h61554 s 00000/00051/00116 d D 1.10 24/10/24 12:52:16 bevans 10 9 c Updated e s 00001/00001/00166 d D 1.9 24/10/19 21:11:03 bevans 9 8 c Updated e s 00011/00003/00156 d D 1.8 21/10/22 21:14:45 bevans 8 7 c Updated e s 00022/00003/00137 d D 1.7 21/10/22 21:07:22 bevans 7 6 c Updated e s 00001/00000/00139 d D 1.6 21/10/22 20:43:27 bevans 6 5 c Updated e s 00008/00005/00131 d D 1.5 21/10/22 20:41:17 bevans 5 4 c Updated e s 00037/00003/00099 d D 1.4 21/10/21 16:47:53 bevans 4 3 c Updated e s 00030/00006/00072 d D 1.3 21/10/14 19:15:34 bevans 3 2 c Updated e s 00002/00000/00076 d D 1.2 21/10/14 18:24:22 bevans 2 1 c Updated e s 00076/00000/00000 d D 1.1 21/10/14 18:14:31 bevans 1 0 c date and time created 21/10/14 18:14:31 by bevans e u U f i f e 0 t T I 1
y[n] = x[n] + x[n - 1] for n ≥ 0
As a necessary condition for LTI properties to hold, the LTI system must be at rest. This means that the initial condition x[-1] = 0.
The LTI system is a version of the two-point averaging filter in which the coefficients of 1/2 and 1/2 have been scaled by 2.
h[n] = d[n] + d[n - 1] for n ≥ 0
D 4
ystep[n] = u[n] + u[n - 1] for n ≥ 0
j w oo -j w n 1 -j w n -j w -j w
H(e ) = Sum h[n] e = Sum h[n] e = h[0] + h[1] e = 1 + e
n = -oo n=0
D 5
We can factor the frequency response into polar form per lecture slide 9-9:
E 5
I 5
D 8
We can factor the frequency response into polar form per lecture slide 9-9 by
E 8
I 8
We can factor the frequency response into magnitude-phase form per lecture slide 9-9 by
E 8
factoring out the phase shift corresponding to the delay equal to the index of
the midpoint of the impulse response, which is at an index of 1/2:
E 5
j w -j (w/2) j (w/2) -j (w/2) -j (w/2) H(e ) = e ( e + e ) = e ( 2 cos(w/2) ) j w -j (w/2) H(e ) = 2 cos(w/2) e
D 5 freqz( [ 1 1] ); E 5 I 5 freqz( [1 1] ); E 5will plot the magnitude and phase response for an LTI system with impulse response d[n] + d[n - 1]. The magnitude response, by default, will be plotted in decibels vs. discrete-time frequency, where AdB = 20 log10 | A |. E 4
I 8
As in problem 6.1(a), we can factor the frequency response into magnitude-phase form per lecture slide 9-9 by factoring out the phase shift corresponding to the delay equal to the index of the midpoint of the impulse response, which is at an index of 1 and hence the phase shift is exp(-j w).
E 8 I 7
When we cascade two LTI systems with impulse responses h1[n] and h2[n], as we had seen on lecture slide 8-11 and in Signal Processing First Section 5-7,
y[n] = h1[n] * h2[n] * x[n]
We can write the input-output relationship for the cascade of two LTI systems as a single LTI system
y[n] = h[n] * x[n]
where
h[n] = h1[n] * h2[n] D 10
E 7 E 3
E 2 In homework problem 6.3(a), a linear time-invariant (LTI) system with D 3 input signalx[n] and output signal y[n] is described by E 3 I 3 input signal x[n] and output signal y[n] is described by E 3
D 3 y[n] = x[n] + x[n - 1] for n ≥ 0 E 3 I 3 y[n] = x[n] + x[n - 1] for n ≥ 0 E 3
As a necessary condition for LTI properties to hold, the LTI system must be at rest. This means that the initial condition x[-1] = 0.
The LTI system is a version of the two-point averaging filter in which the coefficients of 1/2 and 1/2 have been scaled by 2.
D 3 h[n] = d[n] + d[n - 1] for n ≥ E 3 I 3 h[n] = d[n] + d[n - 1] for n ≥ 0 E 3
D 3
D 3
oo -n 1 -1 -1
E 3
I 3
oo -n 1 -n -1
E 3
H(z) = Sum h[n] z = Sum h[n] z = h[0] + h[1] z
n = -oo n=0
-1
H(z) = 1 + z
D 7 Zero is at z + 1 = 0 or z = -1. E 7 I 7 Zero is at z + 1 = 0 or z = -1. E 7
D 7 Pole is at z = 0. E 7 I 7 Pole is at z = 0. E 7
D 3
h = [1 1];
E 3
I 3
h = [1 1];
E 5
I 5
h = [1 1]; E 5 E 3 zplane(h); D 5Note that zplane has the same syntax as freqz. E 5E 5 I 5
E 6 Homework problems 6.3(b) and 6.3(c) are very similar. E 10

bevans@ece.utexas.edu
E 1