028500f04e
Initial commit of working python and ESP8266 code.
80 lines
2.8 KiB
Python
80 lines
2.8 KiB
Python
from __future__ import print_function
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from __future__ import division
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import numpy as np
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from scipy.interpolate import interp1d
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import matplotlib
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matplotlib.use('TkAgg')
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import matplotlib.pylab as plt
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plt.style.use('lawson')
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import microphone as mic
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# Number of frequency bands used for beat detection
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N_subbands = 64
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# FFT statistics for a few previous updates
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N_history = int(1.0 * mic.FPS)
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ys_historical_energy = np.zeros(shape=(N_subbands, N_history))
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ys_beat_threshold = 6.0
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ys_variance_threshold = 0.0
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# def A_weighting(fs):
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# """Design of an A-weighting filter.
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# b, a = A_weighting(fs) designs a digital A-weighting filter for
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# sampling frequency `fs`. Usage: y = scipy.signal.lfilter(b, a, x).
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# Warning: `fs` should normally be higher than 20 kHz. For example,
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# fs = 48000 yields a class 1-compliant filter.
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# References:
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# [1] IEC/CD 1672: Electroacoustics-Sound Level Meters, Nov. 1996.
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# """
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# # Definition of analog A-weighting filter according to IEC/CD 1672.
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# f1 = 20.598997
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# f2 = 107.65265
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# f3 = 737.86223
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# f4 = 12194.217
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# A1000 = 1.9997
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# NUMs = [(2 * np.pi * f4)**2 * (10**(A1000 / 20)), 0, 0, 0, 0]
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# DENs = np.polymul([1, 4 * np.pi * f4, (2 * np.pi * f4)**2],
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# [1, 4 * np.pi * f1, (2 * np.pi * f1)**2])
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# DENs = np.polymul(np.polymul(DENs, [1, 2 * np.pi * f3]),
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# [1, 2 * np.pi * f2])
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# # Use the bilinear transformation to get the digital filter.
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# # (Octave, MATLAB, and PyLab disagree about Fs vs 1/Fs)
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# return bilinear(NUMs, DENs, fs)
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def beat_detect(ys):
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global ys_historical_energy
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# Beat energy criterion
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current_energy = ys * ys
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mean_energy = np.mean(ys_historical_energy, axis=1)
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has_beat_energy = current_energy > mean_energy * ys_beat_threshold
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ys_historical_energy = np.roll(ys_historical_energy, shift=1, axis=1)
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ys_historical_energy[:, 0] = current_energy
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# Beat variance criterion
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ys_variance = np.var(ys_historical_energy, axis=1)
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has_beat_variance = ys_variance > ys_variance_threshold
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# Combined energy + variance detection
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has_beat = has_beat_energy * has_beat_variance
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return has_beat
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def fft(data):
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"""Returns |fft(data)|"""
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yL, yR = np.split(np.abs(np.fft.fft(data)), 2)
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ys = np.add(yL, yR[::-1])
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xs = np.arange(mic.CHUNK / 2, dtype=float) * float(mic.RATE) / mic.CHUNK
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return xs, ys
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def fft_log_partition(data, fmin=30, fmax=20000, subbands=64):
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"""Returns FFT partitioned into subbands that are logarithmically spaced"""
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xs, ys = fft(data)
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xs_log = np.logspace(np.log10(fmin), np.log10(fmax), num=subbands * 32)
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f = interp1d(xs, ys)
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ys_log = f(xs_log)
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X, Y = [], []
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for i in range(0, subbands * 32, 32):
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X.append(np.mean(xs_log[i:i + 32]))
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Y.append(np.mean(ys_log[i:i + 32]))
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return np.array(X), np.array(Y)
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