4.6 Fourier Coefficients from Laplace 261
0 0.2 0.4 0.6 0.8 1
0
0.2
0.4
0.6
0.8
1
t
Period
0 50 100
0
0.1
0.2
0.3
0.4
0.5
0.6
Magnitude line spectrum
|X
|k
Ω (rad/sec)
0 50 100
0
1
2
3
4
Phase line spectrum
<X
k
Ω (rad/sec)
FIGURE 4.7
Period of full-wave rectified signalx(t)and its magnitude and phase line spectra.
and using the Laplace transform we have
X 1 (s)e−0.5s=
π
s^2 +π^2
[1+e−s]
so that
X 1 (s)=
π
s^2 +π^2
[e0.5s+e−0.5s]
The Fourier coefficients are then
Xk=
1
T 0
X 1 (s)|s=j 0 k
whereT 0 =1 and 0 = 2 π, giving
Xk=
π
(j 2 πk)^2 +π^2
2 cos( 2 πk/ 2 )
=
2 (− 1 )k
π( 1 − 4 k^2 )