8.2 Discrete-Time Signals 459nExample 8.7
A “causal” sinusoid, obtained from a signal generator after it is switched on, isx(t)={
2 cos( 0 t−π/ 4 ) t≥ 0
0 otherwiseThe signalx(t)is sampled using a sampling period ofTs=0.1 sec to obtain a discrete-time signalx[n]=x(t)|t=0.1n=2 cos(0.1 0 n−π/ 4 ) n≥ 0and zero otherwise. Determine if this discrete-time signal has finite energy and finite power and
compare these characteristics with those of the continuous-time signalx(t)when 0 =πand when
0 =3.2 rad/sec (an upper approximation ofπ).SolutionThe continuous-time signalx(t)has infinite energy, and so does the discrete-time signalx[n], for
both values of 0. Indeed, its energy isεx=∑∞
n=−∞x[n]^2 =∑∞
n= 04 cos^2 (0.1 0 n−π/ 4 )→∞Although the continuous-time and the discrete-time signals have infinite energy, they have finite
power. That the continuous-time signal has finite power can be shown as indicated in Chapter 1.
For the discrete-time signalx[n], we have for the two frequencies:- For 0 =π,x 1 [n]=2 cos(πn/ 10 −π/ 4 )=2 cos( 2 πn/ 20 −π/ 4 )forn≥0 and zero other-
wise. Thus,x[n] repeats everyN 0 =20 samples forn≥0, and its power is
Px= lim
N→∞1
2 N+ 1
∑N
n=−N|x 1 [n]|^2 = lim
N→∞1
2 N+ 1
∑N
n= 0|x 1 [n]|^2= lim
N→∞1
2 N+ 1
N
^1
N 0
N∑ 0 − 1
n= 0|x 1 [n]|^2
︸ ︷︷ ︸
power of period,n≥ 0=
1
2 N 0
N∑ 0 − 1
n= 0|x 1 [n]|^2 <∞where we used the causality of the signal(x 1 [n]=0 forn< 0 ), and consideredNperiods of
x 1 [n] forn≥0, and for each computed its power to get the final result. Thus, for 0 =π
the discrete-time signalx 1 [n] has finite power and can be computed using a period forn≥0.