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May 2, 2013 09:17
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Systems & Signals practical, investigating z-domain transfer functions.
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# | |
# Copyright (c) 2011 Christopher Felton | |
# | |
# This program is free software: you can redistribute it and/or modify | |
# it under the terms of the GNU Lesser General Public License as published by | |
# the Free Software Foundation, either version 3 of the License, or | |
# (at your option) any later version. | |
# | |
# This program is distributed in the hope that it will be useful, | |
# but WITHOUT ANY WARRANTY; without even the implied warranty of | |
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the | |
# GNU Lesser General Public License for more details. | |
# | |
# You should have received a copy of the GNU Lesser General Public License | |
# along with this program. If not, see <http://www.gnu.org/licenses/>. | |
# | |
# The following is derived from the slides presented by | |
# Alexander Kain for CS506/606 "Special Topics: Speech Signal Processing" | |
# CSLU / OHSU, Spring Term 2011. | |
import numpy as np | |
import matplotlib.pyplot as plt | |
from matplotlib import patches | |
from matplotlib.figure import Figure | |
from matplotlib import rcParams | |
def zplane(b,a,filename=None): | |
"""Plot the complex z-plane given a transfer function. | |
""" | |
# get a figure/plot | |
ax = plt.subplot(111) | |
# create the unit circle | |
uc = patches.Circle((0,0), radius=1, fill=False, | |
color='black', ls='dashed') | |
ax.add_patch(uc) | |
# The coefficients are less than 1, normalize the coeficients | |
if np.max(b) > 1: | |
kn = np.max(b) | |
b = b/float(kn) | |
else: | |
kn = 1 | |
if np.max(a) > 1: | |
kd = np.max(a) | |
a = a/float(kd) | |
else: | |
kd = 1 | |
# Get the poles and zeros | |
p = np.roots(a) | |
z = np.roots(b) | |
k = kn/float(kd) | |
# Plot the zeros and set marker properties | |
t1 = plt.plot(z.real, z.imag, 'go', ms=10) | |
plt.setp( t1, markersize=10.0, markeredgewidth=1.0, | |
markeredgecolor='k', markerfacecolor='g') | |
# Plot the poles and set marker properties | |
t2 = plt.plot(p.real, p.imag, 'rx', ms=10) | |
plt.setp( t2, markersize=12.0, markeredgewidth=3.0, | |
markeredgecolor='r', markerfacecolor='r') | |
ax.spines['left'].set_position('center') | |
ax.spines['bottom'].set_position('center') | |
ax.spines['right'].set_visible(False) | |
ax.spines['top'].set_visible(False) | |
# set the ticks | |
r = 1.5; plt.axis('scaled'); plt.axis([-r, r, -r, r]) | |
ticks = [-1, -.5, .5, 1]; plt.xticks(ticks); plt.yticks(ticks) | |
if filename is None: | |
plt.show() | |
else: | |
plt.savefig(filename) | |
return z, p, k |
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# Copyright Robert Ketteringham 2013 | |
# Licensed under WTFPL | |
# With help from: | |
# http://www.scipy.org/Cookbook/FIRFilter | |
# http://mpastell.com/2009/11/05/iir-filter-design-with-python-and-scipy/ | |
import numpy as np | |
import matplotlib.pyplot as plt | |
from scipy import signal | |
from pylab import unwrap | |
from plot_zplane import zplane | |
def H(theta_1 = 3 * np.pi / 4.0, | |
theta_2 = np.pi / 4.0, | |
r_1 = 0.95, | |
r_2 = 0.95): | |
return np.array([[1, -2 * np.cos(theta_1) * r_1, r_1**2], | |
[1, -2 * np.cos(theta_2) * r_2, r_2**2]]) | |
def helper1bc(num, den): | |
# Calculate Magnitude response | |
freqs, response = signal.freqz(num, den) | |
# Calculate phase response | |
# Unwrap uses small deltas to tell when the result of arctan has been wrapped | |
phase = unwrap(np.arctan2(np.imag(response), np.real(response))) | |
# Calculate impulse response | |
impulse = np.zeros(50) | |
impulse [0] = 1 | |
t = np.arange(50) | |
iresponse = signal.lfilter(num, den, impulse) | |
# Normalize axis | |
freqs = freqs / np.pi # rad -> Hz | |
mag = 20 * np.log10(abs(response)) # DB | |
# Append reversed results (for symmetry) | |
# Normal list addition doesn't work because numpy tries to add the values of arrays | |
freqs = np.hstack((freqs, freqs[-1] + freqs)) | |
mag = np.hstack((mag, mag[::-1])) | |
phase = np.hstack((phase, phase[::-1])) | |
# Plot Magnitude | |
plt.subplot(311) | |
plt.xlabel("Frequency (Hz)") | |
plt.ylabel("Gain (DB)") | |
plt.title("Frequency Response") | |
plt.plot(freqs, mag) | |
# Plot Phase | |
plt.subplot(312) | |
plt.xlabel("Frequency (Hz)") | |
plt.ylabel("Phase (radians)") | |
plt.title("Phase Response") | |
plt.plot(freqs, phase) | |
# Plot response | |
plt.subplot(313) | |
plt.ylabel("Amplitude") | |
plt.xlabel("n (samples)") | |
plt.title("Impulse Response") | |
plt.stem(t, iresponse) | |
#Show | |
plt.subplots_adjust(hspace=0.5) | |
plt.show() | |
# Question 1 | |
def q1a(): | |
# zplane takes two arguments, the numerator and the denominator, each being lists | |
# star extracts elements from a list and uses them as arguments to a function | |
zplane(*H()) | |
def q1b(): | |
for r_1 in [0.0, 0.5, 0.8, 1.0, 1.05]: | |
# Get transfer function | |
num, den = H(r_1=r_1) | |
helper1bc(num, den) | |
def q1c(): | |
for r_2 in [0.0, 0.5, 0.8, 1.0, 1.05]: | |
# Get transfer function | |
num, den = H(r_2=r_2) | |
helper1bc(num, den) | |
def q1d(): | |
for theta_1 in np.pi * np.array([0.0, 0.25 , 0.5, 0.75, 1]): | |
# Get transfer function | |
num, den = H(theta_1=theta_1) | |
helper1bc(num, den) | |
def q1e(): | |
for theta_2 in np.pi * np.array([0.0, 0.25 , 0.5, 0.75, 1]): | |
# Get transfer function | |
num, den = H(theta_2=theta_2) | |
helper1bc(num, den) | |
def q1f(): | |
num, den = H(r_2=1.0) | |
t = np.arange(100) | |
for i, w in enumerate(np.array([0.22, 0.25, 0.27]) * np.pi): | |
inp = np.sin(t * w) | |
response = signal.lfilter(num, den, inp) | |
plt.subplot(3, 1, (i + 1)) | |
plt.ylabel("Amplitude") | |
plt.xlabel("n (samples)") | |
plt.title("w = " + str(w) +" (rad/sample)") | |
plt.stem(t, response) | |
#Show | |
plt.subplots_adjust(hspace=0.5) | |
plt.show() | |
# Question 2 | |
def q2(): | |
num = [.0038, .0001, .0051, .0001, .0038] | |
den = [1., -3.2821, 4.236, -2.5275, .5865] | |
# Q2a | |
helper1bc(num, den) | |
# Q2b | |
t = np.arange(100) | |
for i, w in enumerate(np.array([0.02, 0.1, 0.25, 0.4]) * np.pi): | |
inp = np.sin(t * w) | |
response = signal.lfilter(num, den, inp) | |
plt.subplot(4, 1, (i + 1)) | |
plt.ylabel("Amplitude") | |
plt.xlabel("n (samples)") | |
plt.title("w = " + str(w) +" (rad/sample)") | |
plt.stem(t, response) | |
#Show | |
plt.subplots_adjust(hspace=0.5) | |
plt.show() | |
# Q2c | |
zplane(np.array(num), np.array(den)) | |
q1a() | |
q1b() | |
q1c() | |
q1d() | |
q1e() | |
q1f() | |
q2() |
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