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Makes the resample backend configurable to make the soxr dependency o…
…ptional. (#377)
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Original file line number | Diff line number | Diff line change |
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""" | ||
Very basic tests to verify that all resampling backends | ||
can be called and are doing their job. | ||
""" | ||
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import matplotlib.pyplot as plt | ||
import numpy as np | ||
import pytest | ||
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import pyroomacoustics as pra | ||
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@pytest.mark.parametrize( | ||
"fs_in, fs_out, backend", | ||
[ | ||
(240, 160, None), | ||
(240, 160, "soxr"), | ||
(240, 160, "samplerate"), | ||
(240, 160, "scipy"), | ||
], | ||
) | ||
def test_downsample(fs_in, fs_out, backend): | ||
"""Idea use a sine above Nyquist of fs_out. It should disappear.""" | ||
assert fs_in > fs_out | ||
f_sine = fs_out / 2.0 + (fs_in - fs_out) / 2.0 * 0.75 | ||
time = np.arange(fs_in * 10) / fs_in | ||
signal_in = np.sin(2.0 * np.pi * time * f_sine) | ||
signal_in = signal_in * np.hanning(signal_in.shape[0]) | ||
signal_out = pra.resample(signal_in, fs_in, fs_out, backend=backend) | ||
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assert abs(signal_out).max() < 1e-3 | ||
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@pytest.mark.parametrize( | ||
"fs_in, fs_out, backend", | ||
[ | ||
(160, 240, None), | ||
(160, 240, "soxr"), | ||
(160, 240, "samplerate"), | ||
(160, 240, "scipy"), | ||
], | ||
) | ||
def test_upsample(fs_in, fs_out, backend): | ||
"""Idea use a sine above Nyquist of fs_out. It should disappear.""" | ||
assert fs_in < fs_out | ||
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# make a random signal | ||
signal_in = np.random.randn(10 * fs_in) | ||
signal_in = signal_in * np.hanning(signal_in.shape[0]) | ||
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signal_out = pra.resample(signal_in, fs_in, fs_out, backend=backend) | ||
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# the test relies on upper frequency being empty | ||
f_cut = fs_in / 2.0 + (fs_out - fs_in) / 2.0 * 0.75 | ||
signal_out_filt = pra.highpass(signal_out, fs_out, fc=f_cut) | ||
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assert abs(signal_out_filt).max() < 1e-3 | ||
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if __name__ == "__main__": | ||
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test_cases = [] | ||
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# Test 1 is the eigenmike impulse response | ||
# Reads the file containing the Eigenmike's directivity measurements | ||
eigenmike = pra.MeasuredDirectivityFile("EM32_Directivity") | ||
fs_tgt = 16000 | ||
fs_file = eigenmike.fs | ||
test_cases.append((fs_file, fs_tgt, eigenmike.impulse_responses[0, 0])) | ||
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# Test 2 is a sine | ||
fs_in = 240 | ||
fs_out = 160 | ||
f_sine = fs_out / 2.0 + (fs_in - fs_out) / 2.0 * 0.95 | ||
time = np.arange(fs_in * 10) / fs_in | ||
signal_in = np.sin(2.0 * np.pi * time * f_sine) | ||
signal_in = signal_in * np.hanning(signal_in.shape[0]) | ||
test_cases.append((fs_in, fs_out, signal_in)) | ||
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# Test 3 is some random noise | ||
np.random.seed(0) | ||
fs_in = 160 | ||
fs_out = 240 | ||
signal_in = np.random.randn(fs_in * 10) | ||
test_cases.append((fs_in, fs_out, signal_in)) | ||
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for fs_in, fs_out, rir_original in test_cases: | ||
time_file = np.arange(rir_original.shape[0]) / fs_file | ||
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rirs = {} | ||
for backend in ["soxr", "samplerate", "scipy"]: | ||
rirs[backend] = pra.resample(rir_original, fs_file, fs_tgt, backend=backend) | ||
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fig, ax = plt.subplots(1, 1) | ||
ax.plot(time_file, rir_original, label="Original") | ||
for idx, (backend, rir) in enumerate(rirs.items()): | ||
time_rir = np.arange(rir.shape[0]) / fs_tgt | ||
ax.plot(time_rir, rir, label=backend, linewidth=(3 - idx)) | ||
ax.legend() | ||
plt.show() |
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