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(<br />

58<br />

Signals and Spectra Chap. 2<br />

Time Domain<br />

<br />

(<br />

t<br />

Frequency Domain<br />

1.0T<br />

T Sa(∏Tf)<br />

1.0<br />

T<br />

– –– 2<br />

T ––2<br />

3<br />

– –– T<br />

2<br />

– –– T<br />

1<br />

– –– T<br />

1 ––T<br />

2 ––T<br />

(a) Rectangular Pulse and Its Spectrum<br />

2WSa(2∏Wt)<br />

–– T<br />

T<br />

0.5T<br />

t<br />

f<br />

2W<br />

<br />

(<br />

–––<br />

f<br />

2W<br />

W<br />

1.0<br />

3<br />

– ––––<br />

2W<br />

1<br />

– –––<br />

W<br />

1<br />

– ––––<br />

2W<br />

1<br />

–––<br />

2W<br />

1<br />

t<br />

–W<br />

W<br />

f<br />

(b) Sa(x) Pulse and Its Spectrum<br />

<br />

(<br />

–– t<br />

T<br />

(<br />

1.0T<br />

0.5T<br />

T Sa 2 (∏Tf)<br />

– T<br />

–– W<br />

3 ––T<br />

1.0<br />

t<br />

–<br />

2<br />

– –– T<br />

1<br />

– –– T<br />

1 ––T<br />

2 ––T<br />

f<br />

(c) Triangular Pulse and Its Spectrum<br />

Figure 2–6 Spectra of rectangular, ( sin x)/x, and triangular pulses.<br />

where W is the absolute bandwidth in hertz. This Fourier transform pair is also shown in Fig. 2–6b.<br />

The spectra shown in Fig. 2–6 are real because the time domain pulses are real and even. If<br />

the pulses are offset in time to destroy the even symmetry, the spectra will be complex. For<br />

example, let<br />

v(t) = e 1, 0 6 t 6 T t = T/2<br />

f =ßa b<br />

0, t elsewhere T<br />

Then, using the time delay theorem and Eq. (2–55), we get the spectrum<br />

V(f) = T e -jpfT Sa (pTf)<br />

(2–57)

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