Digital Signal Processing Reference
In-Depth Information
FIGURE B.6
Two-sided spectrum in Example B.3.
Similarly, applying Equation
(B.19)
leads to
lim
n
/
0
¼ 2 j1j ¼ 2
jc
0
j ¼
0:0002
sin ð
n
2; 000p 0:0002=2Þ
ðn 2; 000p 0:0002=2Þ
0:001
10
sinð
x
Þ
x
Note: We use the fact that lim
x
/
0
¼ 1:0 (see L'Hospital's rule in Appendix G).
¼ 2
¼ 1:8710
j
c
1
j
¼
j
c
1
j
¼
0:0002
sin ð1 2; 000p 0:0002=2Þ
ð1 2; 000p 0:0002=2Þ
sin ð0:2pÞ
0:2p
0:001
10
¼ 2
¼ 1:5137
jc
2
j ¼ jc
2
j ¼
0:0002
sin ð2 2; 000p 0:0002=2Þ
ð2 2; 000p 0:0002=2Þ
sin ð0:4pÞ
0:4p
0:001
10
¼ 2
¼ 1:0091
jc
3
j¼jc
3
j¼
0:0002
sin ð3 2; 000p 0:0002=2Þ
ð3 2; 000p 0:0002=2Þ
sin ð0:6pÞ
0:6p
0:001
10
¼ 2
¼ 0:4677
jc
4
j ¼ jc
4
j ¼
0:0002
sin ð4 2; 000p 0:0002=2Þ
ð4 2; 000p 0:0002=2Þ
sin ð0:8pÞ
0:8p
0:001
10
Figure B.6
shows the two-sided amplitude spectral plot.
The following example illustrates the use of table information to determine the Fourier series
expansion of the periodic waveform.
Table B.1
consists of the Fourier series expansions for common
periodic signals in the sine-cosine form while
Table B.2
shows the expansions in the complex
exponential form.
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