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Sec. 2–5 Fourier Series 71<br />

2–5 FOURIER SERIES<br />

The Fourier series is a particular type of orthogonal series that is very useful in solving engineering<br />

problems, especially communication problems. The orthogonal functions that are<br />

used are either sinusoids or, equivalently, complex exponential functions. †<br />

Complex Fourier Series<br />

The complex Fourier series uses the orthogonal exponential functions<br />

w n (t) = e jnv 0t<br />

(2–87)<br />

where n ranges over all possible integer values, negative, positive, and zero; v 0 = 2p/T 0 ,<br />

where T 0 = (b - a) is the length of the interval over which the series, Eq. (2–83), is valid;<br />

and, from Example 2–12, K n = T 0 . The Fourier series theorem follows from Eq. (2–83).<br />

THEOREM. A physical waveform (i.e., finite energy) may be represented over the interval<br />

a 6 t 6 a + T 0 by the complex exponential Fourier series<br />

w(t) =<br />

n=q<br />

a<br />

n=-q<br />

c n e jnv 0t<br />

where the complex (phasor) Fourier coefficients are<br />

(2–88)<br />

c n = 1 T 0 La<br />

and where v 0 = 2pf 0 = 2p/T 0 .<br />

a+T 0<br />

w(t)e -jnv 0t<br />

dt<br />

(2–89)<br />

If the waveform w(t) is periodic with period T 0 , this Fourier series representation is<br />

valid over all time (i.e., over the interval -q 6 t 6 +q), because w(t) and w n(t) are<br />

periodic with the same fundamental period T 0 . For this case of periodic waveforms, the choice<br />

of a value for the parameter a is arbitrary and is usually taken to be a = 0 or a = -T 0 /2 for<br />

mathematical convenience. The frequency f 0 = 1/T 0 is said to be the fundamental frequency<br />

and the frequency nf 0 is said to be the nth harmonic frequency, when n 7 1. The Fourier<br />

coefficient c 0 is equivalent to the DC value of the waveform w(t), because, when n = 0,<br />

Eq. (2–89) is identical to Eq. (2–4).<br />

c n is, in general, a complex number. Furthermore, it is a phasor, since it is the coefficient<br />

of a function of the type e jvt . Consequently, Eq. (2–88) is said to be a complex or phasor<br />

Fourier series.<br />

Some properties of the complex Fourier series are as follows:<br />

1. If w(t) is real,<br />

*<br />

c n = c -n<br />

(2–90)<br />

† Mathematicians generally call any orthogonal series a Fourier series.

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