[z, p, k] = dsp.zplane(bb, aa)
    plt.title('Pol/Nullstellenplan')
    plt.grid('on')
    #    plt.text(-0.95,0.0 ,'(2)')
    plt.axis([-1.1, 1.1, -1.1, 1.1])
    plt.tight_layout()
    if DEF_PRINT == True:
        plt.savefig((PRINT_PATH + 'PZ' + PRINT_TYPE))

#=========================================
## Impulsantwort
#=========================================

if SHOW_IMPZ == True:
    plt.figure(2)
    [h, td] = dsp.impz(bb, aa, f_S)  #Impulsantwort / Koeffizienten
    [ml, sl, bl] = plt.stem(td, h)
    plt.grid('on')
    plt.setp(ml, 'markerfacecolor', 'r', 'markersize', 8)
    plt.xlabel(my_x_axis_t)
    plt.ylabel(r'$h[n] \rightarrow $', fontsize=20)
    plt.title(r'Impulsantwort $h[n]$')
    plt.tight_layout()
    if PLT_AUTOx: dsp.format_ticks('x', f_scale * 1000, "%.3g")
    if DEF_PRINT == True:
        plt.savefig((PRINT_PATH + 'impz' + PRINT_TYPE))

#=========================================
## Linear frequency plot
#=========================================
if SHOW_LIN_H_f == True:
示例#2
0
ylabel(r'$\angle H(e^{j\Omega}) / \pi \rightarrow $')
plot(f, angle(H)/pi)
subplot(313)
tau, w = dsp.grpdelay(b,a, nfft = 2048, Fs = 200, whole=0)
plot(w, tau)
ymin, ymax = ylim(); dy = max(ymax - ymin, 1) * 0.05
ylim(ymin - dy, ymax + dy) # set reasonable range
xlabel(r'$f$ / Hz $\rightarrow$')
ylabel(r'$\tau_g(e^{j \Omega}) / T_S \rightarrow$')
#plt.tight_layout()

#-------------------------------------------------------
fig3 = figure(3)
plt.suptitle('Filtereigenschaften', fontsize=18)
#
h, t = dsp.impz(b,a) # impulse response
ax31 = fig3.add_subplot(311)
ax31.stem(range(len(h)),h)
ax31.grid('on')
ax31.set_ylabel(r'Impulsantwort' '\n' r'$h[n]\, \rightarrow$')
ax31.yaxis.set_label_coords(-0.1, 0.5)
#
yn = np.convolve(xn,h) # Faltung (Convolution) von x und h
ax32 = fig3.add_subplot(312)
ax32.grid('on')
ax32.stem(range(len(yn)),yn)
ax32.set_xlabel(r'$n \, \rightarrow$')
ax32.set_ylabel(r'Filterausgang' '\n' r'$y[n]\, \rightarrow$')
ax32.yaxis.set_label_coords(-0.1, 0.5)
#
w,h = sig.freqz(h); f =  w / (2*pi*Ts)
    [z, p, k] = dsp.zplane(bb, aa)
    plt.title('Pol/Nullstellenplan')
    plt.grid('on')
#    plt.text(-0.95,0.0 ,'(2)')
    plt.axis([-1.1, 1.1, -1.1, 1.1])
    plt.tight_layout() 
    if DEF_PRINT == True:
        plt.savefig((PRINT_PATH +'PZ' + PRINT_TYPE))

#=========================================
## Impulsantwort
#=========================================

if SHOW_IMPZ == True:
    plt.figure(2)
    [h, td]=dsp.impz(bb, aa, f_S)  #Impulsantwort / Koeffizienten
    [ml, sl, bl] = plt.stem(td, h) 
    plt.grid('on')
    plt.setp(ml, 'markerfacecolor', 'r', 'markersize', 8)
    plt.xlabel(my_x_axis_t)
    plt.ylabel(r'$h[n] \rightarrow $', fontsize = 20)
    plt.title(r'Impulsantwort $h[n]$')
    plt.tight_layout()
    if PLT_AUTOx: dsp.format_ticks('x', f_scale*1000, "%.3g")
    if DEF_PRINT == True:
        plt.savefig((PRINT_PATH + 'impz' + PRINT_TYPE))

#=========================================
## Linear frequency plot
#=========================================
if SHOW_LIN_H_f == True:
示例#4
0
                               subplot, title, clf, xlim, ylim)

import sys
sys.path.append('..')
import dsp_fpga_lib as dsp

# -- Impulse response (lin / log) ---
f1 = 50
Ts = 5e-3
n = arange(0, 50)  # sample n
t = arange(0, 49., 0.1)  # feiner aufgelöst
xn = 1.5 + 0.5 * cos(2.0 * pi * f1 * n * Ts)  # x[n]
b = [0.1, 0]
a = [1, -0.9]  # Koeffizienten
#   H(z) = (0.1 z + 0) / (z - 0.9)
[h, k] = dsp.impz(b, a, N=30)  # -> h[k]
figure(1)
subplot(211)
stem(k, h, 'r')  # x[n], red stems
ylabel(r'$h[k] \rightarrow$')
grid(True)
title(r'Impulsantwort $h[n]$')
subplot(212)
stem(k, 20 * log10(abs(h)), 'r')
xlabel(r'$k \rightarrow$')
grid(True)
ylabel(r'$20 \log\, h[k] \rightarrow$')
# ------- Filtered signal -------------
figure(2)
yn = sig.lfilter(b, a, xn)  #filter xn with h
f = intp.interp1d(n, yn, kind='cubic')
from matplotlib.pyplot import (figure, plot, stem, grid, xlabel, ylabel,
    subplot, title, clf, xlim, ylim)

import sys
sys.path.append('..')
import dsp_fpga_lib as dsp

alpha = 0.9; f_S = 1 
b = [1, 0] # z + 0
# b = [1 0 0] # z^2 + 0
a = [1, -alpha] # z - 0.9; Add., 1 Verzögerung
#a = [1 +alpha] # z + 0.9; Subtr., 1 Verz.
#a = [1 0 -alpha] # z^2 - 0.9; Add., 2 Verz.
#a = [1 0 +alpha] # z^2 - 0.9; Subtr., 2 Verz.

dsp.zplane(b,a)#, plt_ax = ax)  # Plotte P/N Diagramm
# H(f) entlang der oberen Hälfte des EK:
[W,H] = sig.freqz(b,a,1024, f_S)
fig2 = figure(2)
plot(W/(2*pi),abs(H),linewidth = 2) # H(F)
xlabel(r'$F$  bzw. $\Omega / 2 \pi$') 
ylabel(r'$|H(F)| \; \rightarrow$')
# Berechne 20 Werte der Impulsantwort:
[himp,t] = dsp.impz(b,a,20,f_S) 
figure(3)
(ml, sl, bl) = stem(t,himp) # Impulsantwort
plt.setp(ml,'markerfacecolor','r',
	'markersize',8)
plt.setp(sl,'linewidth',2)
xlabel('$n$'); ylabel(r'$h[n]$')
plt.show()
from matplotlib.pyplot import (figure, plot, stem, grid, xlabel, ylabel,
    subplot, title, clf, xlim, ylim)

import sys
sys.path.append('..')
import dsp_fpga_lib as dsp

alpha = 0.9; f_S = 1 
b = [1, 0] # z + 0
# b = [1 0 0] # z^2 + 0
a = [1, -alpha] # z - 0.9; Add., 1 Verzögerung
#a = [1 +alpha] # z + 0.9; Subtr., 1 Verz.
#a = [1 0 -alpha] # z^2 - 0.9; Add., 2 Verz.
#a = [1 0 +alpha] # z^2 - 0.9; Subtr., 2 Verz.

dsp.zplane(b,a)#, plt_ax = ax)  # Plotte P/N Diagramm
# H(f) entlang der oberen Hälfte des EK:
[W,H] = sig.freqz(b,a,1024, f_S)
fig2 = figure(2)
plot(W/(2*pi),abs(H),linewidth = 2) # H(F)
xlabel(r'$F$  bzw. $\Omega / 2 \pi$') 
ylabel(r'$|H(F)| \; \rightarrow$')
# Berechne 20 Werte der Impulsantwort:
[himp,t] = dsp.impz(b,a,20,f_S) 
figure(3)
(ml, sl, bl) = stem(t,himp) # Impulsantwort
plt.setp(ml,'markerfacecolor','r',
	'markersize',8)
plt.setp(sl,'linewidth',2)
xlabel('$n$'); ylabel(r'$h[n]$')
plt.show()
示例#7
0
plot(f, angle(H) / pi)
subplot(313)
tau, w = dsp.grpdelay(b, a, nfft=2048, Fs=200, whole=0)
plot(w, tau)
ymin, ymax = ylim()
dy = max(ymax - ymin, 1) * 0.05
ylim(ymin - dy, ymax + dy)  # set reasonable range
xlabel(r'$f$ / Hz $\rightarrow$')
ylabel(r'$\tau_g(e^{j \Omega}) / T_S \rightarrow$')
#plt.tight_layout()

#-------------------------------------------------------
fig3 = figure(3)
plt.suptitle('Filtereigenschaften', fontsize=18)
#
h, t = dsp.impz(b, a)  # impulse response
ax31 = fig3.add_subplot(311)
ax31.stem(range(len(h)), h)
ax31.grid('on')
ax31.set_ylabel(r'Impulsantwort' '\n' r'$h[n]\, \rightarrow$')
ax31.yaxis.set_label_coords(-0.1, 0.5)
#
yn = np.convolve(xn, h)  # Faltung (Convolution) von x und h
ax32 = fig3.add_subplot(312)
ax32.grid('on')
ax32.stem(range(len(yn)), yn)
ax32.set_xlabel(r'$n \, \rightarrow$')
ax32.set_ylabel(r'Filterausgang' '\n' r'$y[n]\, \rightarrow$')
ax32.yaxis.set_label_coords(-0.1, 0.5)
#
w, h = sig.freqz(h)
示例#8
0
import matplotlib.pyplot as plt
from matplotlib.pyplot import (figure, plot, stem, grid, xlabel, ylabel,
    subplot, title, clf, xlim, ylim)

import sys
sys.path.append('..')
import dsp_fpga_lib as dsp

# -- Impulse response (lin / log) ---
f1 = 50; Ts = 5e-3 
n = arange(0, 50) # sample n
t = arange(0, 49., 0.1) # feiner aufgelöst
xn = 1.5 + 0.5*cos(2.0*pi*f1*n*Ts) # x[n]
b = [0.1, 0]; a = [1, -0.9] # Koeffizienten
#   H(z) = (0.1 z + 0) / (z - 0.9)
[h, k] = dsp.impz(b, a, N = 30) # -> h[k]
figure(1)
subplot(211)
stem(k, h, 'r') # x[n], red stems
ylabel(r'$h[k] \rightarrow$'); grid(True)
title(r'Impulsantwort $h[n]$')
subplot(212)
stem(k, 20*log10(abs(h)), 'r') 
xlabel(r'$k \rightarrow$'); grid(True)
ylabel(r'$20 \log\, h[k] \rightarrow$')
# ------- Filtered signal -------------
figure(2); 
yn = sig.lfilter(b,a,xn) #filter xn with h
f = intp.interp1d(n, yn, kind = 'cubic')
yt = f(t) # y(t), interpolated
plot(t, yt, color='#cc0000', linewidth=3)