Mercurial > hg > cm
view cortical_model.py @ 0:5609fd93e935
First commit.
author | Carl Bussey <c.bussey@se10.qmul.ac.uk> |
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date | Sat, 25 Jan 2014 20:00:38 +0000 |
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children | dc43033a2c20 |
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""" A module used for auditory analysis. Models currently implemented: * Frequency-modulation analysis model based on the human auditory system. Model implementations in progress: * Glasberg and Moore model Packaged dependencies: * utils.py and/or utils.pyc * erb.dat * outMidFir.dat External dependencies: * scipy * numpy * copy * matplotlib """ import utils import scipy.signal as sp import numpy as np from copy import deepcopy import matplotlib.pyplot as plt def get_partial_loudness(): """ A function to calculate the partial loudness of an excitation pattern at given ERB. TO DO """ return def get_excitation_i(input, fs, SPL, rectify=False): """ A function to calculate the excitation intensity of the input signal. Parameters: * input (type: array-like matrix of floats) - signal normalised to an amplitude range of -1 to 1. (Required) * fs (type: numerical) - sample frequency of the signal, input. (Required) * SPL (type: double) - the sound pressure level (SPL) at 0 dBFS, e.g., the SPL of a sine wave with peaks at amplitude 1 and troughs at amplitude -1. (Required) * rectify (type: boolean) - Specifies whether to include half wave rectification, modelling the direction of that the cochlear nerves vibrate. True to include, False to ignore. (Optional; Default = False) Returns: * gtfs (type: numpy array of floats) - array with size ((39,) + np.shape(input)) containing the excitation pattern (in sound intensity) for each ERB of input signal. The excitation pattern for the nth ERB can be accessed with gtfs[n]. """ input = np.array(input) inputOMFir = outMidFir(input) inputPa = v_Pascal(inputOMFir, SPL) gtfs = gamma_tone_filter(inputPa, fs) if (rectify): gtfs = half_rectification(gtfs) gtfs = pa_i(gtfs) gtfs = at_normalise(gtfs) return gtfs def plot_excitation_tf(fs = 44100, outMidFilt = True, xscale = 'log', yscale = 'log'): """ A function that plots the transfer function of the outer middle ear and each gammatone filter. Parameters: * fs (type: numerical) - the sampling frequency of the signal. (Optional; Default = 44100) * outMidFilt (type: boolean) - filter the signal by the outer and middle ear FIR filter. (Optional; Default = True) * xscale (type: string) - the scale of the frequency axis. Values are 'log' or 'linear'. (Optional; Default = 'log') * yscale (type: string) - the scale of the amplitude axis. Values are 'log' or 'linear'. (Optional; Default = 'log') Returns: * y (type: numpy array of floats) - array with size ((39,np.ceil(fs))) containing the impulse response of the signal at each gammatone filter (and optionally, including the outer middle ear response). The response at the nth gammatone filter can be accessed by y[n]. """ input = np.zeros(np.ceil(fs)) input[0] = 1 if(outMidFilt): input = outMidFir(input) y = gamma_tone_filter(input, fs) for i in range(np.shape(y)[0]): utils.plot_fft(y[i],xscale, yscale, False) plt.show() return y def get_modulation_i(input, fs): """ A function to calculate the modulation intensity of the input intensity signal. The function implements a filter bank of bandpass filters with cut off frequencies ranging from 0.25 to 16 Hz. Parameters: * input (type: array-like matrix of floats) - the input intensity signal. E.g., use get_excitation_i() to obtain excitation intensity and use as input. * fs (type: numerical) - sampling frequency of input signal Returns: * y (type: numpy array of floats) - array with size ((10,) + np.shape(input)) containing the modulation intensity of the signal at each modulation filter. The modulation intensity for the nth filter can be accessed with y[n]. """ input = np.array(input) b = fir_antialias(fs) input_lp = sp.lfilter(b,(1),input_fr) input_ds = downsample(input_lp, fs) fc = np.array(utils.exp_sequence(-2,4,10)) bw = fc/2 y = decomposition(input_ds, fs, fc, bw) return y def outMidFir(input): """ A function to filter the input signal with the response of the outer and middle ear. Parameters: * input (type: array-like matrix of floats) - signal normalised to an amplitude range of -1 to 1. (Required) Returns: * y (type: numpy array of floats) - array with dimensions equal to the input signal filtered by the response of the outer and middle ear. """ input = np.array(input) b = utils.load_outMidFir_coeff() y = sp.lfilter(b, (1), input) return y def gamma_tone_filter(input, fs): """ A function to filter to decompose the input signal into 39 different gammatones filtered signals modelling the ERBs. Parameters: * input (type: array-like matrix of floats) - signal normalised to an amplitude range of -1 to 1. (Required) * fs (type: numerical) - sample frequency of the signal, input. (Required) Returns: * y (type: numpy array of floats) - array with size ((39),np.shape(input)) containing the impulse response of the signal at each gammatone filter. The response at the nth gammatone filter can be accessed by y[n]. """ input = np.array(input) fc, bw = utils.load_erb_data() y = decomposition(input,fs,fc,bw) return y def v_Pascal(input, SPL): """ A function to convert a signal, normalised to an amplitude range of -1 to 1, to a signal represented in pressure (units: Pascal). Parameters: * input (type: array-like matrix of floats) - signal normalised to an amplitude range of -1 to 1. (Required) * SPL (type: double) - the sound pressure level (SPL) at 0 dBFS, e.g., the SPL of a sine wave with peaks at amplitude 1 and troughs at amplitude -1. (Required) Returns: * y (type: numpy array of floats) - array with dimensions equal to the input signal containing the input represented as a pressure signal. """ input = np.array(input) y = np.sign(input)*(0.00002*10**(np.log10(np.abs(input))+dBFS/20)) return y def pa_i(input, C=406): """ A function to convert a pressure signal (unit: Pascal) to an intensity signal. Parameters: * input (type: array-like matrix of floats) - pressure signal (unit: Pascal) (Required) * C (type: double) - the acoustic impedance of the air (Optional; Default = 406) Returns: * y (type: numpy array of floats) - array with dimensions equal to the input signal containing the input represented as a pressure signal. """ input = np.array(input) y = (input**2) / C return y def at_normalise(input): """ A function to normalise an intensity signal with the audibility threshold. Parameters: * input (type: array-like matrix of floats) - intensity signal (unit: Pascal) (Required) Returns: * y (type: numpy array of floats) - array with dimensions equal to the input signal containing the input normalised with the audibility threshold. """ input = np.array(input) y = input / 1*(10**12) return def downsample(input, factor=100): """ A function to downsample a signal, input, with sampling frequency, fs, by a downsample factor of factor. NOTE: It is advised to use the fir_antialias() function before downsampling to remove any high frequencies which would otherwise represented as low frequencies due to aliasing. Parameters: * input (type: array-like matrix of floats) - input signal. (Required) * factor - downsample factor (Optional; Default = 100) Returns: * output (type: numpy array of floats) - array with outer dimensions equivalent to the to the input, and inner dimension equal to np.floor(lenIn / factor) where lenIn is the length of the inner dimension. """ input = np.array(input) shapeIn = np.shape(input) nDim = np.shape(shapeIn) lenIn = shapeIn[nDim[0]-1] lenOut = np.floor(lenIn / factor) n = np.linspace(0,lenIn,lenOut, endpoint=False).astype(np.int) output = input[...,n] return output def antialias_fir(fs, fc=100, order=64): """ A function which returns the b coefficients for a lowpass fir filter with specified requirements. Made specifically to remove aliasing when downsampling, but can be used for any application that requires a lowpass filter. Parameters: * fs (type: numerical) - sampling frequency of the signal to be filtered (Required) * fc (type: numerical) - unnormalised cut off frequency of the filter (Optional; Default = 100) * order (type: numerical int) - the order of the filter (number of taps minus 1) (Optional; Default = 64) Returns: * b (type: numpy array of floats) - an array of size order + 1 (i.e. a coefficient for each tap) """ nyquist = 0.5*fs fcNorm = fc/nyquist b = sp.firwin(order+1, fcNorm) return b def half_rectification(input): """ A function which performs a half-wave rectification on the input signal. Parameters: * input (type: array-like matrix of floats) - input signal. (Required) Returns: * y (type: numpy array of floats) - an array with dimensions of input containing the half-wave rectification of input. """ y = np.array(input) y[y<0] = 0 return y def decomposition(input, fs, fc, bw, order=1024, verbose = False): """ A function to run the input filter through a bandpass filter bank of length equal to the length of fc. Each bandpass filter is designed by defining the centre frequencies, fc, and bandwidths, bw. Parameters: * input (type: array-like matrix of floats) - input signal. (Required) * fs (type: numerical) - the sampling frequency of the input signal. (Required) * fc (type: array-like vector of floats) - the centre off frequencies (unnormalised) of each bandpass filter. The length of this vector determines the number of filters in the bank. * bw (type: array-like vector of floats) - the bandwidths (unnormalised) of each bandpass filter. Must be equal to or more than the length of fc. If the length is more, all elements exceeding the length of fc - 1 will be ignored. * order (type: numerical int) - the order of the filter (number of taps minus 1) (Optional; Default = 1024) * verbose (type: boolean) - determines whether to display the current subroutine/progress of the procedure. (Optional; Default = False) Returns: * y (type: numpy array of floats) - an array with inner dimensions equal to that of the input and outer dimension equal to the length of fc (i.e. the number of bandpass filters in the bank) containing the outputs to each filter. The output signal of the nth filter can be accessed using y[n]. """ input = np.array(input) nFreqs = len(fc) shape = (nFreqs,) + np.shape(input) shape = shape[0:] y = np.zeros(shape) if(verbose): print "Running frequency decomposition." for i in range(nFreqs): if(verbose): print str(100.0*i/nFreqs) + "% complete." low = fc[i]-bw[i]/2; high = fc[i]+bw[i]/2; if(verbose): print "Low: " + str(low) + "; High: " + str(high) b = fir_bandpass(low, high, fs, order, verbose) x = deepcopy(input) y[i] = sp.lfilter(b,(1),x) return y def fir_bandpass(low, high, fs, order = 1024, verbose = False): """ A function which returns the b coefficients for a bandpass fir filter with specified requirements. Parameters: * low - the lower cutoff frequency of the filter. (Required) * high - the upper cutoff frequency of the filter. (Required) * fs (type: numerical) - sampling frequency of the signal to be filtered. (Required) * order (type: numerical int) - the order of the filter (number of taps minus 1) (Optional; Default = 1024) * verbose (type: boolean) - determines whether to display the current progress (or info on the current subroutine) of the procedure. (Optional; Default = False) Returns: * b (type: numpy array of floats) - an array of size order + 1 (i.e. a coefficient for each tap). """ nyquist = 0.5*fs lowNorm = low/nyquist highNorm = high/nyquist if(verbose): print "Low: " + str(lowNorm) + "; High: " + str(highNorm) b = sp.firwin(order+1, [lowNorm, highNorm], pass_zero=False) return b