4.10 Other Properties of the Fourier Series 281
FIGURE 4.16
Nonsymmetric periodic signals.
2
− 2 − 1 0 1
− 2 − 1 01 2 3
2
(^23)
t
t
··· ···
··· ···
x(t)
y(t)
Solution
The given signalx(t)is neither even nor odd, but the advance signalx(t+0.5)is even with a period
ofT 0 =2, 0 =π. Then between−1 and 1 the shifted period is
x 1 (t+0.5)=2[u(t+0.5)−u(t−0.5)]
so that its Laplace transform is
X 1 (s)e0.5s=
2
s
[
e0.5s−e−0.5s
]
which gives the Fourier coefficients
Xk=
1
2
2
jkπ
[
ejkπ/^2 −e−jkπ/^2
]
e−jkπ/^2
=
1
0.5πk
sin(0.5πk)e−jkπ/^2
after replacingsbyjko=jkπand dividing by the periodT 0 =2. These coefficients are complex
as corresponding to a signal that is neither even nor odd. The dc coefficient isX 0 =1.
The given signaly(t)is neither even nor odd, and cannot be made even or odd by shifting. The even
and odd components of a period ofy(t)are shown in Figure 4.17. The even and odd components
of a periody 1 (t)between−1 and 1 are
y 1 e(t)=[u(t+ 1 )−u(t− 1 )]
︸ ︷︷ ︸
rectangular pulse
+[r(t+ 1 )− 2 r(t)+r(t− 1 )]
︸ ︷︷ ︸
triangle
y 1 o(t)=t[u(t+ 1 )−u(t− 1 )]=[(t+ 1 )u(t+ 1 )−u(t+ 1 )]−[(t− 1 )u(t− 1 )+u(t− 1 )]
=r(t+ 1 )−r(t− 1 )−u(t+ 1 )−u(t− 1 )