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h = freqs(b,a,w)
[h,w] = freqs(b,a,n)
freqs
freqs returns the complex frequency response H(jω) (Laplace transform) of an analog filter
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given the numerator and denominator coefficients in vectors b and a.
h = freqs(b,a,w) returns the complex frequency response of the analog filter specified by coefficient vectors b and a. freqs evaluates the frequency response along the imaginary axis in the complex plane at the angular frequencies in rad/sec specified in real vector w, where w is a vector containing more than one frequency.
[h,w] = freqs(b,a,n) uses n frequency points to compute the frequency response h, where n is a real, scalar value. The frequency vector w is auto-generated and has length n. If you omit n as an input, 200 frequency points are used. If you do not need the generated frequency vector returned, you can use the form h = freqs(b,a,n) to return only the frequency response h.
freqs with no output arguments plots the magnitude and phase response versus frequency in the current figure window.
freqs works only for real input systems and positive frequencies.
Find and graph the frequency response of the transfer function given by:
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a = [1 0.4 1]; b = [0.2 0.3 1]; w = logspace(-1,1); freqs(b,a,w)

You can also create the plot with
h = freqs(b,a,w); mag = abs(h); phase = angle(h); subplot(2,1,1), loglog(w,mag) subplot(2,1,2), semilogx(w,phase)
To convert to hertz, degrees, and decibels, use
f = w/(2*pi); mag = 20*log10(mag); phase = phase*180/pi;
freqs evaluates the polynomials at each frequency point, then divides the numerator response by the denominator response:
s = i*w; h = polyval(b,s)./polyval(a,s);
abs, angle, freqz, invfreqs, logspace, polyval
![]() | flattopwin | freqspace | ![]() |
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