew install automake coreutils mpich gnu-sed + - name: Check for ASCII encoding + run: ./tools/check_encoding.py diff --git a/CMakeLists.txt b/CMakeLists.txt index 9765fa25e..cd0d1c6d9 100644 --- a/CMakeLists.txt +++ b/CMakeLists.txt @@ -8,7 +8,7 @@ endif (NOT PROJECT) cmake_minimum_required(VERSION 3.0) project(ccppphys - VERSION 3.0.0 + VERSION 4.0.0 LANGUAGES C CXX Fortran) # Use rpaths on MacOSX @@ -19,7 +19,7 @@ endif(POLICY CMP0042) #------------------------------------------------------------------------------ set(PACKAGE "ccpp-physics") -set(AUTHORS "Grant J. Firl" "Dom Heinzeller") +set(AUTHORS "Grant Firl" "Dom Heinzeller" "Man Zhang" "Laurie Carson") #------------------------------------------------------------------------------ # Set OpenMP flags for C/C++/Fortran @@ -58,12 +58,8 @@ if(NOT CMAKE_BUILD_TYPE AND NOT CMAKE_CONFIGURATION_TYPES) endif() #------------------------------------------------------------------------------ -# By default we want a shared library (unless a static build is requested) -if(STATIC) - option(BUILD_SHARED_LIBS "Build a static library" OFF) -else(STATIC) - option(BUILD_SHARED_LIBS "Build a shared library" ON) -endif(STATIC) +# Request a static build +option(BUILD_SHARED_LIBS "Build a shared library" OFF) #------------------------------------------------------------------------------ # Set the sources: physics type definitions @@ -327,45 +323,18 @@ elseif (${CMAKE_Fortran_COMPILER_ID} STREQUAL "PGI") endif (${CMAKE_Fortran_COMPILER_ID} STREQUAL "GNU") #------------------------------------------------------------------------------ -if(STATIC) - add_library(ccppphys STATIC ${SCHEMES} ${SCHEMES_SFX_OPT} ${CAPS}) - # Generate list of Fortran modules from defined sources - foreach(source_f90 ${CAPS}) - get_filename_component(tmp_source_f90 ${source_f90} NAME) - string(REGEX REPLACE ".F90" ".mod" tmp_module_f90 ${tmp_source_f90}) - string(TOLOWER ${tmp_module_f90} module_f90) - list(APPEND MODULES_F90 ${CMAKE_CURRENT_BINARY_DIR}/${module_f90}) - endforeach() -else(STATIC) - add_library(ccppphys SHARED ${SCHEMES} ${SCHEMES_SFX_OPT} ${CAPS}) -endif(STATIC) - -if (NOT STATIC) - target_link_libraries(ccppphys LINK_PUBLIC ${LIBS} ${BACIO_LIB4} ${SP_LIBd} ${W3NCO_LIBd}) -endif (NOT STATIC) +add_library(ccppphys STATIC ${SCHEMES} ${SCHEMES_SFX_OPT} ${CAPS}) +# Generate list of Fortran modules from defined sources +foreach(source_f90 ${CAPS}) + get_filename_component(tmp_source_f90 ${source_f90} NAME) + string(REGEX REPLACE ".F90" ".mod" tmp_module_f90 ${tmp_source_f90}) + string(TOLOWER ${tmp_module_f90} module_f90) + list(APPEND MODULES_F90 ${CMAKE_CURRENT_BINARY_DIR}/${module_f90}) +endforeach() set_target_properties(ccppphys PROPERTIES VERSION ${PROJECT_VERSION} SOVERSION ${PROJECT_VERSION_MAJOR}) -# DH* Hack for PGI compiler: rename objects in scheme cap object files for ISO_C compliancy, -# this is only needed for dynamics builds - static build generates plain Fortran code. -if (${CMAKE_Fortran_COMPILER_ID} STREQUAL "PGI") - if (NOT STATIC) - set(CAPOBJS) - foreach(cap ${CAPS}) - string(REPLACE "_cap.F90" "_cap.F90.o" capobj "./${CMAKE_FILES_DIRECTORY}/ccppphys.dir/${cap}") - list(APPEND CAPOBJS ${capobj}) - endforeach(cap) - - add_custom_command(TARGET ccppphys - PRE_LINK - COMMAND ${CMAKE_CURRENT_SOURCE_DIR}/pgifix.py --cmake ${CAPOBJS} - WORKING_DIRECTORY ${CMAKE_CURRENT_BINARY_DIR} - COMMENT "Running pgifix_wrapper.py over all scheme caps") - endif (NOT STATIC) -endif (${CMAKE_Fortran_COMPILER_ID} STREQUAL "PGI") -# *DH end hack for PGI compiler - if (PROJECT STREQUAL "CCPP-FV3") # Define where to install the library install(TARGETS ccppphys diff --git a/pgifix.py b/pgifix.py deleted file mode 100755 index cc6af76d2..000000000 --- a/pgifix.py +++ /dev/null @@ -1,93 +0,0 @@ -#!/usr/bin/env python - -import argparse -import os -import subprocess -import sys - -parser = argparse.ArgumentParser(description='Fix cap objects produced by PGI compiler') -parser.add_argument("--cmake", default=False, action='store_true') -parser.add_argument("caps", nargs='+') - -FIXCMD_TEMPLATE = 'objcopy ' - -def parse_args(): - args = parser.parse_args() - cmake = args.cmake - caps = args.caps - return (cmake, caps) - -def execute(cmd, debug = True, abort = True): - """Runs a local command in a shell. Waits for completion and - returns status, stdout and stderr. If abort = True, abort in - case an error occurs during the execution of the command.""" - - if debug: - print 'Executing "{0}"'.format(cmd) - p = subprocess.Popen(cmd, stdout = subprocess.PIPE, - stderr = subprocess.PIPE, shell = True) - (stdout, stderr) = p.communicate() - status = p.returncode - if debug: - message = 'Execution of "{0}" returned with exit code {1}\n'.format(cmd, status) - message += ' stdout: "{0}"\n'.format(stdout.rstrip('\n')) - message += ' stderr: "{0}"'.format(stderr.rstrip('\n')) - print message - if not status == 0: - message = 'Execution of command {0} failed, exit code {1}\n'.format(cmd, status) - message += ' stdout: "{0}"\n'.format(stdout.rstrip('\n')) - message += ' stderr: "{0}"'.format(stderr.rstrip('\n')) - if abort: - raise Exception(message) - else: - print message - return (status, stdout.rstrip('\n'), stderr.rstrip('\n')) - -def correct_cap_object_names(fixcmd, cmake, cap): - (cappath, capname) = os.path.split(cap) - # Determine pgi-prepended prefix to remove, different - # for cmake builds and make builds (object filename) - if cmake: - pgiprefix = capname.rstrip('.F90.o').lower() + '_' - else: - pgiprefix = capname.rstrip('.o').lower() + '_' - # Get list of all symbols in cap object - nmcmd = 'nm {0}'.format(cap) - (status, stdout, stderr) = execute(nmcmd) - del nmcmd - # Parse all symbols and generate objcopy command - found = False - for line in stdout.split('\n'): - try: - (address, symboltype, objectname) = line.split() - except ValueError: - continue - if not symboltype == 'T': - continue - if objectname.startswith(pgiprefix): - newname = objectname[len(pgiprefix):] - else: - continue - if newname.endswith('_cap'): - fixcmd += '--redefine-sym {0}={1} '.format(objectname, newname) - found = True - if not found: - raise Exception('Unable to rename CCPP scheme caps in cap "{0}"'.format(cap)) - return fixcmd - -def correct_object_names(fixcmd, cap): - tmp = cap + '.tmp' - fixcmd += '{0} {1}'.format(cap, tmp) - execute(fixcmd) - mvcmd = 'mv -v {0} {1}'.format(tmp, cap) - execute(mvcmd) - -def main(): - (cmake, caps) = parse_args() - for cap in caps: - fixcmd = FIXCMD_TEMPLATE - fixcmd = correct_cap_object_names(fixcmd, cmake, cap) - correct_object_names(fixcmd, cap) - -if __name__ == '__main__': - main() diff --git a/physics/GFS_DCNV_generic.F90 b/physics/GFS_DCNV_generic.F90 index d7305cbe5..1622f4b52 100644 --- a/physics/GFS_DCNV_generic.F90 +++ b/physics/GFS_DCNV_generic.F90 @@ -17,8 +17,8 @@ end subroutine GFS_DCNV_generic_pre_finalize !! \htmlinclude GFS_DCNV_generic_pre_run.html !! #endif - subroutine GFS_DCNV_generic_pre_run (im, levs, ldiag3d, do_cnvgwd, do_ca, cplchm,& - isppt_deep, gu0, gv0, gt0, gq0_water_vapor, & + subroutine GFS_DCNV_generic_pre_run (im, levs, ldiag3d, do_cnvgwd, cplchm, & + gu0, gv0, gt0, gq0_water_vapor, & save_u, save_v, save_t, save_qv, ca_deep, & dqdti, errmsg, errflg) @@ -27,7 +27,7 @@ subroutine GFS_DCNV_generic_pre_run (im, levs, ldiag3d, do_cnvgwd, do_ca, cplchm implicit none integer, intent(in) :: im, levs - logical, intent(in) :: ldiag3d, do_cnvgwd, do_ca, cplchm, isppt_deep + logical, intent(in) :: ldiag3d, do_cnvgwd, cplchm real(kind=kind_phys), dimension(im,levs), intent(in) :: gu0 real(kind=kind_phys), dimension(im,levs), intent(in) :: gv0 real(kind=kind_phys), dimension(im,levs), intent(in) :: gt0 @@ -49,15 +49,7 @@ subroutine GFS_DCNV_generic_pre_run (im, levs, ldiag3d, do_cnvgwd, do_ca, cplchm errmsg = '' errflg = 0 - if (do_ca) then - do k=1,levs - do i=1,im - gq0_water_vapor(i,k) = gq0_water_vapor(i,k)*(1.0 + ca_deep(i)/500.) - enddo - enddo - endif - - if (ldiag3d .or. isppt_deep) then + if (ldiag3d) then do k=1,levs do i=1,im save_t(i,k) = gt0(i,k) @@ -73,7 +65,7 @@ subroutine GFS_DCNV_generic_pre_run (im, levs, ldiag3d, do_cnvgwd, do_ca, cplchm enddo endif - if (ldiag3d .or. cplchm .or. isppt_deep) then + if (ldiag3d .or. cplchm) then do k=1,levs do i=1,im save_qv(i,k) = gq0_water_vapor(i,k) @@ -102,19 +94,19 @@ end subroutine GFS_DCNV_generic_post_finalize !> \section arg_table_GFS_DCNV_generic_post_run Argument Table !! \htmlinclude GFS_DCNV_generic_post_run.html !! - subroutine GFS_DCNV_generic_post_run (im, levs, lssav, ldiag3d, ras, cscnv, do_ca, & - isppt_deep, frain, rain1, dtf, cld1d, save_u, save_v, save_t, save_qv, gu0, gv0, gt0, & + subroutine GFS_DCNV_generic_post_run (im, levs, lssav, ldiag3d, ras, cscnv, & + frain, rain1, dtf, cld1d, save_u, save_v, save_t, save_qv, gu0, gv0, gt0, & gq0_water_vapor, ud_mf, dd_mf, dt_mf, con_g, npdf3d, num_p3d, ncnvcld3d, & rainc, cldwrk, dt3dt, dq3dt, du3dt, dv3dt, upd_mf, dwn_mf, det_mf, & cnvw, cnvc, cnvw_phy_f3d, cnvc_phy_f3d, & - cape, tconvtend, qconvtend, uconvtend, vconvtend, errmsg, errflg) + errmsg, errflg) use machine, only: kind_phys implicit none integer, intent(in) :: im, levs - logical, intent(in) :: lssav, ldiag3d, ras, cscnv, do_ca, isppt_deep + logical, intent(in) :: lssav, ldiag3d, ras, cscnv real(kind=kind_phys), intent(in) :: frain, dtf real(kind=kind_phys), dimension(im), intent(in) :: rain1, cld1d @@ -135,9 +127,6 @@ subroutine GFS_DCNV_generic_post_run (im, levs, lssav, ldiag3d, ras, cscnv, do_c ! as long as these do not get used when not allocated (it is still invalid Fortran code, though). real(kind=kind_phys), dimension(:,:), intent(inout) :: cnvw_phy_f3d, cnvc_phy_f3d - real(kind=kind_phys), dimension(im), intent(inout) :: cape - real(kind=kind_phys), dimension(im,levs), intent(inout) :: tconvtend, qconvtend, uconvtend, vconvtend - character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg @@ -148,11 +137,6 @@ subroutine GFS_DCNV_generic_post_run (im, levs, lssav, ldiag3d, ras, cscnv, do_c errflg = 0 if (.not. ras .and. .not. cscnv) then - if(do_ca) then - do i=1,im - cape(i) = cld1d(i) - enddo - endif if (npdf3d == 3 .and. num_p3d == 4) then do k=1,levs do i=1,im @@ -198,18 +182,6 @@ subroutine GFS_DCNV_generic_post_run (im, levs, lssav, ldiag3d, ras, cscnv, do_c endif ! if (lssav) - - if (isppt_deep) then - do k=1,levs - do i=1,im - tconvtend(i,k) = gt0(i,k) - save_t(i,k) - qconvtend(i,k) = gq0_water_vapor(i,k) - save_qv(i,k) - uconvtend(i,k) = gu0(i,k) - save_u(i,k) - vconvtend(i,k) = gv0(i,k) - save_v(i,k) - enddo - enddo - endif - end subroutine GFS_DCNV_generic_post_run end module GFS_DCNV_generic_post diff --git a/physics/GFS_DCNV_generic.meta b/physics/GFS_DCNV_generic.meta index 07c75eafc..f632833f9 100644 --- a/physics/GFS_DCNV_generic.meta +++ b/physics/GFS_DCNV_generic.meta @@ -33,14 +33,6 @@ type = logical intent = in optional = F -[do_ca] - standard_name = flag_for_cellular_automata - long_name = cellular automata main switch - units = flag - dimensions = () - type = logical - intent = in - optional = F [cplchm] standard_name = flag_for_chemistry_coupling long_name = flag controlling cplchm collection (default off) @@ -49,14 +41,6 @@ type = logical intent = in optional = F -[isppt_deep] - standard_name = flag_for_combination_of_sppt_with_isppt_deep - long_name = switch for combination with isppt_deep. - units = flag - dimensions = () - type = logical - intent = in - optional = F [gu0] standard_name = x_wind_updated_by_physics long_name = zonal wind updated by physics @@ -217,22 +201,6 @@ type = logical intent = in optional = F -[do_ca] - standard_name = flag_for_cellular_automata - long_name = cellular automata main switch - units = flag - dimensions = () - type = logical - intent = in - optional = F -[isppt_deep] - standard_name = flag_for_combination_of_sppt_with_isppt_deep - long_name = switch for combination with isppt_deep. - units = flag - dimensions = () - type = logical - intent = in - optional = F [frain] standard_name = dynamics_to_physics_timestep_ratio long_name = ratio of dynamics timestep to physics timestep @@ -518,51 +486,6 @@ kind = kind_phys intent = inout optional = F -[cape] - standard_name = convective_available_potential_energy_for_coupling - long_name = convective available potential energy for coupling - units = m2 s-2 - dimensions = (horizontal_dimension) - type = real - kind = kind_phys - intent = inout - optional = F -[tconvtend] - standard_name = tendency_of_air_temperature_due_to_deep_convection_for_coupling_on_physics_timestep - long_name = tendency of air temperature due to deep convection - units = K - dimensions = (horizontal_dimension,vertical_dimension) - type = real - kind = kind_phys - intent = inout - optional = F -[qconvtend] - standard_name = tendency_of_water_vapor_specific_humidity_due_to_deep_convection_for_coupling_on_physics_timestep - long_name = tendency of specific humidity due to deep convection - units = kg kg-1 - dimensions = (horizontal_dimension,vertical_dimension) - type = real - kind = kind_phys - intent = inout - optional = F -[uconvtend] - standard_name = tendency_of_x_wind_due_to_deep_convection_for_coupling_on_physics_timestep - long_name = tendency_of_x_wind_due_to_deep_convection - units = m s-1 - dimensions = (horizontal_dimension,vertical_dimension) - type = real - kind = kind_phys - intent = inout - optional = F -[vconvtend] - standard_name = tendency_of_y_wind_due_to_deep_convection_for_coupling_on_physics_timestep - long_name = tendency_of_y_wind_due_to_deep_convection - units = m s-1 - dimensions = (horizontal_dimension,vertical_dimension) - type = real - kind = kind_phys - intent = inout - optional = F [errmsg] standard_name = ccpp_error_message long_name = error message for error handling in CCPP diff --git a/physics/GFS_MP_generic.F90 b/physics/GFS_MP_generic.F90 index ab68e206a..291808fb8 100644 --- a/physics/GFS_MP_generic.F90 +++ b/physics/GFS_MP_generic.F90 @@ -85,7 +85,7 @@ subroutine GFS_MP_generic_post_run(im, ix, levs, kdt, nrcm, ncld, nncl, ntcw, nt rann, xlat, xlon, gt0, gq0, prsl, prsi, phii, tsfc, ice, snow, graupel, save_t, save_qv, rain0, ice0, snow0, & graupel0, del, rain, domr_diag, domzr_diag, domip_diag, doms_diag, tprcp, srflag, sr, cnvprcp, totprcp, totice, & totsnw, totgrp, cnvprcpb, totprcpb, toticeb, totsnwb, totgrpb, dt3dt, dq3dt, rain_cpl, rainc_cpl, snow_cpl, pwat, & - do_sppt, dtdtr, dtdtc, drain_cpl, dsnow_cpl, lsm, lsm_ruc, lsm_noahmp, raincprv, rainncprv, iceprv, snowprv, & + do_sppt, ca_global, dtdtr, dtdtc, drain_cpl, dsnow_cpl, lsm, lsm_ruc, lsm_noahmp, raincprv, rainncprv, iceprv, snowprv, & graupelprv, draincprv, drainncprv, diceprv, dsnowprv, dgraupelprv, dtp, errmsg, errflg) ! use machine, only: kind_phys @@ -114,7 +114,7 @@ subroutine GFS_MP_generic_post_run(im, ix, levs, kdt, nrcm, ncld, nncl, ntcw, nt real(kind=kind_phys), dimension(:,:), intent(inout) :: dt3dt, dq3dt ! Stochastic physics / surface perturbations - logical, intent(in) :: do_sppt + logical, intent(in) :: do_sppt, ca_global real(kind=kind_phys), dimension(im,levs), intent(inout) :: dtdtr real(kind=kind_phys), dimension(im,levs), intent(in) :: dtdtc real(kind=kind_phys), dimension(im), intent(inout) :: drain_cpl @@ -375,7 +375,7 @@ subroutine GFS_MP_generic_post_run(im, ix, levs, kdt, nrcm, ncld, nncl, ntcw, nt enddo ! Stochastic physics / surface perturbations - if (do_sppt) then + if (do_sppt .or. ca_global) then !--- radiation heating rate dtdtr(1:im,:) = dtdtr(1:im,:) + dtdtc(1:im,:)*dtf endif diff --git a/physics/GFS_MP_generic.meta b/physics/GFS_MP_generic.meta index ddf8cb813..c7082da3a 100644 --- a/physics/GFS_MP_generic.meta +++ b/physics/GFS_MP_generic.meta @@ -722,6 +722,14 @@ type = logical intent = in optional = F +[ca_global] + standard_name = flag_for_global_cellular_automata + long_name = switch for global ca + units = flag + dimensions = () + type = logical + intent = in + optional = F [dtdtr] standard_name = tendency_of_air_temperature_due_to_radiative_heating_on_physics_time_step long_name = temp. change due to radiative heating per time step diff --git a/physics/GFS_PBL_generic.F90 b/physics/GFS_PBL_generic.F90 index ff59aa465..abce53772 100644 --- a/physics/GFS_PBL_generic.F90 +++ b/physics/GFS_PBL_generic.F90 @@ -84,7 +84,8 @@ subroutine GFS_PBL_generic_pre_run (im, levs, nvdiff, ntrac, ntwa, ntia, ntgl, ntoz, ntke, ntkev, nqrimef, trans_aero, ntchs, ntchm, & imp_physics, imp_physics_gfdl, imp_physics_thompson, imp_physics_wsm6, & imp_physics_zhao_carr, imp_physics_mg, imp_physics_fer_hires, cplchm, ltaerosol, & - hybedmf, do_shoc, satmedmf, qgrs, vdftra, errmsg, errflg) + hybedmf, do_shoc, satmedmf, qgrs, vdftra, lheatstrg, z0fac, e0fac, zorl, & + u10m, v10m, hflx, evap, hflxq, evapq, hffac, hefac, errmsg, errflg) use machine, only : kind_phys use GFS_PBL_generic_common, only : set_aerosol_tracer_index @@ -102,11 +103,25 @@ subroutine GFS_PBL_generic_pre_run (im, levs, nvdiff, ntrac, real(kind=kind_phys), dimension(im, levs, ntrac), intent(in) :: qgrs real(kind=kind_phys), dimension(im, levs, nvdiff), intent(inout) :: vdftra + ! For canopy heat storage + logical, intent(in) :: lheatstrg + real(kind=kind_phys), intent(in) :: z0fac, e0fac + real(kind=kind_phys), dimension(im), intent(in) :: zorl, u10m, v10m + real(kind=kind_phys), dimension(im), intent(in) :: hflx, evap + real(kind=kind_phys), dimension(im), intent(out) :: hflxq, evapq + real(kind=kind_phys), dimension(im), intent(out) :: hffac, hefac + + ! CCPP error handling variables character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg - !local variables + ! Parameters for canopy heat storage parametrization + real (kind=kind_phys), parameter :: z0min=0.2, z0max=1.0 + real (kind=kind_phys), parameter :: u10min=2.5, u10max=7.5 + + ! Local variables integer :: i, k, kk, k1, n + real(kind=kind_phys) :: tem, tem1, tem2 ! Initialize CCPP error handling variables errmsg = '' @@ -258,6 +273,35 @@ subroutine GFS_PBL_generic_pre_run (im, levs, nvdiff, ntrac, ! endif +! --- ... Boundary Layer and Free atmospheic turbulence parameterization +! +! in order to achieve heat storage within canopy layer, in the canopy heat +! storage parameterization the kinematic sensible and latent heat fluxes +! (hflx & evap) as surface boundary forcings to the pbl scheme are +! reduced as a function of surface roughness +! + do i=1,im + hflxq(i) = hflx(i) + evapq(i) = evap(i) + hffac(i) = 1.0 + hefac(i) = 1.0 + enddo + if (lheatstrg) then + do i=1,im + tem = 0.01 * zorl(i) ! change unit from cm to m + tem1 = (tem - z0min) / (z0max - z0min) + hffac(i) = z0fac * min(max(tem1, 0.0), 1.0) + tem = sqrt(u10m(i)**2+v10m(i)**2) + tem1 = (tem - u10min) / (u10max - u10min) + tem2 = 1.0 - min(max(tem1, 0.0), 1.0) + hffac(i) = tem2 * hffac(i) + hefac(i) = 1. + e0fac * hffac(i) + hffac(i) = 1. + hffac(i) + hflxq(i) = hflx(i) / hffac(i) + evapq(i) = evap(i) / hefac(i) + enddo + endif + end subroutine GFS_PBL_generic_pre_run end module GFS_PBL_generic_pre @@ -286,8 +330,9 @@ subroutine GFS_PBL_generic_post_run (im, levs, nvdiff, ntrac, dqdt, dusfc_cpl, dvsfc_cpl, dtsfc_cpl, & dqsfc_cpl, dusfci_cpl, dvsfci_cpl, dtsfci_cpl, dqsfci_cpl, dusfc_diag, dvsfc_diag, dtsfc_diag, dqsfc_diag, & dusfci_diag, dvsfci_diag, dtsfci_diag, dqsfci_diag, dt3dt, du3dt_PBL, du3dt_OGWD, dv3dt_PBL, dv3dt_OGWD, dq3dt, & - dq3dt_ozone, rd, cp,fvirt, hvap, t1, q1, prsl, hflx, ushfsfci, oceanfrac, fice, dusfc_cice, dvsfc_cice, dtsfc_cice, & - dqsfc_cice, wet, dry, icy, wind, stress_ocn, hflx_ocn, evap_ocn, ugrs1, vgrs1, dkt_cpl, dkt, errmsg, errflg) + dq3dt_ozone, rd, cp, fvirt, hvap, t1, q1, prsl, hflx, ushfsfci, oceanfrac, flag_cice, dusfc_cice, dvsfc_cice, & + dtsfc_cice, dqsfc_cice, wet, dry, icy, wind, stress_wat, hflx_wat, evap_wat, ugrs1, vgrs1, dkt_cpl, dkt, hffac, hefac, & + errmsg, errflg) use machine, only : kind_phys use GFS_PBL_generic_common, only : set_aerosol_tracer_index @@ -301,13 +346,14 @@ subroutine GFS_PBL_generic_post_run (im, levs, nvdiff, ntrac, integer, intent(in) :: imp_physics_zhao_carr, imp_physics_mg, imp_physics_fer_hires logical, intent(in) :: ltaerosol, cplflx, cplchm, lssav, ldiag3d, lsidea logical, intent(in) :: hybedmf, do_shoc, satmedmf, shinhong, do_ysu + logical, dimension(:), intent(in) :: flag_cice real(kind=kind_phys), intent(in) :: dtf real(kind=kind_phys), intent(in) :: rd, cp, fvirt, hvap - real(kind=kind_phys), dimension(:), intent(in) :: t1, q1, hflx, oceanfrac, fice + real(kind=kind_phys), dimension(:), intent(in) :: t1, q1, hflx, oceanfrac real(kind=kind_phys), dimension(:,:), intent(in) :: prsl real(kind=kind_phys), dimension(:), intent(in) :: dusfc_cice, dvsfc_cice, dtsfc_cice, dqsfc_cice, & - wind, stress_ocn, hflx_ocn, evap_ocn, ugrs1, vgrs1 + wind, stress_wat, hflx_wat, evap_wat, ugrs1, vgrs1 real(kind=kind_phys), dimension(im, levs, nvdiff), intent(in) :: dvdftra real(kind=kind_phys), dimension(im), intent(in) :: dusfc1, dvsfc1, dtsfc1, dqsfc1, xmu real(kind=kind_phys), dimension(im, levs), intent(in) :: dudt, dvdt, dtdt, htrsw, htrlw @@ -328,13 +374,15 @@ subroutine GFS_PBL_generic_post_run (im, levs, nvdiff, ntrac, real(kind=kind_phys), dimension(:,:), intent(inout) :: dkt_cpl real(kind=kind_phys), dimension(:,:), intent(in) :: dkt + ! From canopy heat storage - reduction factors in latent/sensible heat flux due to surface roughness + real(kind=kind_phys), dimension(im), intent(in) :: hffac, hefac + character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg real(kind=kind_phys), parameter :: zero = 0.0d0 real(kind=kind_phys), parameter :: one = 1.0d0 real(kind=kind_phys), parameter :: huge = 9.9692099683868690E36 ! NetCDF float FillValue, same as in GFS_typedefs.F90 - real(kind=kind_phys), parameter :: epsln = 1.0d-10 ! same as in GFS_physics_driver.F90 integer :: i, k, kk, k1, n real(kind=kind_phys) :: tem, tem1, rho @@ -502,29 +550,36 @@ subroutine GFS_PBL_generic_post_run (im, levs, nvdiff, ntrac, if (cplflx) then do i=1,im if (oceanfrac(i) > zero) then ! Ocean only, NO LAKES - if (fice(i) > one - epsln) then ! no open water, use results from CICE - dusfci_cpl(i) = dusfc_cice(i) - dvsfci_cpl(i) = dvsfc_cice(i) - dtsfci_cpl(i) = dtsfc_cice(i) - dqsfci_cpl(i) = dqsfc_cice(i) + if ( .not. wet(i)) then ! no open water + if (flag_cice(i)) then !use results from CICE + dusfci_cpl(i) = dusfc_cice(i) + dvsfci_cpl(i) = dvsfc_cice(i) + dtsfci_cpl(i) = dtsfc_cice(i) + dqsfci_cpl(i) = dqsfc_cice(i) + else !use PBL fluxes when CICE fluxes is unavailable + dusfci_cpl(i) = dusfc1(i) + dvsfci_cpl(i) = dvsfc1(i) + dtsfci_cpl(i) = dtsfc1(i) + dqsfci_cpl(i) = dqsfc1(i) + end if elseif (icy(i) .or. dry(i)) then ! use stress_ocean from sfc_diff for opw component at mixed point tem1 = max(q1(i), 1.e-8) rho = prsl(i,1) / (rd*t1(i)*(one+fvirt*tem1)) if (wind(i) > zero) then - tem = - rho * stress_ocn(i) / wind(i) + tem = - rho * stress_wat(i) / wind(i) dusfci_cpl(i) = tem * ugrs1(i) ! U-momentum flux dvsfci_cpl(i) = tem * vgrs1(i) ! V-momentum flux else dusfci_cpl(i) = zero dvsfci_cpl(i) = zero endif - dtsfci_cpl(i) = cp * rho * hflx_ocn(i) ! sensible heat flux over open ocean - dqsfci_cpl(i) = hvap * rho * evap_ocn(i) ! latent heat flux over open ocean + dtsfci_cpl(i) = cp * rho * hflx_wat(i) ! sensible heat flux over open ocean + dqsfci_cpl(i) = hvap * rho * evap_wat(i) ! latent heat flux over open ocean else ! use results from PBL scheme for 100% open ocean dusfci_cpl(i) = dusfc1(i) dvsfci_cpl(i) = dvsfc1(i) - dtsfci_cpl(i) = dtsfc1(i) - dqsfci_cpl(i) = dqsfc1(i) + dtsfci_cpl(i) = dtsfc1(i)*hffac(i) + dqsfci_cpl(i) = dqsfc1(i)*hefac(i) endif ! dusfc_cpl (i) = dusfc_cpl(i) + dusfci_cpl(i) * dtf @@ -547,12 +602,12 @@ subroutine GFS_PBL_generic_post_run (im, levs, nvdiff, ntrac, do i=1,im dusfc_diag (i) = dusfc_diag(i) + dusfc1(i)*dtf dvsfc_diag (i) = dvsfc_diag(i) + dvsfc1(i)*dtf - dtsfc_diag (i) = dtsfc_diag(i) + dtsfc1(i)*dtf - dqsfc_diag (i) = dqsfc_diag(i) + dqsfc1(i)*dtf + dtsfc_diag (i) = dtsfc_diag(i) + dtsfc1(i)*hffac(i)*dtf + dqsfc_diag (i) = dqsfc_diag(i) + dqsfc1(i)*hefac(i)*dtf dusfci_diag(i) = dusfc1(i) dvsfci_diag(i) = dvsfc1(i) - dtsfci_diag(i) = dtsfc1(i) - dqsfci_diag(i) = dqsfc1(i) + dtsfci_diag(i) = dtsfc1(i)*hffac(i) + dqsfci_diag(i) = dqsfc1(i)*hefac(i) enddo if (ldiag3d) then diff --git a/physics/GFS_PBL_generic.meta b/physics/GFS_PBL_generic.meta index 5f4362103..c94d15916 100644 --- a/physics/GFS_PBL_generic.meta +++ b/physics/GFS_PBL_generic.meta @@ -307,6 +307,113 @@ kind = kind_phys intent = inout optional = F +[lheatstrg] + standard_name = flag_for_canopy_heat_storage + long_name = flag for canopy heat storage parameterization + units = flag + dimensions = () + type = logical + intent = in + optional = F +[z0fac] + standard_name = surface_roughness_fraction_factor + long_name = surface roughness fraction factor for canopy heat storage parameterization + units = none + dimensions = () + type = real + kind = kind_phys + intent = in + optional = F +[e0fac] + standard_name = latent_heat_flux_fraction_factor_relative_to_sensible_heat_flux + long_name = latent heat flux fraction factor relative to sensible heat flux for canopy heat storage parameterization + units = none + dimensions = () + type = real + kind = kind_phys + intent = in + optional = F +[zorl] + standard_name = surface_roughness_length + long_name = surface roughness length + units = cm + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = in + optional = F +[u10m] + standard_name = x_wind_at_10m + long_name = 10 meter u wind speed + units = m s-1 + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = in + optional = F +[v10m] + standard_name = y_wind_at_10m + long_name = 10 meter v wind speed + units = m s-1 + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = in + optional = F +[hflx] + standard_name = kinematic_surface_upward_sensible_heat_flux + long_name = kinematic surface upward sensible heat flux + units = K m s-1 + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = in + optional = F +[evap] + standard_name = kinematic_surface_upward_latent_heat_flux + long_name = kinematic surface upward latent heat flux + units = kg kg-1 m s-1 + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = in + optional = F +[hflxq] + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness + long_name = kinematic surface upward sensible heat flux reduced by surface roughness + units = K m s-1 + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = out + optional = F +[evapq] + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness + long_name = kinematic surface upward latent heat flux reduced by surface roughness + units = kg kg-1 m s-1 + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = out + optional = F +[hefac] + standard_name = surface_upward_latent_heat_flux_reduction_factor + long_name = surface upward latent heat flux reduction factor from canopy heat storage + units = none + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = out + optional = F +[hffac] + standard_name = surface_upward_sensible_heat_flux_reduction_factor + long_name = surface upward sensible heat flux reduction factor from canopy heat storage + units = none + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = out + optional = F [errmsg] standard_name = ccpp_error_message long_name = error message for error handling in CCPP @@ -1079,13 +1186,12 @@ kind = kind_phys intent = in optional = F -[fice] - standard_name = sea_ice_concentration - long_name = ice fraction over open water - units = frac +[flag_cice] + standard_name = flag_for_cice + long_name = flag for cice + units = flag dimensions = (horizontal_dimension) - type = real - kind = kind_phys + type = logical intent = in optional = F [dusfc_cice] @@ -1157,7 +1263,7 @@ kind = kind_phys intent = in optional = F -[stress_ocn] +[stress_wat] standard_name = surface_wind_stress_over_ocean long_name = surface wind stress over ocean units = m2 s-2 @@ -1166,7 +1272,7 @@ kind = kind_phys intent = in optional = F -[hflx_ocn] +[hflx_wat] standard_name = kinematic_surface_upward_sensible_heat_flux_over_ocean long_name = kinematic surface upward sensible heat flux over ocean units = K m s-1 @@ -1175,7 +1281,7 @@ kind = kind_phys intent = in optional = F -[evap_ocn] +[evap_wat] standard_name = kinematic_surface_upward_latent_heat_flux_over_ocean long_name = kinematic surface upward latent heat flux over ocean units = kg kg-1 m s-1 @@ -1220,6 +1326,24 @@ kind = kind_phys intent = in optional = F +[hefac] + standard_name = surface_upward_latent_heat_flux_reduction_factor + long_name = surface upward latent heat flux reduction factor from canopy heat storage + units = none + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = in + optional = F +[hffac] + standard_name = surface_upward_sensible_heat_flux_reduction_factor + long_name = surface upward sensible heat flux reduction factor from canopy heat storage + units = none + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = in + optional = F [errmsg] standard_name = ccpp_error_message long_name = error message for error handling in CCPP diff --git a/physics/GFS_debug.F90 b/physics/GFS_debug.F90 index 6bf39d491..4a096449d 100644 --- a/physics/GFS_debug.F90 +++ b/physics/GFS_debug.F90 @@ -18,6 +18,7 @@ module GFS_diagtoscreen interface print_var module procedure print_logic_0d + module procedure print_logic_1d module procedure print_int_0d module procedure print_int_1d module procedure print_real_0d @@ -116,6 +117,7 @@ subroutine GFS_diagtoscreen_run (Model, Statein, Stateout, Sfcprop, Coupling, do impi=0,mpisize-1 do iomp=0,ompsize-1 if (mpirank==impi .and. omprank==iomp) then + call print_var(mpirank,omprank, blkno, 'Model%kdt' , Model%kdt) ! Sfcprop call print_var(mpirank,omprank, blkno, 'Sfcprop%slmsk' , Sfcprop%slmsk) call print_var(mpirank,omprank, blkno, 'Sfcprop%oceanfrac', Sfcprop%oceanfrac) @@ -478,17 +480,12 @@ subroutine GFS_diagtoscreen_run (Model, Statein, Stateout, Sfcprop, Coupling, call print_var(mpirank,omprank, blkno, 'Coupling%sfc_wts' , Coupling%sfc_wts ) end if if (Model%do_ca) then - call print_var(mpirank,omprank, blkno, 'Coupling%tconvtend', Coupling%tconvtend ) - call print_var(mpirank,omprank, blkno, 'Coupling%qconvtend', Coupling%qconvtend ) - call print_var(mpirank,omprank, blkno, 'Coupling%uconvtend', Coupling%uconvtend ) - call print_var(mpirank,omprank, blkno, 'Coupling%vconvtend', Coupling%vconvtend ) - call print_var(mpirank,omprank, blkno, 'Coupling%ca_out ', Coupling%ca_out ) + call print_var(mpirank,omprank, blkno, 'Coupling%ca1 ', Coupling%ca1 ) call print_var(mpirank,omprank, blkno, 'Coupling%ca_deep ', Coupling%ca_deep ) call print_var(mpirank,omprank, blkno, 'Coupling%ca_turb ', Coupling%ca_turb ) call print_var(mpirank,omprank, blkno, 'Coupling%ca_shal ', Coupling%ca_shal ) call print_var(mpirank,omprank, blkno, 'Coupling%ca_rad ', Coupling%ca_rad ) call print_var(mpirank,omprank, blkno, 'Coupling%ca_micro ', Coupling%ca_micro ) - call print_var(mpirank,omprank, blkno, 'Coupling%cape ', Coupling%cape ) end if if(Model%imp_physics == Model%imp_physics_thompson .and. Model%ltaerosol) then call print_var(mpirank,omprank, blkno, 'Coupling%nwfa2d', Coupling%nwfa2d) @@ -557,6 +554,30 @@ subroutine print_int_0d(mpirank,omprank,blkno,name,var) end subroutine print_int_0d + subroutine print_logic_1d(mpirank,omprank,blkno,name,var) + + use machine, only: kind_phys + + implicit none + + integer, intent(in) :: mpirank, omprank, blkno + character(len=*), intent(in) :: name + logical, intent(in) :: var(:) + + integer :: i + +#ifdef PRINT_SUM + write(0,'(2a,3i6,2i8)') 'XXX: ', trim(name), mpirank, omprank, blkno, size(var), count(var) +#elif defined(PRINT_CHKSUM) + write(0,'(2a,3i6,2i8)') 'XXX: ', trim(name), mpirank, omprank, blkno, size(var), count(var) +#else + do i=ISTART,min(IEND,size(var(:))) + write(0,'(2a,3i6,i6,1x,l)') 'XXX: ', trim(name), mpirank, omprank, blkno, i, var(i) + end do +#endif + + end subroutine print_logic_1d + subroutine print_int_1d(mpirank,omprank,blkno,name,var) use machine, only: kind_phys diff --git a/physics/GFS_stochastics.F90 b/physics/GFS_stochastics.F90 index 99f84e3b1..9b4533cf9 100644 --- a/physics/GFS_stochastics.F90 +++ b/physics/GFS_stochastics.F90 @@ -26,7 +26,8 @@ end subroutine GFS_stochastics_finalize !! -# defines random seed indices for radiation (in a reproducible way) !! -# interpolates coefficients for prognostic ozone calculation !! -# performs surface data cycling via the GFS gcycle routine - subroutine GFS_stochastics_run (im, km, do_sppt, use_zmtnblck, do_shum, do_skeb, & + subroutine GFS_stochastics_run (im, km, kdt, do_sppt, use_zmtnblck, do_shum, & + do_skeb, do_ca,ca_global,ca1,si,vfact_ca, & zmtnblck, sppt_wts, skebu_wts, skebv_wts, shum_wts,& sppt_wts_inv, skebu_wts_inv, skebv_wts_inv, & shum_wts_inv, diss_est, & @@ -42,11 +43,13 @@ subroutine GFS_stochastics_run (im, km, do_sppt, use_zmtnblck, do_shum, do_skeb, integer, intent(in) :: im integer, intent(in) :: km + integer, intent(in) :: kdt logical, intent(in) :: do_sppt + logical, intent(in) :: do_ca + logical, intent(in) :: ca_global logical, intent(in) :: use_zmtnblck logical, intent(in) :: do_shum logical, intent(in) :: do_skeb - !logical, intent(in) :: isppt_deep real(kind_phys), dimension(1:im), intent(in) :: zmtnblck ! sppt_wts only allocated if do_sppt == .true. real(kind_phys), dimension(:,:), intent(inout) :: sppt_wts @@ -85,17 +88,16 @@ subroutine GFS_stochastics_run (im, km, do_sppt, use_zmtnblck, do_shum, do_skeb, ! drain_cpl, dsnow_cpl only allocated if cplflx == .true. or cplchm == .true. real(kind_phys), dimension(:), intent(in) :: drain_cpl real(kind_phys), dimension(:), intent(in) :: dsnow_cpl - ! tconvtend ... vconvtend only allocated if isppt_deep == .true. - !real(kind_phys), dimension(:,:), intent(in) :: tconvtend - !real(kind_phys), dimension(:,:), intent(in) :: qconvtend - !real(kind_phys), dimension(:,:), intent(in) :: uconvtend - !real(kind_phys), dimension(:,:), intent(in) :: vconvtend + real(kind_phys), dimension(1:km), intent(in) :: si + real(kind_phys), dimension(1:km), intent(inout) :: vfact_ca + real(kind_phys), dimension(1:im), intent(in) :: ca1 character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg !--- local variables integer :: k, i real(kind=kind_phys) :: upert, vpert, tpert, qpert, qnew, sppt_vwt + real(kind=kind_phys), dimension(1:im,1:km) :: ca ! Initialize CCPP error handling variables errmsg = '' @@ -126,22 +128,11 @@ subroutine GFS_stochastics_run (im, km, do_sppt, use_zmtnblck, do_shum, do_skeb, endif sppt_wts_inv(i,k)=sppt_wts(i,k) - !if(isppt_deep)then - - ! upert = (gu0(i,k) - ugrs(i,k) - uconvtend(i,k)) + uconvtend(i,k) * sppt_wts(i,k) - ! vpert = (gv0(i,k) - vgrs(i,k) - vconvtend(i,k)) + vconvtend(i,k) * sppt_wts(i,k) - ! tpert = (gt0(i,k) - tgrs(i,k) - dtdtr(i,k) - tconvtend(i,k)) + tconvtend(i,k) * sppt_wts(i,k) - ! qpert = (gq0(i,k) - qgrs(i,k) - qconvtend(i,k)) + qconvtend(i,k) * sppt_wts(i,k) - - !else - upert = (gu0(i,k) - ugrs(i,k)) * sppt_wts(i,k) vpert = (gv0(i,k) - vgrs(i,k)) * sppt_wts(i,k) tpert = (gt0(i,k) - tgrs(i,k) - dtdtr(i,k)) * sppt_wts(i,k) qpert = (gq0(i,k) - qgrs(i,k)) * sppt_wts(i,k) - !endif - gu0(i,k) = ugrs(i,k)+upert gv0(i,k) = vgrs(i,k)+vpert @@ -154,21 +145,6 @@ subroutine GFS_stochastics_run (im, km, do_sppt, use_zmtnblck, do_shum, do_skeb, enddo enddo - !if(isppt_deep)then - ! tprcp(:) = tprcp(:) + (sppt_wts(:,15) - 1 )*rainc(:) - ! totprcp(:) = totprcp(:) + (sppt_wts(:,15) - 1 )*rainc(:) - ! cnvprcp(:) = cnvprcp(:) + (sppt_wts(:,15) - 1 )*rainc(:) - !! ! bucket precipitation adjustment due to sppt - ! totprcpb(:) = totprcpb(:) + (sppt_wts(:,15) - 1 )*rainc(:) - ! cnvprcpb(:) = cnvprcpb(:) + (sppt_wts(:,15) - 1 )*rainc(:) - - ! if (cplflx) then !Need to make proper adjustments for deep convection only perturbations - ! rain_cpl(:) = rain_cpl(:) + (sppt_wts(:,15) - 1.0)*drain_cpl(:) - ! snow_cpl(:) = snow_cpl(:) + (sppt_wts(:,15) - 1.0)*dsnow_cpl(:) - ! endif - - !else - ! instantaneous precip rate going into land model at the next time step tprcp(:) = sppt_wts(:,15)*tprcp(:) totprcp(:) = totprcp(:) + (sppt_wts(:,15) - 1 )*rain(:) @@ -183,7 +159,75 @@ subroutine GFS_stochastics_run (im, km, do_sppt, use_zmtnblck, do_shum, do_skeb, snow_cpl(:) = snow_cpl(:) + (sppt_wts(:,15) - 1.0)*dsnow_cpl(:) endif - !endif + endif + + if (do_ca .and. ca_global) then + + if(kdt == 1)then + do k=1,km + if (si(k) .lt. 0.1 .and. si(k) .gt. 0.025) then + vfact_ca(k) = (si(k)-0.025)/(0.1-0.025) + else if (si(k) .lt. 0.025) then + vfact_ca(k) = 0.0 + else + vfact_ca(k) = 1.0 + endif + enddo + vfact_ca(2)=vfact_ca(3)*0.5 + vfact_ca(1)=0.0 + endif + + do k = 1,km + do i = 1,im + sppt_vwt=1.0 + if (zmtnblck(i).EQ.0.0) then + sppt_vwt=1.0 + else + if (k.GT.zmtnblck(i)+2) then + sppt_vwt=1.0 + endif + if (k.LE.zmtnblck(i)) then + sppt_vwt=0.0 + endif + if (k.EQ.zmtnblck(i)+1) then + sppt_vwt=0.333333 + endif + if (k.EQ.zmtnblck(i)+2) then + sppt_vwt=0.666667 + endif + endif + + ca(i,k)=((ca1(i)-1.)*sppt_vwt*vfact_ca(k))+1.0 + + upert = (gu0(i,k) - ugrs(i,k)) * ca(i,k) + vpert = (gv0(i,k) - vgrs(i,k)) * ca(i,k) + tpert = (gt0(i,k) - tgrs(i,k) - dtdtr(i,k)) * ca(i,k) + qpert = (gq0(i,k) - qgrs(i,k)) * ca(i,k) + gu0(i,k) = ugrs(i,k)+upert + gv0(i,k) = vgrs(i,k)+vpert + !negative humidity check + qnew = qgrs(i,k)+qpert + if (qnew >= 1.0e-10) then + gq0(i,k) = qnew + gt0(i,k) = tgrs(i,k) + tpert + dtdtr(i,k) + endif + enddo + enddo + + ! instantaneous precip rate going into land model at the next time step + tprcp(:) = ca(:,15)*tprcp(:) + totprcp(:) = totprcp(:) + (ca(:,15) - 1 )*rain(:) + ! acccumulated total and convective preciptiation + cnvprcp(:) = cnvprcp(:) + (ca(:,15) - 1 )*rainc(:) + ! bucket precipitation adjustment due to sppt + totprcpb(:) = totprcpb(:) + (ca(:,15) - 1 )*rain(:) + cnvprcpb(:) = cnvprcpb(:) + (ca(:,15) - 1 )*rainc(:) + + if (cplflx) then + rain_cpl(:) = rain_cpl(:) + (ca(:,15) - 1.0)*drain_cpl(:) + snow_cpl(:) = snow_cpl(:) + (ca(:,15) - 1.0)*dsnow_cpl(:) + endif + endif diff --git a/physics/GFS_stochastics.meta b/physics/GFS_stochastics.meta index 9232c8d6a..c4fad912e 100644 --- a/physics/GFS_stochastics.meta +++ b/physics/GFS_stochastics.meta @@ -17,6 +17,14 @@ type = integer intent = in optional = F +[kdt] + standard_name = index_of_time_step + long_name = current forecast iteration + units = index + dimensions = () + type = integer + intent = in + optional = F [do_sppt] standard_name = flag_for_stochastic_surface_physics_perturbations long_name = flag for stochastic surface physics perturbations @@ -67,6 +75,49 @@ kind = kind_phys intent = inout optional = F +[do_ca] + standard_name = flag_for_cellular_automata + long_name = cellular automata main switch + units = flag + dimensions = () + type = logical + intent = in + optional = F +[ca_global] + standard_name = flag_for_global_cellular_automata + long_name = switch for global ca + units = flag + dimensions = () + type = logical + intent = in + optional = F +[ca1] + standard_name = cellular_automata_global_pattern + long_name = cellular automata global pattern + units = flag + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = in + optional = F +[vfact_ca] + standard_name = vertical_weight_for_ca + long_name = vertical weight for ca + units = frac + dimensions = (vertical_dimension) + type = real + kind = kind_phys + intent = inout + optional = F +[si] + standard_name = vertical_sigma_coordinate_for_radiation_initialization + long_name = vertical sigma coordinate for radiation initialization + units = none + dimensions = (number_of_vertical_layers_for_radiation_calculations_plus_one) + type = real + kind = kind_phys + intent = in + optional = F [skebu_wts] standard_name = weights_for_stochastic_skeb_perturbation_of_x_wind long_name = weights for stochastic skeb perturbation of x wind diff --git a/physics/GFS_suite_interstitial.F90 b/physics/GFS_suite_interstitial.F90 index 935dd9430..2f14f0fec 100644 --- a/physics/GFS_suite_interstitial.F90 +++ b/physics/GFS_suite_interstitial.F90 @@ -160,7 +160,7 @@ end subroutine GFS_suite_interstitial_2_finalize subroutine GFS_suite_interstitial_2_run (im, levs, lssav, ldiag3d, lsidea, cplflx, flag_cice, shal_cnv, old_monin, mstrat, & do_shoc, frac_grid, imfshalcnv, dtf, xcosz, adjsfcdsw, adjsfcdlw, cice, pgr, ulwsfc_cice, lwhd, htrsw, htrlw, xmu, ctei_rm, & work1, work2, prsi, tgrs, prsl, qgrs_water_vapor, qgrs_cloud_water, cp, hvap, prslk, suntim, adjsfculw, adjsfculw_lnd, & - adjsfculw_ice, adjsfculw_ocn, dlwsfc, ulwsfc, psmean, dt3dt_lw, dt3dt_sw, dt3dt_pbl, dt3dt_dcnv, dt3dt_scnv, dt3dt_mp, & + adjsfculw_ice, adjsfculw_wat, dlwsfc, ulwsfc, psmean, dt3dt_lw, dt3dt_sw, dt3dt_pbl, dt3dt_dcnv, dt3dt_scnv, dt3dt_mp, & ctei_rml, ctei_r, kinver, dry, icy, wet, frland, huge, errmsg, errflg) implicit none @@ -181,7 +181,7 @@ subroutine GFS_suite_interstitial_2_run (im, levs, lssav, ldiag3d, lsidea, cplfl integer, intent(inout), dimension(im) :: kinver real(kind=kind_phys), intent(inout), dimension(im) :: suntim, dlwsfc, ulwsfc, psmean, ctei_rml, ctei_r - real(kind=kind_phys), intent(in ), dimension(im) :: adjsfculw_lnd, adjsfculw_ice, adjsfculw_ocn + real(kind=kind_phys), intent(in ), dimension(im) :: adjsfculw_lnd, adjsfculw_ice, adjsfculw_wat real(kind=kind_phys), intent( out), dimension(im) :: adjsfculw ! These arrays are only allocated if ldiag3d is .true. @@ -232,11 +232,11 @@ subroutine GFS_suite_interstitial_2_run (im, levs, lssav, ldiag3d, lsidea, cplfl if (flag_cice(i)) then adjsfculw(i) = adjsfculw_lnd(i) * frland(i) & + ulwsfc_cice(i) * tem & - + adjsfculw_ocn(i) * (one - frland(i) - tem) + + adjsfculw_wat(i) * (one - frland(i) - tem) else adjsfculw(i) = adjsfculw_lnd(i) * frland(i) & + adjsfculw_ice(i) * tem & - + adjsfculw_ocn(i) * (one - frland(i) - tem) + + adjsfculw_wat(i) * (one - frland(i) - tem) endif enddo else @@ -246,20 +246,20 @@ subroutine GFS_suite_interstitial_2_run (im, levs, lssav, ldiag3d, lsidea, cplfl elseif (icy(i)) then ! ice (and water) tem = one - cice(i) if (flag_cice(i)) then - if (wet(i) .and. adjsfculw_ocn(i) /= huge) then - adjsfculw(i) = ulwsfc_cice(i)*cice(i) + adjsfculw_ocn(i)*tem + if (wet(i) .and. adjsfculw_wat(i) /= huge) then + adjsfculw(i) = ulwsfc_cice(i)*cice(i) + adjsfculw_wat(i)*tem else adjsfculw(i) = ulwsfc_cice(i) endif else - if (wet(i) .and. adjsfculw_ocn(i) /= huge) then - adjsfculw(i) = adjsfculw_ice(i)*cice(i) + adjsfculw_ocn(i)*tem + if (wet(i) .and. adjsfculw_wat(i) /= huge) then + adjsfculw(i) = adjsfculw_ice(i)*cice(i) + adjsfculw_wat(i)*tem else adjsfculw(i) = adjsfculw_ice(i) endif endif else ! all water - adjsfculw(i) = adjsfculw_ocn(i) + adjsfculw(i) = adjsfculw_wat(i) endif enddo endif diff --git a/physics/GFS_suite_interstitial.meta b/physics/GFS_suite_interstitial.meta index 5c206ef30..08f8b2af0 100644 --- a/physics/GFS_suite_interstitial.meta +++ b/physics/GFS_suite_interstitial.meta @@ -604,7 +604,7 @@ kind = kind_phys intent = in optional = F -[adjsfculw_ocn] +[adjsfculw_wat] standard_name = surface_upwelling_longwave_flux_over_ocean_interstitial long_name = surface upwelling longwave flux at current time over ocean (temporary use as interstitial) units = W m-2 diff --git a/physics/GFS_surface_composites.F90 b/physics/GFS_surface_composites.F90 index 7cd552e69..57158321d 100644 --- a/physics/GFS_surface_composites.F90 +++ b/physics/GFS_surface_composites.F90 @@ -26,12 +26,12 @@ end subroutine GFS_surface_composites_pre_finalize !! subroutine GFS_surface_composites_pre_run (im, frac_grid, flag_cice, cplflx, cplwav2atm, & landfrac, lakefrac, oceanfrac, & - frland, dry, icy, lake, ocean, wet, cice, cimin, zorl, zorlo, zorll, zorl_ocn, & - zorl_lnd, zorl_ice, snowd, snowd_ocn, snowd_lnd, snowd_ice, tprcp, tprcp_ocn, & - tprcp_lnd, tprcp_ice, uustar, uustar_lnd, uustar_ice, weasd, weasd_ocn, & - weasd_lnd, weasd_ice, ep1d_ice, tsfc, tsfco, tsfcl, tsfc_ocn, tsfc_lnd, & - tsfc_ice, tisfc, tice, tsurf, tsurf_ocn, tsurf_lnd, tsurf_ice, gflx_ice, & - tgice, islmsk, semis_rad, semis_ocn, semis_lnd, semis_ice, & + frland, dry, icy, lake, ocean, wet, cice, cimin, zorl, zorlo, zorll, zorl_wat, & + zorl_lnd, zorl_ice, snowd, snowd_wat, snowd_lnd, snowd_ice, tprcp, tprcp_wat, & + tprcp_lnd, tprcp_ice, uustar, uustar_lnd, uustar_ice, weasd, weasd_wat, & + weasd_lnd, weasd_ice, ep1d_ice, tsfc, tsfco, tsfcl, tsfc_wat, tsfc_lnd, & + tsfc_ice, tisfc, tice, tsurf, tsurf_wat, tsurf_lnd, tsurf_ice, gflx_ice, & + tgice, islmsk, semis_rad, semis_wat, semis_lnd, semis_ice, & min_lakeice, min_seaice, errmsg, errflg) implicit none @@ -48,14 +48,14 @@ subroutine GFS_surface_composites_pre_run (im, frac_grid, flag_cice, cplflx, cpl real(kind=kind_phys), dimension(im), intent(in ) :: zorl, snowd, tprcp, uustar, weasd real(kind=kind_phys), dimension(im), intent(inout) :: zorlo, zorll, tsfc, tsfco, tsfcl, tisfc, tsurf - real(kind=kind_phys), dimension(im), intent(inout) :: snowd_ocn, snowd_lnd, snowd_ice, tprcp_ocn, & - tprcp_lnd, tprcp_ice, zorl_ocn, zorl_lnd, zorl_ice, tsfc_ocn, tsfc_lnd, tsfc_ice, tsurf_ocn, & - tsurf_lnd, tsurf_ice, uustar_lnd, uustar_ice, weasd_ocn, weasd_lnd, weasd_ice, ep1d_ice, gflx_ice + real(kind=kind_phys), dimension(im), intent(inout) :: snowd_wat, snowd_lnd, snowd_ice, tprcp_wat, & + tprcp_lnd, tprcp_ice, zorl_wat, zorl_lnd, zorl_ice, tsfc_wat, tsfc_lnd, tsfc_ice, tsurf_wat, & + tsurf_lnd, tsurf_ice, uustar_lnd, uustar_ice, weasd_wat, weasd_lnd, weasd_ice, ep1d_ice, gflx_ice real(kind=kind_phys), dimension(im), intent( out) :: tice real(kind=kind_phys), intent(in ) :: tgice integer, dimension(im), intent(in ) :: islmsk real(kind=kind_phys), dimension(im), intent(in ) :: semis_rad - real(kind=kind_phys), dimension(im), intent(inout) :: semis_ocn, semis_lnd, semis_ice + real(kind=kind_phys), dimension(im), intent(inout) :: semis_wat, semis_lnd, semis_ice real(kind=kind_phys), intent(in ) :: min_lakeice, min_seaice ! CCPP error handling @@ -138,18 +138,18 @@ subroutine GFS_surface_composites_pre_run (im, frac_grid, flag_cice, cplflx, cpl endif do i=1,im - tprcp_ocn(i) = tprcp(i) + tprcp_wat(i) = tprcp(i) tprcp_lnd(i) = tprcp(i) tprcp_ice(i) = tprcp(i) if (wet(i)) then ! Water - zorl_ocn(i) = zorlo(i) - tsfc_ocn(i) = tsfco(i) - tsurf_ocn(i) = tsfco(i) -! weasd_ocn(i) = weasd(i) -! snowd_ocn(i) = snowd(i) - weasd_ocn(i) = zero - snowd_ocn(i) = zero - semis_ocn(i) = 0.984d0 + zorl_wat(i) = zorlo(i) + tsfc_wat(i) = tsfco(i) + tsurf_wat(i) = tsfco(i) +! weasd_wat(i) = weasd(i) +! snowd_wat(i) = snowd(i) + weasd_wat(i) = zero + snowd_wat(i) = zero + semis_wat(i) = 0.984d0 endif if (dry(i)) then ! Land uustar_lnd(i) = uustar(i) @@ -204,8 +204,8 @@ end subroutine GFS_surface_composites_inter_finalize !> \section arg_table_GFS_surface_composites_inter_run Argument Table !! \htmlinclude GFS_surface_composites_inter_run.html !! - subroutine GFS_surface_composites_inter_run (im, dry, icy, wet, semis_ocn, semis_lnd, semis_ice, adjsfcdlw, & - gabsbdlw_lnd, gabsbdlw_ice, gabsbdlw_ocn, & + subroutine GFS_surface_composites_inter_run (im, dry, icy, wet, semis_wat, semis_lnd, semis_ice, adjsfcdlw, & + gabsbdlw_lnd, gabsbdlw_ice, gabsbdlw_wat, & adjsfcusw, adjsfcdsw, adjsfcnsw, errmsg, errflg) implicit none @@ -213,9 +213,9 @@ subroutine GFS_surface_composites_inter_run (im, dry, icy, wet, semis_ocn, semis ! Interface variables integer, intent(in ) :: im logical, dimension(im), intent(in ) :: dry, icy, wet - real(kind=kind_phys), dimension(im), intent(in ) :: semis_ocn, semis_lnd, semis_ice, adjsfcdlw, & + real(kind=kind_phys), dimension(im), intent(in ) :: semis_wat, semis_lnd, semis_ice, adjsfcdlw, & adjsfcdsw, adjsfcnsw - real(kind=kind_phys), dimension(im), intent(inout) :: gabsbdlw_lnd, gabsbdlw_ice, gabsbdlw_ocn + real(kind=kind_phys), dimension(im), intent(inout) :: gabsbdlw_lnd, gabsbdlw_ice, gabsbdlw_wat real(kind=kind_phys), dimension(im), intent(out) :: adjsfcusw ! CCPP error handling @@ -250,7 +250,7 @@ subroutine GFS_surface_composites_inter_run (im, dry, icy, wet, semis_ocn, semis do i=1,im if (dry(i)) gabsbdlw_lnd(i) = semis_lnd(i) * adjsfcdlw(i) if (icy(i)) gabsbdlw_ice(i) = semis_ice(i) * adjsfcdlw(i) - if (wet(i)) gabsbdlw_ocn(i) = semis_ocn(i) * adjsfcdlw(i) + if (wet(i)) gabsbdlw_wat(i) = semis_wat(i) * adjsfcdlw(i) adjsfcusw(i) = adjsfcdsw(i) - adjsfcnsw(i) enddo @@ -285,29 +285,29 @@ end subroutine GFS_surface_composites_post_finalize !! #endif subroutine GFS_surface_composites_post_run ( & - im, cplflx, cplwav2atm, frac_grid, flag_cice, islmsk, dry, wet, icy, landfrac, lakefrac, oceanfrac, & - zorl, zorlo, zorll, zorl_ocn, zorl_lnd, zorl_ice, & - cd, cd_ocn, cd_lnd, cd_ice, cdq, cdq_ocn, cdq_lnd, cdq_ice, rb, rb_ocn, rb_lnd, rb_ice, stress, stress_ocn, stress_lnd, & - stress_ice, ffmm, ffmm_ocn, ffmm_lnd, ffmm_ice, ffhh, ffhh_ocn, ffhh_lnd, ffhh_ice, uustar, uustar_ocn, uustar_lnd, & - uustar_ice, fm10, fm10_ocn, fm10_lnd, fm10_ice, fh2, fh2_ocn, fh2_lnd, fh2_ice, tsurf, tsurf_ocn, tsurf_lnd, tsurf_ice, & - cmm, cmm_ocn, cmm_lnd, cmm_ice, chh, chh_ocn, chh_lnd, chh_ice, gflx, gflx_ocn, gflx_lnd, gflx_ice, ep1d, ep1d_ocn, & - ep1d_lnd, ep1d_ice, weasd, weasd_ocn, weasd_lnd, weasd_ice, snowd, snowd_ocn, snowd_lnd, snowd_ice, tprcp, tprcp_ocn, & - tprcp_lnd, tprcp_ice, evap, evap_ocn, evap_lnd, evap_ice, hflx, hflx_ocn, hflx_lnd, hflx_ice, qss, qss_ocn, qss_lnd, & - qss_ice, tsfc, tsfco, tsfcl, tsfc_ocn, tsfc_lnd, tsfc_ice, tisfc, tice, hice, cice, errmsg, errflg) + im, kice, km, cplflx, cplwav2atm, frac_grid, flag_cice, islmsk, dry, wet, icy, landfrac, lakefrac, oceanfrac, & + zorl, zorlo, zorll, zorl_wat, zorl_lnd, zorl_ice, & + cd, cd_wat, cd_lnd, cd_ice, cdq, cdq_wat, cdq_lnd, cdq_ice, rb, rb_wat, rb_lnd, rb_ice, stress, stress_wat, stress_lnd, & + stress_ice, ffmm, ffmm_wat, ffmm_lnd, ffmm_ice, ffhh, ffhh_wat, ffhh_lnd, ffhh_ice, uustar, uustar_wat, uustar_lnd, & + uustar_ice, fm10, fm10_wat, fm10_lnd, fm10_ice, fh2, fh2_wat, fh2_lnd, fh2_ice, tsurf, tsurf_wat, tsurf_lnd, tsurf_ice, & + cmm, cmm_wat, cmm_lnd, cmm_ice, chh, chh_wat, chh_lnd, chh_ice, gflx, gflx_wat, gflx_lnd, gflx_ice, ep1d, ep1d_wat, & + ep1d_lnd, ep1d_ice, weasd, weasd_wat, weasd_lnd, weasd_ice, snowd, snowd_wat, snowd_lnd, snowd_ice, tprcp, tprcp_wat, & + tprcp_lnd, tprcp_ice, evap, evap_wat, evap_lnd, evap_ice, hflx, hflx_wat, hflx_lnd, hflx_ice, qss, qss_wat, qss_lnd, & + qss_ice, tsfc, tsfco, tsfcl, tsfc_wat, tsfc_lnd, tsfc_ice, tisfc, tice, hice, cice, tiice, stc, errmsg, errflg) implicit none - integer, intent(in) :: im + integer, intent(in) :: im, kice, km logical, intent(in) :: cplflx, frac_grid, cplwav2atm logical, dimension(im), intent(in) :: flag_cice, dry, wet, icy integer, dimension(im), intent(in) :: islmsk real(kind=kind_phys), dimension(im), intent(in) :: landfrac, lakefrac, oceanfrac, & - zorl_ocn, zorl_lnd, zorl_ice, cd_ocn, cd_lnd, cd_ice, cdq_ocn, cdq_lnd, cdq_ice, rb_ocn, rb_lnd, rb_ice, stress_ocn, & - stress_lnd, stress_ice, ffmm_ocn, ffmm_lnd, ffmm_ice, ffhh_ocn, ffhh_lnd, ffhh_ice, uustar_ocn, uustar_lnd, uustar_ice, & - fm10_ocn, fm10_lnd, fm10_ice, fh2_ocn, fh2_lnd, fh2_ice, tsurf_ocn, tsurf_lnd, tsurf_ice, cmm_ocn, cmm_lnd, cmm_ice, & - chh_ocn, chh_lnd, chh_ice, gflx_ocn, gflx_lnd, gflx_ice, ep1d_ocn, ep1d_lnd, ep1d_ice, weasd_ocn, weasd_lnd, weasd_ice, & - snowd_ocn, snowd_lnd, snowd_ice,tprcp_ocn, tprcp_lnd, tprcp_ice, evap_ocn, evap_lnd, evap_ice, hflx_ocn, hflx_lnd, & - hflx_ice, qss_ocn, qss_lnd, qss_ice, tsfc_ocn, tsfc_lnd, tsfc_ice + zorl_wat, zorl_lnd, zorl_ice, cd_wat, cd_lnd, cd_ice, cdq_wat, cdq_lnd, cdq_ice, rb_wat, rb_lnd, rb_ice, stress_wat, & + stress_lnd, stress_ice, ffmm_wat, ffmm_lnd, ffmm_ice, ffhh_wat, ffhh_lnd, ffhh_ice, uustar_wat, uustar_lnd, uustar_ice, & + fm10_wat, fm10_lnd, fm10_ice, fh2_wat, fh2_lnd, fh2_ice, tsurf_wat, tsurf_lnd, tsurf_ice, cmm_wat, cmm_lnd, cmm_ice, & + chh_wat, chh_lnd, chh_ice, gflx_wat, gflx_lnd, gflx_ice, ep1d_wat, ep1d_lnd, ep1d_ice, weasd_wat, weasd_lnd, weasd_ice, & + snowd_wat, snowd_lnd, snowd_ice,tprcp_wat, tprcp_lnd, tprcp_ice, evap_wat, evap_lnd, evap_ice, hflx_wat, hflx_lnd, & + hflx_ice, qss_wat, qss_lnd, qss_ice, tsfc_wat, tsfc_lnd, tsfc_ice real(kind=kind_phys), dimension(im), intent(inout) :: zorl, zorlo, zorll, cd, cdq, rb, stress, ffmm, ffhh, uustar, fm10, & fh2, tsurf, cmm, chh, gflx, ep1d, weasd, snowd, tprcp, evap, hflx, qss, tsfc, tsfco, tsfcl, tisfc @@ -315,11 +315,14 @@ subroutine GFS_surface_composites_post_run ( real(kind=kind_phys), dimension(im), intent(in ) :: tice ! interstitial sea ice temperature real(kind=kind_phys), dimension(im), intent(inout) :: hice, cice + real(kind=kind_phys), dimension(im, kice), intent(in ) :: tiice + real(kind=kind_phys), dimension(im, km), intent(inout) :: stc + character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg ! Local variables - integer :: i + integer :: i, k real(kind=kind_phys) :: txl, txi, txo, tem ! Initialize CCPP error handling variables @@ -337,27 +340,27 @@ subroutine GFS_surface_composites_post_run ( txi = cice(i)*(one - txl) ! txi = ice fraction wrt whole cell txo = max(zero, one - txl - txi) - zorl(i) = txl*zorl_lnd(i) + txi*zorl_ice(i) + txo*zorl_ocn(i) - cd(i) = txl*cd_lnd(i) + txi*cd_ice(i) + txo*cd_ocn(i) - cdq(i) = txl*cdq_lnd(i) + txi*cdq_ice(i) + txo*cdq_ocn(i) - rb(i) = txl*rb_lnd(i) + txi*rb_ice(i) + txo*rb_ocn(i) - stress(i) = txl*stress_lnd(i) + txi*stress_ice(i) + txo*stress_ocn(i) - ffmm(i) = txl*ffmm_lnd(i) + txi*ffmm_ice(i) + txo*ffmm_ocn(i) - ffhh(i) = txl*ffhh_lnd(i) + txi*ffhh_ice(i) + txo*ffhh_ocn(i) - uustar(i) = txl*uustar_lnd(i) + txi*uustar_ice(i) + txo*uustar_ocn(i) - fm10(i) = txl*fm10_lnd(i) + txi*fm10_ice(i) + txo*fm10_ocn(i) - fh2(i) = txl*fh2_lnd(i) + txi*fh2_ice(i) + txo*fh2_ocn(i) - !tsurf(i) = txl*tsurf_lnd(i) + txi*tice(i) + txo*tsurf_ocn(i) - !tsurf(i) = txl*tsurf_lnd(i) + txi*tsurf_ice(i) + txo*tsurf_ocn(i) ! not used again! Moorthi - cmm(i) = txl*cmm_lnd(i) + txi*cmm_ice(i) + txo*cmm_ocn(i) - chh(i) = txl*chh_lnd(i) + txi*chh_ice(i) + txo*chh_ocn(i) - !gflx(i) = txl*gflx_lnd(i) + txi*gflx_ice(i) + txo*gflx_ocn(i) - ep1d(i) = txl*ep1d_lnd(i) + txi*ep1d_ice(i) + txo*ep1d_ocn(i) - !weasd(i) = txl*weasd_lnd(i) + txi*weasd_ice(i) + txo*weasd_ocn(i) - !snowd(i) = txl*snowd_lnd(i) + txi*snowd_ice(i) + txo*snowd_ocn(i) + zorl(i) = txl*zorl_lnd(i) + txi*zorl_ice(i) + txo*zorl_wat(i) + cd(i) = txl*cd_lnd(i) + txi*cd_ice(i) + txo*cd_wat(i) + cdq(i) = txl*cdq_lnd(i) + txi*cdq_ice(i) + txo*cdq_wat(i) + rb(i) = txl*rb_lnd(i) + txi*rb_ice(i) + txo*rb_wat(i) + stress(i) = txl*stress_lnd(i) + txi*stress_ice(i) + txo*stress_wat(i) + ffmm(i) = txl*ffmm_lnd(i) + txi*ffmm_ice(i) + txo*ffmm_wat(i) + ffhh(i) = txl*ffhh_lnd(i) + txi*ffhh_ice(i) + txo*ffhh_wat(i) + uustar(i) = txl*uustar_lnd(i) + txi*uustar_ice(i) + txo*uustar_wat(i) + fm10(i) = txl*fm10_lnd(i) + txi*fm10_ice(i) + txo*fm10_wat(i) + fh2(i) = txl*fh2_lnd(i) + txi*fh2_ice(i) + txo*fh2_wat(i) + !tsurf(i) = txl*tsurf_lnd(i) + txi*tice(i) + txo*tsurf_wat(i) + !tsurf(i) = txl*tsurf_lnd(i) + txi*tsurf_ice(i) + txo*tsurf_wat(i) ! not used again! Moorthi + cmm(i) = txl*cmm_lnd(i) + txi*cmm_ice(i) + txo*cmm_wat(i) + chh(i) = txl*chh_lnd(i) + txi*chh_ice(i) + txo*chh_wat(i) + !gflx(i) = txl*gflx_lnd(i) + txi*gflx_ice(i) + txo*gflx_wat(i) + ep1d(i) = txl*ep1d_lnd(i) + txi*ep1d_ice(i) + txo*ep1d_wat(i) + !weasd(i) = txl*weasd_lnd(i) + txi*weasd_ice(i) + txo*weasd_wat(i) + !snowd(i) = txl*snowd_lnd(i) + txi*snowd_ice(i) + txo*snowd_wat(i) weasd(i) = txl*weasd_lnd(i) + txi*weasd_ice(i) snowd(i) = txl*snowd_lnd(i) + txi*snowd_ice(i) - !tprcp(i) = txl*tprcp_lnd(i) + txi*tprcp_ice(i) + txo*tprcp_ocn(i) + !tprcp(i) = txl*tprcp_lnd(i) + txi*tprcp_ice(i) + txo*tprcp_wat(i) if (.not. flag_cice(i) .and. islmsk(i) == 2) then tem = one - txl @@ -366,24 +369,24 @@ subroutine GFS_surface_composites_post_run ( qss(i) = txl*qss_lnd(i) + tem*qss_ice(i) gflx(i) = txl*gflx_lnd(i) + tem*gflx_ice(i) else - evap(i) = txl*evap_lnd(i) + txi*evap_ice(i) + txo*evap_ocn(i) - hflx(i) = txl*hflx_lnd(i) + txi*hflx_ice(i) + txo*hflx_ocn(i) - qss(i) = txl*qss_lnd(i) + txi*qss_ice(i) + txo*qss_ocn(i) - gflx(i) = txl*gflx_lnd(i) + txi*gflx_ice(i) + txo*gflx_ocn(i) + evap(i) = txl*evap_lnd(i) + txi*evap_ice(i) + txo*evap_wat(i) + hflx(i) = txl*hflx_lnd(i) + txi*hflx_ice(i) + txo*hflx_wat(i) + qss(i) = txl*qss_lnd(i) + txi*qss_ice(i) + txo*qss_wat(i) + gflx(i) = txl*gflx_lnd(i) + txi*gflx_ice(i) + txo*gflx_wat(i) endif - tsfc(i) = txl*tsfc_lnd(i) + txi*tice(i) + txo*tsfc_ocn(i) + tsfc(i) = txl*tsfc_lnd(i) + txi*tice(i) + txo*tsfc_wat(i) zorll(i) = zorl_lnd(i) - zorlo(i) = zorl_ocn(i) + zorlo(i) = zorl_wat(i) if (dry(i)) tsfcl(i) = tsfc_lnd(i) ! over land - if (wet(i)) tsfco(i) = tsfc_ocn(i) ! over lake or ocean when uncoupled + if (wet(i)) tsfco(i) = tsfc_wat(i) ! over lake or ocean when uncoupled ! for coupled model ocean will replace this ! if (icy(i)) tisfc(i) = tsfc_ice(i) ! over ice when uncoupled ! if (icy(i)) tisfc(i) = tice(i) ! over ice when uncoupled ! if (wet(i) .and. .not. cplflx) then -! tsfco(i) = tsfc_ocn(i) ! over lake or ocean when uncoupled +! tsfco(i) = tsfc_wat(i) ! over lake or ocean when uncoupled ! tisfc(i) = tsfc_ice(i) ! over ice when uncoupled ! endif @@ -429,29 +432,30 @@ subroutine GFS_surface_composites_post_run ( !cice(i) = zero !tisfc(i) = tsfc(i) elseif (islmsk(i) == 0) then - zorl(i) = zorl_ocn(i) - cd(i) = cd_ocn(i) - cdq(i) = cdq_ocn(i) - rb(i) = rb_ocn(i) - stress(i) = stress_ocn(i) - ffmm(i) = ffmm_ocn(i) - ffhh(i) = ffhh_ocn(i) - uustar(i) = uustar_ocn(i) - fm10(i) = fm10_ocn(i) - fh2(i) = fh2_ocn(i) - !tsurf(i) = tsurf_ocn(i) - tsfco(i) = tsfc_ocn(i) ! over lake (and ocean when uncoupled) - cmm(i) = cmm_ocn(i) - chh(i) = chh_ocn(i) - gflx(i) = gflx_ocn(i) - ep1d(i) = ep1d_ocn(i) - weasd(i) = weasd_ocn(i) - snowd(i) = snowd_ocn(i) - !tprcp(i) = tprcp_ocn(i) - evap(i) = evap_ocn(i) - hflx(i) = hflx_ocn(i) - qss(i) = qss_ocn(i) - tsfc(i) = tsfc_ocn(i) + zorl(i) = zorl_wat(i) + cd(i) = cd_wat(i) + cdq(i) = cdq_wat(i) + rb(i) = rb_wat(i) + stress(i) = stress_wat(i) + ffmm(i) = ffmm_wat(i) + ffhh(i) = ffhh_wat(i) + uustar(i) = uustar_wat(i) + fm10(i) = fm10_wat(i) + fh2(i) = fh2_wat(i) + !tsurf(i) = tsurf_wat(i) + tsfco(i) = tsfc_wat(i) ! over lake (and ocean when uncoupled) + if( cplflx ) tsfcl(i) = tsfc_wat(i) ! for restart repro comparisons + cmm(i) = cmm_wat(i) + chh(i) = chh_wat(i) + gflx(i) = gflx_wat(i) + ep1d(i) = ep1d_wat(i) + weasd(i) = weasd_wat(i) + snowd(i) = snowd_wat(i) + !tprcp(i) = tprcp_wat(i) + evap(i) = evap_wat(i) + hflx(i) = hflx_wat(i) + qss(i) = qss_wat(i) + tsfc(i) = tsfc_wat(i) !hice(i) = zero !cice(i) = zero !tisfc(i) = tsfc(i) @@ -460,7 +464,7 @@ subroutine GFS_surface_composites_post_run ( cd(i) = cd_ice(i) cdq(i) = cdq_ice(i) rb(i) = rb_ice(i) - stress(i) = cice(i)*stress_ice(i) + (one-cice(i))*stress_ocn(i) + stress(i) = cice(i)*stress_ice(i) + (one-cice(i))*stress_wat(i) ffmm(i) = ffmm_ice(i) ffhh(i) = ffhh_ice(i) uustar(i) = uustar_ice(i) @@ -476,23 +480,27 @@ subroutine GFS_surface_composites_post_run ( ep1d(i) = ep1d_ice(i) weasd(i) = weasd_ice(i) snowd(i) = snowd_ice(i) - !tprcp(i) = cice(i)*tprcp_ice(i) + (one-cice(i))*tprcp_ocn(i) + !tprcp(i) = cice(i)*tprcp_ice(i) + (one-cice(i))*tprcp_wat(i) qss(i) = qss_ice(i) evap(i) = evap_ice(i) hflx(i) = hflx_ice(i) qss(i) = qss_ice(i) tsfc(i) = tsfc_ice(i) + do k=1,kice ! store tiice in stc to reduce output in the nonfrac grid case + stc(i,k)=tiice(i,k) + end do + if( cplflx ) tsfcl(i) = tsfc_ice(i) endif zorll(i) = zorl_lnd(i) - zorlo(i) = zorl_ocn(i) + zorlo(i) = zorl_wat(i) if (flag_cice(i) .and. wet(i)) then ! this was already done for lake ice in sfc_sice txi = cice(i) txo = one - txi - evap(i) = txi * evap_ice(i) + txo * evap_ocn(i) - hflx(i) = txi * hflx_ice(i) + txo * hflx_ocn(i) - tsfc(i) = txi * tsfc_ice(i) + txo * tsfc_ocn(i) + evap(i) = txi * evap_ice(i) + txo * evap_wat(i) + hflx(i) = txi * hflx_ice(i) + txo * hflx_wat(i) + tsfc(i) = txi * tsfc_ice(i) + txo * tsfc_wat(i) else if (islmsk(i) == 2) then tisfc(i) = tice(i) diff --git a/physics/GFS_surface_composites.meta b/physics/GFS_surface_composites.meta index 832d9227e..31ca88d3d 100644 --- a/physics/GFS_surface_composites.meta +++ b/physics/GFS_surface_composites.meta @@ -162,7 +162,7 @@ kind = kind_phys intent = inout optional = F -[zorl_ocn] +[zorl_wat] standard_name = surface_roughness_length_over_ocean_interstitial long_name = surface roughness length over ocean (temporary use as interstitial) units = cm @@ -198,7 +198,7 @@ kind = kind_phys intent = in optional = F -[snowd_ocn] +[snowd_wat] standard_name = surface_snow_thickness_water_equivalent_over_ocean long_name = water equivalent snow depth over ocean units = mm @@ -234,7 +234,7 @@ kind = kind_phys intent = in optional = F -[tprcp_ocn] +[tprcp_wat] standard_name = nonnegative_lwe_thickness_of_precipitation_amount_on_dynamics_timestep_over_ocean long_name = total precipitation amount in each time step over ocean units = m @@ -297,7 +297,7 @@ kind = kind_phys intent = in optional = F -[weasd_ocn] +[weasd_wat] standard_name = water_equivalent_accumulated_snow_depth_over_ocean long_name = water equiv of acc snow depth over ocean units = mm @@ -360,7 +360,7 @@ kind = kind_phys intent = inout optional = F -[tsfc_ocn] +[tsfc_wat] standard_name = surface_skin_temperature_over_ocean_interstitial long_name = surface skin temperature over ocean (temporary use as interstitial) units = K @@ -414,7 +414,7 @@ kind = kind_phys intent = inout optional = F -[tsurf_ocn] +[tsurf_wat] standard_name = surface_skin_temperature_after_iteration_over_ocean long_name = surface skin temperature after iteration over ocean units = K @@ -476,7 +476,7 @@ kind = kind_phys intent = in optional = F -[semis_ocn] +[semis_wat] standard_name = surface_longwave_emissivity_over_ocean_interstitial long_name = surface lw emissivity in fraction over ocean (temporary use as interstitial) units = frac @@ -575,7 +575,7 @@ type = logical intent = in optional = F -[semis_ocn] +[semis_wat] standard_name = surface_longwave_emissivity_over_ocean_interstitial long_name = surface lw emissivity in fraction over ocean (temporary use as interstitial) units = frac @@ -629,7 +629,7 @@ kind = kind_phys intent = inout optional = F -[gabsbdlw_ocn] +[gabsbdlw_wat] standard_name = surface_downwelling_longwave_flux_absorbed_by_ground_over_ocean long_name = total sky surface downward longwave flux absorbed by the ground over ocean units = W m-2 @@ -695,6 +695,22 @@ type = integer intent = in optional = F +[kice] + standard_name = ice_vertical_dimension + long_name = vertical loop extent for ice levels, start at 1 + units = count + dimensions = () + type = integer + intent = in + optional = F +[km] + standard_name = soil_vertical_dimension + long_name = soil vertical layer dimension + units = count + dimensions = () + type = integer + intent = in + optional = F [cplflx] standard_name = flag_for_flux_coupling long_name = flag controlling cplflx collection (default off) @@ -813,7 +829,7 @@ kind = kind_phys intent = inout optional = F -[zorl_ocn] +[zorl_wat] standard_name = surface_roughness_length_over_ocean_interstitial long_name = surface roughness length over ocean (temporary use as interstitial) units = cm @@ -849,7 +865,7 @@ kind = kind_phys intent = inout optional = F -[cd_ocn] +[cd_wat] standard_name = surface_drag_coefficient_for_momentum_in_air_over_ocean long_name = surface exchange coeff for momentum over ocean units = none @@ -885,7 +901,7 @@ kind = kind_phys intent = inout optional = F -[cdq_ocn] +[cdq_wat] standard_name = surface_drag_coefficient_for_heat_and_moisture_in_air_over_ocean long_name = surface exchange coeff heat & moisture over ocean units = none @@ -921,7 +937,7 @@ kind = kind_phys intent = inout optional = F -[rb_ocn] +[rb_wat] standard_name = bulk_richardson_number_at_lowest_model_level_over_ocean long_name = bulk Richardson number at the surface over ocean units = none @@ -957,7 +973,7 @@ kind = kind_phys intent = inout optional = F -[stress_ocn] +[stress_wat] standard_name = surface_wind_stress_over_ocean long_name = surface wind stress over ocean units = m2 s-2 @@ -993,7 +1009,7 @@ kind = kind_phys intent = inout optional = F -[ffmm_ocn] +[ffmm_wat] standard_name = Monin_Obukhov_similarity_function_for_momentum_over_ocean long_name = Monin-Obukhov similarity function for momentum over ocean units = none @@ -1029,7 +1045,7 @@ kind = kind_phys intent = inout optional = F -[ffhh_ocn] +[ffhh_wat] standard_name = Monin_Obukhov_similarity_function_for_heat_over_ocean long_name = Monin-Obukhov similarity function for heat over ocean units = none @@ -1065,7 +1081,7 @@ kind = kind_phys intent = inout optional = F -[uustar_ocn] +[uustar_wat] standard_name = surface_friction_velocity_over_ocean long_name = surface friction velocity over ocean units = m s-1 @@ -1101,7 +1117,7 @@ kind = kind_phys intent = inout optional = F -[fm10_ocn] +[fm10_wat] standard_name = Monin_Obukhov_similarity_function_for_momentum_at_10m_over_ocean long_name = Monin-Obukhov similarity parameter for momentum at 10m over ocean units = none @@ -1137,7 +1153,7 @@ kind = kind_phys intent = inout optional = F -[fh2_ocn] +[fh2_wat] standard_name = Monin_Obukhov_similarity_function_for_heat_at_2m_over_ocean long_name = Monin-Obukhov similarity parameter for heat at 2m over ocean units = none @@ -1173,7 +1189,7 @@ kind = kind_phys intent = inout optional = F -[tsurf_ocn] +[tsurf_wat] standard_name = surface_skin_temperature_after_iteration_over_ocean long_name = surface skin temperature after iteration over ocean units = K @@ -1209,7 +1225,7 @@ kind = kind_phys intent = inout optional = F -[cmm_ocn] +[cmm_wat] standard_name = surface_drag_wind_speed_for_momentum_in_air_over_ocean long_name = momentum exchange coefficient over ocean units = m s-1 @@ -1245,7 +1261,7 @@ kind = kind_phys intent = inout optional = F -[chh_ocn] +[chh_wat] standard_name = surface_drag_mass_flux_for_heat_and_moisture_in_air_over_ocean long_name = thermal exchange coefficient over ocean units = kg m-2 s-1 @@ -1281,7 +1297,7 @@ kind = kind_phys intent = inout optional = F -[gflx_ocn] +[gflx_wat] standard_name = upward_heat_flux_in_soil_over_ocean long_name = soil heat flux over ocean units = W m-2 @@ -1317,7 +1333,7 @@ kind = kind_phys intent = inout optional = F -[ep1d_ocn] +[ep1d_wat] standard_name = surface_upward_potential_latent_heat_flux_over_ocean long_name = surface upward potential latent heat flux over ocean units = W m-2 @@ -1353,7 +1369,7 @@ kind = kind_phys intent = inout optional = F -[weasd_ocn] +[weasd_wat] standard_name = water_equivalent_accumulated_snow_depth_over_ocean long_name = water equiv of acc snow depth over ocean units = mm @@ -1389,7 +1405,7 @@ kind = kind_phys intent = inout optional = F -[snowd_ocn] +[snowd_wat] standard_name = surface_snow_thickness_water_equivalent_over_ocean long_name = water equivalent snow depth over ocean units = mm @@ -1425,7 +1441,7 @@ kind = kind_phys intent = inout optional = F -[tprcp_ocn] +[tprcp_wat] standard_name = nonnegative_lwe_thickness_of_precipitation_amount_on_dynamics_timestep_over_ocean long_name = total precipitation amount in each time step over ocean units = m @@ -1461,7 +1477,7 @@ kind = kind_phys intent = inout optional = F -[evap_ocn] +[evap_wat] standard_name = kinematic_surface_upward_latent_heat_flux_over_ocean long_name = kinematic surface upward latent heat flux over ocean units = kg kg-1 m s-1 @@ -1497,7 +1513,7 @@ kind = kind_phys intent = inout optional = F -[hflx_ocn] +[hflx_wat] standard_name = kinematic_surface_upward_sensible_heat_flux_over_ocean long_name = kinematic surface upward sensible heat flux over ocean units = K m s-1 @@ -1533,7 +1549,7 @@ kind = kind_phys intent = inout optional = F -[qss_ocn] +[qss_wat] standard_name = surface_specific_humidity_over_ocean long_name = surface air saturation specific humidity over ocean units = kg kg-1 @@ -1587,7 +1603,7 @@ kind = kind_phys intent = inout optional = F -[tsfc_ocn] +[tsfc_wat] standard_name = surface_skin_temperature_over_ocean_interstitial long_name = surface skin temperature over ocean (temporary use as interstitial) units = K @@ -1650,6 +1666,24 @@ kind = kind_phys intent = inout optional = F +[tiice] + standard_name = internal_ice_temperature + long_name = sea ice internal temperature + units = K + dimensions = (horizontal_dimension,ice_vertical_dimension) + type = real + kind = kind_phys + intent = inout + optional = F +[stc] + standard_name = soil_temperature + long_name = soil temperature + units = K + dimensions = (horizontal_dimension,soil_vertical_dimension) + type = real + kind = kind_phys + intent = inout + optional = F [errmsg] standard_name = ccpp_error_message long_name = error message for error handling in CCPP diff --git a/physics/GFS_surface_generic.F90 b/physics/GFS_surface_generic.F90 index ac366ae54..904e94dbc 100644 --- a/physics/GFS_surface_generic.F90 +++ b/physics/GFS_surface_generic.F90 @@ -27,7 +27,7 @@ end subroutine GFS_surface_generic_pre_finalize !! subroutine GFS_surface_generic_pre_run (im, levs, vfrac, islmsk, isot, ivegsrc, stype, vtype, slope, & prsik_1, prslk_1, tsfc, phil, con_g, & - sigmaf, soiltyp, vegtype, slopetyp, work3, tsurf, zlvl, do_sppt, dtdtr, & + sigmaf, soiltyp, vegtype, slopetyp, work3, tsurf, zlvl, do_sppt, ca_global,dtdtr,& drain_cpl, dsnow_cpl, rain_cpl, snow_cpl, do_sfcperts, nsfcpert, sfc_wts, & pertz0, pertzt, pertshc, pertlai, pertvegf, z01d, zt1d, bexp1d, xlai1d, vegf1d, & cplflx, flag_cice, islmsk_cice, slimskin_cpl, tisfc, tsfco, fice, hice, & @@ -51,7 +51,7 @@ subroutine GFS_surface_generic_pre_run (im, levs, vfrac, islmsk, isot, ivegsrc, real(kind=kind_phys), dimension(im), intent(inout) :: sigmaf, work3, tsurf, zlvl ! Stochastic physics / surface perturbations - logical, intent(in) :: do_sppt + logical, intent(in) :: do_sppt, ca_global real(kind=kind_phys), dimension(im,levs), intent(out) :: dtdtr real(kind=kind_phys), dimension(im), intent(out) :: drain_cpl real(kind=kind_phys), dimension(im), intent(out) :: dsnow_cpl @@ -102,7 +102,7 @@ subroutine GFS_surface_generic_pre_run (im, levs, vfrac, islmsk, isot, ivegsrc, errflg = 0 ! Set initial quantities for stochastic physics deltas - if (do_sppt) then + if (do_sppt .or. ca_global) then dtdtr = 0.0 endif @@ -215,8 +215,8 @@ end subroutine GFS_surface_generic_post_finalize !! \htmlinclude GFS_surface_generic_post_run.html !! subroutine GFS_surface_generic_post_run (im, cplflx, cplwav, lssav, icy, wet, dtf, ep1d, gflx, tgrs_1, qgrs_1, ugrs_1, vgrs_1,& - adjsfcdlw, adjsfcdsw, adjnirbmd, adjnirdfd, adjvisbmd, adjvisdfd, adjsfculw, adjsfculw_ocn, adjnirbmu, adjnirdfu, & - adjvisbmu, adjvisdfu,t2m, q2m, u10m, v10m, tsfc, tsfc_ocn, pgr, xcosz, evbs, evcw, trans, sbsno, snowc, snohf, & + adjsfcdlw, adjsfcdsw, adjnirbmd, adjnirdfd, adjvisbmd, adjvisdfd, adjsfculw, adjsfculw_wat, adjnirbmu, adjnirdfu, & + adjvisbmu, adjvisdfu,t2m, q2m, u10m, v10m, tsfc, tsfc_wat, pgr, xcosz, evbs, evcw, trans, sbsno, snowc, snohf, & epi, gfluxi, t1, q1, u1, v1, dlwsfci_cpl, dswsfci_cpl, dlwsfc_cpl, dswsfc_cpl, dnirbmi_cpl, dnirdfi_cpl, dvisbmi_cpl, & dvisdfi_cpl, dnirbm_cpl, dnirdf_cpl, dvisbm_cpl, dvisdf_cpl, nlwsfci_cpl, nlwsfc_cpl, t2mi_cpl, q2mi_cpl, u10mi_cpl, & v10mi_cpl, tsfci_cpl, psurfi_cpl, nnirbmi_cpl, nnirdfi_cpl, nvisbmi_cpl, nvisdfi_cpl, nswsfci_cpl, nswsfc_cpl, nnirbm_cpl, & @@ -231,8 +231,8 @@ subroutine GFS_surface_generic_post_run (im, cplflx, cplwav, lssav, icy, wet, dt real(kind=kind_phys), intent(in) :: dtf real(kind=kind_phys), dimension(im), intent(in) :: ep1d, gflx, tgrs_1, qgrs_1, ugrs_1, vgrs_1, adjsfcdlw, adjsfcdsw, & - adjnirbmd, adjnirdfd, adjvisbmd, adjvisdfd, adjsfculw, adjsfculw_ocn, adjnirbmu, adjnirdfu, adjvisbmu, adjvisdfu, & - t2m, q2m, u10m, v10m, tsfc, tsfc_ocn, pgr, xcosz, evbs, evcw, trans, sbsno, snowc, snohf + adjnirbmd, adjnirdfd, adjvisbmd, adjvisdfd, adjsfculw, adjsfculw_wat, adjnirbmu, adjnirdfu, adjvisbmu, adjvisdfu, & + t2m, q2m, u10m, v10m, tsfc, tsfc_wat, pgr, xcosz, evbs, evcw, trans, sbsno, snowc, snohf real(kind=kind_phys), dimension(im), intent(inout) :: epi, gfluxi, t1, q1, u1, v1, dlwsfci_cpl, dswsfci_cpl, dlwsfc_cpl, & dswsfc_cpl, dnirbmi_cpl, dnirdfi_cpl, dvisbmi_cpl, dvisdfi_cpl, dnirbm_cpl, dnirdf_cpl, dvisbm_cpl, dvisdf_cpl, & @@ -287,13 +287,13 @@ subroutine GFS_surface_generic_post_run (im, cplflx, cplwav, lssav, icy, wet, dt dvisdf_cpl (i) = dvisdf_cpl(i) + adjvisdfd(i)*dtf nlwsfci_cpl (i) = adjsfcdlw(i) - adjsfculw(i) if (wet(i)) then - nlwsfci_cpl(i) = adjsfcdlw(i) - adjsfculw_ocn(i) + nlwsfci_cpl(i) = adjsfcdlw(i) - adjsfculw_wat(i) endif nlwsfc_cpl (i) = nlwsfc_cpl(i) + nlwsfci_cpl(i)*dtf t2mi_cpl (i) = t2m(i) q2mi_cpl (i) = q2m(i) tsfci_cpl (i) = tsfc(i) -! tsfci_cpl (i) = tsfc_ocn(i) +! tsfci_cpl (i) = tsfc_wat(i) psurfi_cpl (i) = pgr(i) enddo diff --git a/physics/GFS_surface_generic.meta b/physics/GFS_surface_generic.meta index 250f7a2bd..436e2dc55 100644 --- a/physics/GFS_surface_generic.meta +++ b/physics/GFS_surface_generic.meta @@ -190,6 +190,14 @@ type = logical intent = in optional = F +[ca_global] + standard_name = flag_for_global_cellular_automata + long_name = switch for global ca + units = flag + dimensions = () + type = logical + intent = in + optional = F [dtdtr] standard_name = tendency_of_air_temperature_due_to_radiative_heating_on_physics_time_step long_name = temp. change due to radiative heating per time step @@ -669,7 +677,7 @@ kind = kind_phys intent = in optional = F -[adjsfculw_ocn] +[adjsfculw_wat] standard_name = surface_upwelling_longwave_flux_over_ocean_interstitial long_name = surface upwelling longwave flux at current time over ocean (temporary use as interstitial) units = W m-2 @@ -759,7 +767,7 @@ kind = kind_phys intent = in optional = F -[tsfc_ocn] +[tsfc_wat] standard_name = surface_skin_temperature_over_ocean_interstitial long_name = surface skin temperature over ocean (temporary use as interstitial) units = K diff --git a/physics/cires_ugwp.F90 b/physics/cires_ugwp.F90 index e0abc58ff..07b235c72 100644 --- a/physics/cires_ugwp.F90 +++ b/physics/cires_ugwp.F90 @@ -6,8 +6,8 @@ !! "Unified": a) all GW effects due to both dissipation/breaking; b) identical GW solvers for all GW sources; c) ability to replace solvers. !! Unified Formalism: !! 1. GW Sources: Stochastic and physics based mechanisms for GW-excitations in the lower atmosphere, calibrated by the high-res analyses/forecasts, and observations (3 types of GW sources: orography, convection, fronts/jets). -!! 2. GW Propagation: Unified solver for “propagation, dissipation and breaking” excited from all type of GW sources. -!! 3. GW Effects: Unified representation of GW impacts on the ‘resolved’ flow for all sources (energy-balanced schemes for momentum, heat and mixing). +!! 2. GW Propagation: Unified solver for "propagation, dissipation and breaking" excited from all type of GW sources. +!! 3. GW Effects: Unified representation of GW impacts on the "resolved" flow for all sources (energy-balanced schemes for momentum, heat and mixing). !! https://www.weather.gov/media/sti/nggps/Presentations%202017/02%20NGGPS_VYUDIN_2017_.pdf module cires_ugwp @@ -145,8 +145,8 @@ end subroutine cires_ugwp_finalize !> \section arg_table_cires_ugwp_run Argument Table !! \htmlinclude cires_ugwp_run.html !! - -! subroutines original +!> \section gen_cires_ugwp CIRES UGWP Scheme General Algorithm +!! @{ subroutine cires_ugwp_run(do_ugwp, me, master, im, levs, ntrac, dtp, kdt, lonr, & oro, oro_uf, hprime, nmtvr, oc, theta, sigma, gamma, elvmax, clx, oa4, & do_tofd, ldiag_ugwp, cdmbgwd, xlat, xlat_d, sinlat, coslat, area, & @@ -366,5 +366,6 @@ subroutine cires_ugwp_run(do_ugwp, me, master, im, levs, ntrac, dtp, kdt, lonr gw_dudt = gw_dudt*(1.-pked) + ed_dudt*pked end subroutine cires_ugwp_run - +!! @} +!>@} end module cires_ugwp diff --git a/physics/dcyc2.f b/physics/dcyc2.f index c7a1ddd59..7f052cbf3 100644 --- a/physics/dcyc2.f +++ b/physics/dcyc2.f @@ -47,8 +47,8 @@ end subroutine dcyc2t3_finalize ! call dcyc2t3 ! ! inputs: ! ! ( solhr,slag,sdec,cdec,sinlat,coslat, ! -! xlon,coszen,tsfc_lnd,tsfc_ice,tsfc_ocn, ! -! tf,tsflw,sfcemis_lnd,sfcemis_ice,sfcemis_ocn, ! +! xlon,coszen,tsfc_lnd,tsfc_ice,tsfc_wat, ! +! tf,tsflw,sfcemis_lnd,sfcemis_ice,sfcemis_wat, ! ! sfcdsw,sfcnsw,sfcdlw,swh,swhc,hlw,hlwc, ! ! sfcnirbmu,sfcnirdfu,sfcvisbmu,sfcvisdfu, ! ! sfcnirbmd,sfcnirdfd,sfcvisbmd,sfcvisdfd, ! @@ -58,7 +58,7 @@ end subroutine dcyc2t3_finalize ! dtdt,dtdtc, ! ! outputs: ! ! adjsfcdsw,adjsfcnsw,adjsfcdlw, ! -! adjsfculw_lnd,adjsfculw_ice,adjsfculw_ocn,xmu,xcosz, ! +! adjsfculw_lnd,adjsfculw_ice,adjsfculw_wat,xmu,xcosz, ! ! adjnirbmu,adjnirdfu,adjvisbmu,adjvisdfu, ! ! adjdnnbmd,adjdnndfd,adjdnvbmd,adjdnvdfd) ! ! ! @@ -74,11 +74,11 @@ end subroutine dcyc2t3_finalize ! coszen (im) - real, avg of cosz over daytime sw call interval ! ! tsfc_lnd (im) - real, bottom surface temperature over land (k) ! ! tsfc_ice (im) - real, bottom surface temperature over ice (k) ! -! tsfc_ocn (im) - real, bottom surface temperature over ocean (k) ! +! tsfc_wat (im) - real, bottom surface temperature over ocean (k) ! ! tf (im) - real, surface air (layer 1) temperature (k) ! ! sfcemis_lnd(im) - real, surface emissivity (fraction) o. land (k) ! ! sfcemis_ice(im) - real, surface emissivity (fraction) o. ice (k) ! -! sfcemis_ocn(im) - real, surface emissivity (fraction) o. ocean (k)! +! sfcemis_wat(im) - real, surface emissivity (fraction) o. ocean (k)! ! tsflw (im) - real, sfc air (layer 1) temp in k saved in lw call ! ! sfcdsw (im) - real, total sky sfc downward sw flux ( w/m**2 ) ! ! sfcnsw (im) - real, total sky sfc net sw into ground (w/m**2) ! @@ -115,7 +115,7 @@ end subroutine dcyc2t3_finalize ! adjsfcdlw(im)- real, time step adjusted sfc dn lw flux (w/m**2) ! ! adjsfculw_lnd(im)- real, sfc upw. lw flux at current time (w/m**2)! ! adjsfculw_ice(im)- real, sfc upw. lw flux at current time (w/m**2)! -! adjsfculw_ocn(im)- real, sfc upw. lw flux at current time (w/m**2)! +! adjsfculw_wat(im)- real, sfc upw. lw flux at current time (w/m**2)! ! adjnirbmu(im)- real, t adj sfc nir-beam sw upward flux (w/m2) ! ! adjnirdfu(im)- real, t adj sfc nir-diff sw upward flux (w/m2) ! ! adjvisbmu(im)- real, t adj sfc uv+vis-beam sw upward flux (w/m2) ! @@ -179,8 +179,8 @@ end subroutine dcyc2t3_finalize subroutine dcyc2t3_run & ! --- inputs: & ( solhr,slag,sdec,cdec,sinlat,coslat, & - & xlon,coszen,tsfc_lnd,tsfc_ice,tsfc_ocn,tf,tsflw, & - & sfcemis_lnd, sfcemis_ice, sfcemis_ocn, & + & xlon,coszen,tsfc_lnd,tsfc_ice,tsfc_wat,tf,tsflw, & + & sfcemis_lnd, sfcemis_ice, sfcemis_wat, & & sfcdsw,sfcnsw,sfcdlw,swh,swhc,hlw,hlwc, & & sfcnirbmu,sfcnirdfu,sfcvisbmu,sfcvisdfu, & & sfcnirbmd,sfcnirdfd,sfcvisbmd,sfcvisdfd, & @@ -191,7 +191,7 @@ subroutine dcyc2t3_run & & dtdt,dtdtc, & ! --- outputs: & adjsfcdsw,adjsfcnsw,adjsfcdlw, & - & adjsfculw_lnd,adjsfculw_ice,adjsfculw_ocn,xmu,xcosz, & + & adjsfculw_lnd,adjsfculw_ice,adjsfculw_wat,xmu,xcosz, & & adjnirbmu,adjnirdfu,adjvisbmu,adjvisdfu, & & adjnirbmd,adjnirdfd,adjvisbmd,adjvisdfd, & & errmsg,errflg & @@ -225,8 +225,8 @@ subroutine dcyc2t3_run & & sfcdsw, sfcnsw real(kind=kind_phys), dimension(im), intent(in) :: & - & tsfc_lnd, tsfc_ice, tsfc_ocn, & - & sfcemis_lnd, sfcemis_ice, sfcemis_ocn + & tsfc_lnd, tsfc_ice, tsfc_wat, & + & sfcemis_lnd, sfcemis_ice, sfcemis_wat real(kind=kind_phys), dimension(im), intent(in) :: & & sfcnirbmu, sfcnirdfu, sfcvisbmu, sfcvisdfu, & @@ -246,7 +246,7 @@ subroutine dcyc2t3_run & & adjnirbmd, adjnirdfd, adjvisbmd, adjvisdfd real(kind=kind_phys), dimension(im), intent(out) :: & - & adjsfculw_lnd, adjsfculw_ice, adjsfculw_ocn + & adjsfculw_lnd, adjsfculw_ice, adjsfculw_wat character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg @@ -321,9 +321,9 @@ subroutine dcyc2t3_run & & + (one - sfcemis_ice(i)) * adjsfcdlw(i) endif if (wet(i)) then - tem2 = tsfc_ocn(i) * tsfc_ocn(i) - adjsfculw_ocn(i) = sfcemis_ocn(i) * con_sbc * tem2 * tem2 - & + (one - sfcemis_ocn(i)) * adjsfcdlw(i) + tem2 = tsfc_wat(i) * tsfc_wat(i) + adjsfculw_wat(i) = sfcemis_wat(i) * con_sbc * tem2 * tem2 + & + (one - sfcemis_wat(i)) * adjsfcdlw(i) endif ! if (lprnt .and. i == ipr) write(0,*)' in dcyc3: dry==',dry(i) ! &,' wet=',wet(i),' icy=',icy(i),' tsfc3=',tsfc3(i,:) diff --git a/physics/dcyc2.meta b/physics/dcyc2.meta index 244ebc6bd..53b702b64 100644 --- a/physics/dcyc2.meta +++ b/physics/dcyc2.meta @@ -92,7 +92,7 @@ kind = kind_phys intent = in optional = F -[tsfc_ocn] +[tsfc_wat] standard_name = surface_skin_temperature_over_ocean_interstitial long_name = surface skin temperature over ocean (temporary use as interstitial) units = K @@ -146,7 +146,7 @@ kind = kind_phys intent = in optional = F -[sfcemis_ocn] +[sfcemis_wat] standard_name = surface_longwave_emissivity_over_ocean_interstitial long_name = surface lw emissivity in fraction over ocean (temporary use as interstitial) units = frac @@ -419,7 +419,7 @@ kind = kind_phys intent = out optional = F -[adjsfculw_ocn] +[adjsfculw_wat] standard_name = surface_upwelling_longwave_flux_over_ocean_interstitial long_name = surface upwelling longwave flux at current time over ocean (temporary use as interstitial) units = W m-2 @@ -535,70 +535,3 @@ type = integer intent = out optional = F - -######################################################################## -[ccpp-arg-table] - name = dcyc2t3_post_init - type = scheme - -######################################################################## -[ccpp-arg-table] - name = dcyc2t3_post_finalize - type = scheme - -######################################################################## -[ccpp-arg-table] - name = dcyc2t3_post_run - type = scheme -[im] - standard_name = horizontal_loop_extent - long_name = horizontal loop extent - units = count - dimensions = () - type = integer - intent = in - optional = F -[adjsfcdsw] - standard_name = surface_downwelling_shortwave_flux - long_name = surface downwelling shortwave flux at current time - units = W m-2 - dimensions = (horizontal_dimension) - type = real - kind = kind_phys - intent = in - optional = F -[adjsfcnsw] - standard_name = surface_net_downwelling_shortwave_flux - long_name = surface net downwelling shortwave flux at current time - units = W m-2 - dimensions = (horizontal_dimension) - type = real - kind = kind_phys - intent = in - optional = F -[adjsfcusw] - standard_name = surface_upwelling_shortwave_flux - long_name = surface upwelling shortwave flux at current time - units = W m-2 - dimensions = (horizontal_dimension) - type = real - kind = kind_phys - intent = out - optional = F -[errmsg] - standard_name = ccpp_error_message - long_name = error message for error handling in CCPP - units = none - dimensions = () - type = character - kind = len=* - intent = out - optional = F -[errflg] - standard_name = ccpp_error_flag - long_name = error flag for error handling in CCPP - units = flag - dimensions = () - type = integer - intent = out - optional = F diff --git a/physics/docs/ccppv4_doxyfile b/physics/docs/ccppv4_doxyfile new file mode 100644 index 000000000..e80b27eb9 --- /dev/null +++ b/physics/docs/ccppv4_doxyfile @@ -0,0 +1,467 @@ +# Doxyfile 1.8.11 +DOXYFILE_ENCODING = UTF-8 +PROJECT_NAME = "CCPP Scientific Documentation" +PROJECT_NUMBER = "" +PROJECT_BRIEF = "v4.0" +PROJECT_LOGO = img/dtc_logo.png +OUTPUT_DIRECTORY = doc +CREATE_SUBDIRS = NO +ALLOW_UNICODE_NAMES = NO +OUTPUT_LANGUAGE = English +BRIEF_MEMBER_DESC = YES +REPEAT_BRIEF = NO +ABBREVIATE_BRIEF = +ALWAYS_DETAILED_SEC = NO +INLINE_INHERITED_MEMB = NO +FULL_PATH_NAMES = NO +STRIP_FROM_PATH = +STRIP_FROM_INC_PATH = +SHORT_NAMES = NO +JAVADOC_AUTOBRIEF = NO +QT_AUTOBRIEF = NO +MULTILINE_CPP_IS_BRIEF = NO +INHERIT_DOCS = YES +SEPARATE_MEMBER_PAGES = YES +TAB_SIZE = 4 +ALIASES = +TCL_SUBST = +OPTIMIZE_OUTPUT_FOR_C = NO +OPTIMIZE_OUTPUT_JAVA = NO +OPTIMIZE_FOR_FORTRAN = YES +OPTIMIZE_OUTPUT_VHDL = NO +EXTENSION_MAPPING = .f=FortranFree \ + .F=FortranFree \ + .F90=FortranFree \ + .f90=FortranFree +MARKDOWN_SUPPORT = YES +AUTOLINK_SUPPORT = YES +BUILTIN_STL_SUPPORT = NO +CPP_CLI_SUPPORT = NO +SIP_SUPPORT = NO +IDL_PROPERTY_SUPPORT = YES +DISTRIBUTE_GROUP_DOC = YES +GROUP_NESTED_COMPOUNDS = NO +SUBGROUPING = YES +INLINE_GROUPED_CLASSES = NO +INLINE_SIMPLE_STRUCTS = NO +TYPEDEF_HIDES_STRUCT = YES +LOOKUP_CACHE_SIZE = 0 +EXTRACT_ALL = YES +EXTRACT_PRIVATE = YES +EXTRACT_PACKAGE = YES +EXTRACT_STATIC = YES +EXTRACT_LOCAL_CLASSES = YES +EXTRACT_LOCAL_METHODS = YES +EXTRACT_ANON_NSPACES = YES +HIDE_UNDOC_MEMBERS = NO +HIDE_UNDOC_CLASSES = NO +HIDE_FRIEND_COMPOUNDS = NO +HIDE_IN_BODY_DOCS = NO +INTERNAL_DOCS = YES + +CASE_SENSE_NAMES = NO + +HIDE_SCOPE_NAMES = NO + +HIDE_COMPOUND_REFERENCE= NO + +SHOW_INCLUDE_FILES = NO + +SHOW_GROUPED_MEMB_INC = NO + +FORCE_LOCAL_INCLUDES = NO + +INLINE_INFO = YES + +SORT_MEMBER_DOCS = NO + +SORT_BRIEF_DOCS = NO +SORT_MEMBERS_CTORS_1ST = NO +SORT_GROUP_NAMES = NO +SORT_BY_SCOPE_NAME = NO +STRICT_PROTO_MATCHING = NO +GENERATE_TODOLIST = YES +GENERATE_TESTLIST = YES +GENERATE_BUGLIST = YES +GENERATE_DEPRECATEDLIST= YES +ENABLED_SECTIONS = YES +MAX_INITIALIZER_LINES = 30 +SHOW_USED_FILES = YES +SHOW_FILES = YES +SHOW_NAMESPACES = YES +FILE_VERSION_FILTER = +LAYOUT_FILE = ccpp_dox_layout.xml +CITE_BIB_FILES = library.bib +QUIET = NO +WARNINGS = YES +WARN_IF_UNDOCUMENTED = NO +WARN_IF_DOC_ERROR = YES +WARN_NO_PARAMDOC = NO +WARN_AS_ERROR = NO +WARN_FORMAT = +WARN_LOGFILE = +INPUT = pdftxt/mainpage.txt \ + pdftxt/all_shemes_list.txt \ + pdftxt/GFSv15p2_suite.txt \ + pdftxt/GFSv15p2_no_nsst_suite.txt \ + pdftxt/suite_FV3_GFS_v15p2.xml.txt \ + pdftxt/suite_FV3_GFS_v15p2_no_nsst.xml.txt \ + pdftxt/GFSv16beta_suite.txt \ + pdftxt/GFSv16beta_no_nsst_suite.txt \ + pdftxt/suite_FV3_GFS_v16beta.xml.txt \ + pdftxt/suite_FV3_GFS_v16beta_no_nsst.xml.txt \ + pdftxt/GSD_adv_suite.txt \ + pdftxt/CPT_adv_suite.txt \ + pdftxt/GFS_RRTMG.txt \ + pdftxt/GFS_SFCLYR.txt \ + pdftxt/GFS_NSST.txt \ + pdftxt/GFS_OCEAN.txt \ + pdftxt/GFS_NOAH.txt \ + pdftxt/GFS_SFCSICE.txt \ + pdftxt/GFS_HEDMF.txt \ + pdftxt/GFS_SATMEDMFVDIFQ.txt \ +## pdftxt/GFS_NoahMP.txt \ + pdftxt/GFS_UGWPv0.txt \ + pdftxt/GFS_GWDPS.txt \ + pdftxt/GFS_OZPHYS.txt \ + pdftxt/GFS_H2OPHYS.txt \ + pdftxt/GFS_RAYLEIGH.txt \ + pdftxt/GFS_SAMF.txt \ + pdftxt/GFS_SAMFdeep.txt \ + pdftxt/GFS_SAMFshal.txt \ + pdftxt/GFDL_cloud.txt \ + pdftxt/GFS_CALPRECIPTYPE.txt \ +### pdftxt/rad_cld.txt \ + pdftxt/CPT_CSAW.txt \ + pdftxt/CPT_MG3.txt \ + pdftxt/GSD_MYNN_EDMF.txt \ + pdftxt/GSD_CU_GF_deep.txt \ + pdftxt/GSD_RUCLSM.txt \ + pdftxt/GSD_THOMPSON.txt \ +### pdftxt/GFSphys_namelist.txt \ +### pdftxt/GFS_STOCHY_PHYS.txt \ + pdftxt/suite_input.nml.txt \ +### in-core MP + ../gfdl_fv_sat_adj.F90 \ +### time_vary + ../GFS_time_vary_pre.fv3.F90 \ + ../GFS_rad_time_vary.fv3.F90 \ + ../GFS_phys_time_vary.fv3.F90 \ + ../ozne_def.f \ + ../ozinterp.f90 \ + ../h2o_def.f \ + ../h2ointerp.f90 \ + ../aerclm_def.F \ + ../aerinterp.F90 \ + ../iccn_def.F \ + ../iccninterp.F90 \ + ../sfcsub.F \ + ../gcycle.F90 \ +### Radiation +### ../GFS_rrtmg_pre.F90 \ +### ../rrtmg_sw_pre.F90 \ + ../radsw_main.f \ +### ../rrtmg_sw_post.F90 \ +### ../rrtmg_lw_pre.F90 \ + ../radlw_main.f \ +### ../rrtmg_lw_post.F90 \ + ../radiation_aerosols.f \ + ../radiation_astronomy.f \ + ../radiation_clouds.f \ + ../radiation_gases.f \ + ../radiation_surface.f \ + ../radlw_param.f \ + ../radlw_datatb.f \ + ../radsw_param.f \ + ../radsw_datatb.f \ + ../dcyc2.f \ +### Land Surface + ../sfc_diff.f \ + ../sfc_nst.f \ + ../sfc_ocean.F \ + ../module_nst_model.f90 \ + ../module_nst_parameters.f90 \ + ../module_nst_water_prop.f90 \ + ../sfc_drv.f \ + ../sflx.f \ + ../namelist_soilveg.f \ + ../set_soilveg.f \ +### Sea Ice Surface + ../sfc_sice.f \ +### PBL + ../moninedmf.f \ + ../mfpbl.f \ + ../tridi.f \ +### satmedmf +## ../satmedmfvdif.F \ + ../satmedmfvdifq.F \ + ../mfpbltq.f \ + ../mfscuq.f \ + ../tridi.f \ +### Orographic Gravity Wave + ../GFS_GWD_generic.F90 \ + ../cires_ugwp.F90 \ + ../gwdps.f \ + ../ugwp_driver_v0.F \ + ../cires_ugwp_triggers.F90 \ + ../cires_ugwp_module.F90 \ + ../cires_ugwp_utils.F90 \ + ../cires_ugwp_solvers.F90 \ +### ../cires_ugwp_post.F90 \ +### ../cires_ugwp_initialize.F90 \ + ../cires_vert_wmsdis.F90 \ + ../cires_vert_orodis.F90 \ + ../cires_vert_lsatdis.F90 \ +### Rayleigh Dampling + ../rayleigh_damp.f \ +### Prognostic Ozone + ../ozphys_2015.f \ +### ../ozphys.f \ +### stratospheric h2o + ../h2ophys.f \ +### Deep Convection + ../samfdeepcnv.f \ +### Convective Gravity Wave +### ../gwdc.f \ +### Shallow Convection + ../samfshalcnv.f \ + ../cnvc90.f \ +### Microphysics +### ../gscond.f \ +### ../precpd.f \ + ../module_bfmicrophysics.f \ +### GFDL cloud MP + ../gfdl_cloud_microphys.F90 \ + ../module_gfdl_cloud_microphys.F90 \ +### + ../GFS_MP_generic.F90 \ + ../calpreciptype.f90 \ +### stochy + ../GFS_stochastics.F90 \ +### ../surface_perturbation.F90 \ +### ../../stochastic_physics/stochastic_physics.F90 \ +### CPT + ../m_micro.F90 \ +### ../micro_mg2_0.F90 \ + ../micro_mg3_0.F90 \ + ../micro_mg_utils.F90 \ + ../cldmacro.F \ + ../aer_cloud.F \ + ../cldwat2m_micro.F \ + ../wv_saturation.F \ + ../cs_conv_aw_adj.F90 \ + ../cs_conv.F90 \ +### GSD + ../cu_gf_driver.F90 \ + ../cu_gf_deep.F90 \ + ../cu_gf_sh.F90 \ + ../module_MYNNrad_pre.F90 \ + ../module_MYNNrad_post.F90 \ + ../module_MYNNPBL_wrapper.F90 \ + ../module_bl_mynn.F90 \ +### ../module_MYNNSFC_wrapper.F90 \ +### ../module_sf_mynn.F90 \ + ../sfc_drv_ruc.F90 \ + ../module_sf_ruclsm.F90 \ + ../namelist_soilveg_ruc.F90 \ + ../set_soilveg_ruc.F90 \ + ../module_soil_pre.F90 \ + ../mp_thompson_pre.F90 \ + ../module_mp_thompson_make_number_concentrations.F90 \ + ../mp_thompson.F90 \ + ../module_mp_thompson.F90 \ + ../module_mp_radar.F90 \ + ../mp_thompson_post.F90 \ +### utils + ../funcphys.f90 \ + ../physparam.f \ + ../physcons.F90 \ + ../radcons.f90 \ + ../mersenne_twister.f +INPUT_ENCODING = UTF-8 +FILE_PATTERNS = *.f \ + *.F \ + *.F90 \ + *.f90 \ + *.nml \ + *.txt +RECURSIVE = YES +EXCLUDE = +EXCLUDE_SYMLINKS = NO +EXCLUDE_PATTERNS = +EXCLUDE_SYMBOLS = +EXAMPLE_PATH = ./ +EXAMPLE_PATTERNS = +EXAMPLE_RECURSIVE = NO +IMAGE_PATH = img +INPUT_FILTER = +FILTER_PATTERNS = +FILTER_SOURCE_FILES = NO +FILTER_SOURCE_PATTERNS = +USE_MDFILE_AS_MAINPAGE = +SOURCE_BROWSER = NO +INLINE_SOURCES = NO +STRIP_CODE_COMMENTS = YES +REFERENCED_BY_RELATION = YES +REFERENCES_RELATION = YES +REFERENCES_LINK_SOURCE = YES +SOURCE_TOOLTIPS = YES +USE_HTAGS = NO +VERBATIM_HEADERS = YES +#CLANG_ASSISTED_PARSING = NO +#CLANG_OPTIONS = +ALPHABETICAL_INDEX = NO +COLS_IN_ALPHA_INDEX = 5 +IGNORE_PREFIX = +GENERATE_HTML = YES +HTML_OUTPUT = html +HTML_FILE_EXTENSION = .html +HTML_HEADER = +HTML_FOOTER = +HTML_STYLESHEET = +HTML_EXTRA_STYLESHEET = ccpp_dox_extra_style.css +HTML_EXTRA_FILES = +HTML_COLORSTYLE_HUE = 220 +HTML_COLORSTYLE_SAT = 100 +HTML_COLORSTYLE_GAMMA = 80 +HTML_TIMESTAMP = NO +HTML_DYNAMIC_SECTIONS = NO +HTML_INDEX_NUM_ENTRIES = 100 +GENERATE_DOCSET = NO +DOCSET_FEEDNAME = "Doxygen generated docs" +DOCSET_BUNDLE_ID = org.doxygen.Project +DOCSET_PUBLISHER_ID = org.doxygen.Publisher +DOCSET_PUBLISHER_NAME = Publisher +GENERATE_HTMLHELP = NO +CHM_FILE = +HHC_LOCATION = +GENERATE_CHI = NO +CHM_INDEX_ENCODING = +BINARY_TOC = NO +TOC_EXPAND = NO +GENERATE_QHP = NO +QCH_FILE = +QHP_NAMESPACE = org.doxygen.Project +QHP_VIRTUAL_FOLDER = doc +QHP_CUST_FILTER_NAME = +QHP_CUST_FILTER_ATTRS = +QHP_SECT_FILTER_ATTRS = +QHG_LOCATION = +GENERATE_ECLIPSEHELP = NO +ECLIPSE_DOC_ID = org.doxygen.Project +DISABLE_INDEX = YES +GENERATE_TREEVIEW = YES +ENUM_VALUES_PER_LINE = 4 +TREEVIEW_WIDTH = 250 +EXT_LINKS_IN_WINDOW = NO +FORMULA_FONTSIZE = 10 +FORMULA_TRANSPARENT = YES +USE_MATHJAX = YES +MATHJAX_FORMAT = HTML-CSS +MATHJAX_RELPATH = https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.2 +MATHJAX_EXTENSIONS = +MATHJAX_CODEFILE = +SEARCHENGINE = YES +SERVER_BASED_SEARCH = NO +EXTERNAL_SEARCH = NO +SEARCHENGINE_URL = +SEARCHDATA_FILE = searchdata.xml +EXTERNAL_SEARCH_ID = +EXTRA_SEARCH_MAPPINGS = +GENERATE_LATEX = YES +LATEX_OUTPUT = latex +LATEX_CMD_NAME = latex +MAKEINDEX_CMD_NAME = makeindex +COMPACT_LATEX = YES +PAPER_TYPE = a4 +EXTRA_PACKAGES = amsmath +LATEX_HEADER = +LATEX_FOOTER = +LATEX_EXTRA_STYLESHEET = +LATEX_EXTRA_FILES = +PDF_HYPERLINKS = YES +USE_PDFLATEX = YES +LATEX_BATCHMODE = NO +LATEX_HIDE_INDICES = YES +LATEX_SOURCE_CODE = NO + +LATEX_BIB_STYLE = plainnat + +LATEX_TIMESTAMP = NO + +GENERATE_RTF = NO + +RTF_OUTPUT = rtf +COMPACT_RTF = NO +RTF_HYPERLINKS = NO +RTF_STYLESHEET_FILE = +RTF_EXTENSIONS_FILE = +RTF_SOURCE_CODE = NO +GENERATE_MAN = NO +MAN_OUTPUT = man +MAN_EXTENSION = .3 +MAN_SUBDIR = +MAN_LINKS = NO +GENERATE_XML = NO +XML_OUTPUT = xml +XML_PROGRAMLISTING = YES +GENERATE_DOCBOOK = NO +DOCBOOK_OUTPUT = docbook +DOCBOOK_PROGRAMLISTING = NO +GENERATE_AUTOGEN_DEF = NO +GENERATE_PERLMOD = NO +PERLMOD_LATEX = NO +PERLMOD_PRETTY = YES +PERLMOD_MAKEVAR_PREFIX = +ENABLE_PREPROCESSING = NO +MACRO_EXPANSION = NO +EXPAND_ONLY_PREDEF = NO +SEARCH_INCLUDES = YES +INCLUDE_PATH = +INCLUDE_FILE_PATTERNS = +PREDEFINED = CCPP \ + MULTI_GASES \ + 0 +EXPAND_AS_DEFINED = +SKIP_FUNCTION_MACROS = YES +TAGFILES = +GENERATE_TAGFILE = +ALLEXTERNALS = NO +EXTERNAL_GROUPS = YES +EXTERNAL_PAGES = YES +PERL_PATH = /usr/bin/perl +CLASS_DIAGRAMS = YES +MSCGEN_PATH = +DIA_PATH = +HIDE_UNDOC_RELATIONS = NO +HAVE_DOT = YES +DOT_NUM_THREADS = 0 +DOT_FONTNAME = Helvetica +DOT_FONTSIZE = 10 +DOT_FONTPATH = +CLASS_GRAPH = NO +COLLABORATION_GRAPH = NO +GROUP_GRAPHS = YES +UML_LOOK = YES +UML_LIMIT_NUM_FIELDS = 10 +TEMPLATE_RELATIONS = NO +INCLUDE_GRAPH = YES +INCLUDED_BY_GRAPH = NO +CALL_GRAPH = YES +CALLER_GRAPH = NO +GRAPHICAL_HIERARCHY = YES +DIRECTORY_GRAPH = YES +DOT_IMAGE_FORMAT = svg +INTERACTIVE_SVG = NO +DOT_PATH = +DOTFILE_DIRS = +MSCFILE_DIRS = +DIAFILE_DIRS = +PLANTUML_JAR_PATH = +PLANTUML_INCLUDE_PATH = +DOT_GRAPH_MAX_NODES = 200 +MAX_DOT_GRAPH_DEPTH = 0 +DOT_TRANSPARENT = NO +DOT_MULTI_TARGETS = YES +GENERATE_LEGEND = YES +DOT_CLEANUP = YES diff --git a/physics/docs/library.bib b/physics/docs/library.bib index 7384e08a0..dd2b2042e 100644 --- a/physics/docs/library.bib +++ b/physics/docs/library.bib @@ -1,7 +1,7 @@ %% This BibTeX bibliography file was created using BibDesk. -%% https://bibdesk.sourceforge.io/ +%% http://bibdesk.sourceforge.net/ -%% Created for Grant Firl at 2019-10-25 16:36:06 -0600 +%% Created for Man Zhang at 2020-03-02 13:10:25 -0700 %% Saved with string encoding Unicode (UTF-8) @@ -1859,12 +1859,12 @@ @article{zeng_and_dickinson_1998 @conference{zheng_et_al_2009, Address = {Omaha, Nebraska}, Author = {W. Zheng and H. Wei and J. Meng and M. Ek and K. Mitchell and J. Derber and X. Zeng and Z. Wang}, - Bdsk-File-1 = {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}, Date-Added = {2018-01-26 22:19:06 +0000}, Date-Modified = {2018-01-29 23:51:37 +0000}, Organization = {The 23rd Conference on Weather Analysis and Forecasting (WAF)/19th Conference on Numerical Weather Prediction(NWP)}, Title = {Improvement of land surface skin temperature in NCEP Operational NWP models and its impact on satellite Data Assimilation}, - Year = {2009}} + Year = {2009}, + Bdsk-File-1 = {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}} @article{chen_et_al_1997, Author = {F. Chen and Z. Janjic and K. Mitchell}, @@ -2016,11 +2016,11 @@ @url{Li_2015 Url = {http://cpo.noaa.gov/sites/cpo/MAPP/workshops/rtf_technical_ws/presentations/21_Xu_Li.pdf}, Bdsk-Url-1 = {http://cpo.noaa.gov/sites/cpo/MAPP/workshops/rtf_technical_ws/presentations/21_Xu_Li.pdf}} -@url{li_and_derber_2009, +@webpage{li_and_derber_2009, Author = {Xu Li and John Derber}, - Date-Modified = {2018-07-17 20:46:44 +0000}, + Date-Modified = {2020-02-24 17:06:35 +0000}, Title = {Near Sea Surface Temperatures (NSST) Analysis in NCEP GFS}, - Url = {https://www.jcsda.noaa.gov/documents/meetings/wkshp2008/4/JCSDA_2008_Li.pdf}, + Url = {http://data.jcsda.org/Workshops/6th-workshop-onDA/Session-4/JCSDA_2008_Li.pdf}, Bdsk-Url-1 = {https://www.jcsda.noaa.gov/documents/meetings/wkshp2008/4/JCSDA_2008_Li.pdf}} @article{Fairall_et_al_1996, @@ -2103,7 +2103,6 @@ @article{iacono_et_al_2008 @article{grant_2001, Abstract = {A closure for the fluxes of mass, heat, and moisture at cloud base in the cumulus-capped boundary layer is developed. The cloud-base mass flux is obtained from a simplifed turbulence kinetic energy (TKE) budget for the sub-cloud layer, in which cumulus convection is assumed to be associated with a transport of TKE from the sub-cloud layer to the cloud layer.The heat and moisture fluxes are obtained from a jump model based on the virtual-potential-temperature equation. A key part of this parametrization is the parametrization of the virtual-temperature flux at the top of the transition zone between the sub-cloud and cloud layers.It is argued that pressure fluctuations must be responsible for the transport of TKE from the cloud layer to the sub-cloud layer.}, Author = {A. L. M. Grant}, - Bdsk-File-1 = {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}, Date-Added = {2016-06-15 22:11:22 +0000}, Date-Modified = {2018-07-06 19:02:34 +0000}, Doi = {10.1002/qj.49712757209}, @@ -2117,13 +2116,13 @@ @article{grant_2001 Url = {http://dx.doi.org/10.1002/qj.49712757209}, Volume = {127}, Year = {2001}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1002/qj.49712757209}} @article{zhang_and_wu_2003, Abstract = {Abstract This study uses a 2D cloud-resolving model to investigate the vertical transport of horizontal momentum and to understand the role of a convection-generated perturbation pressure field in the momentum transport by convective systems during part of the Tropical Ocean and Global Atmosphere Coupled Ocean?Atmosphere Response Experiment (TOGA COARE) Intensive Observation Period. It shows that convective updrafts transport a significant amount of momentum vertically. This transport is downgradient in the easterly wind regime, but upgradient during a westerly wind burst. The differences in convective momentum transport between easterly and westerly wind regimes are examined. The perturbation pressure gradient accounts for an important part of the apparent momentum source. In general it is opposite in sign to the product of cloud mass flux and the vertical wind shear, with smaller magnitude. Examination of the dynamic forcing to the pressure field demonstrates that the linear forcing representing the interaction between the convective updrafts and the large-scale wind shear is the dominant term, while the nonlinear forcing is of secondary importance. Thus, parameterization schemes taking into account the linear interaction between the convective updrafts and the large-scale wind shear can capture the essential features of the perturbation pressure field. The parameterization scheme for momentum transport by Zhang and Cho is evaluated using the model simulation data. The parameterized pressure gradient force using the scheme is in excellent agreement with the simulated one. The parameterized apparent momentum source is also in good agreement with the model simulation. Other parameterization methods for the pressure gradient are also discussed.}, Annote = {doi: 10.1175/1520-0469(2003)060<1120:CMTAPP>2.0.CO;2}, Author = {Zhang, Guang J. and Wu, Xiaoqing}, - Bdsk-File-1 = {YnBsaXN0MDDSAQIDBFxyZWxhdGl2ZVBhdGhZYWxpYXNEYXRhXxBBLi4vLi4vQ2xvdWRTdGF0aW9uL2ZpcmxfbGlicmFyeS9maXJsX2xpYnJhcnlfZmlsZXMvWmhhbmcvMjAwMy5wZGZPEQHEAAAAAAHEAAIAAAxNYWNpbnRvc2ggSEQAAAAAAAAAAAAAAAAAAADR5yRSSCsAAAAqjuYIMjAwMy5wZGYAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAFrUP9K0L8MAAAAAAAAAAAACAAUAAAkgAAAAAAAAAAAAAAAAAAAABVpoYW5nAAAQAAgAANHneLIAAAARAAgAANK0kjMAAAABABgAKo7mAChslgAobIsAKGd7ABteBwACmFwAAgBbTWFjaW50b3NoIEhEOlVzZXJzOgBncmFudGY6AENsb3VkU3RhdGlvbjoAZmlybF9saWJyYXJ5OgBmaXJsX2xpYnJhcnlfZmlsZXM6AFpoYW5nOgAyMDAzLnBkZgAADgASAAgAMgAwADAAMwAuAHAAZABmAA8AGgAMAE0AYQBjAGkAbgB0AG8AcwBoACAASABEABIASFVzZXJzL2dyYW50Zi9DbG91ZFN0YXRpb24vZmlybF9saWJyYXJ5L2ZpcmxfbGlicmFyeV9maWxlcy9aaGFuZy8yMDAzLnBkZgATAAEvAAAVAAIADf//AAAACAANABoAJABoAAAAAAAAAgEAAAAAAAAABQAAAAAAAAAAAAAAAAAAAjA=}, Booktitle = {Journal of the Atmospheric Sciences}, Da = {2003/05/01}, Date-Added = {2016-06-14 23:39:50 +0000}, @@ -2142,13 +2141,13 @@ @article{zhang_and_wu_2003 Url = {http://dx.doi.org/10.1175/1520-0469(2003)060<1120:CMTAPP>2.0.CO;2}, Volume = {60}, Year = {2003}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1175/1520-0469(2003)060%3C1120:CMTAPP%3E2.0.CO;2}} @article{fritsch_and_chappell_1980, Abstract = {Abstract A parameterization formulation for incorporating the effects of midlatitude deep convection into mesoscale-numerical models is presented. The formulation is based on the hypothesis that the buoyant energy available to a parcel, in combination with a prescribed period of time for the convection to remove that energy, can be used to regulate the amount of convection in a mesoscale numerical model grid element. Individual clouds are represented as entraining moist updraft and downdraft plumes. The fraction of updraft condensate evaporated in moist downdrafts is determined from an empirical relationship between the vertical shear of the horizontal wind and precipitation efficiency. Vertical transports of horizontal momentum and warming by compensating subsidence are included in the parameterization. Since updraft and downdraft areas are sometimes a substantial fraction of mesoscale model grid-element areas, grid-point temperatures (adjusted for convection) are an area-weighted mean of updraft, downdraft and environmental temperatures.}, Annote = {doi: 10.1175/1520-0469(1980)037<1722:NPOCDM>2.0.CO;2}, Author = {Fritsch, J. M. and Chappell, C. F.}, - Bdsk-File-1 = {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}, Booktitle = {Journal of the Atmospheric Sciences}, Da = {1980/08/01}, Date = {1980/08/01}, @@ -2169,12 +2168,12 @@ @article{fritsch_and_chappell_1980 Volume = {37}, Year = {1980}, Year1 = {1980}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1175/1520-0469(1980)037%3C1722:NPOCDM%3E2.0.CO;2}} @article{bechtold_et_al_2008, Abstract = {Advances in simulating atmospheric variability with the ECMWF model are presented that stem from revisions of the convection and diffusion parametrizations. The revisions concern in particular the introduction of a variable convective adjustment time-scale, a convective entrainment rate proportional to the environmental relative humidity, as well as free tropospheric diffusion coefficients for heat and momentum based on Monin--Obukhov functional dependencies.The forecasting system is evaluated against analyses and observations using high-resolution medium-range deterministic and ensemble forecasts, monthly and seasonal integrations, and decadal integrations with coupled atmosphere-ocean models. The results show a significantly higher and more realistic level of model activity in terms of the amplitude of tropical and extratropical mesoscale, synoptic and planetary perturbations. Importantly, with the higher variability and reduced bias not only the probabilistic scores are improved, but also the midlatitude deterministic scores in the short and medium ranges. Furthermore, for the first time the model is able to represent a realistic spectrum of convectively coupled equatorial Kelvin and Rossby waves, and maintains a realistic amplitude of the Madden--Julian oscillation (MJO) during monthly forecasts. However, the propagation speed of the MJO is slower than observed. The higher tropical tropospheric wave activity also results in better stratospheric temperatures and winds through the deposition of momentum.The partitioning between convective and resolved precipitation is unaffected by the model changes with roughly 62% of the total global precipitation being of the convective type. Finally, the changes in convection and diffusion parametrizations resulted in a larger spread of the ensemble forecasts, which allowed the amplitude of the initial perturbations in the ensemble prediction system to decrease by 30%. Copyright {\copyright} 2008 Royal Meteorological Society}, Author = {Bechtold, Peter and K{\"o}hler, Martin and Jung, Thomas and Doblas-Reyes, Francisco and Leutbecher, Martin and Rodwell, Mark J. and Vitart, Frederic and Balsamo, Gianpaolo}, - Bdsk-File-1 = {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}, Date-Added = {2016-06-14 23:11:58 +0000}, Date-Modified = {2016-06-14 23:11:58 +0000}, Doi = {10.1002/qj.289}, @@ -2188,12 +2187,12 @@ @article{bechtold_et_al_2008 Url = {http://dx.doi.org/10.1002/qj.289}, Volume = {134}, Year = {2008}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1002/qj.289}} @article{han_and_pan_2011, Annote = {doi: 10.1175/WAF-D-10-05038.1}, Author = {Han, Jongil and Pan, Hua-Lu}, - Bdsk-File-1 = {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}, Booktitle = {Weather and Forecasting}, Da = {2011/08/01}, Date = {2011/08/01}, @@ -2214,22 +2213,22 @@ @article{han_and_pan_2011 Volume = {26}, Year = {2011}, Year1 = {2011}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1175/WAF-D-10-05038.1}} @article{pan_and_wu_1995, Author = {Pan, H. -L. and W.-S. Wu}, - Bdsk-File-1 = {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}, Date-Added = {2016-06-14 23:06:41 +0000}, Date-Modified = {2016-06-14 23:06:41 +0000}, Journal = {NMC Office Note, No. 409}, Pages = {40pp}, Title = {Implementing a Mass Flux Convection Parameterization Package for the NMC Medium-Range Forecast Model}, - Year = {1995}} + Year = {1995}, + Bdsk-File-1 = {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}} @article{grell_1993, Annote = {doi: 10.1175/1520-0493(1993)121<0764:PEOAUB>2.0.CO;2}, Author = {Grell, Georg A.}, - Bdsk-File-1 = {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}, Booktitle = {Monthly Weather Review}, Da = {1993/03/01}, Date = {1993/03/01}, @@ -2250,11 +2249,11 @@ @article{grell_1993 Volume = {121}, Year = {1993}, Year1 = {1993}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1175/1520-0493(1993)121%3C0764:PEOAUB%3E2.0.CO;2}} @article{arakawa_and_schubert_1974, Author = {Arakawa, A and Schubert, WH}, - Bdsk-File-1 = {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}, Date-Added = {2016-06-14 23:04:30 +0000}, Date-Modified = {2018-07-18 19:00:17 +0000}, Isi = {A1974S778800004}, @@ -2267,6 +2266,7 @@ @article{arakawa_and_schubert_1974 Title = {Interaction of a cumulus cloud ensemble with the large-scale environment, Part I}, Volume = {31}, Year = {1974}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://ws.isiknowledge.com/cps/openurl/service?url_ver=Z39.88-2004&rft_id=info:ut/A1974S778800004}} @article{harshvardhan_et_al_1989, @@ -2500,7 +2500,6 @@ @article{akmaev_1991 @article{siebesma_et_al_2007, Abstract = {A better conceptual understanding and more realistic parameterizations of convective boundary layers in climate and weather prediction models have been major challenges in meteorological research. In particular, parameterizations of the dry convective boundary layer, in spite of the absence of water phase-changes and its consequent simplicity as compared to moist convection, typically suffer from problems in attempting to represent realistically the boundary layer growth and what is often referred to as countergradient fluxes. The eddy-diffusivity (ED) approach has been relatively successful in representing some characteristics of neutral boundary layers and surface layers in general. The mass-flux (MF) approach, on the other hand, has been used for the parameterization of shallow and deep moist convection. In this paper, a new approach that relies on a combination of the ED and MF parameterizations (EDMF) is proposed for the dry convective boundary layer. It is shown that the EDMF approach follows naturally from a decomposition of the turbulent fluxes into 1) a part that includes strong organized updrafts, and 2) a remaining turbulent field. At the basis of the EDMF approach is the concept that nonlocal subgrid transport due to the strong updrafts is taken into account by the MF approach, while the remaining transport is taken into account by an ED closure. Large-eddy simulation (LES) results of the dry convective boundary layer are used to support the theoretical framework of this new approach and to determine the parameters of the EDMF model. The performance of the new formulation is evaluated against LES results, and it is shown that the EDMF closure is able to reproduce the main properties of dry convective boundary layers in a realistic manner. Furthermore, it will be shown that this approach has strong advantages over the more traditional countergradient approach, especially in the entrainment layer. As a result, this EDMF approach opens the way to parameterize the clear and cumulus-topped boundary layer in a simple and unified way.}, Author = {Siebesma, A. Pier and Soares, Pedro M. M. and Teixeira, Joao}, - Bdsk-File-1 = {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}, Date-Added = {2016-05-20 17:17:49 +0000}, Date-Modified = {2016-05-20 17:17:49 +0000}, Doi = {DOI 10.1175/JAS3888.1}, @@ -2514,12 +2513,12 @@ @article{siebesma_et_al_2007 Title = {A combined eddy-diffusivity mass-flux approach for the convective boundary layer}, Volume = {64}, Year = {2007}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://ws.isiknowledge.com/cps/openurl/service?url_ver=Z39.88-2004&rft_id=info:ut/000245742600011}} @article{soares_et_al_2004, Abstract = {Recently, a new consistent way of parametrizing simultaneously local and non-local turbulent transport for the convective atmospheric boundary layer has been proposed and tested for the clear boundary layer. This approach assumes that in the convective boundary layer the subgrid-scale fluxes result from two different mixing scales: small eddies, that are parametrized by an eddy-diffusivity approach, and thermals, which are represented by a mass-flux contribution. Since the interaction between the cloud layer and the underlying sub-cloud layer predominantly takes place through strong updraughts, this approach offers an interesting avenue of establishing a unified description of the turbulent transport in the cumulus-topped boundary layer. This paper explores the possibility of such a new approach for the cumulus-topped boundary layer. In the sub-cloud and cloud layers, the mass-flux term represents the effect of strong updraughts. These are modelled by a simple entraining parcel, which determines the mean properties of the strong updraughts, the boundary-layer height, the lifting condensation level and cloud top. The residual smaller-scale turbulent transport is parametrized with an eddy-diffusivity approach that uses a turbulent kinetic energy closure. The new scheme is implemented and tested in the research model MesoNH. Copyright {\copyright} 2004 Royal Meteorological Society}, Author = {Soares, P. M. M. and Miranda, P. M. A. and Siebesma, A. P. and Teixeira, J.}, - Bdsk-File-1 = {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}, Date-Added = {2016-05-20 17:17:49 +0000}, Date-Modified = {2016-05-20 17:17:49 +0000}, Doi = {10.1256/qj.03.223}, @@ -2533,11 +2532,11 @@ @article{soares_et_al_2004 Url = {http://dx.doi.org/10.1256/qj.03.223}, Volume = {130}, Year = {2004}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1256/qj.03.223}} @article{troen_and_mahrt_1986, Author = {Troen, IB and Mahrt, L.}, - Bdsk-File-1 = {YnBsaXN0MDDSAQIDBFxyZWxhdGl2ZVBhdGhZYWxpYXNEYXRhXxBBLi4vLi4vQ2xvdWRTdGF0aW9uL2ZpcmxfbGlicmFyeS9maXJsX2xpYnJhcnlfZmlsZXMvVHJvZW4vMTk4Ni5wZGZPEQHEAAAAAAHEAAIAAAxNYWNpbnRvc2ggSEQAAAAAAAAAAAAAAAAAAADR5yRSSCsAAABNeegIMTk4Ni5wZGYAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAE13kNKUWwUAAAAAAAAAAAACAAUAAAkgAAAAAAAAAAAAAAAAAAAABVRyb2VuAAAQAAgAANHneLIAAAARAAgAANKUvXUAAAABABgATXnoAChslgAobIsAKGd7ABteBwACmFwAAgBbTWFjaW50b3NoIEhEOlVzZXJzOgBncmFudGY6AENsb3VkU3RhdGlvbjoAZmlybF9saWJyYXJ5OgBmaXJsX2xpYnJhcnlfZmlsZXM6AFRyb2VuOgAxOTg2LnBkZgAADgASAAgAMQA5ADgANgAuAHAAZABmAA8AGgAMAE0AYQBjAGkAbgB0AG8AcwBoACAASABEABIASFVzZXJzL2dyYW50Zi9DbG91ZFN0YXRpb24vZmlybF9saWJyYXJ5L2ZpcmxfbGlicmFyeV9maWxlcy9Ucm9lbi8xOTg2LnBkZgATAAEvAAAVAAIADf//AAAACAANABoAJABoAAAAAAAAAgEAAAAAAAAABQAAAAAAAAAAAAAAAAAAAjA=}, Date-Added = {2016-05-20 17:17:49 +0000}, Date-Modified = {2016-05-20 17:17:49 +0000}, Doi = {10.1007/BF00122760}, @@ -2551,13 +2550,13 @@ @article{troen_and_mahrt_1986 Url = {http://dx.doi.org/10.1007/BF00122760}, Volume = {37}, Year = {1986}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1007/BF00122760}} @article{macvean_and_mason_1990, Abstract = {Abstract In a recent paper, Kuo and Schubert demonstrated the lack of observational support for the relevance of the criterion for cloud-top entrainment instability proposed by Randall and by Deardorff. Here we derive a new criterion, based on a model of the instability as resulting from the energy released close to cloud top, by Mixing between saturated boundary-layer air and unsaturated air from above the capping inversion. The condition is derived by considering the net conversion from potential to kinetic energy in a system consisting of two layers of fluid straddling cloud-top, when a small amount of mixing occurs between these layers. This contrasts with previous analyses, which only considered the change in buoyancy of the cloud layer when unsaturated air is mixed into it. In its most general form, this new criterion depends on the ratio of the depths of the layers involved in the mixing. It is argued that, for a self-sustaining instability, there must be a net release of kinetic energy on the same depth and time scales as the entrainment process itself. There are two plausible ways in which this requirement may be satisfied. Either one takes the depths of the layers involved in the mixing to each be comparable to the vertical scale of the entrainment process, which is typically of order tens of meters or less, or alternatively, one must allow for the efficiency with which energy released by mixing through a much deeper lower layer becomes available to initiate further entrainment. In both cases the same criterion for instability results. This criterion is much more restrictive than that proposed by Randall and by Deardorff; furthermore, the observational data is then consistent with the predictions of the current theory. Further analysis provides estimates of the turbulent fluxes associated with cloud-top entrainment instability. This analysis effectively constitutes an energetically consistent turbulence closure for models of boundary layers with cloud. The implications for such numerical models are discussed. Comparisons are also made with other possible criteria for cloud-top entrainment instability which have recently been suggested.}, Annote = {doi: 10.1175/1520-0469(1990)047<1012:CTEITS>2.0.CO;2}, Author = {MacVean, M. K. and Mason, P. J.}, - Bdsk-File-1 = {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}, Booktitle = {Journal of the Atmospheric Sciences}, Da = {1990/04/01}, Date-Added = {2016-05-20 17:16:05 +0000}, @@ -2576,11 +2575,11 @@ @article{macvean_and_mason_1990 Url = {http://dx.doi.org/10.1175/1520-0469(1990)047<1012:CTEITS>2.0.CO;2}, Volume = {47}, Year = {1990}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1175/1520-0469(1990)047%3C1012:CTEITS%3E2.0.CO;2}} @article{louis_1979, Author = {Louis, JF}, - Bdsk-File-1 = {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}, Date-Added = {2016-05-20 17:15:52 +0000}, Date-Modified = {2016-05-20 17:15:52 +0000}, Isi = {A1979HT69700004}, @@ -2593,12 +2592,12 @@ @article{louis_1979 Title = {A PARAMETRIC MODEL OF VERTICAL EDDY FLUXES IN THE ATMOSPHERE}, Volume = {17}, Year = {1979}, + Bdsk-File-1 = {YnBsaXN0MDDSAQIDBFxyZWxhdGl2ZVBhdGhZYWxpYXNEYXRhXxBBLi4vLi4vQ2xvdWRTdGF0aW9uL2ZpcmxfbGlicmFyeS9maXJsX2xpYnJhcnlfZmlsZXMvTG91aXMvMTk3OS5wZGZPEQHEAAAAAAHEAAIAAAxNYWNpbnRvc2ggSEQAAAAAAAAAAAAAAAAAAADR5yRSSCsAAAAonogIMTk3OS5wZGYAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAACiej8FuU4pQREYgQ0FSTwACAAUAAAkgAAAAAAAAAAAAAAAAAAAABUxvdWlzAAAQAAgAANHneLIAAAARAAgAAMFutfoAAAABABgAKJ6IAChslgAobIsAKGd7ABteBwACmFwAAgBbTWFjaW50b3NoIEhEOlVzZXJzOgBncmFudGY6AENsb3VkU3RhdGlvbjoAZmlybF9saWJyYXJ5OgBmaXJsX2xpYnJhcnlfZmlsZXM6AExvdWlzOgAxOTc5LnBkZgAADgASAAgAMQA5ADcAOQAuAHAAZABmAA8AGgAMAE0AYQBjAGkAbgB0AG8AcwBoACAASABEABIASFVzZXJzL2dyYW50Zi9DbG91ZFN0YXRpb24vZmlybF9saWJyYXJ5L2ZpcmxfbGlicmFyeV9maWxlcy9Mb3Vpcy8xOTc5LnBkZgATAAEvAAAVAAIADf//AAAACAANABoAJABoAAAAAAAAAgEAAAAAAAAABQAAAAAAAAAAAAAAAAAAAjA=}, Bdsk-Url-1 = {http://ws.isiknowledge.com/cps/openurl/service?url_ver=Z39.88-2004&rft_id=info:ut/A1979HT69700004}} @article{lock_et_al_2000, Abstract = {A new boundary layer turbulent mixing scheme has been developed for use in the UKMO weather forecasting and climate prediction models. This includes a representation of nonlocal mixing (driven by both surface fluxes and cloud-top processes) in unstable layers, either coupled to or decoupled from the surface, and an explicit entrainment parameterization. The scheme is formulated in moist conserved variables so that it can treat both dry and cloudy layers. Details of the scheme and examples of its performance in single-column model tests are presented.}, Author = {Lock, AP and Brown, AR and Bush, MR and Martin, GM and Smith, RNB}, - Bdsk-File-1 = {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}, Date-Added = {2016-05-20 17:15:36 +0000}, Date-Modified = {2016-05-20 17:15:36 +0000}, Isi = {000089461100008}, @@ -2611,13 +2610,13 @@ @article{lock_et_al_2000 Title = {A new boundary layer mixing scheme. {P}art {I}: Scheme description and single-column model tests}, Volume = {128}, Year = {2000}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://ws.isiknowledge.com/cps/openurl/service?url_ver=Z39.88-2004&rft_id=info:ut/000089461100008}} @article{hong_and_pan_1996, Abstract = {Abstract In this paper, the incorporation of a simple atmospheric boundary layer diffusion scheme into the NCEP Medium-Range Forecast Model is described. A boundary layer diffusion package based on the Troen and Mahrt nonlocal diffusion concept has been tested for possible operational implementation. The results from this approach are compared with those from the local diffusion approach, which is the current operational scheme, and verified against FIFE observations during 9?10 August 1987. The comparisons between local and nonlocal approaches are extended to the forecast for a heavy rain case of 15?17 May 1995. The sensitivity of both the boundary layer development and the precipitation forecast to the tuning parameters in the nonlocal diffusion scheme is also investigated. Special attention is given to the interaction of boundary layer processes with precipitation physics. Some results of parallel runs during August 1995 are also presented.}, Annote = {doi: 10.1175/1520-0493(1996)124<2322:NBLVDI>2.0.CO;2}, Author = {Hong, Song-You and Pan, Hua-Lu}, - Bdsk-File-1 = {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}, Booktitle = {Monthly Weather Review}, Da = {1996/10/01}, Date = {1996/10/01}, @@ -2638,13 +2637,13 @@ @article{hong_and_pan_1996 Volume = {124}, Year = {1996}, Year1 = {1996}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1175/1520-0493(1996)124%3C2322:NBLVDI%3E2.0.CO;2}} @article{han_and_pan_2006, Abstract = {Abstract A parameterization of the convection-induced pressure gradient force (PGF) in convective momentum transport (CMT) is tested for hurricane intensity forecasting using NCEP's operational Global Forecast System (GFS) and its nested Regional Spectral Model (RSM). In the parameterization the PGF is assumed to be proportional to the product of the cloud mass flux and vertical wind shear. Compared to control forecasts using the present operational GFS and RSM where the PGF effect in CMT is taken into account empirically, the new PGF parameterization helps increase hurricane intensity by reducing the vertical momentum exchange, giving rise to a closer comparison to the observations. In addition, the new PGF parameterization forecasts not only show more realistically organized precipitation patterns with enhanced hurricane intensity but also reduce the forecast track error. Nevertheless, the model forecasts with the new PGF parameterization still largely underpredict the observed intensity. One of the many possible reasons for the large underprediction may be the absence of hurricane initialization in the models.}, Annote = {doi: 10.1175/MWR3090.1}, Author = {Han, Jongil and Pan, Hua-Lu}, - Bdsk-File-1 = {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}, Booktitle = {Monthly Weather Review}, Da = {2006/02/01}, Date-Added = {2016-05-20 17:11:17 +0000}, @@ -2663,11 +2662,11 @@ @article{han_and_pan_2006 Url = {http://dx.doi.org/10.1175/MWR3090.1}, Volume = {134}, Year = {2006}, + Bdsk-File-1 = {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}, Bdsk-Url-1 = {http://dx.doi.org/10.1175/MWR3090.1}} @article{businger_et_al_1971, Author = {Businger, JA and Wyngaard, JC and Izumi, Y and Bradley, EF}, - Bdsk-File-1 = {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}, Date-Added = {2016-05-20 17:10:50 +0000}, Date-Modified = {2018-07-18 18:58:08 +0000}, Isi = {A1971I822800004}, @@ -2680,6 +2679,7 @@ @article{businger_et_al_1971 Title = {Flux-profile relationships in the atmospheric surface layer}, Volume = {28}, Year = {1971}, + Bdsk-File-1 = {YnBsaXN0MDDSAQIDBFxyZWxhdGl2ZVBhdGhZYWxpYXNEYXRhXxBELi4vLi4vQ2xvdWRTdGF0aW9uL2ZpcmxfbGlicmFyeS9maXJsX2xpYnJhcnlfZmlsZXMvQnVzaW5nZXIvMTk3MS5wZGZPEQHMAAAAAAHMAAIAAAxNYWNpbnRvc2ggSEQAAAAAAAAAAAAAAAAAAADR5yRSSCsAAAAodUUIMTk3MS5wZGYAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAACh1cbTPIxwAAAAAAAAAAAACAAUAAAkgAAAAAAAAAAAAAAAAAAAACEJ1c2luZ2VyABAACAAA0ed4sgAAABEACAAAtM+FjAAAAAEAGAAodUUAKGyWAChsiwAoZ3sAG14HAAKYXAACAF5NYWNpbnRvc2ggSEQ6VXNlcnM6AGdyYW50ZjoAQ2xvdWRTdGF0aW9uOgBmaXJsX2xpYnJhcnk6AGZpcmxfbGlicmFyeV9maWxlczoAQnVzaW5nZXI6ADE5NzEucGRmAA4AEgAIADEAOQA3ADEALgBwAGQAZgAPABoADABNAGEAYwBpAG4AdABvAHMAaAAgAEgARAASAEtVc2Vycy9ncmFudGYvQ2xvdWRTdGF0aW9uL2ZpcmxfbGlicmFyeS9maXJsX2xpYnJhcnlfZmlsZXMvQnVzaW5nZXIvMTk3MS5wZGYAABMAAS8AABUAAgAN//8AAAAIAA0AGgAkAGsAAAAAAAACAQAAAAAAAAAFAAAAAAAAAAAAAAAAAAACOw==}, Bdsk-Url-1 = {http://ws.isiknowledge.com/cps/openurl/service?url_ver=Z39.88-2004&rft_id=info:ut/A1971I822800004}} @article{xu_and_randall_1996, @@ -2870,18 +2870,17 @@ @article{kim_and_arakawa_1995 @techreport{hou_et_al_2002, Author = {Y. Hou and S. Moorthi and K. Campana}, - Bdsk-File-1 = {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}, Date-Added = {2016-05-19 19:52:22 +0000}, Date-Modified = {2016-05-20 15:14:59 +0000}, Institution = {NCEP}, Number = {441}, Title = {Parameterization of Solar Radiation Transfer}, Type = {office note}, - Year = {2002}} + Year = {2002}, + Bdsk-File-1 = {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}} @article{hu_and_stamnes_1993, Author = {Y.X. Hu and K. Stamnes}, - Bdsk-File-1 = {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}, Date-Added = {2016-05-19 19:31:56 +0000}, Date-Modified = {2016-05-20 15:13:12 +0000}, Journal = {J. Climate}, @@ -2889,276 +2888,312 @@ @article{hu_and_stamnes_1993 Pages = {728-742}, Title = {An accurate parameterization of the radiative properties of water clouds suitable for use in climate models}, Volume = {6}, - Year = {1993}} + Year = {1993}, + Bdsk-File-1 = {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}} @article{alexander_et_al_2010, - author = {Alexander, M. J. and Geller, M. and McLandress, C. and Polavarapu, S. and Preusse, P. and Sassi, F. and Sato, K. and Eckermann, S. and Ern, M. and Hertzog, A. and Kawatani, Y. and Pulido, M. and Shaw, T. A. and Sigmond, M. and Vincent, R. and Watanabe, S.}, - title = {Recent developments in gravity-wave effects in climate models and the global distribution of gravity-wave momentum flux from observations and models}, - journal = {Quarterly Journal of the Royal Meteorological Society}, - volume = {136}, - number = {650}, - pages = {1103-1124}, - keywords = {atmosphere, gravity wave, momentum flux, drag, force, wind tendency, climate, global model}, - doi = {10.1002/qj.637}, - url = {https://rmets.onlinelibrary.wiley.com/doi/abs/10.1002/qj.637}, - eprint = {https://rmets.onlinelibrary.wiley.com/doi/pdf/10.1002/qj.637}, - year = {2010}} + Author = {Alexander, M. J. and Geller, M. and McLandress, C. and Polavarapu, S. and Preusse, P. and Sassi, F. and Sato, K. and Eckermann, S. and Ern, M. and Hertzog, A. and Kawatani, Y. and Pulido, M. and Shaw, T. A. and Sigmond, M. and Vincent, R. and Watanabe, S.}, + Doi = {10.1002/qj.637}, + Eprint = {https://rmets.onlinelibrary.wiley.com/doi/pdf/10.1002/qj.637}, + Journal = {Quarterly Journal of the Royal Meteorological Society}, + Keywords = {atmosphere, gravity wave, momentum flux, drag, force, wind tendency, climate, global model}, + Number = {650}, + Pages = {1103-1124}, + Title = {Recent developments in gravity-wave effects in climate models and the global distribution of gravity-wave momentum flux from observations and models}, + Url = {https://rmets.onlinelibrary.wiley.com/doi/abs/10.1002/qj.637}, + Volume = {136}, + Year = {2010}, + Bdsk-Url-1 = {https://rmets.onlinelibrary.wiley.com/doi/abs/10.1002/qj.637}, + Bdsk-Url-2 = {http://dx.doi.org/10.1002/qj.637}} @article{plougonven_and_zhang_2014, - author = {Plougonven, R. and Zhang, F.}, - title = {Internal gravity waves from atmospheric jets and fronts}, - journal = {Reviews of Geophysics}, - volume = {52}, - number = {1}, - pages = {33-76}, - keywords = {gravity waves, stratosphere, atmosphere, jets, fronts, weather}, - doi = {10.1002/2012RG000419}, - url = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1002/2012RG000419}, - eprint = {https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1002/2012RG000419}, - year = {2014}} + Author = {Plougonven, R. and Zhang, F.}, + Doi = {10.1002/2012RG000419}, + Eprint = {https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1002/2012RG000419}, + Journal = {Reviews of Geophysics}, + Keywords = {gravity waves, stratosphere, atmosphere, jets, fronts, weather}, + Number = {1}, + Pages = {33-76}, + Title = {Internal gravity waves from atmospheric jets and fronts}, + Url = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1002/2012RG000419}, + Volume = {52}, + Year = {2014}, + Bdsk-Url-1 = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1002/2012RG000419}, + Bdsk-Url-2 = {http://dx.doi.org/10.1002/2012RG000419}} @article{weinstock_1984, - author = {Weinstock, J.}, - title = {Simplified derivation of an algorithm for nonlinear gravity waves}, - journal = {Journal of Geophysical Research: Space Physics}, - volume = {89}, - number = {A1}, - pages = {345-350}, - doi = {10.1029/JA089iA01p00345}, - url = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/JA089iA01p00345}, - eprint = {https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1029/JA089iA01p00345}, - year = {1984}} + Author = {Weinstock, J.}, + Doi = {10.1029/JA089iA01p00345}, + Eprint = {https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1029/JA089iA01p00345}, + Journal = {Journal of Geophysical Research: Space Physics}, + Number = {A1}, + Pages = {345-350}, + Title = {Simplified derivation of an algorithm for nonlinear gravity waves}, + Url = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/JA089iA01p00345}, + Volume = {89}, + Year = {1984}, + Bdsk-Url-1 = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/JA089iA01p00345}, + Bdsk-Url-2 = {http://dx.doi.org/10.1029/JA089iA01p00345}} @article{holton_1983, - author = {Holton, James R.}, - title = {The Influence of Gravity Wave Breaking on the General Circulation of the Middle Atmosphere}, - journal = {Journal of the Atmospheric Sciences}, - volume = {40}, - number = {10}, - pages = {2497-2507}, - year = {1983}, - doi = {10.1175/1520-0469(1983)040<2497:TIOGWB>2.0.CO;2}, - URL = {https://doi.org/10.1175/1520-0469(1983)040<2497:TIOGWB>2.0.CO;2}, - eprint = {https://doi.org/10.1175/1520-0469(1983)040<2497:TIOGWB>2.0.CO;2}} + Author = {Holton, James R.}, + Doi = {10.1175/1520-0469(1983)040<2497:TIOGWB>2.0.CO;2}, + Eprint = {https://doi.org/10.1175/1520-0469(1983)040<2497:TIOGWB>2.0.CO;2}, + Journal = {Journal of the Atmospheric Sciences}, + Number = {10}, + Pages = {2497-2507}, + Title = {The Influence of Gravity Wave Breaking on the General Circulation of the Middle Atmosphere}, + Url = {https://doi.org/10.1175/1520-0469(1983)040<2497:TIOGWB>2.0.CO;2}, + Volume = {40}, + Year = {1983}, + Bdsk-Url-1 = {https://doi.org/10.1175/1520-0469(1983)040%3C2497:TIOGWB%3E2.0.CO;2}, + Bdsk-Url-2 = {http://dx.doi.org/10.1175/1520-0469(1983)040%3C2497:TIOGWB%3E2.0.CO;2}} @article{geller_et_al_2013, - author = {Geller, M. A. and Alexander, M. Joan and Love, P. T. and Bacmeister, J. and Ern, M. and Hertzog, A. and Manzini, E. and Preusse, P. and Sato, K. and Scaife, A. A. and Zhou, T.}, - title = {A Comparison between Gravity Wave Momentum Fluxes in Observations and Climate Models}, - journal = {Journal of Climate}, - volume = {26}, - number = {17}, - pages = {6383-6405}, - year = {2013}, - doi = {10.1175/JCLI-D-12-00545.1}, - URL = {https://doi.org/10.1175/JCLI-D-12-00545.1}, - eprint = {https://doi.org/10.1175/JCLI-D-12-00545.1}} + Author = {Geller, M. A. and Alexander, M. Joan and Love, P. T. and Bacmeister, J. and Ern, M. and Hertzog, A. and Manzini, E. and Preusse, P. and Sato, K. and Scaife, A. A. and Zhou, T.}, + Doi = {10.1175/JCLI-D-12-00545.1}, + Eprint = {https://doi.org/10.1175/JCLI-D-12-00545.1}, + Journal = {Journal of Climate}, + Number = {17}, + Pages = {6383-6405}, + Title = {A Comparison between Gravity Wave Momentum Fluxes in Observations and Climate Models}, + Url = {https://doi.org/10.1175/JCLI-D-12-00545.1}, + Volume = {26}, + Year = {2013}, + Bdsk-Url-1 = {https://doi.org/10.1175/JCLI-D-12-00545.1}, + Bdsk-Url-2 = {http://dx.doi.org/10.1175/JCLI-D-12-00545.1}} @article{garcia_et_al_2017, - author = {Garcia, R. R. and Smith, A. K. and Kinnison, D. E. and Cámara, Á. and Murphy, D. J.}, - title = {Modification of the Gravity Wave Parameterization in the Whole Atmosphere Community Climate Model: Motivation and Results}, - journal = {Journal of the Atmospheric Sciences}, - volume = {74}, - number = {1}, - pages = {275-291}, - year = {2017}, - doi = {10.1175/JAS-D-16-0104.1}, - URL = {https://doi.org/10.1175/JAS-D-16-0104.1}, - eprint = {https://doi.org/10.1175/JAS-D-16-0104.1}} + Author = {Garcia, R. R. and Smith, A. K. and Kinnison, D. E. and C{\'a}mara, {\'A}. and Murphy, D. J.}, + Doi = {10.1175/JAS-D-16-0104.1}, + Eprint = {https://doi.org/10.1175/JAS-D-16-0104.1}, + Journal = {Journal of the Atmospheric Sciences}, + Number = {1}, + Pages = {275-291}, + Title = {Modification of the Gravity Wave Parameterization in the Whole Atmosphere Community Climate Model: Motivation and Results}, + Url = {https://doi.org/10.1175/JAS-D-16-0104.1}, + Volume = {74}, + Year = {2017}, + Bdsk-Url-1 = {https://doi.org/10.1175/JAS-D-16-0104.1}, + Bdsk-Url-2 = {http://dx.doi.org/10.1175/JAS-D-16-0104.1}} @inproceedings{yudin_et_al_2016, - title={Gravity wave physics in the NOAA Environmental Modeling System}, - author={Yudin, V.A. and Akmaev, R.A. and Fuller-Rowell, T.J. and Alpert, J.C.}, - booktitle={International SPARC Gravity Wave Symposium}, - volume={48}, - number={1}, - pages={012024}, - year={2016}, - organization={}} + Author = {Yudin, V.A. and Akmaev, R.A. and Fuller-Rowell, T.J. and Alpert, J.C.}, + Booktitle = {International SPARC Gravity Wave Symposium}, + Number = {1}, + Pages = {012024}, + Title = {Gravity wave physics in the NOAA Environmental Modeling System}, + Volume = {48}, + Year = {2016}} @inproceedings{alpert_et_al_2018, - title={Integrating Unified Gravity Wave Physics Research into the Next Generation Global Prediction System for NCEP Research to Operations}, - author={Alpert, Jordan C and Yudin, Valery and Fuller-Rowell, Tim and Akmaev, Rashid A}, - booktitle={98th American Meteorological Society Annual Meeting}, - year={2018}, - organization={AMS}} + Author = {Alpert, Jordan C and Yudin, Valery and Fuller-Rowell, Tim and Akmaev, Rashid A}, + Booktitle = {98th American Meteorological Society Annual Meeting}, + Organization = {AMS}, + Title = {Integrating Unified Gravity Wave Physics Research into the Next Generation Global Prediction System for NCEP Research to Operations}, + Year = {2018}} @article{eckermann_2011, - author = {Eckermann, Stephen D.}, - title = {Explicitly Stochastic Parameterization of Nonorographic Gravity Wave Drag}, - journal = {Journal of the Atmospheric Sciences}, - volume = {68}, - number = {8}, - pages = {1749-1765}, - year = {2011}, - doi = {10.1175/2011JAS3684.1}, - URL = {https://doi.org/10.1175/2011JAS3684.1}, - eprint = {https://doi.org/10.1175/2011JAS3684.1}} + Author = {Eckermann, Stephen D.}, + Doi = {10.1175/2011JAS3684.1}, + Eprint = {https://doi.org/10.1175/2011JAS3684.1}, + Journal = {Journal of the Atmospheric Sciences}, + Number = {8}, + Pages = {1749-1765}, + Title = {Explicitly Stochastic Parameterization of Nonorographic Gravity Wave Drag}, + Url = {https://doi.org/10.1175/2011JAS3684.1}, + Volume = {68}, + Year = {2011}, + Bdsk-Url-1 = {https://doi.org/10.1175/2011JAS3684.1}, + Bdsk-Url-2 = {http://dx.doi.org/10.1175/2011JAS3684.1}} @article{lott_et_al_2012, - author = {Lott, F. and Guez, L. and Maury, P.}, - title = {A stochastic parameterization of non-orographic gravity waves: Formalism and impact on the equatorial stratosphere}, - journal = {Geophysical Research Letters}, - volume = {39}, - number = {6}, - pages = {}, - keywords = {Quasi-Biennial Oscillation, Rossby-gravity waves, gravity waves, stochastic parameterization, stratospheric dynamics}, - doi = {10.1029/2012GL051001}, - url = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/2012GL051001}, - eprint = {https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1029/2012GL051001}, - year = {2012}} + Author = {Lott, F. and Guez, L. and Maury, P.}, + Doi = {10.1029/2012GL051001}, + Eprint = {https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1029/2012GL051001}, + Journal = {Geophysical Research Letters}, + Keywords = {Quasi-Biennial Oscillation, Rossby-gravity waves, gravity waves, stochastic parameterization, stratospheric dynamics}, + Number = {6}, + Title = {A stochastic parameterization of non-orographic gravity waves: Formalism and impact on the equatorial stratosphere}, + Url = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/2012GL051001}, + Volume = {39}, + Year = {2012}, + Bdsk-Url-1 = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/2012GL051001}, + Bdsk-Url-2 = {http://dx.doi.org/10.1029/2012GL051001}} @conference{yudin_et_al_2018, - author = {Yudin, V. 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Part 2: Broad and quasi monochromatic spectra, and implementation}, + Url = {http://www.sciencedirect.com/science/article/pii/S1364682696000806}, + Volume = {59}, + Year = {1997}, + Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/pii/S1364682696000806}, + Bdsk-Url-2 = {https://doi.org/10.1016/S1364-6826(96)00080-6}} @article{alexander_and_dunkerton_1999, - author = {Alexander, M. J. and Dunkerton, T. J.}, - title = {A Spectral Parameterization of Mean-Flow Forcing due to Breaking Gravity Waves}, - journal = {Journal of the Atmospheric Sciences}, - volume = {56}, - number = {24}, - pages = {4167-4182}, - year = {1999}, - doi = {10.1175/1520-0469(1999)056<4167:ASPOMF>2.0.CO;2}, - URL = {https://doi.org/10.1175/1520-0469(1999)056<4167:ASPOMF>2.0.CO;2}, - eprint = {https://doi.org/10.1175/1520-0469(1999)056<4167:ASPOMF>2.0.CO;2}} + Author = {Alexander, M. J. and Dunkerton, T. J.}, + Doi = {10.1175/1520-0469(1999)056<4167:ASPOMF>2.0.CO;2}, + Eprint = {https://doi.org/10.1175/1520-0469(1999)056<4167:ASPOMF>2.0.CO;2}, + Journal = {Journal of the Atmospheric Sciences}, + Number = {24}, + Pages = {4167-4182}, + Title = {A Spectral Parameterization of Mean-Flow Forcing due to Breaking Gravity Waves}, + Url = {https://doi.org/10.1175/1520-0469(1999)056<4167:ASPOMF>2.0.CO;2}, + Volume = {56}, + Year = {1999}, + Bdsk-Url-1 = {https://doi.org/10.1175/1520-0469(1999)056%3C4167:ASPOMF%3E2.0.CO;2}, + Bdsk-Url-2 = {http://dx.doi.org/10.1175/1520-0469(1999)056%3C4167:ASPOMF%3E2.0.CO;2}} @article{scinocca_2003, - author = {Scinocca, John F.}, - title = {An Accurate Spectral Nonorographic Gravity Wave Drag Parameterization for General Circulation Models}, - journal = {Journal of the Atmospheric Sciences}, - volume = {60}, - number = {4}, - pages = {667-682}, - year = {2003}, - doi = {10.1175/1520-0469(2003)060<0667:AASNGW>2.0.CO;2}, - URL = {https://doi.org/10.1175/1520-0469(2003)060<0667:AASNGW>2.0.CO;2}, - eprint = {https://doi.org/10.1175/1520-0469(2003)060<0667:AASNGW>2.0.CO;2}} + Author = {Scinocca, John F.}, + Doi = {10.1175/1520-0469(2003)060<0667:AASNGW>2.0.CO;2}, + Eprint = {https://doi.org/10.1175/1520-0469(2003)060<0667:AASNGW>2.0.CO;2}, + Journal = {Journal of the Atmospheric Sciences}, + Number = {4}, + Pages = {667-682}, + Title = {An Accurate Spectral Nonorographic Gravity Wave Drag Parameterization for General Circulation Models}, + Url = {https://doi.org/10.1175/1520-0469(2003)060<0667:AASNGW>2.0.CO;2}, + Volume = {60}, + Year = {2003}, + Bdsk-Url-1 = {https://doi.org/10.1175/1520-0469(2003)060%3C0667:AASNGW%3E2.0.CO;2}, + Bdsk-Url-2 = {http://dx.doi.org/10.1175/1520-0469(2003)060%3C0667:AASNGW%3E2.0.CO;2}} @article{shaw_and_shepherd_2009, - author = {Shaw, Tiffany A. and Shepherd, Theodore G.}, - title = {A Theoretical Framework for Energy and Momentum Consistency in Subgrid-Scale Parameterization for Climate Models}, - journal = {Journal of the Atmospheric Sciences}, - volume = {66}, - 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R. and Marsh, D. R. and Kinnison, D. E. and Boville, B. A. and Sassi, F.}, - title = {Simulation of secular trends in the middle atmosphere, 1950–2003}, - journal = {Journal of Geophysical Research: Atmospheres}, - volume = {112}, - number = {D9}, - pages = {}, - keywords = {global change, ozone depletion, water vapor trends, temperature trends}, - doi = {10.1029/2006JD007485}, - url = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/2006JD007485}, - eprint = {https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1029/2006JD007485}, - year = {2007}} + Author = {Garcia, R. R. and Marsh, D. R. and Kinnison, D. E. and Boville, B. A. and Sassi, F.}, + Doi = {10.1029/2006JD007485}, + Eprint = {https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1029/2006JD007485}, + Journal = {Journal of Geophysical Research: Atmospheres}, + Keywords = {global change, ozone depletion, water vapor trends, temperature trends}, + Number = {D9}, + Title = {Simulation of secular trends in the middle atmosphere, 1950--2003}, + Url = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/2006JD007485}, + Volume = {112}, + Year = {2007}, + Bdsk-Url-1 = {https://agupubs.onlinelibrary.wiley.com/doi/abs/10.1029/2006JD007485}, + Bdsk-Url-2 = {http://dx.doi.org/10.1029/2006JD007485}} @article{eckermann_et_al_2009, - title = "High-altitude data assimilation system experiments for the northern summer mesosphere season of 2007", - journal = "Journal of Atmospheric and Solar-Terrestrial Physics", - volume = "71", - number = "3", - pages = "531 - 551", - year = "2009", - note = "Global Perspectives on the Aeronomy of the Summer Mesopause Region", - issn = "1364-6826", - doi = "https://doi.org/10.1016/j.jastp.2008.09.036", - url = "http://www.sciencedirect.com/science/article/pii/S1364682608002575", - author = "Stephen D. Eckermann and Karl W. Hoppel and Lawrence Coy and John P. McCormack and David E. Siskind and Kim Nielsen and Andrew Kochenash and Michael H. Stevens and Christoph R. Englert and Werner Singer and Mark Hervig", - keywords = "Data assimilation, Polar mesospheric cloud, Tide, Planetary wave, Mesosphere",} + Author = {Stephen D. Eckermann and Karl W. Hoppel and Lawrence Coy and John P. McCormack and David E. Siskind and Kim Nielsen and Andrew Kochenash and Michael H. Stevens and Christoph R. Englert and Werner Singer and Mark Hervig}, + Doi = {https://doi.org/10.1016/j.jastp.2008.09.036}, + Issn = {1364-6826}, + Journal = {Journal of Atmospheric and Solar-Terrestrial Physics}, + Keywords = {Data assimilation, Polar mesospheric cloud, Tide, Planetary wave, Mesosphere}, + Note = {Global Perspectives on the Aeronomy of the Summer Mesopause Region}, + Number = {3}, + Pages = {531 - 551}, + Title = {High-altitude data assimilation system experiments for the northern summer mesosphere season of 2007}, + Url = {http://www.sciencedirect.com/science/article/pii/S1364682608002575}, + Volume = {71}, + Year = {2009}, + Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/pii/S1364682608002575}, + Bdsk-Url-2 = {https://doi.org/10.1016/j.jastp.2008.09.036}} @inproceedings{alpert_et_al_2019, - title={Atmospheric Gravity Wave Sources Correlated with Resolved-scale GW Activity and Sub-grid Scale Parameterization in the FV3gfs Model}, - author={Alpert, Jordan C and Yudin, Valery A and Strobach, Edward}, - booktitle={AGU Fall Meeting 2019}, - year={2019}, - organization={AGU}} - -@Article{ern_et_al_2018, - AUTHOR = {Ern, M. and Trinh, Q. T. and Preusse, P. and Gille, J. C. and Mlynczak, M. G. and Russell III, J. M. and Riese, M.}, - TITLE = {GRACILE: a comprehensive climatology of atmospheric gravity wave parameters based on satellite limb soundings}, - JOURNAL = {Earth System Science Data}, - VOLUME = {10}, - YEAR = {2018}, - NUMBER = {2}, - PAGES = {857--892}, - URL = {https://www.earth-syst-sci-data.net/10/857/2018/}, - DOI = {10.5194/essd-10-857-2018}} + Author = {Alpert, Jordan C and Yudin, Valery A and Strobach, Edward}, + Booktitle = {AGU Fall Meeting 2019}, + Organization = {AGU}, + Title = {Atmospheric Gravity Wave Sources Correlated with Resolved-scale GW Activity and Sub-grid Scale Parameterization in the FV3gfs Model}, + Year = {2019}} + +@article{ern_et_al_2018, + Author = {Ern, M. and Trinh, Q. T. and Preusse, P. and Gille, J. C. and Mlynczak, M. G. and Russell III, J. M. and Riese, M.}, + Doi = {10.5194/essd-10-857-2018}, + Journal = {Earth System Science Data}, + Number = {2}, + Pages = {857--892}, + Title = {GRACILE: a comprehensive climatology of atmospheric gravity wave parameters based on satellite limb soundings}, + Url = {https://www.earth-syst-sci-data.net/10/857/2018/}, + Volume = {10}, + Year = {2018}, + Bdsk-Url-1 = {https://www.earth-syst-sci-data.net/10/857/2018/}, + Bdsk-Url-2 = {http://dx.doi.org/10.5194/essd-10-857-2018}} @inproceedings{yudin_et_al_2019, - title={Longitudinal Variability of Wave Dynamics in Weather Models Extended into the Mesosphere and Thermosphere}, - author={Yudin V.A. , S. I. Karol, R.A. Akmaev, T. Fuller-Rowell, D. Kleist, A. Kubaryk, and C. Thompson}, - booktitle={Space Weather Workshop}, - year={2019},} + Author = {Yudin V.A. , S. I. Karol, R.A. Akmaev, T. Fuller-Rowell, D. Kleist, A. Kubaryk, and C. Thompson}, + Booktitle = {Space Weather Workshop}, + Title = {Longitudinal Variability of Wave Dynamics in Weather Models Extended into the Mesosphere and Thermosphere}, + Year = {2019}} diff --git a/physics/docs/pdftxt/CPT_adv_suite.txt b/physics/docs/pdftxt/CPT_adv_suite.txt index 132d8bd11..26d514d51 100644 --- a/physics/docs/pdftxt/CPT_adv_suite.txt +++ b/physics/docs/pdftxt/CPT_adv_suite.txt @@ -3,31 +3,28 @@ \section csawmg_suite_overview Overview -The advanced csawmg physics suite uses the parameterizations in the following order: +The csawmg physics suite uses the parameterizations in the following order: - \ref GFS_RRTMG - \ref GFS_SFCLYR - \ref GFS_NSST - \ref GFS_NOAH - \ref GFS_SFCSICE - \ref GFS_HEDMF - - \ref GFS_GWDPS + - \ref GFS_UGWP_v0 - \ref GFS_RAYLEIGH - \ref GFS_OZPHYS - \ref GFS_H2OPHYS - \ref CSAW_scheme - - \ref GFS_GWDC - \ref GFS_SAMFshal - \ref CPT_MG3 - \ref mod_cs_conv_aw_adj - \ref GFS_CALPRECIPTYPE \section sdf_cpt_suite Suite Definition File - -The advanced csawmg physics suite uses the parameterizations in the following order, as defined in \c SCM_csawmg : \code - + @@ -56,9 +53,10 @@ The advanced csawmg physics suite uses the parameterizations in the following or GFS_suite_stateout_reset get_prs_fv3 GFS_suite_interstitial_1 - dcyc2t3 GFS_surface_generic_pre GFS_surface_composites_pre + dcyc2t3 + GFS_surface_composites_inter GFS_suite_interstitial_2 @@ -75,7 +73,6 @@ The advanced csawmg physics suite uses the parameterizations in the following or GFS_surface_composites_post - dcyc2t3_post sfc_diag sfc_diag_post GFS_surface_generic_post @@ -83,8 +80,9 @@ The advanced csawmg physics suite uses the parameterizations in the following or hedmf GFS_PBL_generic_post GFS_GWD_generic_pre - gwdps - gwdps_post + cires_ugwp + cires_ugwp_post + GFS_GWD_generic_post rayleigh_damp GFS_suite_stateout_update ozphys_2015 @@ -96,12 +94,8 @@ The advanced csawmg physics suite uses the parameterizations in the following or cs_conv cs_conv_post GFS_DCNV_generic_post - gwdc_pre - gwdc - gwdc_post GFS_SCNV_generic_pre samfshalcnv - samfshalcnv_post GFS_SCNV_generic_post GFS_suite_interstitial_4 cnvc90 @@ -111,21 +105,20 @@ The advanced csawmg physics suite uses the parameterizations in the following or m_micro_post cs_conv_aw_adj GFS_MP_generic_post - sfc_sice_post maximum_hourly_diagnostics - \endcode -\section cpt_nml_option Namelist Option +\section cpt_nml_option Namelist \code &gfs_physics_nml fhzero = 6. ldiag3d = .true. fhcyc = 24. + nst_anl = .true. use_ufo = .true. pre_rad = .false. crtrh = 0.93,0.90,0.95 @@ -147,25 +140,40 @@ The advanced csawmg physics suite uses the parameterizations in the following or shal_cnv = .true. cal_pre = .false. redrag = .true. - dspheat = .true. + dspheat = .false. hybedmf = .true. satmedmf = .false. - lheatstrg = .true. + lheatstrg = .false. random_clds = .true. trans_trac = .true. - cnvcld = .true. + cnvcld = .false. imfshalcnv = 2 imfdeepcnv = -1 cdmbgwd = 3.5,0.25 prslrd0 = 0. ivegsrc = 1 isot = 1 + lsm = 1 + iopt_dveg = 2 + iopt_crs = 1 + iopt_btr = 1 + iopt_run = 1 + iopt_sfc = 1 + iopt_frz = 1 + iopt_inf = 1 + iopt_rad = 1 + iopt_alb = 2 + iopt_snf = 4 + iopt_tbot = 2 + iopt_stc = 1 oz_phys = .false. oz_phys_2015 = .true. debug = .false. + ras = .false. cscnv = .true. do_shoc = .false. + shoc_parm = 7000.0,1.0,2.0,0.7,-999.0 do_aw = .true. shoc_cld = .false. h2o_phys = .true. @@ -173,8 +181,6 @@ The advanced csawmg physics suite uses the parameterizations in the following or xkzm_h = 0.5 xkzm_m = 0.5 xkzm_s = 1.0 - nstf_name = 2,1,1,0,5 - nst_anl = .true. ccwf = 1.0,1.0 dlqf = 0.25,0.05 mg_dcs = 200.0 @@ -190,12 +196,13 @@ The advanced csawmg physics suite uses the parameterizations in the following or mg_do_ice_gmao = .false. mg_do_liq_liu = .true. cs_parm = 8.0,4.0,1.0e3,3.5e3,20.0,1.0,0.0,1.0,0.6,0.0 - shoc_parm = 7000.0,1.0,2.0,0.7,-999.0 ctei_rm = 0.60,0.23 max_lon = 8000 max_lat = 4000 rhcmax = 0.9999999 effr_in = .true. + + nstf_name = 2,1,1,0,5 ltaerosol = .false. lradar = .false. cplflx = .false. @@ -203,6 +210,22 @@ The advanced csawmg physics suite uses the parameterizations in the following or iaufhrs = 30 iau_inc_files = "''" / + +&cires_ugwp_nml + knob_ugwp_solver = 2 + knob_ugwp_source = 1,1,0,0 + knob_ugwp_wvspec = 1,25,25,25 + knob_ugwp_azdir = 2,4,4,4 + knob_ugwp_stoch = 0,0,0,0 + knob_ugwp_effac = 1,1,1,1 + knob_ugwp_doaxyz = 1 + knob_ugwp_doheat = 1 + knob_ugwp_dokdis = 1 + knob_ugwp_ndx4lh = 1 + knob_ugwp_version = 0 + launch_level = 25 +/ +/ \endcode diff --git a/physics/docs/pdftxt/GFS_OCEAN.txt b/physics/docs/pdftxt/GFS_OCEAN.txt new file mode 100644 index 000000000..b384aec84 --- /dev/null +++ b/physics/docs/pdftxt/GFS_OCEAN.txt @@ -0,0 +1,17 @@ +/** +\page GFS_OCEAN GFS Simple Ocean Scheme +\section des_sfcocean Description + +The Sea Surface Temperature (SST) is a required field in Numerical Weather Prediciton (NWP) systems because it +functions as the lower boundary condition for the calculation of air-sea heat fluxes. The GFS Simple Ocean Scheme +does not change the SST. Therefore, the SST stays constant throughout the forecast unless it is updated by other processes. +In some models, such as the UFS atmosphere, the SST can change if forcing towards the climatology is turned on. + +\section intra_sfcocean Intraphysics Communication +\ref arg_table_sfc_ocean_run + + + + + +*/ diff --git a/physics/docs/pdftxt/GFS_OZPHYS.txt b/physics/docs/pdftxt/GFS_OZPHYS.txt index fadaf95a5..3a2ddc173 100644 --- a/physics/docs/pdftxt/GFS_OZPHYS.txt +++ b/physics/docs/pdftxt/GFS_OZPHYS.txt @@ -1,5 +1,5 @@ /** -\page GFS_OZPHYS GFS Ozone Photochemistry Scheme +\page GFS_OZPHYS GFS Ozone Photochemistry (2015) Scheme \section des_ozone Description In recent years, the leading NWP centers have extended the vertical range of their NWP and DA systems from the surface up through the stratosphere (~10-50 km altitude) and lower mesosphere (~50-65 km). Some diff --git a/physics/docs/pdftxt/GFS_UGWPv0.txt b/physics/docs/pdftxt/GFS_UGWPv0.txt new file mode 100644 index 000000000..e6ea3b6f4 --- /dev/null +++ b/physics/docs/pdftxt/GFS_UGWPv0.txt @@ -0,0 +1,117 @@ +/** +\page GFS_UGWP_v0 CIRES Unified Gravity Wave Physics Scheme - Version 0 +\section des_UGWP Description + +Gravity waves (GWs) are generated by a variety of sources in the atmosphere +including orographic GWs (OGWs; quasi-stationary waves) and non-orographic +GWs (NGWs; non-stationary oscillations). When the Version 0 of the Unified +Gravity Wave Physics (UGWP v0) is invoked, the subgrid OGWs and NGWs are +parameterized. For the subgrid-scale parameterization of OGWs, the UGWP +invokes a separate scheme, the \subpage GFS_GWDPS, which is used in the operational +Global Forecast System (GFS) version 15. + +The NGW physics scheme parameterizes the effects of non-stationary waves +unresolved by dynamical cores. These non-stationary oscillations with periods +bounded by Coriolis and Brunt-Väisälä frequencies and typical horizontal +scales from tens to several hundreds of kilometers, are forced by the +imbalance of convective and frontal/jet dynamics in the troposphere and +lower stratosphere (Fritts 1984 \cite fritts_1984; Alexander et al. +2010 \cite alexander_et_al_2010; Plougonven and Zhang 2014 \cite plougonven_and_zhang_2014). +The NGWs propagate upwards and the amplitudes exponentially grow with +altitude until instability and breaking of waves occur. Convective and +dynamical instability induced by GWs with large amplitudes can trigger +production of small-scale turbulence and self-destruction of waves. +The latter process in the theory of atmospheric GWs is frequently referred +as the wave saturation (Lindzen 1981 \cite lindzen_1981; Weinstock +1984 \cite weinstock_1984; Fritts 1984 \cite fritts_1984). Herein, +“saturation” or "breaking" refers to any processes that act to reduce +wave amplitudes due to instabilities and/or interactions arising from +large-amplitude perturbations limiting the exponential growth of GWs +with height. Background dissipation processes such as molecular diffusion +and radiative cooling, in contrast, act independently of GW amplitudes. +In the middle atmosphere, impacts of NGW saturation (or breaking) and +dissipation on the large-scale circulation, mixing, and transport have +been acknowledged in the physics of global weather and climate models +after pioneering studies by Lindzen 1981 \cite lindzen_1981 and Holton +1983 \cite holton_1983. Comprehensive reviews on the physics of NGWs +and OGWs in climate and weather models have been discussted in Alexander +et al. 2010 \cite alexander_et_al_2010, Geller et al. +2013 \cite geller_et_al_2013, and Garcia et al. 2017 \cite garcia_et_al_2017. +They are formulated using different aspects of the nonlinear and linear +propagation, instability, breaking and dissipation of waves along with +different specifications of GW sources (Garcia et al. 2007 \cite garcia_et_al_2007; +Richter et al 2010 \cite richter_et_al_2010; Eckermann et al. +2009 \cite eckermann_et_al_2009; Eckermann 2011 \cite eckermann_2011; +Lott et al. 2012 \cite lott_et_al_2012). + +Several studies have demonstrated the importance of NGW physics to improve +model predictions in the stratosphere and upper atmosphere (Alexander et al. + 2010 \cite alexander_et_al_2010; Geller et al. 2013). In order to describe +the effects of unresolved GWs in global forecast models, the representation of +subgrid OGWs and NGWs has been implemented in the self-consistent manner using the +UGWP framework. + +The concept of UGWP was first proposed and implemented in the Unified +Forecast System (UFS)with model top at different levels by scientists from +the University of Colorado Cooperative Institute for Research in the +Environmental Sciences (CIRES) at NOAA's Space Weather Prediction Center (SWPC) +and from NOAA's Environmental Modeling Center (EMC) (Alpert et al. +2019 \cite alpert_et_al_2019; Yudin et al. 2016 \cite yudin_et_al_2016; +Yudin et al. 2018 \cite yudin_et_al_2018). The UGWP considers identical +GW propagation solvers for OGWs and NGWs with different approaches for +specification of subgrid wave sources. The current set of the input and +control paramters for UGWP version 0 (UGWP v0) enables options for GW +effects, including momentum deposition (also called GW drag), heat +deposition, and mixing by eddy viscosity, conductivity and diffusion; +however, note that the eddy mixing effects induced by instability of GWs +are not activated in this version. + +Namelist paramters control the number of directional azimuths in which +waves can propagate, number of waves in a single direction, and the level +above the surface at which NGWs can be launched. Among the input parameters, +the GW efficiency factors reflect intermittency of wave excitation. +They should vary with horizontal resolution, reflecting the capability of +the dynamical core to resolve mesoscale wave activity with the enhancement +of model resolution. + +Prescribed distributions for vertical momentum flux (VMF) of NGWs have been employed +in global numerical weather prediction and reanalysis models to ease tuning of GW +schemes to the climatology of the middle atmosphere dynamics in the absence of +the global wind data above about 35 km (Eckermann et al. 2009 \cite eckermann_et_al_2009; +Molod et al. 2015 \cite molod_et_al_2015). These distributions of VMF +qualitatively describe the general features of the latitudinal and seasonal + variations of the global GW activity in the lower stratosphere, observed from the +ground and space (Ern et al. 2018 \cite ern_et_al_2018). Subgrid GW sources can also be +parameterized to respond to year-to-year variations of solar input and +anthropogenic emissions (Richter et al 2010 \cite richter_et_al_2010; +2014 \cite richter_et_al_2014). + +Note that in UGWP v0, the momentum and heat deposition due to GW breaking +and dissipation have been tested in the multi-year simulations and +medium-range forecasts using a configuration of the UFS weather model +using 127 levels with model top at approximately 80 km. + +Along with the GW heat and momentum depositions, GW eddy mixing is an +important element of the Whole Atmosphere Model (WAM) physics, as shown +in WAM simulations with the spectral dynamics (Yudin et al. 2018 \cite yudin_et_al_2018). +The impact of eddy mixing effects in the middle and upper atmosphere, +which is not included in this version, need to be tested, evaluated, and +orchestrated with the representation of the subgrid turbulent diffusion and +the numerical dissipation. + +The representation of subgrid GWs is particularly important for WAMs that +extend into the thermosphere (top lid at ~600 km). In the mesosphere and +thermosphere, the background attenuation of subgrid waves due to molecular +and turbulent diffusion, radiative damping and ion drag will be the +additional mechanism of NGW and OGW dissipation along with convective +and dynamical instability of waves described by the linear +(Lindzen 1981 \cite lindzen_1981) and nonlinear +(Weinstock 1984 \cite weinstock_1984; Hines 1997 \cite hines_1997) saturation theories. + +\section intra_UGWPv0 Intraphysics Communication +\ref arg_table_cires_ugwp_run + +\section gen_al_ugwpv0 General Algorithm +\ref gen_cires_ugwp + +*/ diff --git a/physics/docs/pdftxt/GFSv14_suite.txt b/physics/docs/pdftxt/GFSv14_suite.txt index 23f611a25..d1dcb038c 100644 --- a/physics/docs/pdftxt/GFSv14_suite.txt +++ b/physics/docs/pdftxt/GFSv14_suite.txt @@ -75,7 +75,6 @@ The GFS v14 suite uses the parameterizations in the following order, as defined - dcyc2t3_post sfc_diag sfc_diag_post GFS_surface_generic_post diff --git a/physics/docs/pdftxt/GFSv15_suite.txt b/physics/docs/pdftxt/GFSv15_suite.txt index 6b5fddcf8..abf446224 100644 --- a/physics/docs/pdftxt/GFSv15_suite.txt +++ b/physics/docs/pdftxt/GFSv15_suite.txt @@ -85,7 +85,6 @@ The GFS v15 suite uses the parameterizations in the following order, as defined GFS_surface_composites_post - dcyc2t3_post sfc_diag sfc_diag_post GFS_surface_generic_post diff --git a/physics/docs/pdftxt/GFSv15_suite_TKEEDMF.txt b/physics/docs/pdftxt/GFSv15_suite_TKEEDMF.txt index 56a1f97f5..6215fe361 100644 --- a/physics/docs/pdftxt/GFSv15_suite_TKEEDMF.txt +++ b/physics/docs/pdftxt/GFSv15_suite_TKEEDMF.txt @@ -76,7 +76,6 @@ The GFS v15plus suite uses the parameterizations in the following order, as defi GFS_surface_composites_post - dcyc2t3_post sfc_diag sfc_diag_post GFS_surface_generic_post diff --git a/physics/docs/pdftxt/GFSv15p2_no_nsst_suite.txt b/physics/docs/pdftxt/GFSv15p2_no_nsst_suite.txt new file mode 100644 index 000000000..982afc860 --- /dev/null +++ b/physics/docs/pdftxt/GFSv15p2_no_nsst_suite.txt @@ -0,0 +1,127 @@ +/** +\page GFS_v15p2_no_nsst_page GFS_v15p2_no_nsst Suite + +\section gfsv15_no_nsst_suite_overview Overview + +Suite GFS_v15p2_no_nsst is a companion suite of GFS_v15p2 with GRIB2 data initialization. + +The GFS_v15p2_no_nsst physics suite uses the parameterizations in the following order: + - \ref GFS_RRTMG + - \ref GFS_SFCLYR + - \ref GFS_OCEAN + - \ref GFS_NOAH + - \ref GFS_SFCSICE + - \ref GFS_HEDMF + - \ref GFS_UGWP_v0 + - \ref GFS_RAYLEIGH + - \ref GFS_OZPHYS + - \ref GFS_H2OPHYS + - \ref GFS_SAMFdeep + - \ref GFS_SAMFshal + - \ref GFDL_cloud + - \ref GFS_CALPRECIPTYPE + +\section sdf_gfsv15p2_no_nsst Suite Definition File +- For GRIB2 initialization data: \subpage suite_FV3_GFS_v15p2_no_nsst_xml + +\section gfs15p2nonsst_nml_opt_des Namelist + +- \b &gfs_physics_nml +\n \c fhzero = 6 +\n \c h2o_phys = .true. +\n \c ldiag3d = .false. +\n \c fhcyc = 24 +\n \c use_ufo = .true. +\n \c pre_rad = .false. +\n \c ncld = 5 +\n \c imp_physics = 11 +\n \c pdfcld = .false. +\n \c fhswr = 3600. +\n \c fhlwr = 3600. +\n \c ialb = 1 +\n \c iems = 1 +\n \c iaer = 111 +\n \c ico2 = 2 +\n \c isubc_sw = 2 +\n \c isubc_lw = 2 +\n \c isol = 2 +\n \c lwhtr = .true. +\n \c swhtr = .true. +\n \c cnvgwd = .true. +\n \c shal_cnv = .true. +\n \c cal_pre = .false. +\n \c redrag = .true. +\n \c dspheat = .true. +\n \c hybedmf = .true. +\n \c random_clds = .false. +\n \c trans_trac = .true. +\n \c cnvcld = .true. +\n \c imfshalcnv = 2 +\n \c imfdeepcnv = 2 +\n \c cdmbgwd = 3.5,0.25 [1.0,1.2] [0.2,2.5] [0.125,3.0] ! [C768] [C384] [C192] [C96]L64 +\n \c prslrd0 = 0. +\n \c ivegsrc = 1 +\n \c isot = 1 +\n \c debug = .false. +\n \c oz_phys = .F. +\n \c oz_phys_2015 = .T. +\n \c nstf_name = 0,0,0,0,0 +\n \c nst_anl = .true. +\n \c psautco = 0.0008,0.0005 +\n \c prautco = 0.00015,0.00015 +\n \c lgfdlmprad = .true. +\n \c effr_in = .true. +\n \c do_sppt = .false. +\n \c do_shum = .false. +\n \c do_skeb = .false. +\n \c do_sfcperts = .false. + +- \b &gfdl_cloud_microphysics_nml +\n \c sedi_transport = .true. +\n \c do_sedi_heat = .false. +\n \c rad_snow = .true. +\n \c rad_graupel = .true. +\n \c rad_rain = .true. +\n \c const_vi = .F. +\n \c const_vs = .F. +\n \c const_vg = .F. +\n \c const_vr = .F. +\n \c vi_max = 1. +\n \c vs_max = 2. +\n \c vg_max = 12. +\n \c vr_max = 12. +\n \c qi_lim = 1. +\n \c prog_ccn = .false. +\n \c do_qa = .true. +\n \c fast_sat_adj = .true. +\n \c tau_l2v = 225. +\n \c tau_v2l = 150. +\n \c tau_g2v = 900. +\n \c rthresh = 10.e-6 +\n \c dw_land = 0.16 +\n \c dw_ocean = 0.10 +\n \c ql_gen = 1.0e-3 +\n \c ql_mlt = 1.0e-3 +\n \c qi0_crt = 8.0E-5 +\n \c qs0_crt = 1.0e-3 +\n \c tau_i2s = 1000. +\n \c c_psaci = 0.05 +\n \c c_pgacs = 0.01 +\n \c rh_inc = 0.30 +\n \c rh_inr = 0.30 +\n \c rh_ins = 0.30 +\n \c ccn_l = 300. +\n \c ccn_o = 100. +\n \c c_paut = 0.5 +\n \c c_cracw = 0.8 +\n \c use_ppm = .false. +\n \c use_ccn = .true. +\n \c mono_prof = .true. +\n \c z_slope_liq = .true. +\n \c z_slope_ice = .true. +\n \c de_ice = .false. +\n \c fix_negative = .true. +\n \c icloud_f = 1 +\n \c mp_time = 150. + +*/ diff --git a/physics/docs/pdftxt/GFSv15p2_suite.txt b/physics/docs/pdftxt/GFSv15p2_suite.txt new file mode 100644 index 000000000..944fd49f1 --- /dev/null +++ b/physics/docs/pdftxt/GFSv15p2_suite.txt @@ -0,0 +1,133 @@ +/** +\page GFS_v15p2_page GFS_v15p2 Suite + +\section gfs1_suite_overview Overview + +Suite GFS_v15p2 has the parameterizations used in the GFS v15 implemented operationally +in June 2019. + +The GFS_v15p2 physics suite uses the parameterizations in the following order: + - \ref GFS_RRTMG + - \ref GFS_SFCLYR + - \ref GFS_NSST + - \ref GFS_OCEAN + - \ref GFS_NOAH + - \ref GFS_SFCSICE + - \ref GFS_HEDMF + - \ref GFS_UGWP_v0 + - \ref GFS_RAYLEIGH + - \ref GFS_OZPHYS + - \ref GFS_H2OPHYS + - \ref GFS_SAMFdeep + - \ref GFS_SAMFshal + - \ref GFDL_cloud + - \ref GFS_CALPRECIPTYPE + +\section sdf_gfsv15p2 Suite Definition File +- For NEMSIO initialization data: \subpage suite_FV3_GFS_v15p2_xml + +\section gfs15p2_nml_opt_des Namelist + +- \b &gfs_physics_nml +\n \c fhzero = 6 +\n \c h2o_phys = .true. +\n \c ldiag3d = .false. +\n \c fhcyc = 24 +\n \c use_ufo = .true. +\n \c pre_rad = .false. +\n \c ncld = 5 +\n \c imp_physics = 11 +\n \c pdfcld = .false. +\n \c fhswr = 3600. +\n \c fhlwr = 3600. +\n \c ialb = 1 +\n \c iems = 1 +\n \c iaer = 111 +\n \c ico2 = 2 +\n \c isubc_sw = 2 +\n \c isubc_lw = 2 +\n \c isol = 2 +\n \c lwhtr = .true. +\n \c swhtr = .true. +\n \c cnvgwd = .true. +\n \c shal_cnv = .true. +\n \c cal_pre = .false. +\n \c redrag = .true. +\n \c dspheat = .true. +\n \c hybedmf = .true. +\n \c random_clds = .false. +\n \c trans_trac = .true. +\n \c cnvcld = .true. +\n \c imfshalcnv = 2 +\n \c imfdeepcnv = 2 +\n \c cdmbgwd = 3.5,0.25 [1.0,1.2] [0.2,2.5] [0.125,3.0] ! [C768] [C384] [C192] [C96]L64 +\n \c prslrd0 = 0. +\n \c ivegsrc = 1 +\n \c isot = 1 +\n \c debug = .false. +\n \c oz_phys = .F. +\n \c oz_phys_2015 = .T. +\n \c nstf_name = @[NSTF_NAME] +\n \c nst_anl = .true. +\n \c psautco = 0.0008,0.0005 +\n \c prautco = 0.00015,0.00015 +\n \c lgfdlmprad = .true. +\n \c effr_in = .true. +\n \c do_sppt = .false. +\n \c do_shum = .false. +\n \c do_skeb = .false. +\n \c do_sfcperts = .false. + +- \b &gfdl_cloud_microphysics_nml +\n \c sedi_transport = .true. +\n \c do_sedi_heat = .false. +\n \c rad_snow = .true. +\n \c rad_graupel = .true. +\n \c rad_rain = .true. +\n \c const_vi = .F. +\n \c const_vs = .F. +\n \c const_vg = .F. +\n \c const_vr = .F. +\n \c vi_max = 1. +\n \c vs_max = 2. +\n \c vg_max = 12. +\n \c vr_max = 12. +\n \c qi_lim = 1. +\n \c prog_ccn = .false. +\n \c do_qa = .true. +\n \c fast_sat_adj = .true. +\n \c tau_l2v = 225. +\n \c tau_v2l = 150. +\n \c tau_g2v = 900. +\n \c rthresh = 10.e-6 +\n \c dw_land = 0.16 +\n \c dw_ocean = 0.10 +\n \c ql_gen = 1.0e-3 +\n \c ql_mlt = 1.0e-3 +\n \c qi0_crt = 8.0E-5 +\n \c qs0_crt = 1.0e-3 +\n \c tau_i2s = 1000. +\n \c c_psaci = 0.05 +\n \c c_pgacs = 0.01 +\n \c rh_inc = 0.30 +\n \c rh_inr = 0.30 +\n \c rh_ins = 0.30 +\n \c ccn_l = 300. +\n \c ccn_o = 100. +\n \c c_paut = 0.5 +\n \c c_cracw = 0.8 +\n \c use_ppm = .false. +\n \c use_ccn = .true. +\n \c mono_prof = .true. +\n \c z_slope_liq = .true. +\n \c z_slope_ice = .true. +\n \c de_ice = .false. +\n \c fix_negative = .true. +\n \c icloud_f = 1 +\n \c mp_time = 150. + +\note nstf_name = \f$[2,0,0,0,0]^1 [2,1,0,0,0]^2 \f$ +- \f$^1\f$ NSST is on and coupled with spin up off +- \f$^2\f$ NSST is on and coupled with spin up on + +*/ diff --git a/physics/docs/pdftxt/GFSv16beta_no_nsst_suite.txt b/physics/docs/pdftxt/GFSv16beta_no_nsst_suite.txt new file mode 100644 index 000000000..3e5205199 --- /dev/null +++ b/physics/docs/pdftxt/GFSv16beta_no_nsst_suite.txt @@ -0,0 +1,167 @@ +/** +\page GFS_v16beta_no_nsst_page GFS_v16beta_no_nsst Suite + +\section gfsv16beta_no_nsst_suite_overview Overview + +Suite GFS_v16beta_no_nsst is a companion suite of GFS_v16beta with GRIB2 data initialization. + +The GFS_v16beta_no_nsst physics suite uses the parameterizations in the following order: + - \ref GFS_RRTMG + - \ref GFS_SFCLYR + - \ref GFS_OCEAN + - \ref GFS_NOAH + - \ref GFS_SFCSICE + - \ref GFS_SATMEDMFVDIFQ + - \ref GFS_UGWP_v0 + - \ref GFS_RAYLEIGH + - \ref GFS_OZPHYS + - \ref GFS_H2OPHYS + - \ref GFS_SAMFdeep + - \ref GFS_SAMFshal + - \ref GFDL_cloud + - \ref GFS_CALPRECIPTYPE + +\section sdf_gfsv16bnonsst Suite Definition File +- For GRIB2 initialization data: \subpage suite_FV3_GFS_v16beta_no_nsst_xml + +\section gfs16betanonsst_nml_opt_des Namelist + +- \b &gfs_physics_nml +\n \c fhzero = 6 +\n \c h2o_phys = .true. +\n \c ldiag3d = .false. +\n \c fhcyc = 24 +\n \c use_ufo = .true. +\n \c pre_rad = .false. +\n \c ncld = 5 +\n \c imp_physics = 11 +\n \c pdfcld = .false. +\n \c fhswr = 3600. +\n \c fhlwr = 3600. +\n \c ialb = 1 +\n \c iems = 1 +\n \c iaer = 5111 +\n \c icliq_sw = 2 +\n \c iovr_lw = 3 +\n \c iovr_sw = 3 +\n \c ico2 = 2 +\n \c isubc_sw = 2 +\n \c isubc_lw = 2 +\n \c isol = 2 +\n \c lwhtr = .true. +\n \c swhtr = .true. +\n \c cnvgwd = .true. +\n \c shal_cnv = .true. +\n \c cal_pre = .false. +\n \c redrag = .true. +\n \c dspheat = .true. +\n \c hybedmf = .false. +\n \c satmedmf = .true. +\n \c isatmedmf = 1 +\n \c lheatstrg = .true. +\n \c random_clds = .false. +\n \c trans_trac = .true. +\n \c cnvcld = .true. +\n \c imfshalcnv = 2 +\n \c imfdeepcnv = 2 +\n \c cdmbgwd = 4.0,0.15,1.0,1.0 [1.1,0.72,1.0,1.0] [0.23,1.5,1.0,1.0] [0.14,1.8,1.0,1.0] ! [C768] [C384] [C192] [C96]L64 +\n \c prslrd0 = 0. +\n \c ivegsrc = 1 +\n \c isot = 1 +\n \c lsoil = 4 +\n \c lsm = 1 +\n \c iopt_dveg = 1 +\n \c iopt_crs = 1 +\n \c iopt_btr = 1 +\n \c iopt_run = 1 +\n \c iopt_sfc = 1 +\n \c iopt_frz = 1 +\n \c iopt_inf = 1 +\n \c iopt_rad = 1 +\n \c iopt_alb = 2 +\n \c iopt_snf = 4 +\n \c iopt_tbot = 2 +\n \c iopt_stc = 1 +\n \c debug = .false. +\n \c oz_phys = .F. +\n \c oz_phys_2015 = .T. +\n \c nstf_name = 0,0,0,0,0 +\n \c nst_anl = .true. +\n \c psautco = 0.0008,0.0005 +\n \c prautco = 0.00015,0.00015 +\n \c lgfdlmprad = .true. +\n \c effr_in = .true. +\n \c ldiag_ugwp = .false. +\n \c do_ugwp = .false. +\n \c do_tofd = .true. +\n \c do_sppt = .false. +\n \c do_shum = .false. +\n \c do_skeb = .false. +\n \c do_sfcperts = .false. + + +- \b &gfdl_cloud_microphysics_nml +\n \c sedi_transport = .true. +\n \c do_sedi_heat = .false. +\n \c rad_snow = .true. +\n \c rad_graupel = .true. +\n \c rad_rain = .true. +\n \c const_vi = .F. +\n \c const_vs = .F. +\n \c const_vg = .F. +\n \c const_vr = .F. +\n \c vi_max = 1. +\n \c vs_max = 2. +\n \c vg_max = 12. +\n \c vr_max = 12. +\n \c qi_lim = 1. +\n \c prog_ccn = .false. +\n \c do_qa = .true. +\n \c fast_sat_adj = .true. +\n \c tau_l2v = 225. +\n \c tau_v2l = 150. +\n \c tau_g2v = 900. +\n \c rthresh = 10.e-6 +\n \c dw_land = 0.16 +\n \c dw_ocean = 0.10 +\n \c ql_gen = 1.0e-3 +\n \c ql_mlt = 1.0e-3 +\n \c qi0_crt = 8.0E-5 +\n \c qs0_crt = 1.0e-3 +\n \c tau_i2s = 1000. +\n \c c_psaci = 0.05 +\n \c c_pgacs = 0.01 +\n \c rh_inc = 0.30 +\n \c rh_inr = 0.30 +\n \c rh_ins = 0.30 +\n \c ccn_l = 300. +\n \c ccn_o = 100. +\n \c c_paut = 0.5 +\n \c c_cracw = 0.8 +\n \c use_ppm = .false. +\n \c use_ccn = .true. +\n \c mono_prof = .true. +\n \c z_slope_liq = .true. +\n \c z_slope_ice = .true. +\n \c de_ice = .false. +\n \c fix_negative = .true. +\n \c icloud_f = 1 +\n \c mp_time = 150. +\n \c reiflag = 2 + + +- \b &cires_ugwp_nml +\n \c knob_ugwp_solver = 2 +\n \c knob_ugwp_source = 1,1,0,0 +\n \c knob_ugwp_wvspec = 1,25,25,25 +\n \c knob_ugwp_azdir = 2,4,4,4 +\n \c knob_ugwp_stoch = 0,0,0,0 +\n \c knob_ugwp_effac = 1,1,1,1 +\n \c knob_ugwp_doaxyz = 1 +\n \c knob_ugwp_doheat = 1 +\n \c knob_ugwp_dokdis = 1 +\n \c knob_ugwp_ndx4lh = 1 +\n \c knob_ugwp_version = 0 +\n \c launch_level = 27 + +*/ diff --git a/physics/docs/pdftxt/GFSv16beta_suite.txt b/physics/docs/pdftxt/GFSv16beta_suite.txt new file mode 100644 index 000000000..8389d0c40 --- /dev/null +++ b/physics/docs/pdftxt/GFSv16beta_suite.txt @@ -0,0 +1,176 @@ +/** +\page GFS_v16beta_page GFS_v16beta Suite + +\section gfsv16beta_suite_overview Overview + +Version 16 of the Global Forecast System (GFS) will be implemented operationally by the NOAA +National Centers for Environmental Prediction (NCEP) in 2021. GFS_v16beta is a prototype of +the GFS_v16 suite. The main difference between the GFS_v15p2 and GFS_v16beta suites is the +replacement of the K-based EDMF PBL scheme with a moist TKE based one. + + +The GFS_v16beta physics suite uses the parameterizations in the following order: + - \ref GFS_RRTMG + - \ref GFS_SFCLYR + - \ref GFS_NSST + - \ref GFS_OCEAN + - \ref GFS_NOAH + - \ref GFS_SFCSICE + - \ref GFS_SATMEDMFVDIFQ + - \ref GFS_UGWP_v0 + - \ref GFS_RAYLEIGH + - \ref GFS_OZPHYS + - \ref GFS_H2OPHYS + - \ref GFS_SAMFdeep + - \ref GFS_SAMFshal + - \ref GFDL_cloud + - \ref GFS_CALPRECIPTYPE + +\section sdf_gfsv16b Suite Definition File +- For NEMSIO initialization data: \subpage suite_FV3_GFS_v16beta_xml + +\section gfs16beta_nml_opt_des Namelist + +- \b &gfs_physics_nml +\n \c fhzero = 6 +\n \c h2o_phys = .true. +\n \c ldiag3d = .false. +\n \c fhcyc = 24 +\n \c use_ufo = .true. +\n \c pre_rad = .false. +\n \c ncld = 5 +\n \c imp_physics = 11 +\n \c pdfcld = .false. +\n \c fhswr = 3600. +\n \c fhlwr = 3600. +\n \c ialb = 1 +\n \c iems = 1 +\n \c iaer = 5111 +\n \c icliq_sw = 2 +\n \c iovr_lw = 3 +\n \c iovr_sw = 3 +\n \c ico2 = 2 +\n \c isubc_sw = 2 +\n \c isubc_lw = 2 +\n \c isol = 2 +\n \c lwhtr = .true. +\n \c swhtr = .true. +\n \c cnvgwd = .true. +\n \c shal_cnv = .true. +\n \c cal_pre = .false. +\n \c redrag = .true. +\n \c dspheat = .true. +\n \c hybedmf = .false. +\n \c satmedmf = .true. +\n \c isatmedmf = 1 +\n \c lheatstrg = .true. +\n \c random_clds = .false. +\n \c trans_trac = .true. +\n \c cnvcld = .true. +\n \c imfshalcnv = 2 +\n \c imfdeepcnv = 2 +\n \c cdmbgwd = 4.0,0.15,1.0,1.0 [1.1,0.72,1.0,1.0] [0.23,1.5,1.0,1.0] [0.14,1.8,1.0,1.0] ! [C768] [C384] [C192] [C96]L64 +\n \c prslrd0 = 0. +\n \c ivegsrc = 1 +\n \c isot = 1 +\n \c lsoil = 4 +\n \c lsm = 1 +\n \c iopt_dveg = 1 +\n \c iopt_crs = 1 +\n \c iopt_btr = 1 +\n \c iopt_run = 1 +\n \c iopt_sfc = 1 +\n \c iopt_frz = 1 +\n \c iopt_inf = 1 +\n \c iopt_rad = 1 +\n \c iopt_alb = 2 +\n \c iopt_snf = 4 +\n \c iopt_tbot = 2 +\n \c iopt_stc = 1 +\n \c debug = .false. +\n \c oz_phys = .F. +\n \c oz_phys_2015 = .T. +\n \c nstf_name = @[NSTF_NAME] +\n \c nst_anl = .true. +\n \c psautco = 0.0008,0.0005 +\n \c prautco = 0.00015,0.00015 +\n \c lgfdlmprad = .true. +\n \c effr_in = .true. +\n \c ldiag_ugwp = .false. +\n \c do_ugwp = .false. +\n \c do_tofd = .true. +\n \c do_sppt = .false. +\n \c do_shum = .false. +\n \c do_skeb = .false. +\n \c do_sfcperts = .false. + + +- \b &gfdl_cloud_microphysics_nml +\n \c sedi_transport = .true. +\n \c do_sedi_heat = .false. +\n \c rad_snow = .true. +\n \c rad_graupel = .true. +\n \c rad_rain = .true. +\n \c const_vi = .F. +\n \c const_vs = .F. +\n \c const_vg = .F. +\n \c const_vr = .F. +\n \c vi_max = 1. +\n \c vs_max = 2. +\n \c vg_max = 12. +\n \c vr_max = 12. +\n \c qi_lim = 1. +\n \c prog_ccn = .false. +\n \c do_qa = .true. +\n \c fast_sat_adj = .true. +\n \c tau_l2v = 225. +\n \c tau_v2l = 150. +\n \c tau_g2v = 900. +\n \c rthresh = 10.e-6 +\n \c dw_land = 0.16 +\n \c dw_ocean = 0.10 +\n \c ql_gen = 1.0e-3 +\n \c ql_mlt = 1.0e-3 +\n \c qi0_crt = 8.0E-5 +\n \c qs0_crt = 1.0e-3 +\n \c tau_i2s = 1000. +\n \c c_psaci = 0.05 +\n \c c_pgacs = 0.01 +\n \c rh_inc = 0.30 +\n \c rh_inr = 0.30 +\n \c rh_ins = 0.30 +\n \c ccn_l = 300. +\n \c ccn_o = 100. +\n \c c_paut = 0.5 +\n \c c_cracw = 0.8 +\n \c use_ppm = .false. +\n \c use_ccn = .true. +\n \c mono_prof = .true. +\n \c z_slope_liq = .true. +\n \c z_slope_ice = .true. +\n \c de_ice = .false. +\n \c fix_negative = .true. +\n \c icloud_f = 1 +\n \c mp_time = 150. +\n \c reiflag = 2 + + +- \b &cires_ugwp_nml +\n \c knob_ugwp_solver = 2 +\n \c knob_ugwp_source = 1,1,0,0 +\n \c knob_ugwp_wvspec = 1,25,25,25 +\n \c knob_ugwp_azdir = 2,4,4,4 +\n \c knob_ugwp_stoch = 0,0,0,0 +\n \c knob_ugwp_effac = 1,1,1,1 +\n \c knob_ugwp_doaxyz = 1 +\n \c knob_ugwp_doheat = 1 +\n \c knob_ugwp_dokdis = 1 +\n \c knob_ugwp_ndx4lh = 1 +\n \c knob_ugwp_version = 0 +\n \c launch_level = 27 + +\note nstf_name = \f$[2,0,0,0,0]^1 [2,1,0,0,0]^2\f$ +- \f$^1\f$ NSST is on and coupled with spin up off +- \f$^2\f$ NSST is on and coupled with spin up on + +*/ diff --git a/physics/docs/pdftxt/GSD_adv_suite.txt b/physics/docs/pdftxt/GSD_adv_suite.txt index fb662bc22..39c5ebd20 100644 --- a/physics/docs/pdftxt/GSD_adv_suite.txt +++ b/physics/docs/pdftxt/GSD_adv_suite.txt @@ -1,47 +1,38 @@ /** -\page GSD_v0_page GSD_v0 Suite +\page GSD_v1_page GSD_v1 Suite \section gsd_suite_overview Overview -The original Rapid Update Cycle (RUC), implemented in 1994, was designed to provide accurate short-range (0 to 12-hr) -numerical forecast guidance for weather-sensitive users, including those in the U.S. aviation community. -The RUC started to run every hour starting in 1998. Significant weather forecasting problems that occur in the 0- to -12-hr range include severe weather in all seasons (for example, tornadoes, severe thunderstorms, crippling snow, and -ice storms) and hazards to aviation (for example, clear air turbulence, icing, and downbursts). The RUC soon became a -key model for short-range convectiion forecasts and for the pre-convective environments. +Suite GSD_v1 contains the parameterizations used in the NOAA operational Rapid Refresh (RAP) +and High-Resolution Rapid Refresh (HRRR) models. These models runs at 13- and 3- km resolution, +respectively. -The RAP, which replaced the RUC in 2012, runs hourly at the National Centers for Environmental Prediction (NCEP), providing -high frequency updates of current conditions and short-range forecasts over North America at 13km resolution. A CONUS-nested -version at 3-km resolution called the High Resolution Rapid Refresh (HRRR), was implemented in the fall of 2014. Additional Model Information Links: - https://rapidrefresh.noaa.gov - https://rapidrefresh.noaa.gov/hrrr/ -The advanced GSD RAP/HRRR physics suite uses the parameterizations in the following order: +The GSD_v1 physics suite uses the parameterizations in the following order: - \ref GFS_RRTMG - \ref GFS_SFCLYR - \ref GFS_NSST - \ref GSD_RUCLSM - \ref GSD_MYNNEDMF - - \ref GFS_GWDPS + - \ref GFS_UGWP_v0 - \ref GFS_RAYLEIGH - \ref GFS_OZPHYS - \ref GFS_H2OPHYS - \ref GSD_CU_GF - \ref cu_gf_deep_group - \ref cu_gf_sh_group - - \ref GFS_GWDC - \ref GSD_THOMPSON - \ref GFS_CALPRECIPTYPE \section sdf_gsdsuite Suite Definition File - -The GSD RAP/HRRR physics suite uses the parameterizations in the following order, as defined in \c SCM_GSD_v0: \code - + @@ -72,9 +63,10 @@ The GSD RAP/HRRR physics suite uses the parameterizations in the following order GFS_suite_stateout_reset get_prs_fv3 GFS_suite_interstitial_1 - dcyc2t3 GFS_surface_generic_pre GFS_surface_composites_pre + dcyc2t3 + GFS_surface_composites_inter GFS_suite_interstitial_2 @@ -85,19 +77,22 @@ The GSD RAP/HRRR physics suite uses the parameterizations in the following order sfc_nst sfc_nst_post lsm_ruc + lsm_ruc_sfc_sice_pre + sfc_sice + lsm_ruc_sfc_sice_post GFS_surface_loop_control_part2 GFS_surface_composites_post - dcyc2t3_post sfc_diag sfc_diag_post GFS_surface_generic_post mynnedmf_wrapper GFS_GWD_generic_pre - gwdps - gwdps_post + cires_ugwp + cires_ugwp_post + GFS_GWD_generic_post rayleigh_damp GFS_suite_stateout_update ozphys_2015 @@ -108,9 +103,6 @@ The GSD RAP/HRRR physics suite uses the parameterizations in the following order cu_gf_driver_pre cu_gf_driver GFS_DCNV_generic_post - gwdc_pre - gwdc - gwdc_post GFS_SCNV_generic_pre GFS_SCNV_generic_post GFS_suite_interstitial_4 @@ -126,73 +118,149 @@ The GSD RAP/HRRR physics suite uses the parameterizations in the following order - \endcode -\section gsd_nml_option Namelist Option +\section gsd_nml_option Namelist \code &gfs_physics_nml - fhzero = 6. - h2o_phys = .true. - ldiag3d = .true. - fhcyc = 0. - nst_anl = .true. - use_ufo = .true. - pre_rad = .false. - ncld = 5 - imp_physics = 8 - ltaerosol = .true. - lradar = .true. - ttendlim = -999. - pdfcld = .false. - fhswr = 3600. - fhlwr = 3600. - ialb = 1 - iems = 1 - iaer = 111 - ico2 = 2 - isubc_sw = 2 - isubc_lw = 2 - isol = 2 - lwhtr = .true. - swhtr = .true. - cnvgwd = .true. - shal_cnv = .true. - cal_pre = .false. - redrag = .true. - dspheat = .true. - hybedmf = .false. - satmedmf = .false. - lheatstrg = .false. - do_mynnedmf = .true. - do_mynnsfclay = .false. - random_clds = .false. - trans_trac = .true. - cnvcld = .true. - imfshalcnv = 3 - imfdeepcnv = 3 - cdmbgwd = 3.5,0.25 - prslrd0 = 0. - ivegsrc = 1 - isot = 1 - debug = .false. - oz_phys = .false. - oz_phys_2015 = .true. - nstf_name = 2,1,1,0,5 - cplflx = .false. - iau_delthrs = 6 - iaufhrs = 30 - iau_inc_files = "''" - do_sppt = .false. - do_shum = .false. - do_skeb = .false. - do_sfcperts = .false. - lsm = 2 - lsoil_lsm = 9 + fhzero = 6. + h2o_phys = .true. + ldiag3d = .true. + fhcyc = 0. + nst_anl = .true. + use_ufo = .true. + pre_rad = .false. + ncld = 5 + imp_physics = 8 + ltaerosol = .true. + lradar = .true. + ttendlim = 0.004 + pdfcld = .false. + fhswr = 3600. + fhlwr = 3600. + ialb = 1 + iems = 1 + iaer = 111 + ico2 = 2 + isubc_sw = 2 + isubc_lw = 2 + isol = 2 + lwhtr = .true. + swhtr = .true. + cnvgwd = .true. + shal_cnv = .true. + cal_pre = .false. + redrag = .true. + dspheat = .true. + hybedmf = .false. + satmedmf = .false. + lheatstrg = .false. + do_mynnedmf = .true. + do_mynnsfclay = .false. + random_clds = .false. + trans_trac = .true. + cnvcld = .true. + imfshalcnv = 3 + imfdeepcnv = 3 + cdmbgwd = 3.5,0.25 + prslrd0 = 0. + ivegsrc = 1 + isot = 1 + debug = .false. + oz_phys = .false. + oz_phys_2015 = .true. + nstf_name = 2,1,1,0,5 + cplflx = .false. + iau_delthrs = 6 + iaufhrs = 30 + iau_inc_files = "''" + do_sppt = .false. + do_shum = .false. + do_skeb = .false. + do_sfcperts = .false. + lsm = 3 + lsoil_lsm = 9 + iopt_dveg = 2 + iopt_crs = 1 + iopt_btr = 1 + iopt_run = 1 + iopt_sfc = 1 + iopt_frz = 1 + iopt_inf = 1 + iopt_rad = 1 + iopt_alb = 2 + iopt_snf = 4 + iopt_tbot = 2 + iopt_stc = 1 icloud_bl = 1 bl_mynn_tkeadvect = .true. bl_mynn_edmf = 1 bl_mynn_edmf_mom = 1 + gwd_opt = 1 +/ + +&gfdl_cloud_microphysics_nml + sedi_transport = .true. + do_sedi_heat = .false. + rad_snow = .true. + rad_graupel = .true. + rad_rain = .true. + const_vi = .F. + const_vs = .F. + const_vg = .F. + const_vr = .F. + vi_max = 1. + vs_max = 2. + vg_max = 12. + vr_max = 12. + qi_lim = 1. + prog_ccn = .false. + do_qa = .false. + fast_sat_adj = .false. + tau_l2v = 225. + tau_v2l = 150. + tau_g2v = 900. + rthresh = 10.e-6 + dw_land = 0.16 + dw_ocean = 0.10 + ql_gen = 1.0e-3 + ql_mlt = 1.0e-3 + qi0_crt = 8.0E-5 + qs0_crt = 1.0e-3 + tau_i2s = 1000. + c_psaci = 0.05 + c_pgacs = 0.01 + rh_inc = 0.30 + rh_inr = 0.30 + rh_ins = 0.30 + ccn_l = 300. + ccn_o = 100. + c_paut = 0.5 + c_cracw = 0.8 + use_ppm = .false. + use_ccn = .true. + mono_prof = .true. + z_slope_liq = .true. + z_slope_ice = .true. + de_ice = .false. + fix_negative = .true. + icloud_f = 1 + mp_time = 150. +/ + +&cires_ugwp_nml + knob_ugwp_solver = 2 + knob_ugwp_source = 1,1,0,0 + knob_ugwp_wvspec = 1,25,25,25 + knob_ugwp_azdir = 2,4,4,4 + knob_ugwp_stoch = 0,0,0,0 + knob_ugwp_effac = 1,1,1,1 + knob_ugwp_doaxyz = 1 + knob_ugwp_doheat = 1 + knob_ugwp_dokdis = 1 + knob_ugwp_ndx4lh = 1 + knob_ugwp_version = 0 + launch_level = 25 / \endcode diff --git a/physics/docs/pdftxt/UGWPv0.txt b/physics/docs/pdftxt/UGWPv0.txt deleted file mode 100644 index da7009b79..000000000 --- a/physics/docs/pdftxt/UGWPv0.txt +++ /dev/null @@ -1,21 +0,0 @@ -/** -\page UGWPv0 Unified Gravity Wave Physics Version 0 -\section des_UGWP Description - -Gravity waves (GWs) are generated by a variety of sources in the atmosphere including orographic GWs (OGWs; quasi-stationary waves) and non-orographic GWs (NGWs; non-stationary oscillations). The subgrid scale parameterization scheme for OGWs can be found in Section \ref GFS_GWDPS. This scheme represents the operational version of the subgrid scale orography effects in Version 15 of Global Forecast System (GFS). - -The NGW physics scheme parameterizes the effects of non-stationary subgrid-scale waves in the global atmosphere models extended into the stratosphere, mesosphere, and thermosphere. These non-stationary oscillations with periods bounded by Coriolis and Brunt-Väisälä frequencies and typical horizontal scales from tens to several hundreds of kilometers are forced by the imbalance of convective and frontal/jet dynamics in the troposphere and lower stratosphere (Fritts 1984 \cite fritts_1984; Alexander et al. 2010 \cite alexander_et_al_2010; Plougonven and Zhang 2014 \cite plougonven_and_zhang_2014). The NGWs propagate upwards and the amplitudes exponentially grow with altitude until instability and breaking of waves occur. Convective and dynamical instability induced by GWs with large amplitudes can trigger production of small-scale turbulence and self-destruction of waves. The latter process in the theory of atmospheric GWs is frequently referred as the wave saturation (Lindzen 1981 \cite lindzen_1981; Weinstock 1984 \cite weinstock_1984; Fritts 1984 \cite fritts_1984). Herein, “saturation” or "breaking" refers to any processes that act to reduce wave amplitudes due to instabilities and/or interactions arising from large-amplitude perturbations limiting the exponential growth of GWs with height. Background dissipation processes such as molecular diffusion and radiative cooling, in contrast, act independently of GW amplitudes. In the middle atmosphere, impacts of NGW saturation (or breaking) and dissipation on the large-scale circulation, mixing, and transport have been acknowledged in the physics of global weather and climate models after pioneering studies by Lindzen 1981 \cite lindzen_1981 and Holton 1983 \cite holton_1983. Comprehensive reviews on the physics of NGWs and OGWs in the climate research and weather forecasting highlighted the variety of parameterization schemes for NGWs （Alexander et al. 2010 \cite alexander_et_al_2010; Geller et al. 2013 \cite geller_et_al_2013; Garcia et al. 2017 \cite garcia_et_al_2017). They are formulated using different aspects of the nonlinear and linear propagation, instability, breaking and dissipation of waves along with different specifications of GW sources (Garcia et al. 2007 \cite garcia_et_al_2007; Richter et al 2010 \cite richter_et_al_2010; Eckermann et al. 2009 \cite eckermann_et_al_2009; Eckermann 2011 \cite eckermann_2011; Lott et al. 2012 \cite lott_et_al_2012). - -The current operational GFS physics parameterizes effects of stationary OGWs and convective GWs, neglecting the impacts of non-stationary subgrid scale GW physics. This leads to well-known shortcomings in the global model predictions in the stratosphere and upper atmosphere (Alexander et al. 2010 \cite alexander_et_al_2010; Geller et al. 2013). In order to describe the effects of unresolved GWs by dynamical cores in global forecast models, subgrid scales physics of stationary and non-stationary GWs needs to be implemented in the self-consistent manner under the Unified Gravity Wave Physics (UGWP) framework. - -The concept of UGWP and the related programming architecture implemented in FV3GFS was first proposed by CU-CIRES, NOAA Space Weather Prediction Center (SWPC) and Environmental Modeling Center (EMC) for the Unified Forecast System (UFS) with variable positions of the model top lids (Alpert et al. 2019 \cite alpert_et_al_2019; Yudin et al. 2016 \cite yudin_et_al_2016; Yudin et al. 2018 \cite yudin_et_al_2018). As above, the UGWP considers identical GW propagation solvers for OGWs and NGWs with different approaches for specification of subgrid wave sources. The current set of the input and control parameters for UGWP version 0 (UGWP-v0) can select different options for GW effects including momentum deposition (also called GW drag), heat deposition, and mixing by eddy viscosity, conductivity and diffusion. The input GW parameters can control the number of directional azimuths in which waves can propagate, number of waves in single direction, and the interface model layer from the surface at which NGWs can be launched. Among the input parameters, the GW efficiency factors reflect intermittency of wave excitation. They can vary with horizontal resolutions, reflecting capability of the FV3 dynamical core to resolve mesoscale wave activity with the enhancement of model resolution. The prescribed distributions for vertical momentum flux (VMF) of NGWs have been employed in the global forecast models of NWP centers and reanalysis projects to ease tuning of GW schemes to the climatology of the middle atmosphere dynamics in the absence of the global wind data above about 35 km (Eckermann et al. 2009 \cite eckermann_et_al_2009; Molod et al. 2015 \cite molod_et_al_2015). These distributions of VMF qualitatively describe the general features of the latitudinal and seasonal variations of the global GW activity in the lower stratosphere, observed from the ground and space (Ern et al. 2018 \cite ern_et_al_2018). For the long-term climate projections, global models seek to establish communication between model physics and dynamics. This provides variable in time and space excitation of subgrid GWs under year-to-year variations of solar input and anthropogenic emissions (Richter et al 2010 \cite richter_et_al_2010; 2014 \cite richter_et_al_2014). - -Note that in the first release of UGWP (UGWP-v0), the momentum and heat deposition due to GW breaking and dissipation have been tested in the multi-year simulations and medium-range forecasts using FV3GFS-L127 configuration with top lid at about 80 km. In addition, the eddy mixing effects induced by instability of GWs are not activated in this version. Along with the GW heat and momentum depositions, GW eddy mixing is an important element of the Whole Atmosphere Model (WAM) physics, as shown in WAM simulations with the spectral dynamics (Yudin et al. 2018 \cite yudin_et_al_2018). The additional impact of eddy mixing effects in the middle and upper atmosphere need to be further tested, evaluated, and orchestrated with the subgrid turbulent diffusion of the GFS physics (work in progress). In UFS, the WAM with FV3 dynamics (FV3-WAM) will represent the global atmosphere model configuration extended into the thermosphere (top lid at ~600 km). In the mesosphere and thermosphere, the background attenuation of subgrid waves due to molecular and turbulent diffusion, radiative damping and ion drag will be the additional mechanism of NGW and OGW dissipation along with convective and dynamical instability of waves described by the linear (Lindzen 1981 \cite lindzen_1981) and nonlinear (Weinstock 1984 \cite weinstock_1984; Hines 1997 \cite hines_1997) saturation theories. - -\section intra_UGWPv0 Intraphysics Communication -\ref arg_table_cires_ugwp_run - -\section gen_al_ugwpv0 General Algorithm -\ref cires_ugwp_run - -*/ diff --git a/physics/docs/pdftxt/all_shemes_list.txt b/physics/docs/pdftxt/all_shemes_list.txt index 7e5e3298e..4d7d08e90 100644 --- a/physics/docs/pdftxt/all_shemes_list.txt +++ b/physics/docs/pdftxt/all_shemes_list.txt @@ -1,11 +1,10 @@ /** \page allscheme_page Parameterizations and Suites Overview -\section allscheme_overview Physics Parameterizations +\section allscheme_overview Physical Parameterizations -In the CCPP-Physics v3.0 release, each parameterization is in its own modern Fortran module, - which facilitates model development and -code maintenance. While some individual parameterization can be invoked for the GMTB SCM, most users will assemble the +In the CCPP, each parameterization is in its own modern Fortran module, which facilitates model development and +code maintenance. While some individual parameterization can be invoked for the SCM, most users will assemble the parameterizations in suites. - \b Radiation @@ -38,19 +37,18 @@ parameterizations in suites. - \b Ozone \b Photochemical \b Production \b and \b Loss - \subpage GFS_OZPHYS - - \ref GFS_ozphys_2015 - \b Water \b Vapor \b Photochemical \b Production \b and \b Loss - \subpage GFS_H2OPHYS - \b Gravity \b Wave \b Drag - - \subpage GFS_GWDPS - - \subpage GFS_GWDC - - \subpage UGWPv0 + - \subpage GFS_UGWP_v0 + - \subpage GFS_GWDPS - \b Surface \b Layer \b and \b Simplified \b Ocean \b and \b Sea \b Ice \b Representation - \subpage GFS_SFCLYR - \subpage GFS_NSST + - \subpage GFS_OCEAN - \subpage GFS_SFCSICE - \b Others @@ -82,25 +80,34 @@ to the parameterization. \section allsuite_overview Physics Suites -The CCPP v3 includes the suite used in the GFS v15 implemented operationally in June 2019 (suite GFS_v15). Additionally, it includes three -developmental suites which are undergoing testing for possible future implementation in the UFS. Suite GFS_v15plus is identical to suite -GFS_v15 except for a replacement in the PBL parameterization (Han et al. 2019 \cite Han_2019 ). Suite csawmg differs from GFS_v15 as it +The CCPP includes the suite GFS_v15p2, which has the same parameterizations used in the GFS v15 implemented operationally in June 2019, and suite +GFS_v16beta, i.e., the beta version of the suite planned for GFS v16 to be implemented operationally in 2021. Suite GFS_v16beta is identical to +Suite GFS_v15p2 except for an update in the PBL parameterization (Han et al. 2019 \cite Han_2019 ). Additionally, CCPP v4 includes two +developmental suites which are undergoing testing to inform future implementations of the UFS. Suite csawmg differs from GFS_v15p2 as it contains different convection and microphysics schemes made available through a NOAA Climate Process Team (CPT) with components developed -at multiple research centers and universities, including Colorado State, Utah, NASA, NCAR, and EMC. Suite GSD_v0 differs from GFS_v15 as it +at multiple research centers and universities, including Colorado State, Utah, NASA, NCAR, and EMC. Suite GSD_v1 differs from GFS_v15p2 as it uses the convection, microphysics, and boundary layer schemes employed in the Rapid Refresh (RAP) and High-Resolution Rapid Refresh (HRRR \cite Benjamin_2016 ) operational models and was assembled by NOAA/GSD. An assessment of an earlier version of these suites can be found in the UFS portal -and in the GMTB website . +and in the DTC website . Two variant suites labelled as \a no_nsst are simplification of GFS_v15p2 and GFS_v16beta. +This simplification is needed when the UFS is initialized with files in GRIdded Binary Edition 2 (GRIB2) format instead of files in NOAA Environmental Modeling +System (NEMS) Input/Output (NEMSIO) format because the fields necesary to predict (SST) are not available in the GRIB2 files. Table 1. Physics suite options included in this documentation. \tableofcontents -| Phys suites | GFS_v15 | GFS_v15plus | csawmg | GSD_v0 | -|------------------|----------------------|----------------------|---------------------|----------------------| -| Deep Cu | \ref GFS_SAMFdeep | \ref GFS_SAMFdeep | \ref CSAW_scheme | \ref GSD_CU_GF | -| Shallow Cu | \ref GFS_SAMFshal | \ref GFS_SAMFshal | \ref GFS_SAMFshal | \ref GSD_MYNNEDMF and \ref cu_gf_sh_group | -| Microphysics | \ref GFDL_cloud | \ref GFDL_cloud | \ref CPT_MG3 | \ref GSD_THOMPSON | -| PBL/TURB | \ref GFS_HEDMF | \ref GFS_SATMEDMF | \ref GFS_HEDMF | \ref GSD_MYNNEDMF | -| Land | \ref GFS_NOAH | \ref GFS_NOAH | \ref GFS_NOAH | \ref GSD_RUCLSM | +| Physics suites | GFS_v15p2 | GFS_v16beta | csawmg | GSD_v1 | GFS_v15p2_no_nsst | GFS_v16beta_no_nsst | +|------------------|----------------------|--------------------------|---------------------|---------------------------------------------|-------------------------|---------------------------| +| Deep Cu | \ref GFS_SAMFdeep | \ref GFS_SAMFdeep | \ref CSAW_scheme | \ref GSD_CU_GF | \ref GFS_SAMFdeep | \ref GFS_SAMFdeep | +| Shallow Cu | \ref GFS_SAMFshal | \ref GFS_SAMFshal | \ref GFS_SAMFshal | \ref GSD_MYNNEDMF and \ref cu_gf_sh_group | \ref GFS_SAMFshal | \ref GFS_SAMFshal | +| Microphysics | \ref GFDL_cloud | \ref GFDL_cloud | \ref CPT_MG3 | \ref GSD_THOMPSON | \ref GFDL_cloud | \ref GFDL_cloud | +| PBL/TURB | \ref GFS_HEDMF | \ref GFS_SATMEDMFVDIFQ | \ref GFS_HEDMF | \ref GSD_MYNNEDMF | \ref GFS_HEDMF | \ref GFS_SATMEDMFVDIFQ | +| Radiation | \ref GFS_RRTMG | \ref GFS_RRTMG | \ref GFS_RRTMG | \ref GFS_RRTMG | \ref GFS_RRTMG | \ref GFS_RRTMG | +| Surface Layer | \ref GFS_SFCLYR | \ref GFS_SFCLYR | \ref GFS_SFCLYR | \ref GFS_SFCLYR | \ref GFS_SFCLYR | \ref GFS_SFCLYR | +| Land | \ref GFS_NOAH | \ref GFS_NOAH | \ref GFS_NOAH | \ref GSD_RUCLSM | \ref GFS_NOAH | \ref GFS_NOAH | +| Gravity Wave Drag| \ref GFS_UGWP_v0 | \ref GFS_UGWP_v0 | \ref GFS_UGWP_v0 | \ref GFS_UGWP_v0 | \ref GFS_UGWP_v0 | \ref GFS_UGWP_v0 | +| Ocean | \ref GFS_NSST | \ref GFS_NSST | \ref GFS_NSST | \ref GFS_NSST | \ref GFS_OCEAN | \ref GFS_OCEAN | +| Ozone | \ref GFS_OZPHYS | \ref GFS_OZPHYS | \ref GFS_OZPHYS | \ref GFS_OZPHYS | \ref GFS_OZPHYS | \ref GFS_OZPHYS | +| Water Vapor | \ref GFS_H2OPHYS | \ref GFS_H2OPHYS | \ref GFS_H2OPHYS | \ref GFS_H2OPHYS | \ref GFS_H2OPHYS | \ref GFS_H2OPHYS | \tableofcontents diff --git a/physics/docs/pdftxt/mainpage.txt b/physics/docs/pdftxt/mainpage.txt index 2ac121f3c..fdf7d1294 100644 --- a/physics/docs/pdftxt/mainpage.txt +++ b/physics/docs/pdftxt/mainpage.txt @@ -1,22 +1,26 @@ /** \mainpage Introduction -Welcome to the scientific documentation for the parameterizations available in the Common -Community Physics Package (CCPP) v3.0 public release. +Welcome to the scientific documentation for the parameterizations and suites available in the Common +Community Physics Package (CCPP) v4. -The CCPP-Physics is envisioned to contain parameterizations used by NOAA operational models for weather through -seasonal prediction timescales, as well as developmental schemes under consideration for upcoming +The CCPP-Physics is envisioned to contain parameterizations used in NOAA's Unified Forecast System (UFS) +applications for weather through seasonal prediction timescales, encompassing operational schemes as well as +developmental schemes under consideration for upcoming operational implementations. This version contains all parameterizations of the current operational GFS, -plus additional developmental schemes. The CCPP can currently be used with the Single Column Model (SCM) developed -by the Global Model Test Bed (GMTB) of the Developmental Testbed Center, as well as with the atmospheric component -of NOAA's Unified Forecast System (UFS-Atmosphere), which employs the the non-hydrostatic -Finite-Volume Cubed-Sphere (FV3) dynamic core. +plus additional developmental schemes. There are four suites supported for use with the Single Column Model (SCM) +developed by the Development Testbed Center (GFS_v15p2, GFS_v16beta, GSD_v1, and csawmg), and four suites +supported for use with the atmospheric component of the UFS (i.e., GFS_v15p2, GFS_v15p2_no_nsst, GFS_v16beta and +GFS_v16beta_no_nsst). The variants labelled as \a no_nsst are a simplification of GFS_v15p2 and GFS_v16beta suites +. This simplification is needed when the UFS is initialized with files in GRIdded Binary Edition 2 (GRIB2) +format instead of files in NOAA Environmental Modeling System (NEMS) Input/Output (NEMSIO) format because the +fields necessary to predict (SST) are not available in the GRIB2 files. In this website you will find documentation on various aspects of each parameterization, including a high-level overview of its function, the input/output argument list, and a description of the algorithm. -The latest CCPP public release is Version 3.0 (June 2019), and more details on it may be found on the - CCPP website hosted by the Global Model Test -Bed (GMTB) of the Developmental Testbed Center (DTC). +The latest CCPP public release is Version 4.0 (March 2020), and more details on it may be found on the + CCPP website hosted by +the Developmental Testbed Center (DTC). */ diff --git a/physics/docs/pdftxt/suite_FV3_GFS_v15p2.xml.txt b/physics/docs/pdftxt/suite_FV3_GFS_v15p2.xml.txt new file mode 100644 index 000000000..4074ddfc7 --- /dev/null +++ b/physics/docs/pdftxt/suite_FV3_GFS_v15p2.xml.txt @@ -0,0 +1,100 @@ +/** +\page suite_FV3_GFS_v15p2_xml suite_FV3_GFS_v15p2.xml + +\code + + + + + + + fv_sat_adj + + + + + GFS_time_vary_pre + GFS_rrtmg_setup + GFS_rad_time_vary + GFS_phys_time_vary + + + + + GFS_suite_interstitial_rad_reset + GFS_rrtmg_pre + rrtmg_sw_pre + rrtmg_sw + rrtmg_sw_post + rrtmg_lw_pre + rrtmg_lw + rrtmg_lw_post + GFS_rrtmg_post + + + + + GFS_suite_interstitial_phys_reset + GFS_suite_stateout_reset + get_prs_fv3 + GFS_suite_interstitial_1 + GFS_surface_generic_pre + GFS_surface_composites_pre + dcyc2t3 + GFS_surface_composites_inter + GFS_suite_interstitial_2 + + + + sfc_diff + GFS_surface_loop_control_part1 + sfc_nst_pre + sfc_nst + sfc_nst_post + lsm_noah + sfc_sice + GFS_surface_loop_control_part2 + + + + GFS_surface_composites_post + sfc_diag + sfc_diag_post + GFS_surface_generic_post + GFS_PBL_generic_pre + hedmf + GFS_PBL_generic_post + GFS_GWD_generic_pre + cires_ugwp + cires_ugwp_post + GFS_GWD_generic_post + rayleigh_damp + GFS_suite_stateout_update + ozphys_2015 + h2ophys + GFS_DCNV_generic_pre + get_phi_fv3 + GFS_suite_interstitial_3 + samfdeepcnv + GFS_DCNV_generic_post + GFS_SCNV_generic_pre + samfshalcnv + GFS_SCNV_generic_post + GFS_suite_interstitial_4 + cnvc90 + GFS_MP_generic_pre + gfdl_cloud_microphys + GFS_MP_generic_post + maximum_hourly_diagnostics + + + + + GFS_stochastics + + + + +\endcode + +*/ diff --git a/physics/docs/pdftxt/suite_FV3_GFS_v15p2_no_nsst.xml.txt b/physics/docs/pdftxt/suite_FV3_GFS_v15p2_no_nsst.xml.txt new file mode 100644 index 000000000..7a60f5e1c --- /dev/null +++ b/physics/docs/pdftxt/suite_FV3_GFS_v15p2_no_nsst.xml.txt @@ -0,0 +1,99 @@ +/** +\page suite_FV3_GFS_v15p2_no_nsst_xml suite_FV3_GFS_v15p2_no_nsst.xml + +\code + + + + + + + fv_sat_adj + + + + + GFS_time_vary_pre + GFS_rrtmg_setup + GFS_rad_time_vary + GFS_phys_time_vary + + + + + GFS_suite_interstitial_rad_reset + GFS_rrtmg_pre + rrtmg_sw_pre + rrtmg_sw + rrtmg_sw_post + rrtmg_lw_pre + rrtmg_lw + rrtmg_lw_post + GFS_rrtmg_post + + + + + GFS_suite_interstitial_phys_reset + GFS_suite_stateout_reset + get_prs_fv3 + GFS_suite_interstitial_1 + GFS_surface_generic_pre + GFS_surface_composites_pre + dcyc2t3 + GFS_surface_composites_inter + GFS_suite_interstitial_2 + + + + sfc_diff + GFS_surface_loop_control_part1 + sfc_ocean + lsm_noah + sfc_sice + GFS_surface_loop_control_part2 + + + + GFS_surface_composites_post + sfc_diag + sfc_diag_post + GFS_surface_generic_post + GFS_PBL_generic_pre + hedmf + GFS_PBL_generic_post + GFS_GWD_generic_pre + cires_ugwp + cires_ugwp_post + GFS_GWD_generic_post + rayleigh_damp + GFS_suite_stateout_update + ozphys_2015 + h2ophys + get_phi_fv3 + GFS_suite_interstitial_3 + GFS_DCNV_generic_pre + samfdeepcnv + GFS_DCNV_generic_post + GFS_SCNV_generic_pre + samfshalcnv + GFS_SCNV_generic_post + GFS_suite_interstitial_4 + cnvc90 + GFS_MP_generic_pre + gfdl_cloud_microphys + GFS_MP_generic_post + maximum_hourly_diagnostics + + + + + GFS_stochastics + + + + +\endcode + +*/ + diff --git a/physics/docs/pdftxt/suite_FV3_GFS_v16beta.xml.txt b/physics/docs/pdftxt/suite_FV3_GFS_v16beta.xml.txt new file mode 100644 index 000000000..4abafe01a --- /dev/null +++ b/physics/docs/pdftxt/suite_FV3_GFS_v16beta.xml.txt @@ -0,0 +1,100 @@ +/** +\page suite_FV3_GFS_v16beta_xml suite_FV3_GFS_v16beta.xml + +\code + + + + + + + fv_sat_adj + + + + + GFS_time_vary_pre + GFS_rrtmg_setup + GFS_rad_time_vary + GFS_phys_time_vary + + + + + GFS_suite_interstitial_rad_reset + GFS_rrtmg_pre + rrtmg_sw_pre + rrtmg_sw + rrtmg_sw_post + rrtmg_lw_pre + rrtmg_lw + rrtmg_lw_post + GFS_rrtmg_post + + + + + GFS_suite_interstitial_phys_reset + GFS_suite_stateout_reset + get_prs_fv3 + GFS_suite_interstitial_1 + GFS_surface_generic_pre + GFS_surface_composites_pre + dcyc2t3 + GFS_surface_composites_inter + GFS_suite_interstitial_2 + + + + sfc_diff + GFS_surface_loop_control_part1 + sfc_nst_pre + sfc_nst + sfc_nst_post + lsm_noah + sfc_sice + GFS_surface_loop_control_part2 + + + + GFS_surface_composites_post + sfc_diag + sfc_diag_post + GFS_surface_generic_post + GFS_PBL_generic_pre + satmedmfvdifq + GFS_PBL_generic_post + GFS_GWD_generic_pre + cires_ugwp + cires_ugwp_post + GFS_GWD_generic_post + rayleigh_damp + GFS_suite_stateout_update + ozphys_2015 + h2ophys + GFS_DCNV_generic_pre + get_phi_fv3 + GFS_suite_interstitial_3 + samfdeepcnv + GFS_DCNV_generic_post + GFS_SCNV_generic_pre + samfshalcnv + GFS_SCNV_generic_post + GFS_suite_interstitial_4 + cnvc90 + GFS_MP_generic_pre + gfdl_cloud_microphys + GFS_MP_generic_post + maximum_hourly_diagnostics + + + + + GFS_stochastics + + + + +\endcode + +*/ diff --git a/physics/docs/pdftxt/suite_FV3_GFS_v16beta_no_nsst.xml.txt b/physics/docs/pdftxt/suite_FV3_GFS_v16beta_no_nsst.xml.txt new file mode 100644 index 000000000..e783be1f9 --- /dev/null +++ b/physics/docs/pdftxt/suite_FV3_GFS_v16beta_no_nsst.xml.txt @@ -0,0 +1,97 @@ +/** +\page suite_FV3_GFS_v16beta_no_nsst_xml suite_FV3_GFS_v16beta_no_nsst.xml + +\code + + + + + + + fv_sat_adj + + + + + GFS_time_vary_pre + GFS_rrtmg_setup + GFS_rad_time_vary + GFS_phys_time_vary + + + + + GFS_suite_interstitial_rad_reset + GFS_rrtmg_pre + rrtmg_sw_pre + rrtmg_sw + rrtmg_sw_post + rrtmg_lw_pre + rrtmg_lw + rrtmg_lw_post + GFS_rrtmg_post + + + + + GFS_suite_interstitial_phys_reset + GFS_suite_stateout_reset + get_prs_fv3 + GFS_suite_interstitial_1 + GFS_surface_generic_pre + GFS_surface_composites_pre + dcyc2t3 + GFS_surface_composites_inter + GFS_suite_interstitial_2 + + + + sfc_diff + GFS_surface_loop_control_part1 + sfc_ocean + lsm_noah + sfc_sice + GFS_surface_loop_control_part2 + + + + GFS_surface_composites_post + sfc_diag + sfc_diag_post + GFS_surface_generic_post + GFS_PBL_generic_pre + satmedmfvdifq + GFS_PBL_generic_post + GFS_GWD_generic_pre + cires_ugwp + cires_ugwp_post + GFS_GWD_generic_post + rayleigh_damp + GFS_suite_stateout_update + ozphys_2015 + h2ophys + get_phi_fv3 + GFS_suite_interstitial_3 + GFS_DCNV_generic_pre + samfdeepcnv + GFS_DCNV_generic_post + GFS_SCNV_generic_pre + samfshalcnv + GFS_SCNV_generic_post + GFS_suite_interstitial_4 + cnvc90 + GFS_MP_generic_pre + gfdl_cloud_microphys + GFS_MP_generic_post + maximum_hourly_diagnostics + + + + + GFS_stochastics + + + + +\endcode +*/ diff --git a/physics/docs/pdftxt/suite_input.nml.txt b/physics/docs/pdftxt/suite_input.nml.txt index fcb55d84f..2565c58eb 100644 --- a/physics/docs/pdftxt/suite_input.nml.txt +++ b/physics/docs/pdftxt/suite_input.nml.txt @@ -1,20 +1,24 @@ /** -\page GFSsuite_nml Namelist Options Description +\page CCPPsuite_nml_desp Namelist Options Description -At runtime, the SCM and the UFS Atmosphere access runtime configurations from file \c input.nml. This file contains -various namelists that control aspects of the I/O, dynamics, physics etc. Most physics-related options are grouped into -two namelists:\b &gfs_physics_nml and \b &gfdl_cloud_microphysics_nml, with additional specifications for stochastic physics in +The SCM and the UFS Atmosphere access runtime configurations from file \c input.nml. This file contains +various namelists records that control aspects of the I/O, dynamics, physics etc. Most physics-related options are in +reords \b &gfs_physics_nml and \b &cires_ugwp_nml. When using the GFDL microphysics scheme, variables in namelist +\b &gfdl_cloud_microphysics_nml are also used. Additional specifications for stochastic physics are in namelists \b &stochy_nam and \b &nam_sfcperts. - Namelist \b &gfdl_cloud_microphysics_nml is only relevant when the GFDL microphysics is used, and its variables are defined in module_gfdl_cloud_microphys.F90. +- Namelist \b &cires_ugwp_nml specifies options for the use of CIRES Unified Gravity Wave Physics Version 0. + - Namelist \b &gfs_physics_nml pertains to all of the suites used, but some of the variables are only relevant for specific parameterizations. Its variables are defined in file GFS_typedefs.F90 in the host model. - Namelist \b &stochy_nam specifies options for the use of SPPT, SKEB and SHUM, while namelist \b &nam_sfcperts specifies whether and how stochastic perturbations are used in the Noah Land Surface Model. +
NML Description
option DDT in Host Model Description Default Value @@ -117,13 +121,19 @@ and how stochastic perturbations are used in the Noah Land Surface Model.
  • =2 future development (not yet)
    		• 0 -
    iaer gfs_control_type aerosol flag "abc" (volcanic, LW, SW): \n +
    iaer gfs_control_type 4-digit aerosol flag (dabc for aermdl, volcanic, LW, SW): \n
      -
    • a: stratospheric volcanic aerosols -
    • b: tropospheric aerosols for LW -
    • c: tropospheric aerosols for SW \n - 0: aerosol effect is not included; \n - 1: aerosol effect is included +
    • d:tropospheric aerosol model scheme flag \n + =0 or none, opac-climatology aerosol scheme \n + =1 use gocart climatology aerosol scheme \n + =2 use gocart prognostic aerosol scheme \n + =5 opac-clim new spectral mapping +
    • a:=0 use background stratospheric aerosol \n + =1 include stratospheric volcanic aerosol +
    • b:=0 no tropospheric aerosol in LW radiation \n + =1 include tropospheric aerosol in LW +
    • c:=0 no tropospheric aerosol in SW radiation \n + =1 include tropospheric aerosol in SW
    		1
    ico2 gfs_control_type \f$CO_2\f$ data source control flag:\n @@ -159,7 +169,7 @@ and how stochastic perturbations are used in the Noah Land Surface Model. 0
    lwhtr gfs_control_type logical flag for output of longwave heating rate .true.
    swhtr gfs_control_type logical flag for output of shortwave heating rate .true. -
    cnvgwd gfs_control_type logical flag for convective gravity wave drag scheme .false. +
    cnvgwd gfs_control_type logical flag for convective gravity wave drag scheme dependent on maxval(cdmbgwd(3:4) == 0.0) .false.
    shal_cnv gfs_control_type logical flag for calling shallow convection .false.
    lmfshal gfs_control_type flag for mass-flux shallow convection scheme in the cloud fraction calculation shal_cnv .and. (imfshalcnv > 0)
    lmfdeep2 gfs_control_type flag for mass-flux deep convection scheme in the cloud fraction calculation imfdeepcnv == 2 .or. 3 .or.4 @@ -168,6 +178,12 @@ and how stochastic perturbations are used in the Noah Land Surface Model.
    dspheat gfs_control_type logical flag for using TKE dissipative heating to temperature tendency in hybrid EDMF and TKE-EDMF schemes .false.
    hybedmf gfs_control_type logical flag for calling hybrid EDMF PBL scheme .false.
    satmedmf gfs_control_type logical flag for calling TKE EDMF PBL scheme .false. +
    isatmedmf gfs_control_type flag for scale-aware TKE-based moist EDMF scheme \n +
      +
    • 0: initial version of satmedmf (Nov.2018) +
    • 1: updated version of satmedmf (as of May 2019) +
    +     		0
    do_mynnedmf gfs_control_type flag to activate MYNN-EDMF scheme .false.
    random_clds gfs_control_type logical flag for whether clouds are random .false.
    trans_trac gfs_control_type logical flag for convective transport of tracers .false. @@ -187,6 +203,7 @@ and how stochastic perturbations are used in the Noah Land Surface Model. 1
    imfdeepcnv gfs_control_type flag for mass-flux deep convective scheme:\n
      +
    • -1: Chikira-Sugiyama deep convection (with \b cscnv = .T.)
    • 1: July 2010 version of SAS convective scheme (operational version as of 2016)
    • 2: scale- & aerosol-aware mass-flux deep convective scheme (2017)
    • 3: scale- & aerosol-aware Grell-Freitas scheme (GSD) @@ -194,12 +211,18 @@ and how stochastic perturbations are used in the Noah Land Surface Model.
    		1
    lgfdlmprad gfs_control_type flag for GFDL mp scheme and radiation consistency .false. -
    cdmbgwd(2) gfs_control_type multiplication factors for mountain blocking and orographic gravity wave drag 2.0,0.25 +
    cdmbgwd(4) gfs_control_type multiplication factors for mountain blocking(1), orographic gravity wave drag(2) +
      +
    • [1]: GWDPS mountain blocking +
    • [2]: GWDPS orographic gravity wave drag +
    • [3]: the modulation total momentum flux of NGWs by intensities of the total precipitation +
    • [4]: TKE for future tests and applications +
    +     		2.0,0.25,1.0,1.0
    prslrd0 gfs_control_type pressure level above which to apply Rayleigh damping 0.0d0
    lsm gfs_control_type flag for land surface model to use \n
      -
    • 0: OSU LSM -
    • 1: NOAH LSM +
    • 1: Noah LSM
    • 2: RUC LSM
    		1 @@ -221,14 +244,14 @@ and how stochastic perturbations are used in the Noah Land Surface Model.
    debug gfs_control_type flag for debug printout .false.
    nstf_name(5) gfs_control_type NSST related paramters:\n
      -
    • nstf_name(1): 0=NSSTM off, 1= NSSTM on but uncoupled, 2= NSSTM on and coupled -
    • nstf_name(2): 1=NSSTM spin up on, 0=NSSTM spin up off -
    • nstf_name(3): 1=NSST analysis on, 0=NSSTM analysis off +
    • nstf_name(1): 0=NSST off, 1= NSST on but uncoupled, 2= NSST on and coupled +
    • nstf_name(2): 1=NSST spin up on, 0=NSST spin up off +
    • nstf_name(3): 1=NSST analysis on, 0=NSST analysis off
    • nstf_name(4): zsea1 in mm
    • nstf_name(5): zesa2 in mm
    		/0,0,1,0,5/ -
    nst_anl gfs_control_type flag for NSSTM analysis in gcycle/sfcsub .false. +
    nst_anl gfs_control_type flag for NSST analysis in gcycle/sfcsub .false.
    effr_in gfs_control_type logical flag for using input cloud effective radii calculation .false.
    aero_in gfs_control_type logical flag for using aerosols in Morrison-Gettelman microphysics .false.
    iau_delthrs gfs_control_type incremental analysis update (IAU) time interval in hours 6 @@ -342,7 +365,14 @@ and how stochastic perturbations are used in the Noah Land Surface Model. 1
    lsoil_lsm gfs_control_type number of soil layers internal to land surface model -1 -
    \b Stochastic \b Physics \b Specific \b Parameters +
    ldiag_ugwp GFS_control_type flag for CIRES UGWP diagnostics .false. +
    do_ugwp GFS_control_type flag for CIRES UGWP revised OGW +
      +
    • .T.: revised gwdps_v0 +
    • .F.: GFS operational orographic gwdps +
    +     		.false. +
    do_tofd GFS_control_type flag for turbulent orographic form drag .false.
    do_sppt gfs_control_type flag for stochastic SPPT option .false.
    do_shum gfs_control_type flag for stochastic SHUM option .false.
    do_skeb gfs_control_type flag for stochastic SKEB option .false. @@ -389,42 +419,61 @@ and how stochastic perturbations are used in the Noah Land Surface Model.
    skebint compns_stochy_mod 0
    \b &gfdl_cloud_microphysics_nml
    sedi_transport gfdl_cloud_microphys_mod logical flag for turning on horizontal momentum transport during sedimentation .true. +
    do_sedi_w gfdl_cloud_microphys_mod \a .true. to turn on vertical motion transport during sedimentation. (not supported in GFS physics) .false.
    do_sedi_heat gfdl_cloud_microphys_mod logical flag for turning on horizontal heat transport during sedimentation .true.
    rad_snow gfdl_cloud_microphys_mod logical flag for considering snow in cloud fraction calculation .true.
    rad_graupel gfdl_cloud_microphys_mod logical flag for considering graupel in cloud fraction calculation .true.
    rad_rain gfdl_cloud_microphys_mod logical flag for considering rain in cloud fraction calculation .true. +
    cld_min gfdl_cloud_microphys_mod minimum cloud fraction. If total cloud condensate exceeds 1.0e-6 kg/kg, cloud fraction cannot be less than \p cld_min 0.05
    const_vi gfdl_cloud_microphys_mod logical flag for using constant cloud ice fall speed .false.
    const_vs gfdl_cloud_microphys_mod logical flag for using constant snow fall speed .false.
    const_vg gfdl_cloud_microphys_mod logical flag for using constant graupel fall speed .false.
    const_vr gfdl_cloud_microphys_mod logical flag for using constant rain fall speed .false. +
    vi_fac gfdl_cloud_microphys_mod tunable factor for cloud ice fall or the constant cloud ice fall speed when \p const_vi is .true. 1. +
    vr_fac gfdl_cloud_microphys_mod tunable factor for rain fall or the constant rain fall speed when \p const_vr is .true. 1. +
    vs_fac gfdl_cloud_microphys_mod tunable factor for snow fall or the constant snow fall speed when \p const_vs is .true. 1. +
    vg_fac gfdl_cloud_microphys_mod tunable factor for graupel fall or the constant graupel fall speed when \p const_vg is .true. 1.
    vi_max gfdl_cloud_microphys_mod maximum fall speed for cloud ice 0.5
    vs_max gfdl_cloud_microphys_mod maximum fall speed for snow 5.0
    vg_max gfdl_cloud_microphys_mod maximum fall speed for graupel 8.0
    vr_max gfdl_cloud_microphys_mod maximum fall speed for rain 12.0
    qi_lim gfdl_cloud_microphys_mod cloud ice limiter to prevent large ice built up in cloud ice freezing and deposition 1.
    prog_ccn gfdl_cloud_microphys_mod logical flag for activating prognostic CCN (not supported in GFS Physics) .false. -
    do_qa gfdl_cloud_microphys_mod logical flag for activating inline cloud fraction diagnosis in fast saturation adjustment .true. -
    fast_sat_adj gfdl_cloud_microphys_mod logical flag for adjusting cloud water evaporation/freezing, cloud ice deposition when fast saturation adjustment is activated .true. +
    do_qa gfdl_cloud_microphys_mod \a .true. to activate inline cloud fraction diagnosis in fast saturation adjustment. \a .false. to activate inline cloud fraction diagnosis in major cloud microphysics .true. +
    fast_sat_adj gfdl_cloud_microphys_mod logical flag for adjusting cloud water evaporation (cloud water -> water vapor), cloud water freezing (cloud water -> cloud ice), cloud ice deposition (water vapor -> cloud ice) when fast saturation adjustment is activated (\b do_sat_adj = .true. in \b fv_core_nml block) .true.
    tau_l2v gfdl_cloud_microphys_mod time scale for evaporation of cloud water to water vapor. Increasing(decreasing) \p tau_l2v can decrease(boost) deposition of cloud water to water vapor 300.
    tau_v2l gfdl_cloud_microphys_mod time scale for condensation of water vapor to cloud water. Increasing(decreasing) \p tau_v2l can decrease(boost) condensation of water vapor to cloud water 150.
    tau_g2v gfdl_cloud_microphys_mod time scale for sublimation of graupel to water vapor. Increasing(decreasing) \p tau_g2v can decrease(boost) sublimation of graupel to water vapor 900. +
    tau_g2r gfdl_cloud_microphys_mod time scale for graupel melting. Increasing(decreasing) \p tau_g2r can decrease(boost) melting of graupel to rain (graupel-> rain) 600. +
    tau_v2g gfdl_cloud_microphys_mod time scale for deposition of water vapor to graupel. Increasing(decreasing) \p tau_v2g can decrease(boost) deposition of water vapor to graupel (water vapor -> graupel) 21600. +
    tau_l2r gfdl_cloud_microphys_mod time scale for autoconversion of cloud water to rain. Increasing(decreasing) \p tau_l2r can decrese(boost) autoconversion of cloud water to rain (cloud water -> rain) 900. +
    tau_r2g gfdl_cloud_microphys_mod time scale for freezing of rain to graupel. Increasing(decreasing) \p tau_r2g can decrease(boost) freezing of rain to graupel (rain->graupel) 900. +
    tau_i2s gfdl_cloud_microphys_mod time scale for autoconversion of cloud ice to snow. Increasing(decreasing) \p tau_i2s can decrease(boost) autoconversion of cloud ice to snow (cloud ice -> snow) 1000. +
    tau_imlt gfdl_cloud_microphys_mod time scale for cloud ice melting. Increasing(decreasing) \p tau_imlt can decrease(boost) melting of cloud ice to cloud water or rain (cloud ice -> cloud water or rain) 600. +
    tau_smlt gfdl_cloud_microphys_mod time scale for snow melting. Increasing(decreasing) \p tau_smlt can decrease(boost) melting of snow to cloud water or rain (snow-> cloud water or rain) 900.
    rthresh gfdl_cloud_microphys_mod critical cloud water radius for autoconversion (cloud water -> rain). Increasing(decreasing) of \p rthresh makes the autoconversion harder(easier) 10.0e-6
    dw_land gfdl_cloud_microphys_mod base value for subgrid deviation/variability over land 0.20
    dw_ocean gfdl_cloud_microphys_mod base value for subgrid deviation/variability over ocean 0.10
    ql_gen gfdl_cloud_microphys_mod maximum value for cloud water generated from condensation of water vapor (water vapor-> cloud water) 1.0e-3 -
    ql_mlt gfdl_cloud_microphys_mod maximum value of cloud water allowed from melted cloud ice (cloud ice -> cloud water or rain) 2.0e-3 -
    qi0_crt gfdl_cloud_microphys_mod threshold of cloud ice to snow autoconversion (cloud ice -> snow) 1.0e-4 -
    qs0_crt gfdl_cloud_microphys_mod threshold of snow to graupel autoconversion (snow -> graupel) 1.0e-3 -
    tau_i2s gfdl_cloud_microphys_mod time scale for autoconversion of cloud ice to snow 1000. -
    c_psaci gfdl_cloud_microphys_mod accretion efficiency of cloud ice to snow 0.02 -
    c_pgacs gfdl_cloud_microphys_mod accretion efficiency of snow to graupel 2.0e-3 +
    qi_gen gfdl_cloud_microphys_mod maximum value of cloud ice generated from deposition of water vapor (water vapor->cloud ice) or freezing(cloud water -> cloud ice). Increasing(decreasing) \p qi_gen can increas(decrease) cloud ice 1.82e-6 +
    ql_mlt gfdl_cloud_microphys_mod maximum value of cloud water allowed from melted cloud ice (cloud ice -> cloud water or rain). Exceedance of which will become rain. Increasing(decreasing) \p ql_mlt can increase(decrease) cloud water and decrease(increase) rain 2.0e-3 +
    qs_mlt gfdl_cloud_microphys_mod maximum value of cloud water allowed from melted snow (snow -> cloud water or rain). Exceedance of which will become rain. Increasing(decreasing) \p qs_mlt can increas(decrease) cloud water and decrease (increase) rain 1.0e-6 +
    ql0_max gfdl_cloud_microphys_mod threshold of cloud water to rain autoconversion (cloud water -> rain). Increasing(decreasing) \p ql0_max can increase(decrease) rain and decrease(increase) cloud water 2.0e-3 +
    qi0_max gfdl_cloud_microphys_mod maximum value of cloud ice generated from other sources like convection. Exceedance of which will become snow. Increasing(decreasing) \p qi0_max can increase(decrease) cloud ice and decrease(increase) snow 1.0e-4 +
    qi0_crt gfdl_cloud_microphys_mod threshold of cloud ice to snow autoconversion (cloud ice -> snow). Increasing(decreasing) \p qi0_crt can increase(decrease) cloud ice and decrease(increase) snow 1.0e-4 +
    qs0_crt gfdl_cloud_microphys_mod threshold of snow to graupel autoconversion (snow -> graupel). Increasing(decreasing) \p qs0_crt can increase(decrease) snow and decrease(increase) graupel 1.0e-3 +
    qc_crt gfdl_cloud_microphys_mod minimum value of cloud condensate to allow partial cloudiness. Partial cloud can only exist when total cloud condensate exceeds \p qc_crt 5.0e-8 +
    c_psaci gfdl_cloud_microphys_mod accretion efficiency of cloud ice to snow (cloud ice -> snow). Increasing(decreasing) of \p c_psaci can boost(decrease) the accretion of cloud ice to snow 0.02 +
    c_pgacs gfdl_cloud_microphys_mod accretion efficiency of snow to graupel (snow -> graupel). Increasing(decreasing) of \p c_pgacs can boost(decrease) the accretion of snow to graupel 2.0e-3
    rh_inc gfdl_cloud_microphys_mod relative humidity increment for complete evaporation of cloud water and cloud ice 0.25
    rh_inr gfdl_cloud_microphys_mod relative humidity increment for sublimation of snow 0.25
    rh_ins gfdl_cloud_microphys_mod relative humidity increment for minimum evaporation of rain 0.25 -
    ccn_l gfdl_cloud_microphys_mod base CCN over land \f$cm^{-3}\f$ 270. -
    ccn_o gfdl_cloud_microphys_mod base CCN over ocean \f$cm^{-3}\f$ 90. -
    c_paut gfdl_cloud_microphys_mod autoconversion efficiency of cloud water to rain 0.55 -
    c_cracw gfdl_cloud_microphys_mod accretion efficiency of cloud water to rain 0.9 +
    rthresh gfdl_cloud_microphys_mod critical cloud water radius for autoconversion(cloud water->rain). Increasing(decreasing) of \p rthresh makes the autoconversion harder(easier) 1.0e-5 +
    ccn_l gfdl_cloud_microphys_mod base CCN over land. Increasing(decreasing) \p ccn_l can on the one hand boost(decrease) the autoconversion of cloud water to rain, on the other hand make the autoconversion harder(easier). The unit is \f$cm^{-3}\f$ 270. +
    ccn_o gfdl_cloud_microphys_mod base CCN over ocean. Increasing(decreasing) \p ccn_o can on the one hand boost(decrease) the autoconversion of cloud water to rain, on the other hand make the autoconversion harder(easier). The unit is \f$cm^{-3}\f$ 90. +
    c_paut gfdl_cloud_microphys_mod autoconversion efficiency of cloud water to rain (cloud water -> rain). Increasing(decreasing) of \p c_paut can boost(decrease) the autoconversion of cloud water to rain 0.55 +
    c_cracw gfdl_cloud_microphys_mod accretion efficiency of cloud water to rain (cloud water -> rain). Increasing(decreasing) of \p c_cracw can boost(decrease) the accretion of cloud water to rain 0.9 +
    sat_adj0 gfdl_cloud_microphys_mod adjust factor for condensation of water vapor to cloud water (water vapor->cloud water) and deposition of water vapor to cloud ice 0.9
    use_ppm gfdl_cloud_microphys_mod \e true to use PPM fall scheme; \e false to use time-implicit monotonic fall scheme .false.
    use_ccn gfdl_cloud_microphys_mod \e true to compute prescribed CCN. It should be .true. when \p prog_ccn = .false. .false.
    mono_prof gfdl_cloud_microphys_mod \e true to turn on terminal fall with monotonic PPM scheme. This is used together with \p use_ppm=.true. .true. @@ -433,6 +482,68 @@ and how stochastic perturbations are used in the Noah Land Surface Model.
    de_ice gfdl_cloud_microphys_mod \e true to convert excessive cloud ice to snow to prevent ice over-built from other sources like convection scheme (not supported in GFS physics) .false.
    fix_negative gfdl_cloud_microphys_mod \e true to fix negative water species using nearby points .false.
    icloud_f gfdl_cloud_microphys_mod flag (0,1,or 2) for cloud fraction diagnostic scheme 0 -
    mp_time gfdl_cloud_microphys_mod time step of GFDL cloud microphysics 150. +
    irain_f gfdl_cloud_microphys_mod flag (0 or 1) for cloud water autoconversion to rain scheme. 0: with subgrid variability; 1: no subgrid variability 0 +
    mp_time gfdl_cloud_microphys_mod time step of GFDL cloud microphysics (MP). If \p mp_time isn't divisible by physics time step or is larger than physics time step, the actual MP time step becomes \p dt/NINT[dt/MIN(dt,mp_time)] 150. +
    alin gfdl_cloud_microphys_mod parameter \a a in Lin et al.(1983). Constant in empirical formula for \f$U_R\f$. Increasing(decreasing) \p alin can boost(decrease) accretion of cloud water by rain and rain evaporation 842. +
    clin gfdl_cloud_microphys_mod parameter \a c in Lin et al.(1983). Constant in empirical formula for \f$U_S\f$. Increasing(decreasing) \p clin can boost(decrease) accretion of cloud water by snow, accretion of cloud ice by snow, snow sublimation and deposition, and snow melting 4.8 +
    t_min gfdl_cloud_microphys_mod temperature threshold for instant deposition. Deposit all water vapor to cloud ice when temperature is lower than \p t_min 178. +
    t_sub gfdl_cloud_microphys_mod temperature threshold for sublimation. Cloud ice, snow or graupel stops(starts) sublimation when temperature is lower(higher) then \p t_sub 184. +
    mp_print gfdl_cloud_microphys_mod \a .true. to turn on GFDL cloud microphysics debugging print out. (not supported in GFS physics) .false. +
    \b &cires_ugwp_nml +
    knob_ugwp_version cires_ugwp_module parameter selects a version of the UGWP implementation in FV3GFS-127L \n +
      +
    • 0: default version delivered to EMC in Jan 2019 for implementation +
    • 1: version of UGWP under development that plans to consider the physics-based sources of NGWs (\b knob_ugwp_wvspec [2:4]), options for stochastic and deterministic excitation of waves (\b knob_ugwp_stoch), and switches between different UGWP schemes (\b knob_ugwp_solver) +
    +     		0 +
    knob_ugwp_doaxyz cires_ugwp_module parameter controls application of the momentum deposition for NGW-schemes \n +
      +
    • 0: the momentum tendencies due to NGWs are calculated, but tendencies do not change the horizontal winds +
    • 1: default value; it changes the horizontal momentum tendencies and horizontal winds +
    +     		1 +
    knob_ugwp_doheat cires_ugwp_module parameter controls application of the heat deposition for NGW-schemes \n +
      +
    • 0: the temperature tendencies due to NGWs are calculated but tendencies do not change the temperature state +
    • 1: default value; it changes the temperature tendencies and kinetic temperature +
    +     		1 +
    knob_ugwp_dokdis cires_ugwp_module parameter controls application of the eddy diffusion due to instability of NGWs \n +
      +
    • 0: the eddy diffusion tendencies due to NGWs are calculated but tendencies do not change the model state vector +
    • 1: it computes eddy diffusion coefficient due to instability of NGWs; in UGWP v0, eddy viscosity, heat conductivity and tracer diffusion are not activated +
    +     		0 +
    knob_ugwp_solver cires_ugwp_module parameter controls the selection of UGWP-solvers(wave propagation, dissipation and wave breaking) for NGWs \n +
      +
    • 1: represents the discrete multi-wave solver with background dissipation and linear wave saturation +
    • 2: represents the spectral deterministic solver with background dissipation and spectral saturation +
    • 3: represents the discrete multi-wave solver with the background dissipation, extension of Alexander sand Dunkerton (1999) +
    • 4: represents the spectral solver with background dissipation, extension of Doppler Spread Theory of Hines (1997) +
    +     		1 +
    knob_ugwp_ndx4lh cires_ugwp_module parameter controls the selection of the horizontal wavenumber(wavelength) for NGW schemes \n +
      +
    • 1: selects the \f$4xdx\f$ sub-grid wavelength, where dx is the horizontal resolution of the model configuration (C96-400km; C768-52km) +
    +     		2 +
    knob_ugwp_wvspec cires_ugwp_module four-dimensional array defines number of waves in each arimuthal propagation (as defined by knob_ugwp_azdir) for GWs excited due to the following four sources: \n + (1) sub-grid orography (\b knob_ugwp_wvspec[1]=1), \n + (2) convective (\b knob_ugwp_wvspec[2]=25), \n + (3) frontal (\b knob_ugwp_wvspec[3]=25) activity, \n + (4) \b knob_ugwp_wvspec[4] represents number of wave excited by dynamical imbalances that may mimic both convective and front-jet mechanisms of GW triggering. \n + In UGWP v0, first two elements of the array, \b knob_ugwp_wvspec(1:2), control number of waves for stationary (OGW) and nonstationary waves (NGWs). + 1,32,32,32 +
    knob_ugwp_azdir cires_ugwp_module four-dimensional array that defines number of azimuths for propagation of GWs triggered by four types of physics-based sources (orography, convection, front-jets, and dynamical imbalance). In UGWP v0, first two elements of the array, \b knob_ugwp_azdir(1:2), control number of azimuths for OGW and NGWs respectively. + 2,4,4,4 +
    knob_ugwp_stoch cires_ugwp_module four-dimensional array that control stochastic selection of GWs triggered by four types of physics-based sources. \n + Default values:0,0,0,0 - reflect determinstic selection of GW parameters without stochastic selection + 0,0,0,0 +
    knob_ugwp_effac cires_ugwp_module four-dimensional array that control efficiency of GWs triggerd by four types of physics-based sources. \n + Default values: 1.,1.,1.,1. - reflect that calculated GW-tendencies will be applied for the model state. + 1.,1.,1.,1. +
    launch_level cires_ugwp_module parameter has been introduced by EMC during implementation. It defines the interface model level from the surface at which NGWs are launched. \n + Default value for FV3GFS-64L, launch_level=25 and for FV3GFS-128L, launch_level=52. + 55
    */ diff --git a/physics/drag_suite.F90 b/physics/drag_suite.F90 index 080bee156..0189785e3 100644 --- a/physics/drag_suite.F90 +++ b/physics/drag_suite.F90 @@ -90,7 +90,7 @@ end subroutine drag_suite_init !! the GWD scheme has the same physical basis as in Alpert (1987) with the addition !! of enhancement factors for the amplitude, G, and mountain shape details !! in G(Fr) to account for effects from the mountain blocking. A factor, -!! E m’, is an enhancement factor on the stress in the Alpert '87 scheme. +!! E m', is an enhancement factor on the stress in the Alpert '87 scheme. !! The E ranges from no enhancement to an upper limit of 3, E=E(OA)[1-3], !! and is a function of OA, the Orographic Asymmetry defined in KA (1995) as !! @@ -105,9 +105,9 @@ end subroutine drag_suite_init !! !! !! where Nx is the number of grid intervals for the large scale domain being -!! considered. So the term, E(OA)m’/ \f$ \Delta X \f$ in Kim's scheme represents -!! a multiplier on G shown in Alpert's eq (1), where m’ is the number of mountains -!! in a sub-grid scale box. Kim increased the complexity of m’ making it a +!! considered. So the term, E(OA)m'/ \f$ \Delta X \f$ in Kim's scheme represents +!! a multiplier on G shown in Alpert's eq (1), where m' is the number of mountains +!! in a sub-grid scale box. Kim increased the complexity of m' making it a !! function of the fractional area of the sub-grid mountain and the asymmetry !! and convexity statistics which are found from running a gravity wave !! model for a large number of cases: diff --git a/physics/gcm_shoc.meta b/physics/gcm_shoc.meta index 07f014356..f4d2f3ae9 100644 --- a/physics/gcm_shoc.meta +++ b/physics/gcm_shoc.meta @@ -251,7 +251,7 @@ intent = in optional = F [hflx] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -260,7 +260,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/gcycle.F90 b/physics/gcycle.F90 index 8c5dd041a..bc1bb032c 100644 --- a/physics/gcycle.F90 +++ b/physics/gcycle.F90 @@ -239,6 +239,7 @@ SUBROUTINE GCYCLE (nblks, Model, Grid, Sfcprop, Cldprop) Sfcprop(nb)%smc (ix,ls) = SMCFC1 (len + (ls-1)*npts) Sfcprop(nb)%stc (ix,ls) = STCFC1 (len + (ls-1)*npts) Sfcprop(nb)%slc (ix,ls) = SLCFC1 (len + (ls-1)*npts) + if (ls<=Model%kice) Sfcprop(nb)%tiice (ix,ls) = STCFC1 (len + (ls-1)*npts) enddo ENDDO !-----END BLOCK SIZE LOOP------------------------------ ENDDO !-----END BLOCK LOOP------------------------------- diff --git a/physics/gfdl_fv_sat_adj.F90 b/physics/gfdl_fv_sat_adj.F90 index f5c84cd99..025ee1c34 100644 --- a/physics/gfdl_fv_sat_adj.F90 +++ b/physics/gfdl_fv_sat_adj.F90 @@ -150,6 +150,12 @@ subroutine fv_sat_adj_init(do_sat_adj, kmp, nwat, ngas, rilist, cpilist, & return end if + if (.not.nwat==6) then + write(errmsg,'(a)') 'Logic error: fv_sat_adj requires six water species (nwat=6)' + errflg = 1 + return + end if + if (is_initialized) return ! generate es table (dt = 0.1 deg c) diff --git a/physics/gwdps.f b/physics/gwdps.f index 9454b967d..96ce0205b 100644 --- a/physics/gwdps.f +++ b/physics/gwdps.f @@ -87,7 +87,7 @@ end subroutine gwdps_init !! the GWD scheme has the same physical basis as in Alpert (1987) with the addition !! of enhancement factors for the amplitude, G, and mountain shape details !! in G(Fr) to account for effects from the mountain blocking. A factor, -!! E m’, is an enhancement factor on the stress in the Alpert '87 scheme. +!! E m', is an enhancement factor on the stress in the Alpert '87 scheme. !! The E ranges from no enhancement to an upper limit of 3, E=E(OA)[1-3], !! and is a function of OA, the Orographic Asymmetry defined in Kim and Arakawa (1995) !! \cite kim_and_arakawa_1995 as @@ -103,9 +103,9 @@ end subroutine gwdps_init !! \; (x_{j} \; - \; \bar{x} )^2}{N_{x}} } !!\f] !! where \f$N_{x}\f$ is the number of grid intervals for the large scale domain being -!! considered. So the term, E(OA)m’/ \f$ \Delta X \f$ in Kim's scheme represents -!! a multiplier on G shown in Alpert's eq (1), where m’ is the number of mountains -!! in a sub-grid scale box. Kim increased the complexity of m’ making it a +!! considered. So the term, E(OA)m'/ \f$ \Delta X \f$ in Kim's scheme represents +!! a multiplier on G shown in Alpert's eq (1), where m' is the number of mountains +!! in a sub-grid scale box. Kim increased the complexity of m' making it a !! function of the fractional area of the sub-grid mountain and the asymmetry !! and convexity statistics which are found from running a gravity wave !! model for a large number of cases: diff --git a/physics/lsm_ruc_sfc_sice_interstitial.F90 b/physics/lsm_ruc_sfc_sice_interstitial.F90 index 63f006f1e..27033fcc8 100644 --- a/physics/lsm_ruc_sfc_sice_interstitial.F90 +++ b/physics/lsm_ruc_sfc_sice_interstitial.F90 @@ -21,17 +21,18 @@ end subroutine lsm_ruc_sfc_sice_pre_finalize !! \htmlinclude lsm_ruc_sfc_sice_pre_run.html !! #endif - subroutine lsm_ruc_sfc_sice_pre_run(im, lsoil_ruc, lsoil, land, stc, tslb, errmsg, errflg) + subroutine lsm_ruc_sfc_sice_pre_run(im, lsoil_ruc, lsoil, kice, land, icy, stc, tslb, tiice, errmsg, errflg) implicit none ! Interface variables - integer, intent(in) :: im, lsoil_ruc, lsoil - logical, dimension(im), intent(in) :: land + integer, intent(in) :: im, lsoil_ruc, lsoil, kice + logical, dimension(im), intent(in) :: land, icy ! --- on Noah levels real (kind=kind_phys), dimension(im,lsoil), intent(inout) :: stc ! --- on RUC levels real (kind=kind_phys), dimension(im,lsoil_ruc), intent(in) :: tslb + real (kind=kind_phys), dimension(im,kice), intent(inout) :: tiice character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg @@ -44,7 +45,11 @@ subroutine lsm_ruc_sfc_sice_pre_run(im, lsoil_ruc, lsoil, land, stc, tslb, errms errflg = 0 do i=1,im - if (.not.land(i)) then + if (icy(i)) then + do k=1,kice + tiice(i,k) = tslb(i,k) + end do + else if (.not.land(i)) then do k=1,min(lsoil,lsoil_ruc) stc(i,k) = tslb(i,k) end do @@ -78,15 +83,16 @@ end subroutine lsm_ruc_sfc_sice_post_finalize !! \htmlinclude lsm_ruc_sfc_sice_post_run.html !! #endif - subroutine lsm_ruc_sfc_sice_post_run(im, lsoil_ruc, lsoil, land, stc, tslb, errmsg, errflg) + subroutine lsm_ruc_sfc_sice_post_run(im, lsoil_ruc, lsoil, kice, land, icy, stc, tslb, tiice, errmsg, errflg) implicit none ! Interface variables - integer, intent(in) :: im, lsoil_ruc, lsoil - logical, dimension(im), intent(in) :: land + integer, intent(in) :: im, lsoil_ruc, lsoil, kice + logical, dimension(im), intent(in) :: land, icy ! --- on Noah levels real (kind=kind_phys), dimension(im,lsoil), intent(in) :: stc + real (kind=kind_phys), dimension(im,kice), intent(in) :: tiice ! --- on RUC levels real (kind=kind_phys), dimension(im,lsoil_ruc), intent(inout) :: tslb @@ -101,7 +107,11 @@ subroutine lsm_ruc_sfc_sice_post_run(im, lsoil_ruc, lsoil, land, stc, tslb, errm errflg = 0 do i=1,im - if (.not.land(i)) then + if (icy(i)) then + do k=1,kice + tslb(i,k) = tiice(i,k) + end do + else if (.not.land(i)) then do k=1,min(lsoil,lsoil_ruc) tslb(i,k) = stc(i,k) end do diff --git a/physics/lsm_ruc_sfc_sice_interstitial.meta b/physics/lsm_ruc_sfc_sice_interstitial.meta index c105abe9d..3b8213d78 100644 --- a/physics/lsm_ruc_sfc_sice_interstitial.meta +++ b/physics/lsm_ruc_sfc_sice_interstitial.meta @@ -9,6 +9,14 @@ type = integer intent = in optional = F +[kice] + standard_name = ice_vertical_dimension + long_name = vertical loop extent for ice levels, start at 1 + units = count + dimensions = () + type = integer + intent = in + optional = F [lsoil_ruc] standard_name = soil_vertical_dimension_for_land_surface_model long_name = number of soil layers internal to land surface model @@ -33,6 +41,23 @@ type = logical intent = in optional = F +[icy] + standard_name = flag_nonzero_sea_ice_surface_fraction + long_name = flag indicating presence of some sea ice surface area fraction + units = flag + dimensions = (horizontal_dimension) + type = logical + intent = inout + optional = F +[tiice] + standard_name = internal_ice_temperature + long_name = sea ice internal temperature + units = K + dimensions = (horizontal_dimension,ice_vertical_dimension) + type = real + kind = kind_phys + intent = inout + optional = F [stc] standard_name = soil_temperature long_name = soil temperature @@ -81,6 +106,14 @@ type = integer intent = in optional = F +[kice] + standard_name = ice_vertical_dimension + long_name = vertical loop extent for ice levels, start at 1 + units = count + dimensions = () + type = integer + intent = in + optional = F [lsoil_ruc] standard_name = soil_vertical_dimension_for_land_surface_model long_name = number of soil layers internal to land surface model @@ -105,6 +138,23 @@ type = logical intent = in optional = F +[icy] + standard_name = flag_nonzero_sea_ice_surface_fraction + long_name = flag indicating presence of some sea ice surface area fraction + units = flag + dimensions = (horizontal_dimension) + type = logical + intent = inout + optional = F +[tiice] + standard_name = internal_ice_temperature + long_name = sea ice internal temperature + units = K + dimensions = (horizontal_dimension,ice_vertical_dimension) + type = real + kind = kind_phys + intent = inout + optional = F [stc] standard_name = soil_temperature long_name = soil temperature diff --git a/physics/m_micro.F90 b/physics/m_micro.F90 index 83ff8d554..8b2b4c99f 100644 --- a/physics/m_micro.F90 +++ b/physics/m_micro.F90 @@ -14,8 +14,7 @@ module m_micro contains -!>\ingroup mg_driver -!! This subroutine is the MG initialization. +!> This subroutine is the MG initialization. !> \section arg_table_m_micro_init Argument Table !! \htmlinclude m_micro_init.html !! @@ -103,20 +102,13 @@ end subroutine m_micro_init subroutine m_micro_finalize end subroutine m_micro_finalize -!> \defgroup mg2mg3 Morrison-Gettelman MP scheme Module -!! This module contains the the entity of MG2 and MG3 schemes. -!> @{ -!> \defgroup mg_driver Morrison-Gettelman MP Driver Module +!> \defgroup mg2mg3 Morrison-Gettelman MP Driver Module !! \brief This subroutine is the Morrison-Gettelman MP driver, which computes !! grid-scale condensation and evaporation of cloud condensate. - -#if 0 - +!! !> \section arg_table_m_micro_run Argument Table !! \htmlinclude m_micro_run.html !! -#endif -!>\ingroup mg_driver !>\section detail_m_micro_run MG m_micro_run Detailed Algorithm !> @{ subroutine m_micro_run( im, ix, lm, flipv, dt_i & @@ -1891,7 +1883,7 @@ end subroutine m_micro_run !DONIF Calculate the Brunt_Vaisala frequency !=============================================================================== -!>\ingroup mg_driver +!>\ingroup mg2mg3 !> This subroutine computes profiles of background state quantities for !! the multiple gravity wave drag parameterization. !!\section gw_prof_gen MG gw_prof General Algorithm @@ -1978,7 +1970,7 @@ subroutine gw_prof (pcols, pver, ncol, t, pm, pi, rhoi, ni, ti, & end subroutine gw_prof !> @} -!>\ingroup mg_driver +!>\ingroup mg2mg3 !! This subroutine is to find cloud top based on cloud fraction. subroutine find_cldtop(ncol, pver, cf, kcldtop) implicit none @@ -2012,6 +2004,5 @@ subroutine find_cldtop(ncol, pver, cf, kcldtop) end subroutine find_cldtop -!> @} end module m_micro diff --git a/physics/micro_mg_utils.F90 b/physics/micro_mg_utils.F90 index 89dd7193e..74da36df4 100644 --- a/physics/micro_mg_utils.F90 +++ b/physics/micro_mg_utils.F90 @@ -2656,7 +2656,7 @@ end subroutine graupel_rime_splintering ! prdg(i) = epsg*(q(i)-qvi(i))/abi ! !! make sure not pushed into ice supersat/subsat -!! put this in main mg3 code…..check for it… +!! put this in main mg3 code ... check for it ... !! formula from reisner 2 scheme !! diff --git a/physics/module_MYJPBL_wrapper.meta b/physics/module_MYJPBL_wrapper.meta index a70203def..dd2560e06 100644 --- a/physics/module_MYJPBL_wrapper.meta +++ b/physics/module_MYJPBL_wrapper.meta @@ -446,7 +446,7 @@ intent = inout optional = F [hflx] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -455,7 +455,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/module_MYJSFC_wrapper.F90 b/physics/module_MYJSFC_wrapper.F90 index 1406a99be..8a093cddf 100644 --- a/physics/module_MYJSFC_wrapper.F90 +++ b/physics/module_MYJSFC_wrapper.F90 @@ -37,16 +37,16 @@ SUBROUTINE myjsfc_wrapper_run( & & pblh, slmsk, zorl, ustar, rib, & & cm,ch,stress,ffm,ffh,fm10,fh2, & & landfrac,lakefrac,oceanfrac,fice, & - & z0rl_ocn, z0rl_lnd, z0rl_ice, & ! intent(inout) - & ustar_ocn, ustar_lnd, ustar_ice, & ! intent(inout) - & cm_ocn, cm_lnd, cm_ice, & ! intent(inout) - & ch_ocn, ch_lnd, ch_ice, & ! intent(inout) - & rb_ocn, rb_lnd, rb_ice, & ! intent(inout) - & stress_ocn,stress_lnd,stress_ice, & ! intent(inout) - & fm_ocn, fm_lnd, fm_ice, & ! intent(inout) - & fh_ocn, fh_lnd, fh_ice, & ! intent(inout) - & fm10_ocn, fm10_lnd, fm10_ice, & ! intent(inout) - & fh2_ocn, fh2_lnd, fh2_ice, & ! intent(inout) + & z0rl_wat, z0rl_lnd, z0rl_ice, & ! intent(inout) + & ustar_wat, ustar_lnd, ustar_ice, & ! intent(inout) + & cm_wat, cm_lnd, cm_ice, & ! intent(inout) + & ch_wat, ch_lnd, ch_ice, & ! intent(inout) + & rb_wat, rb_lnd, rb_ice, & ! intent(inout) + & stress_wat,stress_lnd,stress_ice, & ! intent(inout) + & fm_wat, fm_lnd, fm_ice, & ! intent(inout) + & fh_wat, fh_lnd, fh_ice, & ! intent(inout) + & fm10_wat, fm10_lnd, fm10_ice, & ! intent(inout) + & fh2_wat, fh2_lnd, fh2_ice, & ! intent(inout) & wind, con_cp, con_g, con_rd, & & me, lprnt, errmsg, errflg ) ! intent(inout) ! @@ -107,16 +107,16 @@ SUBROUTINE myjsfc_wrapper_run( & real(kind=kind_phys), dimension(im), intent(inout) :: & & landfrac, lakefrac, oceanfrac, fice real(kind=kind_phys), dimension(im), intent(inout) :: & - & z0rl_ocn, z0rl_lnd, z0rl_ice, & - & ustar_ocn, ustar_lnd, ustar_ice, & - & cm_ocn, cm_lnd, cm_ice, & - & ch_ocn, ch_lnd, ch_ice, & - & rb_ocn, rb_lnd, rb_ice, & - & stress_ocn,stress_lnd,stress_ice, & - & fm_ocn, fm_lnd, fm_ice, & - & fh_ocn, fh_lnd, fh_ice, & - & fm10_ocn, fm10_lnd, fm10_ice, & - & fh2_ocn, fh2_lnd, fh2_ice, & + & z0rl_wat, z0rl_lnd, z0rl_ice, & + & ustar_wat, ustar_lnd, ustar_ice, & + & cm_wat, cm_lnd, cm_ice, & + & ch_wat, ch_lnd, ch_ice, & + & rb_wat, rb_lnd, rb_ice, & + & stress_wat,stress_lnd,stress_ice, & + & fm_wat, fm_lnd, fm_ice, & + & fh_wat, fh_lnd, fh_ice, & + & fm10_wat, fm10_lnd, fm10_ice, & + & fh2_wat, fh2_lnd, fh2_ice, & & wind @@ -404,16 +404,16 @@ SUBROUTINE myjsfc_wrapper_run( & do i = 1, im if(flag_iter(i))then - z0rl_ocn(i) = zorl(i) - cm_ocn(i) = cm(i) - ch_ocn(i) = ch(i) - rb_ocn(i) = rib(i) - stress_ocn(i) = stress(i) - fm_ocn(i) = ffm(i) - fh_ocn(i) = ffh(i) - ustar_ocn(i) = ustar(i) - fm10_ocn(i) = fm10(i) - fh2_ocn(i) = fh2(i) + z0rl_wat(i) = zorl(i) + cm_wat(i) = cm(i) + ch_wat(i) = ch(i) + rb_wat(i) = rib(i) + stress_wat(i) = stress(i) + fm_wat(i) = ffm(i) + fh_wat(i) = ffh(i) + ustar_wat(i) = ustar(i) + fm10_wat(i) = fm10(i) + fh2_wat(i) = fh2(i) z0rl_lnd(i) = zorl(i) cm_lnd(i) = cm(i) diff --git a/physics/module_MYJSFC_wrapper.meta b/physics/module_MYJSFC_wrapper.meta index 8100d0b05..67294e6fc 100644 --- a/physics/module_MYJSFC_wrapper.meta +++ b/physics/module_MYJSFC_wrapper.meta @@ -473,7 +473,7 @@ kind = kind_phys intent = in optional = F -[z0rl_ocn] +[z0rl_wat] standard_name = surface_roughness_length_over_ocean_interstitial long_name = surface roughness length over ocean (interstitial) units = cm @@ -500,7 +500,7 @@ kind = kind_phys intent = inout optional = F -[ustar_ocn] +[ustar_wat] standard_name = surface_friction_velocity_over_ocean long_name = surface friction velocity over ocean units = m s-1 @@ -527,7 +527,7 @@ kind = kind_phys intent = inout optional = F -[cm_ocn] +[cm_wat] standard_name = surface_drag_coefficient_for_momentum_in_air_over_ocean long_name = surface exchange coeff for momentum over ocean units = none @@ -554,7 +554,7 @@ kind = kind_phys intent = inout optional = F -[ch_ocn] +[ch_wat] standard_name = surface_drag_coefficient_for_heat_and_moisture_in_air_over_ocean long_name = surface exchange coeff heat & moisture over ocean units = none @@ -581,7 +581,7 @@ kind = kind_phys intent = inout optional = F -[rb_ocn] +[rb_wat] standard_name = bulk_richardson_number_at_lowest_model_level_over_ocean long_name = bulk Richardson number at the surface over ocean units = none @@ -608,7 +608,7 @@ kind = kind_phys intent = inout optional = F -[stress_ocn] +[stress_wat] standard_name = surface_wind_stress_over_ocean long_name = surface wind stress over ocean units = m2 s-2 @@ -635,7 +635,7 @@ kind = kind_phys intent = inout optional = F -[fm_ocn] +[fm_wat] standard_name = Monin_Obukhov_similarity_function_for_momentum_over_ocean long_name = Monin-Obukhov similarity funct for momentum over ocean units = none @@ -662,7 +662,7 @@ kind = kind_phys intent = inout optional = F -[fh_ocn] +[fh_wat] standard_name = Monin_Obukhov_similarity_function_for_heat_over_ocean long_name = Monin-Obukhov similarity function for heat over ocean units = none @@ -689,7 +689,7 @@ kind = kind_phys intent = inout optional = F -[fm10_ocn] +[fm10_wat] standard_name = Monin_Obukhov_similarity_function_for_momentum_at_10m_over_ocean long_name = Monin-Obukhov parameter for momentum at 10m over ocean units = none @@ -716,7 +716,7 @@ kind = kind_phys intent = inout optional = F -[fh2_ocn] +[fh2_wat] standard_name = Monin_Obukhov_similarity_function_for_heat_at_2m_over_ocean long_name = Monin-Obukhov parameter for heat at 2m over ocean units = none diff --git a/physics/module_MYNNPBL_wrapper.meta b/physics/module_MYNNPBL_wrapper.meta index 27b186bd3..eb8fcb0fd 100644 --- a/physics/module_MYNNPBL_wrapper.meta +++ b/physics/module_MYNNPBL_wrapper.meta @@ -291,7 +291,7 @@ intent = out optional = F [hflx] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -300,7 +300,7 @@ intent = in optional = F [qflx] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/module_sf_noahmplsm.f90 b/physics/module_sf_noahmplsm.f90 index a0612d417..02ea70a6e 100644 --- a/physics/module_sf_noahmplsm.f90 +++ b/physics/module_sf_noahmplsm.f90 @@ -291,7 +291,6 @@ subroutine noahmp_sflx (parameters, & qc , soldn , lwdn , & ! in : forcing prcpconv, prcpnonc, prcpshcv, prcpsnow, prcpgrpl, prcphail, & ! in : forcing tbot , co2air , o2air , foln , ficeold , zlvl , & ! in : forcing - lheatstrg , & ! in : canopy heat storage albold , sneqvo , & ! in/out : stc , sh2o , smc , tah , eah , fwet , & ! in/out : canliq , canice , tv , tg , qsfc , qsnow , & ! in/out : @@ -299,9 +298,9 @@ subroutine noahmp_sflx (parameters, & zwt , wa , wt , wslake , lfmass , rtmass , & ! in/out : stmass , wood , stblcp , fastcp , lai , sai , & ! in/out : cm , ch , tauss , & ! in/out : - smcwtd ,deeprech , rech , cpfac , & ! in/out : + smcwtd ,deeprech , rech , & ! in/out : z0wrf , & - fsa , fsr , fira , fshx , ssoil , fcev , & ! out : + fsa , fsr , fira , fsh , ssoil , fcev , & ! out : fgev , fctr , ecan , etran , edir , trad , & ! out : tgb , tgv , t2mv , t2mb , q2v , q2b , & ! out : runsrf , runsub , apar , psn , sav , sag , & ! out : @@ -342,7 +341,6 @@ subroutine noahmp_sflx (parameters, & real , intent(in) :: lwdn !downward longwave radiation (w/m2) real , intent(in) :: sfcprs !pressure (pa) real , intent(inout) :: zlvl !reference height (m) - logical , intent(in) :: lheatstrg ! flag for canopy heat storage parameterization real , intent(in) :: cosz !cosine solar zenith angle [0-1] real , intent(in) :: tbot !bottom condition for soil temp. [k] real , intent(in) :: foln !foliage nitrogen (%) [1-saturated] @@ -401,14 +399,13 @@ subroutine noahmp_sflx (parameters, & real, intent(inout) :: smcwtd !soil water content between bottom of the soil and water table [m3/m3] real, intent(inout) :: deeprech !recharge to or from the water table when deep [m] real, intent(inout) :: rech !recharge to or from the water table when shallow [m] (diagnostic) - real, intent(inout) :: cpfac ! heat capacity enhancement factor due to heat storage ! output real , intent(out) :: z0wrf !combined z0 sent to coupled model real , intent(out) :: fsa !total absorbed solar radiation (w/m2) real , intent(out) :: fsr !total reflected solar radiation (w/m2) real , intent(out) :: fira !total net lw rad (w/m2) [+ to atm] - real , intent(out) :: fshx !total sensible heat (w/m2) [+ to atm] + real , intent(out) :: fsh !total sensible heat (w/m2) [+ to atm] real , intent(out) :: fcev !canopy evap heat (w/m2) [+ to atm] real , intent(out) :: fgev !ground evap heat (w/m2) [+ to atm] real , intent(out) :: fctr !transpiration heat (w/m2) [+ to atm] @@ -458,7 +455,6 @@ subroutine noahmp_sflx (parameters, & real :: taux !wind stress: e-w (n/m2) real :: tauy !wind stress: n-s (n/m2) real :: rhoair !density air (kg/m3) - real :: fsh !total sensible heat (w/m2) [+ to atm] ! real, dimension( 1: 5) :: vocflx !voc fluxes [ug c m-2 h-1] real, dimension(-nsnow+1:nsoil) :: dzsnso !snow/soil layer thickness [m] real :: thair !potential temperature (k) @@ -649,7 +645,6 @@ subroutine noahmp_sflx (parameters, & call energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in isnow ,dt ,rhoair ,sfcprs ,qair , & !in sfctmp ,thair ,lwdn ,uu ,vv ,zlvl , & !in - lheatstrg , & !in co2air ,o2air ,solad ,solai ,cosz ,igs , & !in eair ,tbot ,zsnso ,zsoil , & !in elai ,esai ,fwet ,foln , & !in @@ -658,16 +653,16 @@ subroutine noahmp_sflx (parameters, & z0wrf , & imelt ,snicev ,snliqv ,epore ,t2m ,fsno , & !out sav ,sag ,qmelt ,fsa ,fsr ,taux , & !out - tauy ,fira ,fsh ,fshx ,fcev ,fgev ,fctr , & !out + tauy ,fira ,fsh ,fcev ,fgev ,fctr , & !out trad ,psn ,apar ,ssoil ,btrani ,btran , & !out ponding,ts ,latheav , latheag , frozen_canopy,frozen_ground, & !out tv ,tg ,stc ,snowh ,eah ,tah , & !inout sneqvo ,sneqv ,sh2o ,smc ,snice ,snliq , & !inout albold ,cm ,ch ,dx ,dz8w ,q2 , & !inout #ifdef CCPP - tauss ,cpfac ,errmsg ,errflg , & !inout + tauss ,errmsg ,errflg , & !inout #else - tauss ,cpfac , & !inout + tauss , & !inout #endif !jref:start qc ,qsfc ,psfc , & !in @@ -1428,7 +1423,6 @@ end subroutine error subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in isnow ,dt ,rhoair ,sfcprs ,qair , & !in sfctmp ,thair ,lwdn ,uu ,vv ,zref , & !in - lheatstrg , & !in co2air ,o2air ,solad ,solai ,cosz ,igs , & !in eair ,tbot ,zsnso ,zsoil , & !in elai ,esai ,fwet ,foln , & !in @@ -1437,16 +1431,16 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in z0wrf , & imelt ,snicev ,snliqv ,epore ,t2m ,fsno , & !out sav ,sag ,qmelt ,fsa ,fsr ,taux , & !out - tauy ,fira ,fsh ,fshx ,fcev ,fgev ,fctr , & !out + tauy ,fira ,fsh ,fcev ,fgev ,fctr , & !out trad ,psn ,apar ,ssoil ,btrani ,btran , & !out ponding,ts ,latheav , latheag , frozen_canopy,frozen_ground, & !out tv ,tg ,stc ,snowh ,eah ,tah , & !inout sneqvo ,sneqv ,sh2o ,smc ,snice ,snliq , & !inout albold ,cm ,ch ,dx ,dz8w ,q2 , & !inout #ifdef CCPP - tauss ,cpfac ,errmsg ,errflg, & !inout + tauss ,errmsg ,errflg, & !inout #else - tauss ,cpfac , & !inout + tauss , & !inout #endif !jref:start qc ,qsfc ,psfc , & !in @@ -1528,7 +1522,6 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in real , intent(in) :: igs !growing season index (0=off, 1=on) real , intent(in) :: zref !reference height (m) - logical , intent(in) :: lheatstrg ! flag for canopy heat storage parameterization real , intent(in) :: tbot !bottom condition for soil temp. (k) real , dimension(-nsnow+1:nsoil), intent(in) :: zsnso !layer-bottom depth from snow surf [m] real , dimension( 1:nsoil), intent(in) :: zsoil !layer-bottom depth from soil surf [m] @@ -1563,7 +1556,6 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in real , intent(out) :: tauy !wind stress: n-s (n/m2) real , intent(out) :: fira !total net lw. rad (w/m2) [+ to atm] real , intent(out) :: fsh !total sensible heat (w/m2) [+ to atm] - real , intent(out) :: fshx !total sensible heat (w/m2) [+ to atm] real , intent(out) :: fcev !canopy evaporation (w/m2) [+ to atm] real , intent(out) :: fgev !ground evaporation (w/m2) [+ to atm] real , intent(out) :: fctr !transpiration (w/m2) [+ to atm] @@ -1610,7 +1602,6 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in real , intent(inout) :: tah !canopy air temperature (k) real , intent(inout) :: albold !snow albedo at last time step(class type) real , intent(inout) :: tauss !non-dimensional snow age - real , intent(inout) :: cpfac !heat capacity enhancement factor due to heat storage real , intent(inout) :: cm !momentum drag coefficient real , intent(inout) :: ch !sensible heat exchange coefficient real , intent(inout) :: q1 @@ -1712,11 +1703,6 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in real, parameter :: mpe = 1.e-6 real, parameter :: psiwlt = -150. !metric potential for wilting point (m) real, parameter :: z0 = 0.01 ! bare-soil roughness length (m) (i.e., under the canopy) -! -! parameters for heat storage parametrization -! - real, parameter :: z0min = 0.2 !minimum roughness length for heat storage - real, parameter :: z0max = 1.0 !maximum roughness length for heat storage ! --------------------------------------------------------------------------------------------------- ! initialize fluxes from veg. fraction @@ -1782,13 +1768,6 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in z0m = z0mg zpd = zpdg end if -! -! compute heat capacity enhancement factor as a function of z0m to mimic heat storage -! - if (lheatstrg .and. (.not. parameters%urban_flag) ) then - cpfac = (z0m - z0min) / (z0max - z0min) - cpfac = 1. + min(max(cpfac, 0.0), 1.0) - endif zlvl = max(zpd,parameters%hvt) + zref if(zpdg >= zlvl) zlvl = zpdg + zref @@ -1893,7 +1872,7 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in latheav = hsub frozen_canopy = .true. end if - gammav = cpair*cpfac*sfcprs/(0.622*latheav) + gammav = cpair*sfcprs/(0.622*latheav) if (tg .gt. tfrz) then latheag = hvap @@ -1902,14 +1881,14 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in latheag = hsub frozen_ground = .true. end if - gammag = cpair*cpfac*sfcprs/(0.622*latheag) + gammag = cpair*sfcprs/(0.622*latheag) ! if (sfctmp .gt. tfrz) then ! lathea = hvap ! else ! lathea = hsub ! end if -! gamma = cpair*cpfac*sfcprs/(0.622*lathea) +! gamma = cpair*sfcprs/(0.622*lathea) ! surface temperatures of the ground and canopy and energy fluxes @@ -1924,7 +1903,7 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in uu ,vv ,sfctmp ,thair ,qair , & !in eair ,rhoair ,snowh ,vai ,gammav ,gammag , & !in fwet ,laisun ,laisha ,cwp ,dzsnso , & !in - zlvl ,cpfac ,zpd ,z0m ,fveg , & !in + zlvl ,zpd ,z0m ,fveg , & !in z0mg ,emv ,emg ,canliq ,fsno, & !in canice ,stc ,df ,rssun ,rssha , & !in rsurf ,latheav ,latheag ,parsun ,parsha ,igs , & !in @@ -1980,7 +1959,6 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in tauy = fveg * tauyv + (1.0 - fveg) * tauyb fira = fveg * irg + (1.0 - fveg) * irb + irc fsh = fveg * shg + (1.0 - fveg) * shb + shc - fshx = fveg * shg/cpfac + (1.0 - fveg) * shb + shc/cpfac fgev = fveg * evg + (1.0 - fveg) * evb ssoil = fveg * ghv + (1.0 - fveg) * ghb fcev = evc @@ -1999,7 +1977,6 @@ subroutine energy (parameters,ice ,vegtyp ,ist ,nsnow ,nsoil , & !in tauy = tauyb fira = irb fsh = shb - fshx = shb fgev = evb ssoil = ghb tg = tgb @@ -3305,8 +3282,7 @@ subroutine vege_flux(parameters,nsnow ,nsoil ,isnow ,vegtyp ,veg , & uu ,vv ,sfctmp ,thair ,qair , & !in eair ,rhoair ,snowh ,vai ,gammav ,gammag, & !in fwet ,laisun ,laisha ,cwp ,dzsnso , & !in - zlvl ,cpfac , & !in - zpd ,z0m ,fveg , & !in + zlvl ,zpd ,z0m ,fveg , & !in z0mg ,emv ,emg ,canliq ,fsno, & !in canice ,stc ,df ,rssun ,rssha , & !in rsurf ,latheav ,latheag ,parsun ,parsha ,igs , & !in @@ -3366,7 +3342,6 @@ subroutine vege_flux(parameters,nsnow ,nsoil ,isnow ,vegtyp ,veg , & real, intent(in) :: laisun !sunlit leaf area index, one-sided (m2/m2) real, intent(in) :: laisha !shaded leaf area index, one-sided (m2/m2) real, intent(in) :: zlvl !reference height (m) - real, intent(in) :: cpfac !heat capacity enhancement factor due to heat storage real, intent(in) :: zpd !zero plane displacement (m) real, intent(in) :: z0m !roughness length, momentum (m) @@ -3724,7 +3699,7 @@ subroutine vege_flux(parameters,nsnow ,nsoil ,isnow ,vegtyp ,veg , & cond = cah + cvh + cgh ata = (sfctmp*cah + tg*cgh) / cond bta = cvh/cond - csh = (1.-bta)*rhoair*cpair*cpfac*cvh + csh = (1.-bta)*rhoair*cpair*cvh ! prepare for latent heat flux above veg. @@ -3735,8 +3710,8 @@ subroutine vege_flux(parameters,nsnow ,nsoil ,isnow ,vegtyp ,veg , & cond = caw + cew + ctw + cgw aea = (eair*caw + estg*cgw) / cond bea = (cew+ctw)/cond - cev = (1.-bea)*cew*rhoair*cpair*cpfac/gammav ! barlage: change to vegetation v3.6 - ctr = (1.-bea)*ctw*rhoair*cpair*cpfac/gammav + cev = (1.-bea)*cew*rhoair*cpair/gammav ! barlage: change to vegetation v3.6 + ctr = (1.-bea)*ctw*rhoair*cpair/gammav ! evaluate surface fluxes with current temperature and solve for dts @@ -3744,9 +3719,9 @@ subroutine vege_flux(parameters,nsnow ,nsoil ,isnow ,vegtyp ,veg , & eah = aea + bea*estv ! canopy air e irc = fveg*(air + cir*tv**4) - shc = fveg*rhoair*cpair*cpfac*cvh * ( tv-tah) - evc = fveg*rhoair*cpair*cpfac*cew * (estv-eah) / gammav ! barlage: change to v in v3.6 - tr = fveg*rhoair*cpair*cpfac*ctw * (estv-eah) / gammav + shc = fveg*rhoair*cpair*cvh * ( tv-tah) + evc = fveg*rhoair*cpair*cew * (estv-eah) / gammav ! barlage: change to v in v3.6 + tr = fveg*rhoair*cpair*ctw * (estv-eah) / gammav if (tv > tfrz) then evc = min(canliq*latheav/dt,evc) ! barlage: add if block for canice in v3.6 else @@ -3786,8 +3761,8 @@ subroutine vege_flux(parameters,nsnow ,nsoil ,isnow ,vegtyp ,veg , & air = - emg*(1.-emv)*lwdn - emg*emv*sb*tv**4 cir = emg*sb - csh = rhoair*cpair*cpfac/rahg - cev = rhoair*cpair*cpfac / (gammag*(rawg+rsurf)) ! barlage: change to ground v3.6 + csh = rhoair*cpair/rahg + cev = rhoair*cpair / (gammag*(rawg+rsurf)) ! barlage: change to ground v3.6 cgh = 2.*df(isnow+1)/dzsnso(isnow+1) ! write(*,*)'inside tg=',tg,'stc(1)=',stc(1) @@ -3842,10 +3817,10 @@ subroutine vege_flux(parameters,nsnow ,nsoil ,isnow ,vegtyp ,veg , & ! consistent vegetation air temperature and vapor pressure since tg is not consistent with the tah/eah ! calculation. -! tah = sfctmp + (shg+shc)/(rhoair*cpair*cpfac*cah) -! tah = sfctmp + (shg*fveg+shc)/(rhoair*cpair*cpfac*cah) ! ground flux need fveg -! eah = eair + (evc+fveg*(tr+evg))/(rhoair*caw*cpair*cpfac/gammag ) -! qfx = (qsfc-qair)*rhoair*cpfac*caw !*cpair/gammag +! tah = sfctmp + (shg+shc)/(rhoair*cpair*cah) +! tah = sfctmp + (shg*fveg+shc)/(rhoair*cpair*cah) ! ground flux need fveg +! eah = eair + (evc+fveg*(tr+evg))/(rhoair*caw*cpair/gammag ) +! qfx = (qsfc-qair)*rhoair*caw !*cpair/gammag ! 2m temperature over vegetation ( corrected for low cq2v values ) if (opt_sfc == 1 .or. opt_sfc == 2) then @@ -3858,7 +3833,7 @@ subroutine vege_flux(parameters,nsnow ,nsoil ,isnow ,vegtyp ,veg , & ! q2v = (eah*0.622/(sfcprs - 0.378*eah)) q2v = qsfc else - t2mv = tah - (shg+shc/fveg)/(rhoair*cpair*cpfac) * 1./cah2 + t2mv = tah - (shg+shc/fveg)/(rhoair*cpair) * 1./cah2 ! q2v = (eah*0.622/(sfcprs - 0.378*eah))- qfx/(rhoair*fv)* 1./vkc * log((2.+z0h)/z0h) q2v = qsfc - ((evc+tr)/fveg+evg)/(latheav*rhoair) * 1./cq2v endif diff --git a/physics/moninedmf.meta b/physics/moninedmf.meta index 25fddea02..09abe71a0 100644 --- a/physics/moninedmf.meta +++ b/physics/moninedmf.meta @@ -244,7 +244,7 @@ intent = in optional = F [heat] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -253,7 +253,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/moninedmf_hafs.meta b/physics/moninedmf_hafs.meta index 13bf39396..d600c8eac 100644 --- a/physics/moninedmf_hafs.meta +++ b/physics/moninedmf_hafs.meta @@ -244,7 +244,7 @@ intent = in optional = F [heat] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -253,7 +253,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/moninshoc.meta b/physics/moninshoc.meta index 80d8f71fc..d5fd594ab 100644 --- a/physics/moninshoc.meta +++ b/physics/moninshoc.meta @@ -220,7 +220,7 @@ intent = in optional = F [heat] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -229,7 +229,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/mp_thompson.F90 b/physics/mp_thompson.F90 index 22b8124c1..e3b760738 100644 --- a/physics/mp_thompson.F90 +++ b/physics/mp_thompson.F90 @@ -21,11 +21,9 @@ module mp_thompson contains !> This subroutine is a wrapper around the actual mp_gt_driver(). -#if 0 !! \section arg_table_mp_thompson_init Argument Table !! \htmlinclude mp_thompson_init.html !! -#endif subroutine mp_thompson_init(ncol, nlev, is_aerosol_aware, & nwfa2d, nifa2d, nwfa, nifa, & mpicomm, mpirank, mpiroot, & @@ -129,11 +127,9 @@ subroutine mp_thompson_init(ncol, nlev, is_aerosol_aware, & end subroutine mp_thompson_init -#if 0 !> \section arg_table_mp_thompson_run Argument Table !! \htmlinclude mp_thompson_run.html !! -#endif !>\ingroup aathompson !>\section gen_thompson_hrrr Thompson MP General Algorithm !>@{ diff --git a/physics/samfdeepcnv.f b/physics/samfdeepcnv.f index 83e1efb80..9ec9ba7f3 100644 --- a/physics/samfdeepcnv.f +++ b/physics/samfdeepcnv.f @@ -63,7 +63,7 @@ end subroutine samfdeepcnv_finalize !! + 2) For the "dynamic control", using a reference cloud work function, estimate the change in cloud work function due to the large-scale dynamics. Following the quasi-equilibrium assumption, calculate the cloud base mass flux required to keep the large-scale convective destabilization in balance with the stabilization effect of the convection. !! -# For grid sizes smaller than the threshold value (currently 8 km): !! + 1) compute the cloud base mass flux using the cumulus updraft velocity averaged ove the whole cloud depth. -!! -# For scale awareness, the updraft fraction (sigma) is obtained as a function of cloud base entrainment. Then, the final cloud base mass flux is obtained by the original mass flux multiplied by the (1−sigma) 2 . +!! -# For scale awareness, the updraft fraction (sigma) is obtained as a function of cloud base entrainment. Then, the final cloud base mass flux is obtained by the original mass flux multiplied by the (1-sigma) 2. !! -# For the "feedback control", calculate updated values of the state variables by multiplying the cloud base mass flux and the tendencies calculated per unit cloud base mass flux from the static control. !! !! \section samfdeep_detailed GFS samfdeepcnv Detailed Algorithm @@ -71,12 +71,14 @@ end subroutine samfdeepcnv_finalize subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & & eps,epsm1,fv,grav,hvap,rd,rv, & & t0c,delt,ntk,ntr,delp, & - & prslp,psp,phil,qtr,q1,t1,u1,v1,fscav, & - & do_ca,ca_deep,cldwrk,rn,kbot,ktop,kcnv,islimsk,garea, & + & prslp,psp,phil,qtr,q1,t1,u1,v1,fscav,hwrf_samfdeep, & + & cldwrk,rn,kbot,ktop,kcnv,islimsk,garea, & & dot,ncloud,ud_mf,dd_mf,dt_mf,cnvw,cnvc, & & QLCN, QICN, w_upi, cf_upi, CNV_MFD, & & CNV_DQLDT,CLCN,CNV_FICE,CNV_NDROP,CNV_NICE,mp_phys,mp_phys_mg,& & clam,c0s,c1,betal,betas,evfact,evfactl,pgcon,asolfac, & + & do_ca, ca_closure, ca_entr, ca_trigger, nthresh, ca_deep, & + & rainevap, & & errmsg,errflg) ! use machine , only : kind_phys @@ -92,8 +94,11 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & real(kind=kind_phys), intent(in) :: psp(im), delp(ix,km), & & prslp(ix,km), garea(im), dot(ix,km), phil(ix,km) real(kind=kind_phys), dimension(:), intent(in) :: fscav + logical, intent(in) :: hwrf_samfdeep + real(kind=kind_phys), intent(in) :: nthresh real(kind=kind_phys), intent(in) :: ca_deep(ix) - logical, intent(in) :: do_ca + real(kind=kind_phys), intent(out) :: rainevap(ix) + logical, intent(in) :: do_ca,ca_closure,ca_entr,ca_trigger integer, intent(inout) :: kcnv(im) ! DH* TODO - check dimensions of qtr, ntr+2 correct? *DH @@ -115,7 +120,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! *GJF integer :: mp_phys, mp_phys_mg - real(kind=kind_phys), intent(in) :: clam, c0s, c1, & + real(kind=kind_phys), intent(in) :: clam, c0s, c1, & & betal, betas, asolfac, & & evfact, evfactl, pgcon character(len=*), intent(out) :: errmsg @@ -128,8 +133,10 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & real(kind=kind_phys) clamd, tkemx, tkemn, dtke, & beta, dbeta, betamx, betamn, & cxlame, cxlamd, + & cxlamu, & xlamde, xlamdd, - & crtlame, crtlamd + & crtlamd, + & crtlame ! ! real(kind=kind_phys) detad real(kind=kind_phys) adw, aup, aafac, d0, @@ -137,7 +144,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & & dh, dhh, dp, & dq, dqsdp, dqsdt, dt, & dt2, dtmax, dtmin, - & dxcrtas, dxcrtuf, + & dxcrtas, dxcrtuf, & dv1h, dv2h, dv3h, & dv1q, dv2q, dv3q, & dz, dz1, e1, edtmax, @@ -180,8 +187,8 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & & rntot(im), vshear(im), xaa0(im), & xlamd(im), xk(im), cina(im), & xmb(im), xmbmax(im), xpwav(im), -! & xpwev(im), xlamx(im), delebar(im,ntr), - & xpwev(im), delebar(im,ntr), + & xpwev(im), xlamx(im), delebar(im,ntr), +! & xpwev(im), delebar(im,ntr), & delubar(im), delvbar(im) ! real(kind=kind_phys) c0(im) @@ -192,12 +199,11 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! ! parameters for updraft velocity calculation real(kind=kind_phys) bet1, cd1, f1, gam1, - & bb1, bb2 -! & bb1, bb2, wucb +! & bb1, bb2 + & bb1, bb2, wucb ! c physical parameters ! parameter(grav=grav,asolfac=0.958) -! parameter(grav=grav) ! parameter(elocp=hvap/cp,el2orc=hvap*hvap/(rv*cp)) ! parameter(c0s=.002,c1=.002,d0=.01) ! parameter(d0=.01) @@ -222,6 +228,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & parameter(cinacrmx=-120.,cinacrmn=-80.) parameter(bet1=1.875,cd1=.506,f1=2.0,gam1=.5) parameter(betaw=.03,dxcrtas=8.e3,dxcrtuf=15.e3) + ! ! local variables and arrays real(kind=kind_phys) pfld(im,km), to(im,km), qo(im,km), @@ -271,16 +278,20 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & errmsg = '' errflg = 0 + elocp = hvap/cp el2orc = hvap*hvap/(rv*cp) fact1 = (cvap-cliq)/rv fact2 = hvap/rv-fact1*t0c -! c----------------------------------------------------------------------- !> ## Determine whether to perform aerosol transport - do_aerosols = (itc > 0) .and. (ntc > 0) .and. (ntr > 0) - if (do_aerosols) do_aerosols = (ntr >= itc + ntc - 3) + if(hwrf_samfdeep) then + do_aerosols = .false. + else + do_aerosols = (itc > 0) .and. (ntc > 0) .and. (ntr > 0) + if (do_aerosols) do_aerosols = (ntr >= itc + ntc - 3) + endif ! c----------------------------------------------------------------------- !> ## Compute preliminary quantities needed for static, dynamic, and feedback control portions of the algorithm. @@ -327,8 +338,17 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & xpwav(i)= 0. xpwev(i)= 0. vshear(i) = 0. + rainevap(i) = 0. gdx(i) = sqrt(garea(i)) enddo +! + if (hwrf_samfdeep) then + do i=1,im + scaldfunc(i)=-1.0 + sigmagfm(i)=-1.0 +! sigmuout(i)=-1.0 + enddo + endif ! !> - determine aerosol-aware rain conversion parameter over land do i=1,im @@ -398,22 +418,15 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! model tunable parameters are all here edtmaxl = .3 edtmaxs = .3 -! clam = .1 -! aafac = .1 - aafac = .05 -! betal = .15 -! betas = .15 -! betal = .05 -! betas = .05 -! evef = 0.07 -! evfact = 0.3 -! evfactl = 0.3 -! - crtlame = 1.0e-4 + if (hwrf_samfdeep) then + aafac = .1 + cxlamu = 1.0e-3 + else + aafac = .05 + crtlame = 1.0e-4 + cxlame = 1.0e-4 + endif crtlamd = 1.0e-4 -! -! cxlame = 1.0e-3 - cxlame = 1.0e-4 cxlamd = 1.0e-4 xlamde = 1.0e-4 xlamdd = 1.0e-4 @@ -465,10 +478,17 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo !> - Calculate interface height do k = 1, km1 + do i=1,im + zi(i,k) = 0.5*(zo(i,k)+zo(i,k+1)) + enddo + enddo + if (hwrf_samfdeep) then + do k = 1, km1 do i=1,im - zi(i,k) = 0.5*(zo(i,k)+zo(i,k+1)) + xlamue(i,k) = clam / zi(i,k) enddo - enddo + enddo + endif c c!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! c convert surface pressure to mb from cb @@ -514,6 +534,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! ! initialize tracer variables ! + if(.not.hwrf_samfdeep) then do n = 3, ntr+2 kk = n-2 do k = 1, km @@ -527,6 +548,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo enddo + endif ! !> - Calculate saturation specific humidity and enforce minimum moisture values. do k = 1, km @@ -623,6 +645,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + if (.not.hwrf_samfdeep) then do n = 1, ntr do k = 1, km1 do i=1,im @@ -632,6 +655,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo enddo + endif c c look for the level of free convection as cloud base c @@ -655,6 +679,14 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & do i=1,im if(kbcon(i) == kmax(i)) cnvflg(i) = .false. enddo +!! + if(do_ca .and. ca_trigger)then + do i=1,im + if(ca_deep(i) > nthresh) then + cnvflg(i) = .true. + endif + enddo + endif !! totflg = .true. do i=1,im @@ -706,6 +738,14 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif endif enddo +!! + if(do_ca .and. ca_trigger)then + do i=1,im + if(ca_deep(i) > nthresh) then + cnvflg(i) = .true. + endif + enddo + endif !! totflg = .true. do i=1,im @@ -717,7 +757,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! turbulent entrainment rate assumed to be proportional ! to subcloud mean TKE ! - if(ntk > 0) then + if(.not. hwrf_samfdeep .and. ntk > 0) then ! do i= 1, im if(cnvflg(i)) then @@ -755,13 +795,25 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! else ! - do i= 1, im - if(cnvflg(i)) then - clamt(i) = clam - endif - enddo + if(do_ca .and. ca_entr)then + do i=1,im + if(cnvflg(i)) then + if(ca_deep(i) > nthresh)then + clamt(i) = clam - clamd + else + clamt(i) = clam + endif + endif + enddo + else + do i=1,im + if(cnvflg(i))then + clamt(i) = clam + endif + enddo + endif ! - endif + endif !(.not. hwrf_samfdeep .and. ntk > 0) ! ! also initially assume updraft entrainment rate ! is an inverse function of height @@ -778,39 +830,49 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & c assume that updraft entrainment rate above cloud base is c same as that at cloud base c -!> - Calculate the entrainment rate according to Han and Pan (2011) \cite han_and_pan_2011 , equation 8, after Bechtold et al. (2008) \cite bechtold_et_al_2008, equation 2 given by: +!> - In HWRF samfdeep, calculate the entrainment rate according to Han and Pan (2011) \cite han_and_pan_2011 , equation 8, after Bechtold et al. (2008) \cite bechtold_et_al_2008, equation 2 given by: !! \f[ !! \epsilon = \epsilon_0F_0 + d_1\left(1-RH\right)F_1 !! \f] !! where \f$\epsilon_0\f$ is the cloud base entrainment rate, \f$d_1\f$ is a tunable constant, and \f$F_0=\left(\frac{q_s}{q_{s,b}}\right)^2\f$ and \f$F_1=\left(\frac{q_s}{q_{s,b}}\right)^3\f$ where \f$q_s\f$ and \f$q_{s,b}\f$ are the saturation specific humidities at a given level and cloud base, respectively. The detrainment rate in the cloud is assumed to be equal to the entrainment rate at cloud base. -! do i=1,im -! if(cnvflg(i)) then -! xlamx(i) = xlamue(i,kbcon(i)) -! endif -! enddo -! do k = 2, km1 -! do i=1,im -! if(cnvflg(i).and. -! & (k > kbcon(i) .and. k < kmax(i))) then -! xlamue(i,k) = xlamx(i) -! endif -! enddo -! enddo + if (hwrf_samfdeep) then + do i=1,im + if(cnvflg(i)) then + xlamx(i) = xlamue(i,kbcon(i)) + endif + enddo + do k = 2, km1 + do i=1,im + if(cnvflg(i).and. & + & (k > kbcon(i) .and. k < kmax(i))) then + xlamue(i,k) = xlamx(i) + endif + enddo + enddo + endif c c specify detrainment rate for the updrafts c !! (The updraft detrainment rate is set constant and equal to the entrainment rate at cloud base.) !! !> - The updraft detrainment rate is vertically constant and proportional to clamt - do k = 1, km1 + if (hwrf_samfdeep) then + do k = 1, km1 do i=1,im if(cnvflg(i) .and. k < kmax(i)) then -! xlamud(i,k) = xlamx(i) -! xlamud(i,k) = crtlamd - xlamud(i,k) = 0.001 * clamt(i) + xlamud(i,k) = xlamx(i) endif enddo - enddo + enddo + else + do k = 1, km1 + do i=1,im + if(cnvflg(i) .and. k < kmax(i)) then + xlamud(i,k) = 0.001 * clamt(i) + endif + enddo + enddo + endif c c entrainment functions decreasing with height (fent), c mimicking a cloud ensemble @@ -831,7 +893,18 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & c organized one depending on the environmental relative humidity c (Bechtold et al., 2008; Derbyshire et al., 2011) c - do k = 2, km1 + if (hwrf_samfdeep) then + do k = 2, km1 + do i=1,im + if(cnvflg(i) .and. + & (k > kbcon(i) .and. k < kmax(i))) then + tem = cxlamu * frh(i,k) * fent2(i,k) + xlamue(i,k) = xlamue(i,k)*fent1(i,k) + tem + endif + enddo + enddo + else + do k = 2, km1 do i=1,im if(cnvflg(i) .and. & (k > kbcon(i) .and. k < kmax(i))) then @@ -841,7 +914,8 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & xlamud(i,k) = xlamud(i,k) + tem1 endif enddo - enddo + enddo + endif ! !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! c @@ -900,15 +974,17 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & pwavo(i) = 0. endif enddo + if (.not.hwrf_samfdeep) then ! for tracers - do n = 1, ntr + do n = 1, ntr do i = 1, im if(cnvflg(i)) then indx = kb(i) ecko(i,indx,n) = ctro(i,indx,n) endif enddo - enddo + enddo + endif c c cloud property is modified by the entrainment process c @@ -939,8 +1015,9 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - do n = 1, ntr - do k = 2, km1 + if (.not.hwrf_samfdeep) then + do n = 1, ntr + do k = 2, km1 do i = 1, im if (cnvflg(i)) then if(k > kb(i) .and. k < kmax(i)) then @@ -952,8 +1029,9 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif endif enddo - enddo - enddo + enddo + enddo + endif c c taking account into convection inhibition due to existence of c dry layers below cloud base @@ -986,6 +1064,14 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif endif enddo +!! + if(do_ca .and. ca_trigger)then + do i=1,im + if(ca_deep(i) > nthresh) then + cnvflg(i) = .true. + endif + enddo + endif !! totflg = .true. do i = 1, im @@ -1020,9 +1106,16 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo !> - Turn off convection if the CIN is less than a critical value (cinacr) which is inversely proportional to the large-scale vertical velocity. - do i = 1, im + if(hwrf_samfdeep) then + do i = 1, im + if(cnvflg(i)) then + cinacr = cinacrmx + if(cina(i) < cinacr) cnvflg(i) = .false. + endif + enddo + else !gfs_samfdeep + do i = 1, im if(cnvflg(i)) then -! if(islimsk(i) == 1) then w1 = w1l w2 = w2l @@ -1049,11 +1142,18 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & tem = 1. - tem tem1= .5*(cinacrmx-cinacrmn) cinacr = cinacrmx - tem * tem1 -! -! cinacr = cinacrmx if(cina(i) < cinacr) cnvflg(i) = .false. endif + enddo + endif !hwrf_samfdeep +!! + if(do_ca .and. ca_trigger)then + do i=1,im + if(ca_deep(i) > nthresh) then + cnvflg(i) = .true. + endif enddo + endif !! totflg = .true. do i=1,im @@ -1089,6 +1189,14 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & if(tem < cthk) cnvflg(i) = .false. endif enddo +!! + if(do_ca .and. ca_trigger)then + do i=1,im + if(ca_deep(i) > nthresh) then + cnvflg(i) = .true. + endif + enddo + endif !! totflg = .true. do i = 1, im @@ -1131,22 +1239,23 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & c specify upper limit of mass flux at cloud base c !> - Calculate the maximum value of the cloud base mass flux using the CFL-criterion-based formula of Han and Pan (2011) \cite han_and_pan_2011, equation 7. - do i = 1, im + if(hwrf_samfdeep) then + do i = 1, im + if(cnvflg(i)) then + k = kbcon(i) + dp = 1000. * del(i,k) + xmbmax(i) = dp / (grav * dt2) + endif + enddo + else + do i = 1, im if(cnvflg(i)) then -! xmbmax(i) = .1 -! k = kbcon(i) dp = 1000. * del(i,k) xmbmax(i) = dp / (2. * grav * dt2) -! -! xmbmax(i) = dp / (grav * dt2) -! -! mbdt(i) = 0.1 * dp / grav -! -! tem = dp / (grav * dt2) -! xmbmax(i) = min(tem, xmbmax(i)) endif - enddo + enddo + endif c c compute cloud moisture property and precipitation c @@ -1378,31 +1487,24 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! ! compute updraft velocity square(wu2) !> - Calculate updraft velocity square(wu2) according to Han et al.'s (2017) \cite han_et_al_2017 equation 7. -! -! bb1 = 2. * (1.+bet1*cd1) -! bb2 = 2. / (f1*(1.+gam1)) -! -! bb1 = 3.9 -! bb2 = 0.67 -! -! bb1 = 2.0 -! bb2 = 4.0 ! bb1 = 4.0 bb2 = 0.8 + if (hwrf_samfdeep) then + do i = 1, im + if (cnvflg(i)) then + k = kbcon1(i) + tem = po(i,k) / (rd * to(i,k)) + wucb = -0.01 * dot(i,k) / (tem * grav) + if(wucb.gt.0.) then + wu2(i,k) = wucb * wucb + else + wu2(i,k) = 0. + endif + endif + enddo + endif ! -! do i = 1, im -! if (cnvflg(i)) then -! k = kbcon1(i) -! tem = po(i,k) / (rd * to(i,k)) -! wucb = -0.01 * dot(i,k) / (tem * grav) -! if(wucb > 0.) then -! wu2(i,k) = wucb * wucb -! else -! wu2(i,k) = 0. -! endif -! endif -! enddo do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -1553,28 +1655,41 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - do i = 1, im + + if (hwrf_samfdeep) then + do i = 1, im + beta = betas + if(islimsk(i) == 1) beta = betal if(cnvflg(i)) then - betamn = betas - if(islimsk(i) == 1) betamn = betal - if(ntk > 0) then - betamx = betamn + dbeta - if(tkemean(i) > tkemx) then - beta = betamn - else if(tkemean(i) < tkemn) then - beta = betamx - else - tem = (betamx - betamn) * (tkemean(i) - tkemn) - beta = betamx - tem / dtke - endif - else - beta = betamn - endif dz = (sumx(i)+zi(i,1))/float(kbcon(i)) tem = 1./float(kbcon(i)) xlamd(i) = (1.-beta**tem)/dz endif - enddo + enddo + else + do i = 1, im + if(cnvflg(i)) then + betamn = betas + if(islimsk(i) == 1) betamn = betal + if(ntk > 0) then + betamx = betamn + dbeta + if(tkemean(i) > tkemx) then + beta = betamn + else if(tkemean(i) < tkemn) then + beta = betamx + else + tem = (betamx - betamn) * (tkemean(i) - tkemn) + beta = betamx - tem / dtke + endif + else + beta = betamn + endif + dz = (sumx(i)+zi(i,1))/float(kbcon(i)) + tem = 1./float(kbcon(i)) + xlamd(i) = (1.-beta**tem)/dz + endif + enddo + endif c c determine downdraft mass flux c @@ -1610,6 +1725,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo ! for tracers + if (.not.hwrf_samfdeep) then do n = 1, ntr do i = 1, im if(cnvflg(i)) then @@ -1618,6 +1734,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + endif cj !> - Calculate the cloud properties as a parcel descends, modified by entrainment and detrainment. Discretization follows Appendix B of Grell (1993) \cite grell_1993 . do k = km1, 1, -1 @@ -1647,6 +1764,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + if(.not.hwrf_samfdeep) then do n = 1, ntr do k = km1, 1, -1 do i = 1, im @@ -1660,6 +1778,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo enddo + endif c !> - Compute the amount of moisture that is necessary to keep the downdraft saturated. do k = km1, 1, -1 @@ -1762,6 +1881,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + if (.not.hwrf_samfdeep) then do n = 1, ntr do k = 1, km do i = 1, im @@ -1771,6 +1891,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo enddo + endif do i = 1, im if(cnvflg(i)) then dp = 1000. * del(i,1) @@ -1784,6 +1905,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & & - vo(i,1)) * grav / dp endif enddo + if (.not.hwrf_samfdeep) then do n = 1, ntr do i = 1, im if(cnvflg(i)) then @@ -1793,6 +1915,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + endif c c--- changed due to subsidence and entrainment c @@ -1857,6 +1980,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + if (.not.hwrf_samfdeep) then do n = 1, ntr do k = 2, km1 do i = 1, im @@ -1878,6 +2002,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo enddo + endif c c------- cloud top c @@ -1902,6 +2027,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & & qlko_ktcon(i) * grav / dp endif enddo + if (.not.hwrf_samfdeep) then do n = 1, ntr do i = 1, im if(cnvflg(i)) then @@ -1912,6 +2038,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + endif c c------- final changed variable per unit mass flux c @@ -2278,7 +2405,17 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! compute convective turn-over time ! !> - Following Bechtold et al. (2008) \cite bechtold_et_al_2008, the convective adjustment time (dtconv) is set to be proportional to the convective turnover time, which is computed using the mean updraft velocity (wc) and the cloud depth. It is also proportional to the grid size (gdx). - do i= 1, im + if(hwrf_samfdeep) then + do i= 1, im + if(cnvflg(i)) then + tem = zi(i,ktcon1(i)) - zi(i,kbcon1(i)) + dtconv(i) = tem / wc(i) + dtconv(i) = max(dtconv(i),dtmin) + dtconv(i) = min(dtconv(i),dtmax) + endif + enddo + else + do i= 1, im if(cnvflg(i)) then tem = zi(i,ktcon1(i)) - zi(i,kbcon1(i)) dtconv(i) = tem / wc(i) @@ -2287,7 +2424,8 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & dtconv(i) = max(dtconv(i),dtmin) dtconv(i) = min(dtconv(i),dtmax) endif - enddo + enddo + endif ! !> - Calculate advective time scale (tauadv) using a mean cloud layer wind speed. do i= 1, im @@ -2366,10 +2504,10 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & tfac = tauadv(i) / dtconv(i) tfac = min(tfac, 1.) xmb(i) = -tfac * fld(i) / xk(i) -! xmb(i) = min(xmb(i),xmbmax(i)) endif enddo !! + !> - If the large scale destabilization is less than zero, or the stabilization by the convection is greater than zero, then the scheme returns to the calling routine without modifying the state variables. totflg = .true. do i=1,im @@ -2379,6 +2517,18 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & !! ! !> - For scale-aware parameterization, the updraft fraction (sigmagfm) is first computed as a function of the lateral entrainment rate at cloud base (see Han et al.'s (2017) \cite han_et_al_2017 equation 4 and 5), following the study by Grell and Freitas (2014) \cite grell_and_freitas_2014. + if(hwrf_samfdeep) then + do i = 1, im + if(cnvflg(i)) then + tem = min(max(xlamx(i), 7.e-5), 3.e-4) + tem = 0.2 / tem + tem1 = 3.14 * tem * tem + sigmagfm(i) = tem1 / garea(i) + sigmagfm(i) = max(sigmagfm(i), 0.001) + sigmagfm(i) = min(sigmagfm(i), 0.999) + endif + enddo + else do i = 1, im if(cnvflg(i)) then tem = min(max(xlamue(i,kbcon(i)), 7.e-5), 3.e-4) @@ -2389,6 +2539,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & sigmagfm(i) = min(sigmagfm(i), 0.999) endif enddo + endif ! !> - Then, calculate the reduction factor (scaldfunc) of the vertical convective eddy transport of mass flux as a function of updraft fraction from the studies by Arakawa and Wu (2013) \cite arakawa_and_wu_2013 (also see Han et al.'s (2017) \cite han_et_al_2017 equation 1 and 2). The final cloud base mass flux with scale-aware parameterization is obtained from the mass flux when sigmagfm << 1, multiplied by the reduction factor (Han et al.'s (2017) \cite han_et_al_2017 equation 2). do i = 1, im @@ -2403,13 +2554,15 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & xmb(i) = min(xmb(i),xmbmax(i)) endif enddo - -!> - If stochastic physics using cellular automata is .true. then perturb the mass-flux here: - - if(do_ca)then - do i=1,im - xmb(i) = xmb(i)*(1.0 + ca_deep(i)*5.) - enddo +! + if (do_ca .and. ca_closure)then + do i = 1, im + if(cnvflg(i)) then + if (ca_deep(i) > nthresh) then + xmb(i) = xmb(i)*1.25 + endif + endif + enddo endif !> - Transport aerosols if present @@ -2437,15 +2590,17 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - do n = 1, ntr - do k = 1, km + if (.not.hwrf_samfdeep) then + do n = 1, ntr + do k = 1, km do i = 1, im if (cnvflg(i) .and. k <= kmax(i)) then ctro(i,k,n) = ctr(i,k,n) endif enddo - enddo - enddo + enddo + enddo + endif c!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! c c--- feedback: simply the changes from the cloud with unit mass flux @@ -2464,11 +2619,13 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & delvbar(i) = 0. qcond(i) = 0. enddo - do n = 1, ntr - do i = 1, im - delebar(i,n) = 0. - enddo - enddo + if (.not.hwrf_samfdeep) then + do n = 1, ntr + do i = 1, im + delebar(i,n) = 0. + enddo + enddo + endif do k = 1, km do i = 1, im if (cnvflg(i) .and. k <= kmax(i)) then @@ -2491,9 +2648,10 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - do n = 1, ntr - kk = n+2 - do k = 1, km + if (.not.hwrf_samfdeep) then + do n = 1, ntr + kk = n+2 + do k = 1, km do i = 1, im if (cnvflg(i) .and. k <= kmax(i)) then if(k <= ktcon(i)) then @@ -2503,8 +2661,9 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif endif enddo - enddo - enddo + enddo + enddo + endif !> - Recalculate saturation specific humidity using the updated temperature. do k = 1, km do i = 1, im @@ -2589,6 +2748,13 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + +!LB: + if(do_ca)then + do i = 1,im + rainevap(i)=delqev(i) + enddo + endif cj ! do i = 1, im ! if(me == 31 .and. cnvflg(i)) then @@ -2689,6 +2855,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + if (.not.hwrf_samfdeep) then do n = 1, ntr kk = n+2 do k = 1, km @@ -2716,6 +2883,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo endif + endif ! ! hchuang code change ! @@ -2751,6 +2919,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & ! ! include TKE contribution from deep convection ! + if (.not.hwrf_samfdeep) then if (ntk > 0) then ! do k = 2, km1 @@ -2798,6 +2967,7 @@ subroutine samfdeepcnv_run (im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo endif + endif ! (.not.hwrf_samfdeep) return end subroutine samfdeepcnv_run diff --git a/physics/samfdeepcnv.meta b/physics/samfdeepcnv.meta index 3b54998fc..d76348ca8 100644 --- a/physics/samfdeepcnv.meta +++ b/physics/samfdeepcnv.meta @@ -265,6 +265,21 @@ kind = kind_phys intent = in optional = F +[hwrf_samfdeep] + standard_name = flag_for_hwrf_samfdeepcnv_scheme + long_name = flag for hwrf samfdeepcnv scheme + units = flag + dimensions = () + type = logical +[nthresh] + standard_name = threshold_for_perturbed_vertical_velocity + long_name = threshold used for perturbed vertical velocity + units = m s-1 + dimensions = () + type = real + kind = kind_phys + intent = in + optional = F [do_ca] standard_name = flag_for_cellular_automata long_name = cellular automata main switch @@ -273,6 +288,30 @@ type = logical intent = in optional = F +[ca_closure] + standard_name = flag_for_global_cellular_automata_closure + long_name = switch for ca on closure + units = flag + dimensions = () + type = logical + intent = in + optional = F +[ca_entr] + standard_name = flag_for_global_cellular_automata_entr + long_name = switch for ca on entr + units = flag + dimensions = () + type = logical + intent = in + optional = F +[ca_trigger] + standard_name = flag_for_global_cellular_automata_trigger + long_name = switch for ca on trigger + units = flag + dimensions = () + type = logical + intent = in + optional = F [ca_deep] standard_name = fraction_of_cellular_automata_for_deep_convection long_name = fraction of cellular automata for deep convection @@ -282,6 +321,15 @@ kind = kind_phys intent = in optional = F +[rainevap] + standard_name = physics_field_for_coupling + long_name = physics_field_for_coupling + units = m2 s-2 + dimensions = (horizontal_dimension) + type = real + kind = kind_phys + intent = out + optional = F [cldwrk] standard_name = cloud_work_function long_name = cloud work function diff --git a/physics/samfshalcnv.f b/physics/samfshalcnv.f index ed80a2f54..7a6db70f0 100644 --- a/physics/samfshalcnv.f +++ b/physics/samfshalcnv.f @@ -55,7 +55,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & & prslp,psp,phil,qtr,q1,t1,u1,v1,fscav, & & rn,kbot,ktop,kcnv,islimsk,garea, & & dot,ncloud,hpbl,ud_mf,dt_mf,cnvw,cnvc, & - & clam,c0s,c1,pgcon,asolfac,errmsg,errflg) + & clam,c0s,c1,pgcon,asolfac,hwrf_samfshal,errmsg,errflg) ! use machine , only : kind_phys use funcphys , only : fpvs @@ -82,6 +82,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! real(kind=kind_phys), intent(in) :: clam, c0s, c1, & & asolfac, pgcon + logical, intent(in) :: hwrf_samfshal character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg ! @@ -140,8 +141,8 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! ! parameters for updraft velocity calculation real(kind=kind_phys) bet1, cd1, f1, gam1, - & bb1, bb2 -! & bb1, bb2, wucb +! & bb1, bb2 + & bb1, bb2, wucb cc c physical parameters @@ -167,8 +168,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & parameter(dtke=tkemx-tkemn) parameter(dthk=25.) parameter(cinpcrmx=180.,cinpcrmn=120.) -! parameter(cinacrmx=-120.,cinacrmn=-120.) - parameter(cinacrmx=-120.,cinacrmn=-80.) + parameter(cinacrmx=-120.) parameter(crtlamd=3.e-4) parameter(dtmax=10800.,dtmin=600.) parameter(bet1=1.875,cd1=.506,f1=2.0,gam1=.5) @@ -202,7 +202,8 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! real(kind=kind_phys) tf, tcr, tcrf parameter (tf=233.16, tcr=263.16, tcrf=1.0/(tcr-tf)) -! + + c----------------------------------------------------------------------- ! ! Initialize CCPP error handling variables @@ -215,10 +216,16 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & fact1 = (cvap-cliq)/rv fact2 = hvap/rv-fact1*t0c + if (.not.hwrf_samfshal) then + cinacrmn=-80. + endif + c----------------------------------------------------------------------- + if (.not.hwrf_samfshal) then !> ## Determine whether to perform aerosol transport - do_aerosols = (itc > 0) .and. (ntc > 0) .and. (ntr > 0) - if (do_aerosols) do_aerosols = (ntr >= itc + ntc - 3) + do_aerosols = (itc > 0) .and. (ntc > 0) .and. (ntr > 0) + if (do_aerosols) do_aerosols = (ntr >= itc + ntc - 3) + endif ! !************************************************************************ ! convert input Pa terms to Cb terms -- Moorthi @@ -234,7 +241,8 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & c initialize arrays c !> - Initialize column-integrated and other single-value-per-column variable arrays. - do i=1,im + if(hwrf_samfshal) then + do i=1,im cnvflg(i) = .true. if(kcnv(i) == 1) cnvflg(i) = .false. if(cnvflg(i)) then @@ -253,7 +261,32 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & cina(i) = 0. vshear(i) = 0. gdx(i) = sqrt(garea(i)) - enddo + scaldfunc(i)=-1.0 ! wang initialized + sigmagfm(i)=-1.0 + enddo + + else !gfs_samfshal + do i=1,im + cnvflg(i) = .true. + if(kcnv(i) == 1) cnvflg(i) = .false. + if(cnvflg(i)) then + kbot(i)=km+1 + ktop(i)=0 + endif + rn(i)=0. + kbcon(i)=km + ktcon(i)=1 + ktconn(i)=1 + kb(i)=km + pdot(i) = 0. + qlko_ktcon(i) = 0. + edt(i) = 0. + aa1(i) = 0. + cina(i) = 0. + vshear(i) = 0. + gdx(i) = sqrt(garea(i)) + enddo + endif !! !> - Return to the calling routine if deep convection is present or the surface buoyancy flux is negative. totflg = .true. @@ -303,15 +336,15 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & dt2 = delt ! c model tunable parameters are all here -! clam = .3 -! aafac = .1 - aafac = .05 + if (hwrf_samfshal) then + aafac = .1 + else + aafac = .05 + endif c evef = 0.07 evfact = 0.3 evfactl = 0.3 ! -! pgcon = 0.7 ! Gregory et al. (1997, QJRMS) -! pgcon = 0.55 ! Zhang & Wu (2003,JAS) w1l = -8.e-3 w2l = -4.e-2 w3l = -5.e-3 @@ -351,11 +384,23 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo !> - Calculate interface height - do k = 1, km1 + if(hwrf_samfshal) then + do k = 1, km1 do i=1,im zi(i,k) = 0.5*(zo(i,k)+zo(i,k+1)) + xlamue(i,k) = clam / zi(i,k) enddo - enddo + enddo + do i=1,im + xlamue(i,km) = xlamue(i,km1) + enddo + else + do k = 1, km1 + do i=1,im + zi(i,k) = 0.5*(zo(i,k)+zo(i,k+1)) + enddo + enddo + endif c c pbl height c @@ -410,8 +455,9 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! ! initialize tracer variables ! - do n = 3, ntr+2 - kk = n-2 + if (.not.hwrf_samfshal) then + do n = 3, ntr+2 + kk = n-2 do k = 1, km do i = 1, im if (cnvflg(i) .and. k <= kmax(i)) then @@ -421,7 +467,8 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - enddo + enddo + endif !> - Calculate saturation specific humidity and enforce minimum moisture values. do k = 1, km do i=1,im @@ -517,15 +564,18 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - do n = 1, ntr - do k = 1, km1 + + if (.not.hwrf_samfshal) then + do n = 1, ntr + do k = 1, km1 do i=1,im if (cnvflg(i) .and. k <= kmax(i)-1) then ctro(i,k,n) = .5 * (ctro(i,k,n) + ctro(i,k+1,n)) endif enddo - enddo - enddo + enddo + enddo + endif c c look for the level of free convection as cloud base c @@ -597,6 +647,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ptem1= .5*(cinpcrmx-cinpcrmn) cinpcr = cinpcrmx - ptem * ptem1 tem1 = pfld(i,kb(i)) - pfld(i,kbcon(i)) + if(tem1 > cinpcr) then cnvflg(i) = .false. endif @@ -612,14 +663,27 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! turbulent entrainment rate assumed to be proportional ! to subcloud mean TKE ! - if(ntk > 0) then ! + +!c +!c specify the detrainment rate for the updrafts +!c + if (hwrf_samfshal) then + do i = 1, im + if(cnvflg(i)) then + xlamud(i) = xlamue(i,kbcon(i)) +! xlamud(i) = crtlamd + endif + enddo + else + if(ntk > 0) then do i= 1, im if(cnvflg(i)) then sumx(i) = 0. tkemean(i) = 0. endif enddo + do k = 1, km1 do i = 1, im if(cnvflg(i)) then @@ -687,6 +751,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & xlamud(i) = 0.001 * clamt(i) endif enddo + endif ! hwrf_samfshal c c determine updraft mass flux for the subcloud layers c @@ -742,6 +807,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo ! for tracers + if (.not. hwrf_samfshal) then do n = 1, ntr do i = 1, im if(cnvflg(i)) then @@ -750,6 +816,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + endif c ! cm is an enhancement factor in entrainment rates for momentum ! @@ -778,8 +845,10 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - do n = 1, ntr - do k = 2, km1 + + if (.not.hwrf_samfshal) then + do n = 1, ntr + do k = 2, km1 do i = 1, im if (cnvflg(i)) then if(k > kb(i) .and. k < kmax(i)) then @@ -791,8 +860,9 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif endif enddo - enddo - enddo + enddo + enddo + endif c c taking account into convection inhibition due to existence of c dry layers below cloud base @@ -859,9 +929,17 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo !> - Turn off convection if the CIN is less than a critical value (cinacr) which is inversely proportional to the large-scale vertical velocity. - do i = 1, im + + if (hwrf_samfshal) then + do i = 1, im + if(cnvflg(i)) then + cinacr = cinacrmx + if(cina(i) < cinacr) cnvflg(i) = .false. + endif + enddo + else + do i = 1, im if(cnvflg(i)) then -! if(islimsk(i) == 1) then w1 = w1l w2 = w2l @@ -888,11 +966,10 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & tem = 1. - tem tem1= .5*(cinacrmx-cinacrmn) cinacr = cinacrmx - tem * tem1 -! -! cinacr = cinacrmx if(cina(i) < cinacr) cnvflg(i) = .false. - endif - enddo + endif + enddo + endif !! totflg = .true. do i=1,im @@ -923,20 +1000,23 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & c specify upper limit of mass flux at cloud base c !> - Calculate the maximum value of the cloud base mass flux using the CFL-criterion-based formula of Han and Pan (2011) \cite han_and_pan_2011, equation 7. - do i = 1, im + if(hwrf_samfshal) then + do i = 1, im + if(cnvflg(i)) then + k = kbcon(i) + dp = 1000. * del(i,k) + xmbmax(i) = dp / (grav * dt2) + endif + enddo + else + do i = 1, im if(cnvflg(i)) then -! xmbmax(i) = .1 -! k = kbcon(i) dp = 1000. * del(i,k) xmbmax(i) = dp / (2. * grav * dt2) -! -! xmbmax(i) = dp / (grav * dt2) -! -! tem = dp / (grav * dt2) -! xmbmax(i) = min(tem, xmbmax(i)) endif - enddo + enddo + endif c c compute cloud moisture property and precipitation c @@ -1156,31 +1236,24 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! ! compute updraft velocity square(wu2) !> - Calculate updraft velocity square(wu2) according to Han et al.'s (2017) \cite han_et_al_2017 equation 7. -! -! bb1 = 2. * (1.+bet1*cd1) -! bb2 = 2. / (f1*(1.+gam1)) -! -! bb1 = 3.9 -! bb2 = 0.67 -! -! bb1 = 2.0 -! bb2 = 4.0 ! bb1 = 4.0 bb2 = 0.8 ! -! do i = 1, im -! if (cnvflg(i)) then -! k = kbcon1(i) -! tem = po(i,k) / (rd * to(i,k)) -! wucb = -0.01 * dot(i,k) / (tem * grav) -! if(wucb > 0.) then -! wu2(i,k) = wucb * wucb -! else -! wu2(i,k) = 0. -! endif -! endif -! enddo + if (hwrf_samfshal) then + do i = 1, im + if (cnvflg(i)) then + k = kbcon1(i) + tem = po(i,k) / (rd * to(i,k)) + wucb = -0.01 * dot(i,k) / (tem * grav) + if(wucb > 0.) then + wu2(i,k) = wucb * wucb + else + wu2(i,k) = 0. + endif + endif + enddo + endif do k = 2, km1 do i = 1, im if (cnvflg(i)) then @@ -1314,15 +1387,17 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - do n = 1, ntr - do k = 1, km + if (.not.hwrf_samfshal) then + do n = 1, ntr + do k = 1, km do i = 1, im if(cnvflg(i) .and. k <= kmax(i)) then dellae(i,k,n) = 0. endif enddo - enddo - enddo + enddo + enddo + endif c c--- changed due to subsidence and entrainment c @@ -1367,8 +1442,9 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo - do n = 1, ntr - do k = 2, km1 + if(.not.hwrf_samfshal) then + do n = 1, ntr + do k = 2, km1 do i = 1, im if (cnvflg(i)) then if(k > kb(i) .and. k < ktcon(i)) then @@ -1381,8 +1457,9 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif endif enddo - enddo - enddo + enddo + enddo + endif c c------- cloud top c @@ -1407,6 +1484,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & & qlko_ktcon(i) * grav / dp endif enddo + if (.not.hwrf_samfshal) then do n = 1, ntr do i = 1, im if(cnvflg(i)) then @@ -1417,6 +1495,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + endif ! ! compute convective turn-over time ! @@ -1425,8 +1504,10 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & if(cnvflg(i)) then tem = zi(i,ktcon1(i)) - zi(i,kbcon1(i)) dtconv(i) = tem / wc(i) - tfac = 1. + gdx(i) / 75000. - dtconv(i) = tfac * dtconv(i) + if (.not.hwrf_samfshal) then + tfac = 1. + gdx(i) / 75000. + dtconv(i) = tfac * dtconv(i) + endif dtconv(i) = max(dtconv(i),dtmin) dtconv(i) = max(dtconv(i),dt2) dtconv(i) = min(dtconv(i),dtmax) @@ -1503,13 +1584,15 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! !> - Transport aerosols if present ! - if (do_aerosols) + if (.not.hwrf_samfshal) then + if (do_aerosols) & call samfshalcnv_aerosols(im, ix, km, itc, ntc, ntr, delt, ! & xlamde, xlamdd, cnvflg, jmin, kb, kmax, kbcon, ktcon, fscav, & cnvflg, kb, kmax, kbcon, ktcon, fscav, ! & edto, xlamd, xmb, c0t, eta, etad, zi, xlamue, xlamud, delp, & xmb, c0t, eta, zi, xlamue, xlamud, delp, & qtr, qaero) + endif ! !> ## For the "feedback control", calculate updated values of the state variables by multiplying the cloud base mass flux and the tendencies calculated per unit cloud base mass flux from the static control. !! - Recalculate saturation specific humidity. @@ -1539,11 +1622,13 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & delvbar(i) = 0. qcond(i) = 0. enddo - do n = 1, ntr - do i = 1, im + if (.not. hwrf_samfshal) then + do n = 1, ntr + do i = 1, im delebar(i,n) = 0. - enddo - enddo + enddo + enddo + endif do k = 1, km do i = 1, im if (cnvflg(i)) then @@ -1566,6 +1651,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & endif enddo enddo + if (.not.hwrf_samfshal) then do n = 1, ntr kk = n+2 do k = 1, km @@ -1580,6 +1666,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo enddo + endif ! !> - Recalculate saturation specific humidity using the updated temperature. do k = 1, km @@ -1750,7 +1837,8 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! endif !> - Store aerosol concentrations if present - if (do_aerosols) then + if (.not. hwrf_samfshal) then + if (do_aerosols) then do n = 1, ntc kk = n + itc - 1 do k = 1, km @@ -1762,6 +1850,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & enddo enddo endif + endif ! ! hchuang code change ! @@ -1787,6 +1876,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & ! ! include TKE contribution from shallow convection ! + if (.not.hwrf_samfshal) then if (ntk > 0) then ! do k = 2, km1 @@ -1804,6 +1894,7 @@ subroutine samfshalcnv_run(im,ix,km,itc,ntc,cliq,cp,cvap, & enddo ! endif + endif !! return end subroutine samfshalcnv_run diff --git a/physics/samfshalcnv.meta b/physics/samfshalcnv.meta index 5189afd95..4e7fd3898 100644 --- a/physics/samfshalcnv.meta +++ b/physics/samfshalcnv.meta @@ -422,6 +422,14 @@ kind = kind_phys intent = in optional = F +[hwrf_samfshal] + standard_name = flag_for_hwrf_samfshalcnv_scheme + long_name = flag for hwrf samfshalcnv scheme + units = flag + dimensions = () + type = logical + intent = in + optional = F [errmsg] standard_name = ccpp_error_message long_name = error message for error handling in CCPP diff --git a/physics/satmedmfvdif.meta b/physics/satmedmfvdif.meta index e127f14e5..c33e4b85f 100644 --- a/physics/satmedmfvdif.meta +++ b/physics/satmedmfvdif.meta @@ -357,7 +357,7 @@ intent = in optional = F [heat] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -366,7 +366,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/satmedmfvdifq.F b/physics/satmedmfvdifq.F index 30e195cde..d465b7c5e 100644 --- a/physics/satmedmfvdifq.F +++ b/physics/satmedmfvdifq.F @@ -212,7 +212,7 @@ subroutine satmedmfvdifq_run(ix,im,km,ntrac,ntcw,ntiw,ntke, & parameter(gamcrt=3.,gamcrq=0.,sfcfrac=0.1) parameter(vk=0.4,rimin=-100.) parameter(rbcr=0.25,zolcru=-0.02,tdzmin=1.e-3) - parameter(rlmn=30.,rlmn1=5.,rlmn2=10.) + parameter(rlmn=30.,rlmn1=5.,rlmn2=15.) parameter(rlmx=300.,elmx=300.) parameter(prmin=0.25,prmax=4.0) parameter(pr0=1.0,prtke=1.0,prscu=0.67) @@ -222,7 +222,7 @@ subroutine satmedmfvdifq_run(ix,im,km,ntrac,ntcw,ntiw,ntke, & parameter(aphi5=5.,aphi16=16.) parameter(elmfac=1.0,elefac=1.0,cql=100.) parameter(dw2min=1.e-4,dkmax=1000.,xkgdx=5000.) - parameter(qlcr=3.5e-5,zstblmax=2500.,xkzinv=0.1) + parameter(qlcr=3.5e-5,zstblmax=2500.,xkzinv=0.15) parameter(h1=0.33333333) parameter(ck0=0.4,ck1=0.15,ch0=0.4,ch1=0.15) parameter(ce0=0.4) diff --git a/physics/satmedmfvdifq.meta b/physics/satmedmfvdifq.meta index 4e9b05239..26667a627 100644 --- a/physics/satmedmfvdifq.meta +++ b/physics/satmedmfvdifq.meta @@ -357,7 +357,7 @@ intent = in optional = F [heat] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -366,7 +366,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/sfc_diff.f b/physics/sfc_diff.f index 60d5ceeea..2a723e70c 100644 --- a/physics/sfc_diff.f +++ b/physics/sfc_diff.f @@ -68,19 +68,19 @@ subroutine sfc_diff_run (im,rvrdm1,eps,epsm1,grav, & !intent(in) & flag_iter,redrag, & !intent(in) & u10m,v10m,sfc_z0_type, & !hafs,z0 type !intent(in) & wet,dry,icy, & !intent(in) - & tskin_ocn, tskin_lnd, tskin_ice, & !intent(in) - & tsurf_ocn, tsurf_lnd, tsurf_ice, & !intent(in) - & snwdph_ocn,snwdph_lnd,snwdph_ice, & !intent(in) - & z0rl_ocn, z0rl_lnd, z0rl_ice, & !intent(inout) - & ustar_ocn, ustar_lnd, ustar_ice, & !intent(inout) - & cm_ocn, cm_lnd, cm_ice, & !intent(inout) - & ch_ocn, ch_lnd, ch_ice, & !intent(inout) - & rb_ocn, rb_lnd, rb_ice, & !intent(inout) - & stress_ocn,stress_lnd,stress_ice, & !intent(inout) - & fm_ocn, fm_lnd, fm_ice, & !intent(inout) - & fh_ocn, fh_lnd, fh_ice, & !intent(inout) - & fm10_ocn, fm10_lnd, fm10_ice, & !intent(inout) - & fh2_ocn, fh2_lnd, fh2_ice, & !intent(inout) + & tskin_wat, tskin_lnd, tskin_ice, & !intent(in) + & tsurf_wat, tsurf_lnd, tsurf_ice, & !intent(in) + & snwdph_wat,snwdph_lnd,snwdph_ice, & !intent(in) + & z0rl_wat, z0rl_lnd, z0rl_ice, & !intent(inout) + & ustar_wat, ustar_lnd, ustar_ice, & !intent(inout) + & cm_wat, cm_lnd, cm_ice, & !intent(inout) + & ch_wat, ch_lnd, ch_ice, & !intent(inout) + & rb_wat, rb_lnd, rb_ice, & !intent(inout) + & stress_wat,stress_lnd,stress_ice, & !intent(inout) + & fm_wat, fm_lnd, fm_ice, & !intent(inout) + & fh_wat, fh_lnd, fh_ice, & !intent(inout) + & fm10_wat, fm10_lnd, fm10_ice, & !intent(inout) + & fh2_wat, fh2_lnd, fh2_ice, & !intent(inout) & errmsg, errflg) !intent(out) ! implicit none @@ -100,21 +100,21 @@ subroutine sfc_diff_run (im,rvrdm1,eps,epsm1,grav, & !intent(in) & wind,sigmaf,shdmax, & & z0pert,ztpert ! mg, sfc-perts real(kind=kind_phys), dimension(im), intent(in) :: & - & tskin_ocn, tskin_lnd, tskin_ice, & - & tsurf_ocn, tsurf_lnd, tsurf_ice, & - & snwdph_ocn,snwdph_lnd,snwdph_ice + & tskin_wat, tskin_lnd, tskin_ice, & + & tsurf_wat, tsurf_lnd, tsurf_ice, & + & snwdph_wat,snwdph_lnd,snwdph_ice real(kind=kind_phys), dimension(im), intent(inout) :: & - & z0rl_ocn, z0rl_lnd, z0rl_ice, & - & ustar_ocn, ustar_lnd, ustar_ice, & - & cm_ocn, cm_lnd, cm_ice, & - & ch_ocn, ch_lnd, ch_ice, & - & rb_ocn, rb_lnd, rb_ice, & - & stress_ocn,stress_lnd,stress_ice, & - & fm_ocn, fm_lnd, fm_ice, & - & fh_ocn, fh_lnd, fh_ice, & - & fm10_ocn, fm10_lnd, fm10_ice, & - & fh2_ocn, fh2_lnd, fh2_ice + & z0rl_wat, z0rl_lnd, z0rl_ice, & + & ustar_wat, ustar_lnd, ustar_ice, & + & cm_wat, cm_lnd, cm_ice, & + & ch_wat, ch_lnd, ch_ice, & + & rb_wat, rb_lnd, rb_ice, & + & stress_wat,stress_lnd,stress_ice, & + & fm_wat, fm_lnd, fm_ice, & + & fh_wat, fh_lnd, fh_ice, & + & fm10_wat, fm10_lnd, fm10_ice, & + & fh2_wat, fh2_lnd, fh2_ice character(len=*), intent(out) :: errmsg integer, intent(out) :: errflg ! @@ -220,11 +220,15 @@ subroutine sfc_diff_run (im,rvrdm1,eps,epsm1,grav, & !intent(in) z0max = max(z0max, 1.0e-6) ! czilc = 10.0 ** (- (0.40/0.07) * z0) ! fei's canopy height dependance of czil - czilc = 0.8 +! czilc = 0.8 - tem1 = 1.0 - sigmaf(i) - ztmax = z0max*exp( - tem1*tem1 - & * czilc*ca*sqrt(ustar_lnd(i)*(0.01/1.5e-05))) +! tem1 = 1.0 - sigmaf(i) +! ztmax = z0max*exp( - tem1*tem1 +! & * czilc*ca*sqrt(ustar_lnd(i)*(0.01/1.5e-05))) +! + czilc = 10.0 ** (- 4. * z0max) ! Trier et al. (2011, WAF) + ztmax = z0max * exp( - czilc * ca + & * 258.2 * sqrt(ustar_lnd(i)*z0max) ) ! mg, sfc-perts: add surface perturbations to ztmax/z0max ratio over land @@ -261,11 +265,15 @@ subroutine sfc_diff_run (im,rvrdm1,eps,epsm1,grav, & !intent(in) ! czilc = 10.0 ** (- (0.40/0.07) * z0) ! fei's canopy height ! dependance of czil - czilc = 0.8 +! czilc = 0.8 + +! tem1 = 1.0 - sigmaf(i) +! ztmax = z0max*exp( - tem1*tem1 +! & * czilc*ca*sqrt(ustar_ice(i)*(0.01/1.5e-05))) + czilc = 10.0 ** (- 4. * z0max) ! Trier et al. (2011, WAF) + ztmax = z0max * exp( - czilc * ca + & * 258.2 * sqrt(ustar_ice(i)*z0max) ) - tem1 = 1.0 - sigmaf(i) - ztmax = z0max*exp( - tem1*tem1 - & * czilc*ca*sqrt(ustar_ice(i)*(0.01/1.5e-05))) ztmax = max(ztmax, 1.0e-6) ! call stability @@ -281,17 +289,17 @@ subroutine sfc_diff_run (im,rvrdm1,eps,epsm1,grav, & !intent(in) ! the stuff now put into "stability" if (wet(i)) then ! Some open ocean - tvs = 0.5 * (tsurf_ocn(i)+tskin_ocn(i)) * virtfac - z0 = 0.01 * z0rl_ocn(i) + tvs = 0.5 * (tsurf_wat(i)+tskin_wat(i)) * virtfac + z0 = 0.01 * z0rl_wat(i) z0max = max(1.0e-6, min(z0,z1(i))) - ustar_ocn(i) = sqrt(grav * z0 / charnock) + ustar_wat(i) = sqrt(grav * z0 / charnock) wind10m = sqrt(u10m(i)*u10m(i)+v10m(i)*v10m(i)) !** test xubin's new z0 ! ztmax = z0max - restar = max(ustar_ocn(i)*z0max*visi, 0.000001) + restar = max(ustar_wat(i)*z0max*visi, 0.000001) ! restar = log(restar) ! restar = min(restar,5.) @@ -314,17 +322,17 @@ subroutine sfc_diff_run (im,rvrdm1,eps,epsm1,grav, & !intent(in) ! call stability ! --- inputs: - & (z1(i), snwdph_ocn(i), thv1, wind(i), + & (z1(i), snwdph_wat(i), thv1, wind(i), & z0max, ztmax, tvs, grav, ! --- outputs: - & rb_ocn(i), fm_ocn(i), fh_ocn(i), fm10_ocn(i), fh2_ocn(i), - & cm_ocn(i), ch_ocn(i), stress_ocn(i), ustar_ocn(i)) + & rb_wat(i), fm_wat(i), fh_wat(i), fm10_wat(i), fh2_wat(i), + & cm_wat(i), ch_wat(i), stress_wat(i), ustar_wat(i)) ! ! update z0 over ocean ! if (sfc_z0_type >= 0) then if (sfc_z0_type == 0) then - z0 = (charnock / grav) * ustar_ocn(i) * ustar_ocn(i) + z0 = (charnock / grav) * ustar_wat(i) * ustar_wat(i) ! mbek -- toga-coare flux algorithm ! z0 = (charnock / grav) * ustar(i)*ustar(i) + arnu/ustar(i) @@ -335,19 +343,19 @@ subroutine sfc_diff_run (im,rvrdm1,eps,epsm1,grav, & !intent(in) ! z0 = arnu / (ustar(i) * ff ** pp) if (redrag) then - z0rl_ocn(i) = 100.0 * max(min(z0, z0s_max), 1.e-7) + z0rl_wat(i) = 100.0 * max(min(z0, z0s_max), 1.e-7) else - z0rl_ocn(i) = 100.0 * max(min(z0,.1), 1.e-7) + z0rl_wat(i) = 100.0 * max(min(z0,.1), 1.e-7) endif elseif (sfc_z0_type == 6) then ! wang call znot_m_v6(wind10m, z0) ! wind, m/s, z0, m - z0rl_ocn(i) = 100.0 * z0 ! cm + z0rl_wat(i) = 100.0 * z0 ! cm elseif (sfc_z0_type == 7) then ! wang call znot_m_v7(wind10m, z0) ! wind, m/s, z0, m - z0rl_ocn(i) = 100.0 * z0 ! cm + z0rl_wat(i) = 100.0 * z0 ! cm else - z0rl_ocn(i) = 1.0e-4 + z0rl_wat(i) = 1.0e-4 endif endif diff --git a/physics/sfc_diff.meta b/physics/sfc_diff.meta index 232b0050f..ab99dcb06 100644 --- a/physics/sfc_diff.meta +++ b/physics/sfc_diff.meta @@ -244,7 +244,7 @@ type = logical intent = in optional = F -[tskin_ocn] +[tskin_wat] standard_name = surface_skin_temperature_over_ocean_interstitial long_name = surface skin temperature over ocean (temporary use as interstitial) units = K @@ -271,7 +271,7 @@ kind = kind_phys intent = in optional = F -[tsurf_ocn] +[tsurf_wat] standard_name = surface_skin_temperature_after_iteration_over_ocean long_name = surface skin temperature after iteration over ocean units = K @@ -298,7 +298,7 @@ kind = kind_phys intent = in optional = F -[snwdph_ocn] +[snwdph_wat] standard_name = surface_snow_thickness_water_equivalent_over_ocean long_name = water equivalent snow depth over ocean units = mm @@ -325,7 +325,7 @@ kind = kind_phys intent = in optional = F -[z0rl_ocn] +[z0rl_wat] standard_name = surface_roughness_length_over_ocean_interstitial long_name = surface roughness length over ocean (temporary use as interstitial) units = cm @@ -352,7 +352,7 @@ kind = kind_phys intent = inout optional = F -[ustar_ocn] +[ustar_wat] standard_name = surface_friction_velocity_over_ocean long_name = surface friction velocity over ocean units = m s-1 @@ -379,7 +379,7 @@ kind = kind_phys intent = inout optional = F -[cm_ocn] +[cm_wat] standard_name = surface_drag_coefficient_for_momentum_in_air_over_ocean long_name = surface exchange coeff for momentum over ocean units = none @@ -406,7 +406,7 @@ kind = kind_phys intent = inout optional = F -[ch_ocn] +[ch_wat] standard_name = surface_drag_coefficient_for_heat_and_moisture_in_air_over_ocean long_name = surface exchange coeff heat & moisture over ocean units = none @@ -433,7 +433,7 @@ kind = kind_phys intent = inout optional = F -[rb_ocn] +[rb_wat] standard_name = bulk_richardson_number_at_lowest_model_level_over_ocean long_name = bulk Richardson number at the surface over ocean units = none @@ -460,7 +460,7 @@ kind = kind_phys intent = inout optional = F -[stress_ocn] +[stress_wat] standard_name = surface_wind_stress_over_ocean long_name = surface wind stress over ocean units = m2 s-2 @@ -487,7 +487,7 @@ kind = kind_phys intent = inout optional = F -[fm_ocn] +[fm_wat] standard_name = Monin_Obukhov_similarity_function_for_momentum_over_ocean long_name = Monin-Obukhov similarity function for momentum over ocean units = none @@ -514,7 +514,7 @@ kind = kind_phys intent = inout optional = F -[fh_ocn] +[fh_wat] standard_name = Monin_Obukhov_similarity_function_for_heat_over_ocean long_name = Monin-Obukhov similarity function for heat over ocean units = none @@ -541,7 +541,7 @@ kind = kind_phys intent = inout optional = F -[fm10_ocn] +[fm10_wat] standard_name = Monin_Obukhov_similarity_function_for_momentum_at_10m_over_ocean long_name = Monin-Obukhov similarity parameter for momentum at 10m over ocean units = none @@ -568,7 +568,7 @@ kind = kind_phys intent = inout optional = F -[fh2_ocn] +[fh2_wat] standard_name = Monin_Obukhov_similarity_function_for_heat_at_2m_over_ocean long_name = Monin-Obukhov similarity parameter for heat at 2m over ocean units = none diff --git a/physics/sfc_drv_ruc.F90 b/physics/sfc_drv_ruc.F90 index 3b4b8a118..81eefcce5 100644 --- a/physics/sfc_drv_ruc.F90 +++ b/physics/sfc_drv_ruc.F90 @@ -130,11 +130,9 @@ end subroutine lsm_ruc_finalize !> \defgroup lsm_ruc_group GSD RUC LSM Model !! This module contains the RUC Land Surface Model developed by NOAA/GSD !! (Smirnova et al. 2016 \cite Smirnova_2016). -#if 0 !> \section arg_table_lsm_ruc_run Argument Table !! \htmlinclude lsm_ruc_run.html !! -#endif !>\section gen_lsmruc GSD RUC LSM General Algorithm ! DH* TODO - make order of arguments the same as in the metadata table subroutine lsm_ruc_run & ! inputs @@ -147,7 +145,7 @@ subroutine lsm_ruc_run & ! inputs & imp_physics, imp_physics_gfdl, imp_physics_thompson, & & smcwlt2, smcref2, do_mynnsfclay, & & con_cp, con_rv, con_rd, con_g, con_pi, con_hvap, con_fvirt,& ! constants - & weasd, snwdph, tskin, tskin_ocn, & ! in/outs + & weasd, snwdph, tskin, tskin_wat, & ! in/outs & rainnc, rainc, ice, snow, graupel, & ! in & srflag, smois, tslb, sh2o, keepfr, smfrkeep, & ! in/outs, on RUC levels & canopy, trans, tsurf, tsnow, zorl, & @@ -196,7 +194,7 @@ subroutine lsm_ruc_run & ! inputs real (kind=kind_phys), dimension(lsoil_ruc) :: dzs real (kind=kind_phys), dimension(lsoil_ruc), intent(inout ) :: zs real (kind=kind_phys), dimension(im), intent(inout) :: weasd, & - & snwdph, tskin, tskin_ocn, & + & snwdph, tskin, tskin_wat, & & srflag, canopy, trans, tsurf, zorl, tsnow, & & sfcqc, sfcqv, sfcdew, fice, tice, sfalb, smcwlt2, smcref2 ! --- in @@ -314,7 +312,7 @@ subroutine lsm_ruc_run & ! inputs call rucinit (flag_restart, im, lsoil_ruc, lsoil, nlev, & ! in isot, soiltyp, vegtype, fice, & ! in - land, tskin, tskin_ocn, tg3, & ! in + land, tskin, tskin_wat, tg3, & ! in smc, slc, stc, & ! in smcref2, smcwlt2, & ! inout lsm_ruc, lsm, & ! in @@ -1040,7 +1038,7 @@ end subroutine lsm_ruc_run !! This subroutine contains RUC LSM initialization. subroutine rucinit (restart, im, lsoil_ruc, lsoil, nlev, & ! in isot, soiltyp, vegtype, fice, & ! in - land, tsurf, tsurf_ocn, & ! in + land, tsurf, tsurf_wat, & ! in tg3, smc, slc, stc, & ! in smcref2, smcwlt2, & ! inout lsm_ruc, lsm, & ! in @@ -1057,7 +1055,7 @@ subroutine rucinit (restart, im, lsoil_ruc, lsoil, nlev, & ! in integer, intent(in ) :: lsoil_ruc integer, intent(in ) :: lsoil logical, dimension(im), intent(in ) :: land - real (kind=kind_phys), dimension(im), intent(in ) :: tsurf, tsurf_ocn + real (kind=kind_phys), dimension(im), intent(in ) :: tsurf, tsurf_wat real (kind=kind_phys), dimension(im), intent(inout) :: smcref2 real (kind=kind_phys), dimension(im), intent(inout) :: smcwlt2 real (kind=kind_phys), dimension(im), intent(in ) :: tg3 @@ -1216,7 +1214,7 @@ subroutine rucinit (restart, im, lsoil_ruc, lsoil, nlev, & ! in ! land only version if (land(i)) then tsk(i,j) = tsurf(i) - sst(i,j) = tsurf_ocn(i) + sst(i,j) = tsurf_wat(i) tbot(i,j)= tg3(i) ivgtyp(i,j)=vegtype(i) isltyp(i,j)=soiltyp(i) diff --git a/physics/sfc_drv_ruc.meta b/physics/sfc_drv_ruc.meta index 6eaadfbb4..aa0ad3d0c 100644 --- a/physics/sfc_drv_ruc.meta +++ b/physics/sfc_drv_ruc.meta @@ -782,7 +782,7 @@ kind = kind_phys intent = inout optional = F -[tskin_ocn] +[tskin_wat] standard_name = surface_skin_temperature_over_ocean_interstitial long_name = surface skin temperature over ocean (temporary use as interstitial) units = K diff --git a/physics/sfc_noahmp_drv.f b/physics/sfc_noahmp_drv.f index 5ddd5aefc..bdba632bf 100644 --- a/physics/sfc_noahmp_drv.f +++ b/physics/sfc_noahmp_drv.f @@ -69,9 +69,6 @@ end subroutine noahmpdrv_finalize !! - Calculate the surface specific humidity and convert surface sensible and latent heat fluxes in W m-2 from their kinematic values. !! - If a "guess" run, restore the land-related prognostic fields. ! ! -! lheatstrg- logical, flag for canopy heat storage 1 ! -! parameterization ! -! ! !----------------------------------- subroutine noahmpdrv_run & !................................... @@ -80,7 +77,6 @@ subroutine noahmpdrv_run & & sigmaf, sfcemis, dlwflx, dswsfc, snet, delt, tg3, cm, ch, & & prsl1, prslki, zf, dry, wind, slopetyp, & & shdmin, shdmax, snoalb, sfalb, flag_iter, flag_guess, & - & lheatstrg, & & idveg, iopt_crs, iopt_btr, iopt_run, iopt_sfc, iopt_frz, & & iopt_inf, iopt_rad, iopt_alb, iopt_snf, iopt_tbot, & & iopt_stc, xlatin, xcoszin, iyrlen, julian, & @@ -169,8 +165,6 @@ subroutine noahmpdrv_run & real (kind=kind_phys), intent(in) :: delt logical, dimension(im), intent(in) :: flag_iter, flag_guess - logical, intent(in) :: lheatstrg - real (kind=kind_phys), intent(in) :: con_hvap, con_cp, con_jcal, & & rhoh2o, con_eps, con_epsm1, con_fvirt, & & con_rd, con_hfus @@ -270,8 +264,6 @@ subroutine noahmpdrv_run & & irb,tr,evc,chleaf,chuc,chv2,chb2, & & fpice,pahv,pahg,pahb,pah,co2pp,o2pp,ch2b - real (kind=kind_phys) :: cpfac - integer :: i, k, ice, stype, vtype ,slope,nroot,couple logical :: flag(im) logical :: snowng,frzgra @@ -660,11 +652,6 @@ subroutine noahmpdrv_run & call noahmp_options(idveg ,iopt_crs,iopt_btr,iopt_run,iopt_sfc, & & iopt_frz,iopt_inf,iopt_rad,iopt_alb,iopt_snf,iopt_tbot,iopt_stc) -! -! initialize heat capacity enhancement factor for heat storage parameterization -! - cpfac = 1.0 - if ( vtype == isice_table ) then ice = -1 @@ -752,7 +739,6 @@ subroutine noahmpdrv_run & & qc , swdn , lwdn ,& ! in : forcing & pconv , pnonc , pshcv , psnow , pgrpl , phail ,& ! in : forcing & tbot , co2pp , o2pp , foln , ficeold , zlvl ,& ! in : forcing - & lheatstrg ,& ! in : canopy heat storage & alboldx , sneqvox ,& ! in/out : & tsnsox , slsoil , smsoil , tahx , eahx , fwetx ,& ! in/out : & canliqx , canicex , tvx , tgx , qsfc1d , qsnowx ,& ! in/out : @@ -760,7 +746,7 @@ subroutine noahmpdrv_run & & zwtx , wax , wtx , wslakex , lfmassx , rtmassx,& ! in/out : & stmassx , woodx , stblcpx , fastcpx , xlaix ,xsaix ,& ! in/out : & cmx , chx , taussx ,& ! in/out : - & smcwtdx ,deeprechx, rechx , cpfac ,& ! in/out : + & smcwtdx ,deeprechx, rechx ,& ! in/out : & z0wrf ,& ! out & fsa , fsr , fira , fsh , ssoil , fcev ,& ! out : & fgev , fctr , ecan , etran , edir , trad ,& ! out : @@ -901,7 +887,7 @@ subroutine noahmpdrv_run & ! ssoil = -1.0 *ssoil call penman (sfctmp,sfcprs,chx,t2v,th2,prcp,fdown,ssoil, & - & cpfac,q2,q2sat,etp,snowng,frzgra,ffrozp,dqsdt2,emissi,fsno) + & q2,q2sat,etp,snowng,frzgra,ffrozp,dqsdt2,emissi,fsno) ep(i) = etp @@ -1170,7 +1156,7 @@ end subroutine transfer_mp_parameters !! partial sums/products are also calculated and passed back to the !! calling routine for later use. subroutine penman (sfctmp,sfcprs,ch,t2v,th2,prcp,fdown,ssoil, & - & cpfac,q2,q2sat,etp,snowng,frzgra,ffrozp, & + & q2,q2sat,etp,snowng,frzgra,ffrozp, & & dqsdt2,emissi_in,sncovr) ! etp is calcuated right after ssoil @@ -1181,12 +1167,11 @@ subroutine penman (sfctmp,sfcprs,ch,t2v,th2,prcp,fdown,ssoil, & implicit none logical, intent(in) :: snowng, frzgra real, intent(in) :: ch, dqsdt2,fdown,prcp,ffrozp, & - & q2, q2sat,ssoil,cpfac, sfcprs, sfctmp, & + & q2, q2sat,ssoil, sfcprs, sfctmp, & & t2v, th2,emissi_in,sncovr real, intent(out) :: etp real :: epsca,flx2,rch,rr,t24 real :: a, delta, fnet,rad,rho,emissi,elcp1,lvs - real :: elcpx real, parameter :: elcp = 2.4888e+3, lsubc = 2.501000e+6,cp = 1004.6 real, parameter :: lsubs = 2.83e+6, rd = 287.05, cph2o = 4.1855e+3 @@ -1200,12 +1185,11 @@ subroutine penman (sfctmp,sfcprs,ch,t2v,th2,prcp,fdown,ssoil, & ! prepare partial quantities for penman equation. ! ---------------------------------------------------------------------- emissi=emissi_in - elcpx = elcp / cpfac -! elcp1 = (1.0-sncovr)*elcpx + sncovr*elcpx*lsubs/lsubc +! elcp1 = (1.0-sncovr)*elcp + sncovr*elcp*lsubs/lsubc lvs = (1.0-sncovr)*lsubc + sncovr*lsubs flx2 = 0.0 - delta = elcpx * dqsdt2 + delta = elcp * dqsdt2 ! delta = elcp1 * dqsdt2 t24 = sfctmp * sfctmp * sfctmp * sfctmp rr = t24 * 6.48e-8 / (sfcprs * ch) + 1.0 @@ -1216,7 +1200,7 @@ subroutine penman (sfctmp,sfcprs,ch,t2v,th2,prcp,fdown,ssoil, & ! adjust the partial sums / products with the latent heat ! effects caused by falling precipitation. ! ---------------------------------------------------------------------- - rch = rho * cp * cpfac * ch + rch = rho * cp * ch if (.not. snowng) then if (prcp > 0.0) rr = rr + cph2o * prcp / rch else @@ -1239,7 +1223,7 @@ subroutine penman (sfctmp,sfcprs,ch,t2v,th2,prcp,fdown,ssoil, & ! ---------------------------------------------------------------------- end if rad = fnet / rch + th2- sfctmp - a = elcpx * (q2sat - q2) + a = elcp * (q2sat - q2) ! a = elcp1 * (q2sat - q2) epsca = (a * rr + rad * delta) / (delta + rr) etp = epsca * rch / lsubc diff --git a/physics/sfc_noahmp_drv.meta b/physics/sfc_noahmp_drv.meta index 066bc1e87..1fdee7a4a 100644 --- a/physics/sfc_noahmp_drv.meta +++ b/physics/sfc_noahmp_drv.meta @@ -325,14 +325,6 @@ type = logical intent = in optional = F -[lheatstrg] - standard_name = flag_for_canopy_heat_storage - long_name = flag for canopy heat storage parameterization - units = flag - dimensions = () - type = logical - intent = in - optional = F [idveg] standard_name = flag_for_dynamic_vegetation_option long_name = choice for dynamic vegetation option (see noahmp module for definition) diff --git a/physics/sfc_nst.f b/physics/sfc_nst.f index 3d0507ad9..05b4f817a 100644 --- a/physics/sfc_nst.f +++ b/physics/sfc_nst.f @@ -29,19 +29,16 @@ end subroutine sfc_nst_finalize !! \section NSST_general_algorithm GFS Near-Surface Sea Temperature Scheme General Algorithm !> @{ subroutine sfc_nst_run & -! --- inputs: - & ( im, hvap, cp, hfus, jcal, eps, epsm1, rvrdm1, rd, rhw0, & + & ( im, hvap, cp, hfus, jcal, eps, epsm1, rvrdm1, rd, rhw0, & ! --- inputs: & pi, sbc, ps, u1, v1, t1, q1, tref, cm, ch, & & prsl1, prslki, prsik1, prslk1, wet, xlon, sinlat, & & stress, & & sfcemis, dlwflx, sfcnsw, rain, timestep, kdt, solhr,xcosz, & & wind, flag_iter, flag_guess, nstf_name1, nstf_name4, & & nstf_name5, lprnt, ipr, & -! --- input/output: - & tskin, tsurf, xt, xs, xu, xv, xz, zm, xtts, xzts, dt_cool, & + & tskin, tsurf, xt, xs, xu, xv, xz, zm, xtts, xzts, dt_cool, & ! --- input/output: & z_c, c_0, c_d, w_0, w_d, d_conv, ifd, qrain, & -! --- outputs: - & qsurf, gflux, cmm, chh, evap, hflx, ep, errmsg, errflg & + & qsurf, gflux, cmm, chh, evap, hflx, ep, errmsg, errflg & ! --- outputs: & ) ! ! ===================================================================== ! @@ -675,7 +672,7 @@ end subroutine sfc_nst_pre_finalize !> \section NSST_general_pre_algorithm General Algorithm !! @{ subroutine sfc_nst_pre_run - & (im, wet, tsfc_ocn, tsurf_ocn, tseal, xt, xz, dt_cool, + & (im, wet, tsfc_wat, tsurf_wat, tseal, xt, xz, dt_cool, & z_c, tref, cplflx, oceanfrac, errmsg, errflg) use machine , only : kind_phys @@ -686,12 +683,12 @@ subroutine sfc_nst_pre_run integer, intent(in) :: im logical, dimension(im), intent(in) :: wet real (kind=kind_phys), dimension(im), intent(in) :: - & tsfc_ocn, xt, xz, dt_cool, z_c, oceanfrac + & tsfc_wat, xt, xz, dt_cool, z_c, oceanfrac logical, intent(in) :: cplflx ! --- input/outputs: real (kind=kind_phys), dimension(im), intent(inout) :: - & tsurf_ocn, tseal, tref + & tsurf_wat, tseal, tref ! --- outputs: character(len=*), intent(out) :: errmsg @@ -714,9 +711,9 @@ subroutine sfc_nst_pre_run ! tem = (oro(i)-oro_uf(i)) * rlapse ! DH* 20190927 simplyfing this code because tem is zero !tem = zero - !tseal(i) = tsfc_ocn(i) + tem - tseal(i) = tsfc_ocn(i) - !tsurf_ocn(i) = tsurf_ocn(i) + tem + !tseal(i) = tsfc_wat(i) + tem + tseal(i) = tsfc_wat(i) + !tsurf_wat(i) = tsurf_wat(i) + tem ! *DH endif enddo @@ -736,7 +733,7 @@ subroutine sfc_nst_pre_run endif tseal(i) = tref(i) + dt_warm - dt_cool(i) ! - (Sfcprop%oro(i)-Sfcprop%oro_uf(i))*rlapse - tsurf_ocn(i) = tseal(i) + tsurf_wat(i) = tseal(i) endif enddo endif @@ -779,7 +776,7 @@ end subroutine sfc_nst_post_finalize subroutine sfc_nst_post_run & & ( im, rlapse, tgice, wet, icy, oro, oro_uf, nstf_name1, & & nstf_name4, nstf_name5, xt, xz, dt_cool, z_c, tref, xlon, & - & tsurf_ocn, tsfc_ocn, dtzm, errmsg, errflg & + & tsurf_wat, tsfc_wat, dtzm, errmsg, errflg & & ) use machine , only : kind_phys @@ -797,8 +794,8 @@ subroutine sfc_nst_post_run & & dt_cool, z_c, tref, xlon ! --- input/outputs: - real (kind=kind_phys), dimension(im), intent(inout) :: tsurf_ocn, & - & tsfc_ocn + real (kind=kind_phys), dimension(im), intent(inout) :: tsurf_wat, & + & tsfc_wat ! --- outputs: real (kind=kind_phys), dimension(size(xlon,1)), intent(out) :: & @@ -821,7 +818,7 @@ subroutine sfc_nst_post_run & ! do i = 1, im ! if (wet(i) .and. .not. icy(i)) then -! tsurf_ocn(i) = tsurf_ocn(i) - (oro(i)-oro_uf(i)) * rlapse +! tsurf_wat(i) = tsurf_wat(i) - (oro(i)-oro_uf(i)) * rlapse ! endif ! enddo @@ -838,8 +835,8 @@ subroutine sfc_nst_post_run & ! if (wet(i) .and. .not.icy(i)) then ! if (wet(i) .and. (Model%frac_grid .or. .not. icy(i))) then if (wet(i)) then - tsfc_ocn(i) = max(tgice, tref(i) + dtzm(i)) -! tsfc_ocn(i) = max(271.2, tref(i) + dtzm(i)) - & + tsfc_wat(i) = max(tgice, tref(i) + dtzm(i)) +! tsfc_wat(i) = max(271.2, tref(i) + dtzm(i)) - & ! (oro(i)-oro_uf(i))*rlapse endif enddo diff --git a/physics/sfc_nst.meta b/physics/sfc_nst.meta index ac75aa05d..ff3566ac0 100644 --- a/physics/sfc_nst.meta +++ b/physics/sfc_nst.meta @@ -679,7 +679,7 @@ type = logical intent = in optional = F -[tsfc_ocn] +[tsfc_wat] standard_name = surface_skin_temperature_over_ocean_interstitial long_name = surface skin temperature over ocean (temporary use as interstitial) units = K @@ -688,7 +688,7 @@ kind = kind_phys intent = in optional = F -[tsurf_ocn] +[tsurf_wat] standard_name = surface_skin_temperature_after_iteration_over_ocean long_name = surface skin temperature after iteration over ocean units = K @@ -938,7 +938,7 @@ kind = kind_phys intent = in optional = F -[tsurf_ocn] +[tsurf_wat] standard_name = surface_skin_temperature_after_iteration_over_ocean long_name = surface skin temperature after iteration over ocean units = K @@ -947,7 +947,7 @@ kind = kind_phys intent = inout optional = F -[tsfc_ocn] +[tsfc_wat] standard_name = surface_skin_temperature_over_ocean_interstitial long_name = surface skin temperature over ocean (temporary use as interstitial) units = K diff --git a/physics/sfc_ocean.F b/physics/sfc_ocean.F index 9635f30b8..e21ddb3a7 100644 --- a/physics/sfc_ocean.F +++ b/physics/sfc_ocean.F @@ -1,3 +1,9 @@ +!>\file sfc_ocean.F +!! This file contains an alternative GFS near-surface sea temperature +!! scheme when the model is initialized from GRIB2 data. + +!> This module contains the CCPP-compliant GFS near-surface sea temperature +!! scheme when the model is initialized from GRIB2 data. module sfc_ocean implicit none private @@ -15,19 +21,17 @@ end subroutine sfc_ocean_init subroutine sfc_ocean_finalize() end subroutine sfc_ocean_finalize -#if 0 +!>\defgroup gfs_ocean_main GFS Simple Ocean Scheme Module +!! This subroutine calculates thermodynamical properties over +!! open water. !! \section arg_table_sfc_ocean_run Argument Table !! \htmlinclude sfc_ocean_run.html !! -#endif subroutine sfc_ocean_run & -!................................... -! --- inputs: - & ( im, cp, rd, eps, epsm1, hvap, rvrdm1, ps, t1, q1, & + & ( im, cp, rd, eps, epsm1, hvap, rvrdm1, ps, t1, q1, & ! --- inputs & tskin, cm, ch, prsl1, prslki, wet, wind, & & flag_iter, & -! --- outputs: - & qsurf, cmm, chh, gflux, evap, hflx, ep, & + & qsurf, cmm, chh, gflux, evap, hflx, ep, & ! --- outputs & errmsg, errflg & & ) diff --git a/physics/sfc_sice.f b/physics/sfc_sice.f index 750a6d795..6010fa4c9 100644 --- a/physics/sfc_sice.f +++ b/physics/sfc_sice.f @@ -40,12 +40,12 @@ end subroutine sfc_sice_finalize !> \section detailed_sice_run GFS Sea Ice Driver Detailed Algorithm !> @{ subroutine sfc_sice_run & - & ( im, km, sbc, hvap, tgice, cp, eps, epsm1, rvrdm1, grav, & ! --- inputs: + & ( im, kice, sbc, hvap, tgice, cp, eps, epsm1, rvrdm1, grav, & ! --- inputs: & t0c, rd, ps, t1, q1, delt, & & sfcemis, dlwflx, sfcnsw, sfcdsw, srflag, & & cm, ch, prsl1, prslki, prsik1, prslk1, islimsk, wind, & & flag_iter, lprnt, ipr, cimin, & - & hice, fice, tice, weasd, tskin, tprcp, stc, ep, & ! --- input/outputs: + & hice, fice, tice, weasd, tskin, tprcp, tiice, ep, & ! --- input/outputs: & snwdph, qsurf, snowmt, gflux, cmm, chh, evap, hflx, & ! & cplflx, cplchm, flag_cice, islmsk_cice, & & errmsg, errflg @@ -58,12 +58,12 @@ subroutine sfc_sice_run & ! ! ! call sfc_sice ! ! inputs: ! -! ( im, km, ps, t1, q1, delt, ! +! ( im, kice, ps, t1, q1, delt, ! ! sfcemis, dlwflx, sfcnsw, sfcdsw, srflag, ! ! cm, ch, prsl1, prslki, prsik1, prslk1, islimsk, wind, ! ! flag_iter, ! ! input/outputs: ! -! hice, fice, tice, weasd, tskin, tprcp, stc, ep, ! +! hice, fice, tice, weasd, tskin, tprcp, tiice, ep, ! ! outputs: ! ! snwdph, qsurf, snowmt, gflux, cmm, chh, evap, hflx ) ! ! ! @@ -90,7 +90,7 @@ subroutine sfc_sice_run & ! ==================== defination of variables ==================== ! ! ! ! inputs: size ! -! im, km - integer, horiz dimension and num of soil layers 1 ! +! im, kice - integer, horiz dimension and num of ice layers 1 ! ! ps - real, surface pressure im ! ! t1 - real, surface layer mean temperature ( k ) im ! ! q1 - real, surface layer mean specific humidity im ! @@ -117,7 +117,7 @@ subroutine sfc_sice_run & ! weasd - real, water equivalent accumulated snow depth (mm)im ! ! tskin - real, ground surface skin temperature ( k ) im ! ! tprcp - real, total precipitation im ! -! stc - real, soil temp (k) im,km ! +! tiice - real, temperature of ice internal (k) im,kice ! ! ep - real, potential evaporation im ! ! ! ! outputs: ! @@ -138,7 +138,6 @@ subroutine sfc_sice_run & implicit none ! ! - Define constant parameters - integer, parameter :: kmi = 2 !< 2-layer of ice real(kind=kind_phys), parameter :: zero = 0.0d0, one = 1.0d0 real(kind=kind_phys), parameter :: himax = 8.0d0 !< maximum ice thickness allowed real(kind=kind_phys), parameter :: himin = 0.1d0 !< minimum ice thickness required @@ -148,7 +147,7 @@ subroutine sfc_sice_run & real(kind=kind_phys), parameter :: dsi = one/0.33d0 ! --- inputs: - integer, intent(in) :: im, km, ipr + integer, intent(in) :: im, kice, ipr logical, intent(in) :: lprnt logical, intent(in) :: cplflx logical, intent(in) :: cplchm @@ -170,7 +169,7 @@ subroutine sfc_sice_run & real (kind=kind_phys), dimension(im), intent(inout) :: hice, & & fice, tice, weasd, tskin, tprcp, ep - real (kind=kind_phys), dimension(im,km), intent(inout) :: stc + real (kind=kind_phys), dimension(im,kice), intent(inout) :: tiice ! --- outputs: real (kind=kind_phys), dimension(im), intent(inout) :: snwdph, & @@ -186,7 +185,7 @@ subroutine sfc_sice_run & & focn, snof, rch, rho, & & snowd, theta1 - real (kind=kind_phys) :: t12, t14, tem, stsice(im,kmi) + real (kind=kind_phys) :: t12, t14, tem, stsice(im,kice) &, hflxi, hflxw, q0, qs1, qssi, qssw real (kind=kind_phys) :: cpinv, hvapi, elocp @@ -236,12 +235,12 @@ subroutine sfc_sice_run & endif endif enddo -!> - Update/read sea ice temperature from soil temperature and initialize variables. +! --- ... update sea ice temperature - do k = 1, kmi + do k = 1, kice do i = 1, im if (flag(i)) then - stsice(i,k) = stc(i,k) + stsice(i,k) = tiice(i,k) endif enddo enddo @@ -357,7 +356,7 @@ subroutine sfc_sice_run & !> - Call the three-layer thermodynamics sea ice model ice3lay(). call ice3lay ! --- inputs: ! - & ( im, kmi, fice, flag, hfi, hfd, sneti, focn, delt, ! + & ( im, kice, fice, flag, hfi, hfd, sneti, focn, delt, ! & lprnt, ipr, ! --- outputs: ! & snowd, hice, stsice, tice, snof, snowmt, gflux ) ! @@ -388,10 +387,10 @@ subroutine sfc_sice_run & endif enddo - do k = 1, kmi + do k = 1, kice do i = 1, im if (flag(i)) then - stc(i,k) = min(stsice(i,k), t0c) + tiice(i,k) = min(stsice(i,k), t0c) endif enddo enddo diff --git a/physics/sfc_sice.meta b/physics/sfc_sice.meta index c9641ffaa..dc08e0170 100644 --- a/physics/sfc_sice.meta +++ b/physics/sfc_sice.meta @@ -9,9 +9,9 @@ type = integer intent = in optional = F -[km] - standard_name = soil_vertical_dimension - long_name = vertical loop extent for soil levels, start at 1 +[kice] + standard_name = ice_vertical_dimension + long_name = vertical loop extent for ice levels, start at 1 units = count dimensions = () type = integer @@ -346,11 +346,11 @@ kind = kind_phys intent = inout optional = F -[stc] - standard_name = soil_temperature - long_name = soil temp +[tiice] + standard_name = internal_ice_temperature + long_name = sea ice internal temperature units = K - dimensions = (horizontal_dimension,soil_vertical_dimension) + dimensions = (horizontal_dimension,ice_vertical_dimension) type = real kind = kind_phys intent = inout diff --git a/physics/sflx.f b/physics/sflx.f index 6a5914d02..2740a70ff 100644 --- a/physics/sflx.f +++ b/physics/sflx.f @@ -172,7 +172,6 @@ subroutine gfssflx &! --- input ! consolidated constents/parameters by using ! ! module physcons, and added program documentation! ! sep 2009 -- s. moorthi minor fixes ! -! nov 2018 -- j. han add canopy heat storage parameterization ! ! ! ! ==================== defination of variables ==================== ! ! ! @@ -345,12 +344,6 @@ subroutine gfssflx &! --- input integer :: ice, k, kz ! -! --- parameters for heat storage parametrization -! - real (kind=kind_phys) :: cpx, cpx1, cpfac, xx1, xx2 - real (kind=kind_phys), parameter :: z0min=0.2_kind_phys, & - & z0max=1.0_kind_phys -! !===> ... begin here ! ! --- ... initialization @@ -681,7 +674,11 @@ subroutine gfssflx &! --- input !! overlying green canopy, adapted from section 2.1.2 of !! \cite peters-lidard_et_al_1997. !wz only urban for igbp type - if(ivegsrc == 1 .and. vegtyp == 13) then +! +!jhan urban canopy heat storage effect is included in pbl scheme +! + if((.not.lheatstrg) .and. & + & (ivegsrc == 1 .and. vegtyp == 13)) then df1 = 3.24*(1.-shdfac) + shdfac*df1*exp(sbeta*shdfac) else df1 = df1 * exp( sbeta*shdfac ) @@ -811,22 +808,6 @@ subroutine gfssflx &! --- input fdown = swnet + lwdn endif ! end if_couple_block -! -! --- enhance cp as a function of z0 to mimic heat storage -! - cpx = cp - cpx1 = cp1 - cpfac = 1.0 - if (lheatstrg) then - if ((ivegsrc == 1 .and. vegtyp /= 13) - & .or. ivegsrc == 2) then - xx1 = (z0 - z0min) / (z0max - z0min) - xx2 = 1.0 + min(max(xx1, 0.0), 1.0) - cpx = cp * xx2 - cpx1 = cp1 * xx2 - cpfac = cp / cpx - endif - endif !> - Call penman() to calculate potential evaporation (\a etp), !! and other partial products and sums for later @@ -835,7 +816,7 @@ subroutine gfssflx &! --- input call penman ! --- inputs: ! ! ( sfctmp, sfcprs, sfcems, ch, t2v, th2, prcp, fdown, ! -! cpx, cpfac, ssoil, q2, q2sat, dqsdt2, snowng, frzgra, ! +! ssoil, q2, q2sat, dqsdt2, snowng, frzgra, ! ! --- outputs: ! ! t24, etp, rch, epsca, rr, flx2 ) ! @@ -850,7 +831,7 @@ subroutine gfssflx &! --- input call canres ! --- inputs: ! ! ( nsoil, nroot, swdn, ch, q2, q2sat, dqsdt2, sfctmp, ! -! cpx1, sfcprs, sfcems, sh2o, smcwlt, smcref, zsoil, rsmin, ! +! sfcprs, sfcems, sh2o, smcwlt, smcref, zsoil, rsmin, ! ! rsmax, topt, rgl, hs, xlai, ! ! --- outputs: ! ! rc, pc, rcs, rct, rcq, rcsoil ) ! @@ -872,7 +853,7 @@ subroutine gfssflx &! --- input ! smcdry, cmcmax, dt, shdfac, sbeta, sfctmp, sfcems, ! ! t24, th2, fdown, epsca, bexp, pc, rch, rr, cfactr, ! ! slope, kdt, frzx, psisat, zsoil, dksat, dwsat, ! -! zbot, ice, rtdis, quartz, fxexp, csoil, ! +! zbot, ice, rtdis, quartz, fxexp, csoil, lheatstrg, ! ! --- input/outputs: ! ! cmc, t1, stc, sh2o, tbot, ! ! --- outputs: ! @@ -888,7 +869,7 @@ subroutine gfssflx &! --- input ! cmcmax, dt, df1, sfcems, sfctmp, t24, th2, fdown, epsca, ! ! bexp, pc, rch, rr, cfactr, slope, kdt, frzx, psisat, ! ! zsoil, dwsat, dksat, zbot, shdfac, ice, rtdis, quartz, ! -! fxexp, csoil, flx2, snowng, ! +! fxexp, csoil, flx2, snowng, lheatstrg, ! ! --- input/outputs: ! ! prcp1, cmc, t1, stc, sncovr, sneqv, sndens, snowh, ! ! sh2o, tbot, beta, ! @@ -1074,7 +1055,7 @@ end subroutine alcalc subroutine canres ! --- inputs: ! & ( nsoil, nroot, swdn, ch, q2, q2sat, dqsdt2, sfctmp, & -! & cpx1, sfcprs, sfcems, sh2o, smcwlt, smcref, zsoil, rsmin, & +! & sfcprs, sfcems, sh2o, smcwlt, smcref, zsoil, rsmin, & ! & rsmax, topt, rgl, hs, xlai, & ! --- outputs: ! & rc, pc, rcs, rct, rcq, rcsoil & @@ -1107,7 +1088,6 @@ subroutine canres ! q2sat - real, sat. air humidity at 1st level abv ground 1 ! ! dqsdt2 - real, slope of sat. humidity function wrt temp 1 ! ! sfctmp - real, sfc temperature at 1st level above ground 1 ! -! cpx1 - real, enhanced air heat capacity for heat storage 1 ! ! sfcprs - real, sfc pressure 1 ! ! sfcems - real, sfc emissivity for lw radiation 1 ! ! sh2o - real, volumetric soil moisture nsoil ! @@ -1213,8 +1193,8 @@ subroutine canres ! evaporation (containing rc term). rc = rsmin / (xlai*rcs*rct*rcq*rcsoil) - rr = (4.0*sfcems*sigma1*rd1/cpx1) * (sfctmp**4.0)/(sfcprs*ch) + 1.0 - delta = (lsubc/cpx1) * dqsdt2 + rr = (4.0*sfcems*sigma1*rd1/cp1) * (sfctmp**4.0)/(sfcprs*ch) + 1.0 + delta = (lsubc/cp1) * dqsdt2 pc = (rr + delta) / (rr*(1.0 + rc*ch) + delta) ! @@ -1299,7 +1279,7 @@ subroutine nopac ! & smcdry, cmcmax, dt, shdfac, sbeta, sfctmp, sfcems, & ! & t24, th2, fdown, epsca, bexp, pc, rch, rr, cfactr, & ! & slope, kdt, frzx, psisat, zsoil, dksat, dwsat, & -! & zbot, ice, rtdis, quartz, fxexp, csoil, & +! & zbot, ice, rtdis, quartz, fxexp, csoil, lheatstrg, & ! --- input/outputs: ! & cmc, t1, stc, sh2o, tbot, & ! --- outputs: @@ -1356,6 +1336,8 @@ subroutine nopac ! quartz - real, soil quartz content 1 ! ! fxexp - real, bare soil evaporation exponent 1 ! ! csoil - real, soil heat capacity 1 ! +! lheatstrg- logical, flag for canopy heat storage 1 ! +! parameterization ! ! ! ! input/outputs from and to the calling program: ! ! cmc - real, canopy moisture content 1 ! @@ -1393,6 +1375,8 @@ subroutine nopac ! & zsoil(nsoil), dksat, dwsat, zbot, rtdis(nsoil), & ! & quartz, fxexp, csoil +! logical, intent(in) :: lheatstrg + ! --- input/outputs: ! real (kind=kind_phys), intent(inout) :: cmc, t1, stc(nsoil), & ! & sh2o(nsoil), tbot @@ -1522,7 +1506,11 @@ subroutine nopac ! sub sfc heat flux (see additional comments on veg effect ! sub-sfc heat flx in routine sflx) !wz only urban for igbp type - if(ivegsrc == 1 .and. vegtyp == 13) then +! +!jhan urban canopy heat storage effect is included in pbl scheme +! + if((.not.lheatstrg) .and. & + & (ivegsrc == 1 .and. vegtyp == 13)) then df1 = 3.24*(1.-shdfac) + shdfac*df1*exp(sbeta*shdfac) else df1 = df1 * exp( sbeta*shdfac ) @@ -1539,6 +1527,7 @@ subroutine nopac ! --- inputs: & ( nsoil, smc, smcmax, dt, yy, zz1, zsoil, zbot, & & psisat, bexp, df1, ice, quartz, csoil, vegtyp, & + & shdfac, lheatstrg, & ! --- input/outputs: & stc, t1, tbot, sh2o, & ! --- outputs: @@ -1567,7 +1556,7 @@ subroutine penman !................................... ! --- inputs: ! & ( sfctmp, sfcprs, sfcems, ch, t2v, th2, prcp, fdown, & -! & cpx, cpfac, ssoil, q2, q2sat, dqsdt2, snowng, frzgra, & +! & ssoil, q2, q2sat, dqsdt2, snowng, frzgra, & ! --- outputs: ! & t24, etp, rch, epsca, rr, flx2 & ! & ) @@ -1593,8 +1582,6 @@ subroutine penman ! th2 - real, air potential temp at zlvl abv grnd 1 ! ! prcp - real, precip rate 1 ! ! fdown - real, net solar + downward lw flux at sfc 1 ! -! cpx - real, enhanced air heat capacity for heat storage 1 ! -! cpfac - real, ratio air heat capacity to enhanced one 1 ! ! ssoil - real, upward soil heat flux 1 ! ! q2 - real, mixing ratio at hght zlvl abv ground 1 ! ! q2sat - real, sat mixing ratio at zlvl abv ground 1 ! @@ -1632,11 +1619,11 @@ subroutine penman ! --- ... prepare partial quantities for penman equation. - delta = elcp * cpfac * dqsdt2 + delta = elcp * dqsdt2 t24 = sfctmp * sfctmp * sfctmp * sfctmp rr = t24 * 6.48e-8 / (sfcprs*ch) + 1.0 rho = sfcprs / (rd1*t2v) - rch = rho * cpx * ch + rch = rho * cp * ch ! --- ... adjust the partial sums / products with the latent heat ! effects caused by falling precipitation. @@ -1662,7 +1649,7 @@ subroutine penman ! --- ... finish penman equation calculations. rad = fnet/rch + th2 - sfctmp - a = elcp * cpfac * (q2sat - q2) + a = elcp * (q2sat - q2) epsca = (a*rr + rad*delta) / (delta + rr) etp = epsca * rch / lsubc ! @@ -2336,7 +2323,7 @@ subroutine snopac ! & cmcmax, dt, df1, sfcems, sfctmp, t24, th2, fdown, epsca, & ! & bexp, pc, rch, rr, cfactr, slope, kdt, frzx, psisat, & ! & zsoil, dwsat, dksat, zbot, shdfac, ice, rtdis, quartz, & -! & fxexp, csoil, flx2, snowng, & +! & fxexp, csoil, flx2, snowng, lheatstrg, & ! --- input/outputs: ! & prcp1, cmc, t1, stc, sncovr, sneqv, sndens, snowh, & ! & sh2o, tbot, beta, & @@ -2396,6 +2383,8 @@ subroutine snopac ! csoil - real, soil heat capacity 1 ! ! flx2 - real, freezing rain latent heat flux 1 ! ! snowng - logical, snow flag 1 ! +! lheatstrg- logical, flag for canopy heat storage 1 ! +! parameterization ! ! ! ! input/outputs from and to the calling program: ! ! prcp1 - real, effective precip 1 ! @@ -2442,6 +2431,9 @@ subroutine snopac ! & csoil, fxexp, flx2, zsoil(nsoil), rtdis(nsoil) ! logical, intent(in) :: snowng +! +! logical, intent(in) :: lheatstrg +! ! --- input/outputs: ! real (kind=kind_phys), intent(inout) :: prcp1, t1, sncovr, sneqv, & @@ -2758,6 +2750,7 @@ subroutine snopac ! --- inputs: & ( nsoil, smc, smcmax, dt, yy, zz1, zsoil, zbot, & & psisat, bexp, df1, ice, quartz, csoil, vegtyp, & + & shdfac, lheatstrg, & ! --- input/outputs: & stc, t11, tbot, sh2o, & ! --- outputs: @@ -3278,6 +3271,7 @@ subroutine shflx & ! --- inputs: & ( nsoil, smc, smcmax, dt, yy, zz1, zsoil, zbot, & & psisat, bexp, df1, ice, quartz, csoil, vegtyp, & + & shdfac, lheatstrg, & ! --- input/outputs: & stc, t1, tbot, sh2o, & ! --- outputs: @@ -3312,6 +3306,9 @@ subroutine shflx & ! quartz - real, soil quartz content 1 ! ! csoil - real, soil heat capacity 1 ! ! vegtyp - integer, vegtation type 1 ! +! shdfac - real, aeral coverage of green vegetation 1 ! +! lheatstrg- logical, flag for canopy heat storage 1 ! +! parameterization ! ! ! ! input/outputs: ! ! stc - real, soil temp nsoil ! @@ -3332,7 +3329,10 @@ subroutine shflx & integer, intent(in) :: nsoil, ice, vegtyp real (kind=kind_phys), intent(in) :: smc(nsoil), smcmax, dt, yy, & - & zz1, zsoil(nsoil), zbot, psisat, bexp, df1, quartz, csoil + & zz1, zsoil(nsoil), zbot, psisat, bexp, df1, quartz, csoil, & + & shdfac + + logical, intent(in) :: lheatstrg ! --- input/outputs: real (kind=kind_phys), intent(inout) :: stc(nsoil), t1, tbot, & @@ -3387,7 +3387,7 @@ subroutine shflx & ! --- inputs: & ( nsoil, stc, smc, smcmax, zsoil, yy, zz1, tbot, & & zbot, psisat, dt, bexp, df1, quartz, csoil,vegtyp, & - & shdfac, & + & shdfac, lheatstrg, & ! --- input/outputs: & sh2o, & ! --- outputs: @@ -4054,7 +4054,7 @@ subroutine hrt & ! --- inputs: & ( nsoil, stc, smc, smcmax, zsoil, yy, zz1, tbot, & & zbot, psisat, dt, bexp, df1, quartz, csoil, vegtyp, & - & shdfac, & + & shdfac, lheatstrg, & ! --- input/outputs: & sh2o, & ! --- outputs: @@ -4091,6 +4091,9 @@ subroutine hrt & ! quartz - real, soil quartz content 1 ! ! csoil - real, soil heat capacity 1 ! ! vegtyp - integer, vegetation type 1 ! +! shdfac - real, aeral coverage of green vegetation 1 ! +! lheatstrg- logical, flag for canopy heat storage 1 ! +! parameterization ! ! ! ! input/outputs: ! ! sh2o - real, unfrozen soil moisture nsoil ! @@ -4110,6 +4113,8 @@ subroutine hrt & & smcmax, zsoil(nsoil), yy, zz1, tbot, zbot, psisat, dt, & & bexp, df1, quartz, csoil, shdfac + logical, intent(in) :: lheatstrg + ! --- input/outputs: real (kind=kind_phys), intent(inout) :: sh2o(nsoil) @@ -4131,8 +4136,11 @@ subroutine hrt & ! csoil_loc=csoil - if (ivegsrc == 1)then + if (.not.lheatstrg .and. ivegsrc == 1)then !urban +! +!jhan urban canopy heat storage effect is included in pbl scheme +! if( vegtyp == 13 ) then ! csoil_loc=3.0e6 csoil_loc=3.0e6*(1.-shdfac)+csoil*shdfac ! gvf @@ -4225,7 +4233,7 @@ subroutine hrt & call snksrc & ! --- inputs: & ( nsoil, 1, tavg, smc(1), smcmax, psisat, bexp, dt, & - & qtot, zsoil, shdfac, & + & qtot, zsoil, & ! --- input/outputs: & sh2o(1), & ! --- outputs: @@ -4271,7 +4279,11 @@ subroutine hrt & ! if ( vegtyp == 13 ) df1n = 3.24 ! endif !wz only urban for igbp type - if(ivegsrc == 1 .and. vegtyp == 13) then +! +!jhan urban canopy heat storage effect is included in pbl scheme +! + if((.not.lheatstrg) .and. + & (ivegsrc == 1 .and. vegtyp == 13)) then df1n = 3.24*(1.-shdfac) + shdfac*df1n endif @@ -4315,7 +4327,11 @@ subroutine hrt & ! if ( vegtyp == 13 ) df1n = 3.24 ! endif !wz only urban for igbp type - if(ivegsrc == 1 .and. vegtyp == 13) then +! +!jhan urban canopy heat storage effect is included in pbl scheme +! + if((.not.lheatstrg) .and. + & (ivegsrc == 1 .and. vegtyp == 13)) then df1n = 3.24*(1.-shdfac) + shdfac*df1n endif @@ -4371,7 +4387,7 @@ subroutine hrt & call snksrc & ! --- inputs: & ( nsoil, k, tavg, smc(k), smcmax, psisat, bexp, dt, & - & qtot, zsoil, shdfac, & + & qtot, zsoil, & ! --- input/outputs: & sh2o(k), & ! --- outputs: @@ -4786,7 +4802,7 @@ end subroutine rosr12 subroutine snksrc & ! --- inputs: & ( nsoil, k, tavg, smc, smcmax, psisat, bexp, dt, & - & qtot, zsoil, shdfac, & + & qtot, zsoil, & ! --- input/outputs: & sh2o, & ! --- outputs: @@ -4831,7 +4847,7 @@ subroutine snksrc & integer, intent(in) :: nsoil, k real (kind=kind_phys), intent(in) :: tavg, smc, smcmax, psisat, & - & bexp, dt, qtot, zsoil(nsoil), shdfac + & bexp, dt, qtot, zsoil(nsoil) ! --- input/outputs: real (kind=kind_phys), intent(inout) :: sh2o @@ -4844,15 +4860,6 @@ subroutine snksrc & ! --- external functions: ! real (kind=kind_phys) :: frh2o - -!urban -! if (ivegsrc == 1)then -! if ( vegtyp == 13 ) df1=3.24 -! endif -!wz only urban for igbp type - if(ivegsrc == 1 .and. vegtyp == 13) then - df1 = 3.24*(1.-shdfac) + shdfac*df1 - endif ! !===> ... begin here ! diff --git a/physics/shalcnv.meta b/physics/shalcnv.meta index 533b9cd0e..e0d806a5c 100644 --- a/physics/shalcnv.meta +++ b/physics/shalcnv.meta @@ -358,7 +358,7 @@ intent = in optional = F [heat] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -367,7 +367,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/shinhongvdif.meta b/physics/shinhongvdif.meta index e859fca4d..4ce047aa2 100644 --- a/physics/shinhongvdif.meta +++ b/physics/shinhongvdif.meta @@ -237,7 +237,7 @@ intent = in optional = F [heat] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -246,7 +246,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/physics/ugwp_driver_v0.F b/physics/ugwp_driver_v0.F index 4edd84a7a..af19447dc 100644 --- a/physics/ugwp_driver_v0.F +++ b/physics/ugwp_driver_v0.F @@ -8,6 +8,7 @@ module sso_coorde use machine, only: kind_phys real(kind=kind_phys),parameter :: pgwd = 1._kind_phys real(kind=kind_phys),parameter :: pgwd4 = 1._kind_phys + logical,parameter :: debugprint = .false. end module sso_coorde ! ! @@ -33,7 +34,7 @@ subroutine cires_ugwp_driver_v0(me, master, use physcons, only : con_cp, con_g, con_rd, con_rv use ugwp_wmsdis_init, only : tamp_mpa, ilaunch - use sso_coorde, only : pgwd, pgwd4 + use sso_coorde, only : pgwd, pgwd4, debugprint implicit none !input @@ -91,7 +92,7 @@ subroutine cires_ugwp_driver_v0(me, master, ! ! switches for GW-effects: pogw=1 (OGWs) pngw=1 (NGWs) pked=1 (eddy mixing) ! - if (me == master .and. kdt < 2) then + if (me == master .and. kdt < 2 .and. debugprint) then print * write(6,*) 'FV3GFS execute ugwp_driver_v0 ' ! write(6,*) 'FV3GFS execute ugwp_driver_v0 nmtvr=', nmtvr @@ -120,7 +121,7 @@ subroutine cires_ugwp_driver_v0(me, master, & zmtb, zogw, tau_mtb, tau_ogw, tau_tofd, & du3dt_mtb, du3dt_ogw, du3dt_tms) ! - if (me == master .and. kdt < 2) then + if (me == master .and. kdt < 2 .and. debugprint) then print * write(6,*) 'FV3GFS finished gwdps_v0 in ugwp_driver_v0 ' print * @@ -192,7 +193,7 @@ subroutine cires_ugwp_driver_v0(me, master, & gw_dudt, gw_dvdt, gw_dTdt, gw_kdis, & tau_ngw, me, master, kdt) - if (me == master .and. kdt < 2) then + if (me == master .and. kdt < 2 .and. debugprint) then print * write(6,*)'FV3GFS finished fv3_ugwp_v0 in ugwp_driver_v0 ' write(6,*) ' non-stationary GWs with GMAO/MERRA GW-forcing ' @@ -263,7 +264,20 @@ end subroutine cires_ugwp_driver_v0 !===================================================================== !>\ingroup cires_ugwp_run !> @{ -!!Note for the sub-grid scale orography scheme in UGWP-v0: Due to degraded forecast scores of simulations with revised schemes for subgrid-scale orography effects in FV3GFS, EMC reinstalled the original gwdps-code with updated efficiency factors for the mountain blocking and OGW drag. The GFS OGW is described in the separate section (\ref GFS_GWDPS) and its “call” moved into UGWP-driver subroutine. This combination of NGW and OGW schemes was tested in the FV3GFS-L127 medium-range forecasts (15-30 days) for C96, C192, C384 and C768 resolutions and work in progress to introduce the optimal choice for the scale-aware representations of the efficiency factors that will reflect the better simulations of GW activity by FV3 dynamical core at higher horizontal resolutions. With the MERRA-2 VMF function for NGWs (\ref slat_geos5_tamp) and operational OGW drag scheme (\ref GFS_GWDPS), FV3GFS simulations can successfully forecast the recent major mid-winter sudden stratospheric warming (SSW) events of 2018-02-12 and 2018-12-31 (10-14 days before the SSW onset; Yudin et al. 2019 \cite yudin_et_al_2019). The first multi-year (2015-2018) FV3GFS simulations with UGWP-v0 also produce the equatorial QBO-like oscillations in the zonal wind and temperature anomalies. +!! Note for the sub-grid scale orography scheme in UGWP-v0: Due to degraded forecast +!! scores of simulations with revised schemes for subgrid-scale orography effects in FV3GFS, +!! EMC reinstalled the original gwdps-code with updated efficiency factors for the mountain +!! blocking and OGW drag. The GFS OGW is described in the separate section (\ref GFS_GWDPS) +!! and its "call" moved into UGWP-driver subroutine. This combination of NGW and OGW schemes +!! was tested in the FV3GFS-L127 medium-range forecasts (15-30 days) for C96, C192, C384 and +!! C768 resolutions and work in progress to introduce the optimal choice for the scale-aware +!! representations of the efficiency factors that will reflect the better simulations of GW +!! activity by FV3 dynamical core at higher horizontal resolutions. With the MERRA-2 VMF +!! function for NGWs (\ref slat_geos5_tamp) and operational OGW drag scheme (\ref GFS_GWDPS), +!! FV3GFS simulations can successfully forecast the recent major mid-winter sudden stratospheric +!! warming (SSW) events of 2018-02-12 and 2018-12-31 (10-14 days before the SSW onset; +!! Yudin et al. 2019 \cite yudin_et_al_2019). The first multi-year (2015-2018) FV3GFS simulations +!! with UGWP-v0 also produce the equatorial QBO-like oscillations in the zonal wind and temperature anomalies. !! SUBROUTINE GWDPS_V0(IM, km, imx, do_tofd, & Pdvdt, Pdudt, Pdtdt, Pkdis, U1,V1,T1,Q1,KPBL, @@ -297,7 +311,7 @@ SUBROUTINE GWDPS_V0(IM, km, imx, do_tofd, &, n_tofd, ze_tofd, ztop_tofd use cires_ugwp_module, only : kxw, max_kdis, max_axyz - use sso_coorde, only : pgwd, pgwd4 + use sso_coorde, only : pgwd, pgwd4, debugprint !---------------------------------------- implicit none character(len=8) :: strsolver='PSS-1986' ! current operational solver or 'WAM-2017' @@ -439,7 +453,7 @@ SUBROUTINE GWDPS_V0(IM, km, imx, do_tofd, kxridge = float(IMX)/arad * cdmbgwd(2) - if (me == master .and. kdt == 1) then + if (me == master .and. kdt == 1 .and. debugprint) then print *, ' gwdps_v0 kxridge ', kxridge print *, ' gwdps_v0 scale2 ', cdmbgwd(2) print *, ' gwdps_v0 IMX ', imx @@ -521,7 +535,7 @@ SUBROUTINE GWDPS_V0(IM, km, imx, do_tofd, endif enddo - IF (npt == 0) then + IF (npt == 0 .and. debugprint) then ! print *, 'oro-npt = 0 elvmax ', maxval(elvmaxd), hminmt ! print *, 'oro-npt = 0 hprime ', maxval(hprime), hpmin RETURN ! No gwd/mb calculation done @@ -1060,7 +1074,7 @@ SUBROUTINE GWDPS_V0(IM, km, imx, do_tofd, ! --------------------------- IF( do_tofd ) then axtms(:,:) = 0.0 ; aytms(:,:) = 0.0 - if ( kdt == 1 .and. me == 0) then + if ( kdt == 1 .and. me == 0 .and. debugprint) then print *, 'VAY do_tofd from surface to ', ztop_tofd endif DO I = 1,npt @@ -1164,7 +1178,7 @@ SUBROUTINE GWDPS_V0(IM, km, imx, do_tofd, !============ debug ------------------------------------------------ - if (kdt <= 2 .and. me == 0) then + if (kdt <= 2 .and. me == 0 .and. debugprint) then print *, 'vgw-oro done gwdps_v0 in ugwp-v0 step-proc ', kdt, me ! print *, maxval(pdudt)*86400., minval(pdudt)*86400, 'vgw_axoro' @@ -1286,6 +1300,8 @@ subroutine fv3_ugwp_solv2_v0(klon, klev, dtime, &, zci, zdci, zci4, zci3, zci2 &, zaz_fct, zcosang, zsinang &, nwav, nazd, zcimin, zcimax + + use sso_coorde, only : debugprint ! implicit none !23456 @@ -1411,7 +1427,7 @@ subroutine fv3_ugwp_solv2_v0(klon, klev, dtime, ! rcpd = 1.0/(grav/cpd) ! 1/[g/cp] ! grav2cpd = grav*grav/cpd ! g*(g/cp)= g^2/cp - if (kdt ==1 .and. mpi_id == master) then + if (kdt ==1 .and. mpi_id == master .and. debugprint) then print *, maxval(tm1), minval(tm1), 'vgw: temp-res ' print *, 'ugwp-v0: zcimin=' , zcimin print *, 'ugwp-v0: zcimax=' , zcimax @@ -1839,7 +1855,7 @@ subroutine fv3_ugwp_solv2_v0(klon, klev, dtime, ! !--------------------------------------------------------------------------- ! - if (kdt == 1 .and. mpi_id == master) then + if (kdt == 1 .and. mpi_id == master .and. debugprint) then print *, 'vgw done ' ! print *, maxval(pdudt)*86400., minval(pdudt)*86400, 'vgw ax' @@ -1972,7 +1988,7 @@ subroutine edmix_ugwp_v0(im, levs, dtp, ! adjust PT-profile to bn2(k) = bnv2min -- neutral atmosphere ! adapt "pdtdt = (Ptadj-Ptdyn)/Ptmap" ! - print *,' UGWP-V0 unstab PT(z) via gwdTdt ', bn2(k), k +! print *,' UGWP-V0 unstab PT(z) via gwdTdt ', bn2(k), k rineg = bn2(k)/shr2(k) bn2(k) = max(bn2(k), bnv2min) diff --git a/physics/ysuvdif.meta b/physics/ysuvdif.meta index 12819dee5..fe18e6f45 100644 --- a/physics/ysuvdif.meta +++ b/physics/ysuvdif.meta @@ -264,7 +264,7 @@ intent = in optional = F [heat] - standard_name = kinematic_surface_upward_sensible_heat_flux + standard_name = kinematic_surface_upward_sensible_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward sensible heat flux units = K m s-1 dimensions = (horizontal_dimension) @@ -273,7 +273,7 @@ intent = in optional = F [evap] - standard_name = kinematic_surface_upward_latent_heat_flux + standard_name = kinematic_surface_upward_latent_heat_flux_reduced_by_surface_roughness long_name = kinematic surface upward latent heat flux units = kg kg-1 m s-1 dimensions = (horizontal_dimension) diff --git a/tools/check_encoding.py b/tools/check_encoding.py new file mode 100755 index 000000000..1d24d4679 --- /dev/null +++ b/tools/check_encoding.py @@ -0,0 +1,25 @@ +#!/usr/bin/env python + +#import chardet +import os +import sys + + +SUFFICES = [ '.f', '.F', '.f90', '.F90', '.meta' ] + +for root, dirs, files in os.walk(os.getcwd()): + #print root, dirs, files + for file in files: + suffix = os.path.splitext(file)[1] + #print file, suffix + if suffix in SUFFICES: + with open(os.path.join(root, file)) as f: + contents = f.read() + try: + contents.decode('ascii') + except UnicodeDecodeError: + for line in contents.split('\n'): + try: + line.decode('ascii') + except UnicodeDecodeError: + raise Exception('Detected non-ascii characters in file {}, line: "{}"'.format(os.path.join(root, file), line))