Scilab Reference Manual |
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repfreq — frequency response
[ [frq,] repf]=repfreq(sys,fmin,fmax [,step]) [ [frq,] repf]=repfreq(sys [,frq]) [ frq,repf,splitf]=repfreq(sys,fmin,fmax [,step]) [ frq,repf,splitf]=repfreq(sys [,frq])
sys | : syslin list : SIMO linear system |
fmin,fmax | : two real numbers (lower and upper frequency bounds) |
frq | : real vector of frequencies (Hz) |
step | : logarithmic discretization step |
splitf | : vector of indexes of critical frequencies. |
repf | : vector of the complex frequency response |
repfreq returns the frequency response calculation of a linear system. If sys(s) is the transfer function of Sys, repf(k) equals sys(s) evaluated at s= %i*frq(k)*2*%pi for continuous time systems and at exp(2*%i*%pi*dt*frq(k)) for discrete time systems (dt is the sampling period).
db(k) is the magnitude of repf(k) expressed in dB i.e. db(k)=20*log10(abs(repf(k))) and phi(k) is the phase of repf(k) expressed in degrees.
If fmin,fmax,step are input parameters, the response is calculated for the vector of frequencies frq given by: frq=[10.^((log10(fmin)):step:(log10(fmax))) fmax];
If step is not given, the output parameter frq is calculated by frq=calfrq(sys,fmin,fmax).
Vector frq is splitted into regular parts with the split vector. frq(splitf(k):splitf(k+1)-1) has no critical frequency. sys has a pole in the range [frq(splitf(k)),frq(splitf(k)+1)] and no poles outside.
A=diag([-1,-2]);B=[1;1];C=[1,1]; Sys=syslin('c',A,B,C); frq=0:0.02:5;w=frq*2*%pi; //frq=frequencies in Hz ;w=frequencies in rad/sec; [frq1,rep] =repfreq(Sys,frq); [db,phi]=dbphi(rep); Systf=ss2tf(Sys) //Transfer function of Sys x=horner(Systf,w(2)*sqrt(-1)) // x is Systf(s) evaluated at s = i w(2) rep=20*log(abs(x))/log(10) //magnitude of x in dB db(2) // same as rep ang=atan(imag(x),real(x)); //in rad. ang=ang*180/%pi //in degrees phi(2) repf=repfreq(Sys,frq); repf(2)-x
S. S.
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