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add the magnetosheath #5
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nicolasaunai
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LaboratoryOfPlasmaPhysics:main
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nicolasaunai:toto
Nov 3, 2020
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Original file line number | Diff line number | Diff line change |
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@@ -5,15 +5,14 @@ | |
sys.path.append('.') | ||
from .. import utils | ||
from ..coordinates import coordinates as coords | ||
from ..smath import resolve_poly2 | ||
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def checking_angles(theta, phi): | ||
theta = utils.listify(theta) | ||
phi = utils.listify(phi) | ||
if (len(np.shape(theta)) == 1) & (len(np.shape(phi)) == 1) & (len(theta) > 1) & (len(phi) > 1): | ||
theta, phi = np.meshgrid(theta, phi) | ||
print('theta and phi are both 1D array : applying meshgrid to do a 3D boundaries') | ||
def _checking_angles(theta, phi): | ||
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if isinstance(theta, np.ndarray) and isinstance(theta, np.ndarray) and len(theta.shape) > 1 and len(phi.shape) > 1: | ||
return np.meshgrid(theta, phi) | ||
return theta, phi | ||
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@@ -33,15 +32,14 @@ def _formisano1979(theta, phi, **kwargs): | |
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def formisano1979(theta, phi, **kwargs): | ||
''' | ||
Formisano 2005 magnetopause model. Give the default position of the magnetopause. | ||
Formisano 1979 magnetopause model. Give the default position of the magnetopause. | ||
function's arguments : | ||
- theta : angle in radiant, can be int, float or array (1D or 2D) | ||
- phi : angle in radiant, can be int, float or array (1D or 2D) | ||
kwargs: | ||
- boundary : "magnetopause", "bow_shock" | ||
- base : can be "cartesian" (default) or "spherical" | ||
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information : to get a particular point theta and phi must be an int or a float | ||
(ex : the nose of the boundary is given with the input theta=0 and phi=0). If a plan (2D) of | ||
the boundary is wanted one of the two angle must be an array and the other one must be | ||
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@@ -59,17 +57,25 @@ def formisano1979(theta, phi, **kwargs): | |
else: | ||
raise ValueError("boundary: {} not allowed".format(kwargs["boundary"])) | ||
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theta, phi = checking_angles(theta, phi) | ||
theta, phi = _checking_angles(theta, phi) | ||
r = _formisano1979(theta, phi, coefs = coefs) | ||
base = kwargs.get("base", "cartesian") | ||
if base == "cartesian": | ||
return coords.spherical_to_cartesian(R, theta, phi) | ||
return coords.spherical_to_cartesian(r, theta, phi) | ||
elif base == "spherical": | ||
return r, theta, phi | ||
raise ValueError("unknown base '{}'".format(kwargs["base"])) | ||
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def mp_formisano1979(theta, phi, **kwargs): | ||
return formisano1979(theta, phi, boundary="magnetopause", **kwargs) | ||
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def bs_formisano1979(theta, phi, **kwargs): | ||
return formisano1979(theta, phi, boundary="bow_shock", **kwargs) | ||
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def Fairfield1971(x, args): | ||
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@@ -105,56 +111,11 @@ def Fairfield1971(x, args): | |
return pos.dropna() | ||
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def Formisano1979(x, args): | ||
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''' | ||
Formisano 1979 : Magnetopause and Bow shock models. Give positions of the boudaries in plans (XY) with Z=0 and (XZ) with Y=0. | ||
function's arguments : | ||
- x : X axis (array) in Re (earth radii) | ||
- args : coefficients Aij are determined from many boundary crossings and they depend on upstream conditions. | ||
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--> Default parameter for the bow shock and the magnetopause respectively are : | ||
default_bs_formisano = [0.52,1,1.05,0.13,-0.16,-0.08,47.53,-0.42,0.67,-613] | ||
default_mp_formisano = [0.65,1,1.16,0.03,-0.28,-0.11,21.41,0.46,-0.36,-221] | ||
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return : DataFrame (Pandas) with the position (X,Y,Z) in Re of the wanted boudary to plot (XY) and (XZ) plans. | ||
''' | ||
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a11,a22,a33,a12,a13,a23,a14,a24,a34,a44 = args[0],args[1],args[2],args[3],args[4],args[5],args[6],args[7],args[8],args[9] | ||
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a_y = a22 | ||
b_y = a12*x + a24 | ||
c_y = a11*x**2 + a14*x + a44 | ||
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delta_y =(b_y**2-4*a_y*c_y) | ||
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ym = (-b_y - np.sqrt(delta_y))/(2*a_y) | ||
yp = (-b_y + np.sqrt(delta_y))/(2*a_y) | ||
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a_z = a33 | ||
b_z = a13*x + a34 | ||
c_z = a11*x**2 + a14*x + a44 | ||
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delta_z =(b_z**2-4*a_z*c_z) | ||
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zm = (-b_z - np.sqrt(delta_z))/(2*a_z) | ||
zp = (-b_z + np.sqrt(delta_z))/(2*a_z) | ||
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pos=pd.DataFrame({'X' : np.concatenate([x, x[::-1]]), | ||
'Y' : np.concatenate([yp, ym[::-1]]), | ||
'Z' : np.concatenate([zp, zm[::-1]]),}) | ||
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return pos.dropna() | ||
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def BS_Jerab2005( Np, V, Ma, B, gamma=2.15 ): | ||
def bs_Jerab2005( Np, V, Ma, B, gamma=2.15 ): | ||
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''' | ||
Jerab 2005 Bow shock model. Give positions of the box shock in plans (XY) with Z=0 and (XZ) with Y=0 as a function of the upstream solar wind. | ||
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@@ -215,7 +176,7 @@ def make_Rav(theta,phi): | |
return pos.sort_values('Y') | ||
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def shue1998(theta, phi, **kwargs): | ||
def mp_shue1998(theta, phi, **kwargs): | ||
''' | ||
Shue 1998 Magnetopause model. | ||
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@@ -351,3 +312,60 @@ def quad(i, s): | |
return r+Q | ||
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_models = {"mp_shue": mp_shue1998, | ||
"mp_formisano1979": mp_formisano1979, | ||
"bs_formisano1979": bs_formisano1979, | ||
"bs_jerab": bs_Jerab2005} | ||
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class Magnetosheath: | ||
def __init__(self, **kwargs): | ||
self.magnetopause = _models[kwargs.get("magnetopause", "shue")] | ||
self.bow_shock = _models[kwargs.get("bow_shock", "jerab")] | ||
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def boundaries(self, theta, phi, **kwargs): | ||
return self.magnetopause(theta, phi, **kwargs), self.bow_shock(theta, phi, **kwargs) | ||
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def _interest_points(model, **kwargs): | ||
dup = kwargs.copy() | ||
dup["base"] = "cartesian" | ||
x = model(0, 0, **dup)[0] | ||
y = model(np.pi / 2, 0, **dup)[1] | ||
xf = x - y ** 2 / (4 * x) | ||
return x, y, xf | ||
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def _parabolic_approx(theta, phi, x, xf, **kwargs): | ||
theta, phi = _checking_angles(theta, phi) | ||
K = x - xf | ||
a = np.sin(theta) ** 2 | ||
b = 4 * K * np.cos(theta) | ||
c = -4 * K * x | ||
r = resolve_poly2(a, b, c)[0] | ||
return coords.BaseChoice(kwargs.get("base", "cartesian"), r, theta, phi) | ||
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class ParabolicMagnetosheath: | ||
def __init__(self, **kwargs): | ||
self._magnetopause = _models[kwargs.get("magnetopause", "shue")] | ||
self._bow_shock = _models[kwargs.get("bow_shock", "jerab")] | ||
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def magnetopause(self, theta, phi, **kwargs): | ||
return self._parabolize(theta, phi, **kwargs)[0] | ||
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. zdazcazca |
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def bow_shock(self, theta, phi, **kwargs): | ||
return self._parabolize(theta, phi, **kwargs)[1] | ||
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def _parabolize(self, theta, phi, **kwargs): | ||
xmp, y, xfmp = _interest_points(self._magnetopause, **kwargs) | ||
xbs, y, xfbs = _interest_points(self._bow_shock, **kwargs) | ||
if kwargs.get("confocal", False) is True: | ||
xfmp = xmp / 2 | ||
xfbs = xmp / 2 | ||
mp_coords = _parabolic_approx(theta, phi, xmp, xfmp, **kwargs) | ||
bs_coords = _parabolic_approx(theta, phi, xbs, xfbs, **kwargs) | ||
return mp_coords, bs_coords | ||
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def boundaries(self, theta, phi, **kwargs): | ||
return self._parabolize(theta, phi, **kwargs) |
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Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,59 @@ | ||
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import matplotlib.pyplot as plt | ||
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def layout_EarthEnv_3planes(**kwargs): | ||
#figsize=(15,4.5),xlim=(-30,30),ylim=(-30,30),zlim =(-30,30),alpha=0.5): | ||
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figsize = kwargs.get("kwargs", (15, 4.5)) | ||
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fig, (ax0, ax1, ax2) = plt.subplots(ncols=3,figsize=figsize,constrained_layout=True) | ||
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ax0.set_xlabel('X (Re)') | ||
ax0.set_ylabel('Y (Re)') | ||
ax1.set_xlabel('X (Re)') | ||
ax1.set_ylabel('Z (Re)') | ||
ax2.set_xlabel('Y (Re)') | ||
ax2.set_ylabel('Z (Re)') | ||
ax0.axhline(0, color='k', ls='dotted', alpha=alpha) | ||
ax0.axvline(0, color='k', ls='dotted', alpha=alpha) | ||
ax1.axhline(0, color='k', ls='dotted', alpha=alpha) | ||
ax1.axvline(0, color='k', ls='dotted', alpha=alpha) | ||
ax2.axhline(0, color='k', ls='dotted', alpha=alpha) | ||
ax2.axvline(0, color='k', ls='dotted', alpha=alpha) | ||
ax0.set_xlim(xlim) | ||
ax0.set_ylim(ylim) | ||
ax1.set_xlim(xlim) | ||
ax1.set_ylim(zlim) | ||
ax2.set_xlim(ylim) | ||
ax2.set_ylim(zlim) | ||
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return ax0,ax1,ax2 | ||
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# plot_boundaries(MP, BS, slice_x=22, slice_y=24, slice_z=0) | ||
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def make_YZ_plan(pos): | ||
a = np.linspace(0,2*np.pi,100) | ||
r=abs(pos[(pos.X**2).argmin(): (pos.X**2).argmin()+1].Y.values) | ||
return(r*np.cos(a),r*np.sin(a)) | ||
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def plot_boudaries(MP, BS, **kwargs): | ||
style = kwargs.get("style", ['--k' , '--k']) | ||
alpha = kwargs.get("alpha", 0.6) | ||
axes = kwargs.get("axes", layout_EarthEnv_3planes(**kwargs)) | ||
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if "slice_x" in kwargs: | ||
axes[0].plot() | ||
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axes[0].plot(MP.X,MP.Y,style[0], alpha=alpha) | ||
axes[0].plot(BS.X,BS.Y,style[1], alpha=alpha) | ||
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axes[1].plot(MP.X,MP.Z,style[0], alpha=alpha) | ||
axes[1].plot(BS.X,BS.Z,style[1], alpha=alpha) | ||
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axes[2].plot(make_YZ_plan(MP)[0], make_YZ_plan(MP)[1],style[0],alpha=alpha) | ||
axes[2].plot(make_YZ_plan(BS)[0], make_YZ_plan(BS)[1],style[1],alpha=alpha) |
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Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,28 @@ | ||
import numpy as np | ||
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def norm(u, v, w): | ||
return np.sqrt(u**2 + v**2 + w**2) | ||
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def resolve_poly2(a, b, c): | ||
if isinstance(a, np.ndarray): | ||
r1 = np.zeros_like(a) | ||
r2 = np.zeros_like(a) | ||
a_null = np.where(np.abs(a) < 1e-6)[0] | ||
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delta = b ** 2 - 4 * a * c | ||
np.testing.assert_array_less(-delta, 0) | ||
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r1, r2 = (-b + np.sqrt(delta)) / (2 * a), (-b + np.sqrt(delta)) / (2 * a) | ||
if isinstance(c, np.ndarray): | ||
c = c[a_null] | ||
if isinstance(b, np.ndarray): | ||
b = b[a_null] | ||
r1[a_null] = r2[a_null] = -c / b | ||
else: | ||
delta = b ** 2 - 4 * a * c | ||
np.testing.assert_array_less(-delta, 0) | ||
r1, r2 = (-b + np.sqrt(delta)) / (2 * a), (-b - np.sqrt(delta)) / (2 * a) | ||
if np.abs(a) < 1e-6: | ||
r1 = r2 = -c / b | ||
return r1, r2 |
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