Should ztrans Work Better when Using heaviside() ?

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Paul
Paul il 27 Ott 2022
Commentato: Paul il 28 Ott 2022
Recently ran across peculiar behavior with ztrans.
Define some variables
syms n integer
syms T positive
Set sympref so that heaviside[n] is the discrete-time unit step
sympref('HeavisideAtOrigin',1);
Simple function to take the z-tranform of a signal and then the inverse z-transform, which should return the input signal
g = @(f) [ztrans(f) ; simplify(iztrans(ztrans(f)))];
1. Simple case, works as expected
g([cos(n) sin(n)])
ans = 
2. Introduce symbolic sampling period, still works fine.
g([cos(T*n) sin(T*n)])
ans = 
3. Multiply the simple case by heaviside[n], which shouldn't have any material effect because heaviside[0] = 1
g([cos(n) sin(n)]*heaviside(n))
ans = 
It has no material effect, but we can see that ztrans is accounting for the possibility that heaviside[0] might not be 1, so it appears to be using the general rule
y[n] = f[n]*heaviside[n] = f[0]*heaviside[0]*kroneckerDelta[n] + f[n]*u[n-1]
where u[n] is the discrete-time unit step. The z-transform is then
Y(z) = f[0]*heaviside[0] + Z(f[n+1])/z
As an aside, it seems like it would be easier to solve by
y[n] = f[n]*heaviside[n] = f[n] + (f[0]*heaviside[0] - f[0])*kroneckerDelta(n)
Y(z) = Z(f[n]) - f[0]*h[0]
4. Now introduce the sampling period and heaviside. Based on 2 and 3 above, it would appear that the ztrans should be easily found as would the iztrans.
g([cos(T*n) sin(T*n)]*heaviside(n))
ans = 
But, in neither case is the closed form expression returned for the z-transform. Oddly, iztrans returns the closed form expression for cos, but not for sin.
  4 Commenti
David Goodmanson
David Goodmanson il 27 Ott 2022
Modificato: David Goodmanson il 27 Ott 2022
Yes, my mistake, I spaced out on that.
There are some odd things going on. I tried out complex exponentials and for case 4, the T*n heaviside case, they work. So you could get the correct result with linear combinations of those, but that is not really a satisfactory situation.
I used an arbitrary value p for heaviside(0) in order to show the effect of that. With the output transposed from yours,
syms n integer
syms T positive
syms p
sympref('HeavisideAtOrigin',p);
f = @(q) [cos(q); sin(q); exp(i*q); exp(-i*q)];
fh = @(q) [cos(q); sin(q); exp(i*q); exp(-i*q)]*heaviside(n);
g = @(f) [ztrans(f) simplify(iztrans(ztrans(f)))];
g(f(n)) % case 1
g(f(T*n)) % case 2
g(fh(n)) % case 3
g(fh(T*n)) % case 4
sympref('HeavisideAtOrigin',1/2)
% since the sympref setting is remembered after a session
% (I found that out the hard way).
Case 3 shows the effect of heaviside at the orgin.
% case 1
[(z*(z - cos(1)))/(z^2 - 2*cos(1)*z + 1), cos(n)]
[ (z*sin(1))/(z^2 - 2*cos(1)*z + 1), sin(n)]
[ z/(z - exp(1i)), exp(n*1i)]
[ z/(z - exp(-1i)), exp(-n*1i)]
% case 2
[(z*(z - cos(T)))/(z^2 - 2*cos(T)*z + 1), cos(T*n)]
[ (z*sin(T))/(z^2 - 2*cos(T)*z + 1), sin(T*n)]
[ z/(z - exp(T*1i)), exp(T*n*1i)]
[ z/(z - exp(-T*1i)), exp(-T*n*1i)]
% case 3
[p - (z - (z^2*(z - cos(1)))/(z^2 - 2*cos(1)*z + 1))/z, cos(n) + p*kroneckerDelta(n, 0) - kroneckerDelta(n, 0)]
[ (z*sin(1))/(z^2 - 2*cos(1)*z + 1), sin(n)]
[ p + 1/(z*exp(-1i) - 1), exp(n*1i) + p*kroneckerDelta(n, 0) - kroneckerDelta(n, 0)]
[ p + 1/(z*exp(1i) - 1), exp(-n*1i) + p*kroneckerDelta(n, 0) - kroneckerDelta(n, 0)]
Case 4, who knows why sin and cos are doing what they do.
% case 4
[p + ztrans(cos(T*(n + 1)), n, z)/z, cos(T*n) + p*kroneckerDelta(n, 0) - kroneckerDelta(n, 0)]
[ ztrans(sin(T*(n + 1)), n, z)/z, iztrans(ztrans(sin(T*(n + 1)), n, z)/z, z, n)]
[ p + 1/(z*exp(-T*1i) - 1), exp(T*n*1i) + p*kroneckerDelta(n, 0) - kroneckerDelta(n, 0)]
[ p + 1/(z*exp(T*1i) - 1), exp(-T*n*1i) + p*kroneckerDelta(n, 0) - kroneckerDelta(n, 0)]
Paul
Paul il 28 Ott 2022
Hi David,
% since the sympref setting is remembered after a session
% (I found that out the hard way).
I too am a member of that club. I put
sympref('default')
into my startup.m script and then modify as needed.
Your results with the complex exponentials make the (lack of) results with sin and cos even more puzzling.

Accedi per commentare.

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