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54<br />

Signals and Spectra Chap. 2<br />

Example 2–5 SPECTRUM OF A SINUSOID<br />

Find the spectrum of a sinusoidal voltage waveform that has a frequency f 0 and a peak value of A<br />

volts. That is,<br />

v(t) = A sin v 0 t where v 0 = 2pf 0<br />

From Eq. (2–26), the spectrum is<br />

q<br />

V(f) = Aa ejv0t - e -jv 0t<br />

b e -jvt dt<br />

L 2j<br />

-q<br />

q<br />

= A 2j L-qe -j2p(f-f0)t dt - A 2j L<br />

By Eq. (2–48), these integrals are equivalent to Dirac delta functions. That is,<br />

V(f) = j A 2 [d(f + f 0) - d(f - f 0 )]<br />

Note that this spectrum is imaginary, as expected, because v(t) is real and odd. In addition, a<br />

meaningful expression was obtained for the Fourier transform, although v(t) was of the infinite<br />

energy type and not absolutely integrable. That is, this v(t) does not satisfy the sufficient (but not<br />

necessary) Dirichlet conditions as given by Eqs. (2–31) and (2–32).<br />

The magnitude spectrum is<br />

|V(f)| = A 2 d(f - f 0) + A 2 d(f + f 0)<br />

where A is a positive number. Since only two frequencies (f =;f 0 ) are present, u( f ) is strictly<br />

defined only at these two frequencies. That is, u(f 0 ) = tan -1 (-1/0) = -90° and<br />

u(-f 0 ) = tan -1 (1/0) =+90°. However, because ƒV(f)ƒ = 0 for all frequencies except f =;f 0<br />

and V(f) = |V(f)| e ju(t) , u( f ) can be taken to be any convenient set of values for f Z;f 0 . Thus,<br />

the phase spectrum is taken to be<br />

q<br />

-q<br />

e -j2p(f # f0 )t dt<br />

|V(f)|<br />

¨(f)<br />

A<br />

–– 2<br />

f 0<br />

Weight<br />

is A/2.<br />

+90°<br />

– f 0<br />

f f<br />

–90°<br />

(a) Magnitude Spectrum<br />

Figure 2–4<br />

(b) Phase Spectrum (¨0=0)<br />

Spectrum of a sine wave.

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