Digital Signal Processing Reference
In-Depth Information
The result is obtained from the property of the impulse function
b
f(t 0 ),
a F t 0 F b
B
f(t)d(t - t 0 )dt =
.
0,
otherwise
L
a
In (12.24), only the impulse functions
occur between
In summary, for a periodic sequence
d(Æ), d(Æ- 2p/N),
Á , d(Æ- 2p[N - 1]/N)
0 FÆ62p.
x[n] = x[n + N],
N q
2p
2pk
N
2pk
N
¢
¢
[eq(12.23)]
X(Æ) =
X 0
d
Æ-
k=- q
and
N- 1
1
N a
2pk
N
¢
e j2pkn/N ,
[eq(12.24)]
x[n] =
X 0
k= 0
where, from (12.18),
N- 1
x 0 [n]e -jnÆ .
X 0 (Æ) = a
(12.25)
n= 0
There are N distinct values of
x[n]
and N distinct values of
X 0 (2pk/N).
An example
is now given to illustrate these developments.
Calculation of the DTFT of a periodic sequence
EXAMPLE 12.7
Consider again the periodic signal
x[n]
of Figure 12.4. For this signal,
N = 3, x 0 [0] = 0,
x 0 [1] = 1,
and
x 0 [2] = 1.
From (12.25), the discrete-time Fourier transform of
x 0 [n]
is given
by
N- 1
x 0 [n]e -jnÆ = 0e -j0 + (1)e -jÆ + (1)e -j2Æ
X 0 (Æ) = a
n= 0
= e -jÆ + e -j2Æ .
This transform is periodic and the real part of
X 0 (Æ)
is plotted in Figure 12.6. From (12.23), the
discrete-time Fourier transform of
x[n]
is then
3 q
2p
2pk
3
2pk
3
X(Æ) =
X 0
¢
d
¢
Æ-
,
k=- q
 
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