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Mathematical Methods for Physicists: A concise introduction - Site Map

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FOURIER SERIES AND INTEGRALS<br />

Solution:<br />

The Fourier coecients are readily calculated:<br />

a n ˆ 1 Z 0<br />

Z <br />

<br />

…k† cos nx dx ‡ k cos nx dx<br />

<br />

0<br />

"<br />

ˆ 1<br />

sin nx<br />

0<br />

k sin nx<br />

<br />

n ‡ k n ˆ 0<br />

<br />

0<br />

b n ˆ 1 Z 0<br />

Z <br />

<br />

…k† sin nx dx ‡ k sin nx dx<br />

<br />

0<br />

"<br />

ˆ 1<br />

cos nx<br />

0<br />

k cos nx<br />

<br />

n k n ˆ 2k …1 cos n†<br />

n<br />

<br />

0<br />

Now cos n ˆ1 <strong>for</strong> odd n, and cos n ˆ 1 <strong>for</strong> even n. Thus<br />

b 1 ˆ 4k=; b 2 ˆ 0; b 3 ˆ 4k=3; b 4 ˆ 0; b 5 ˆ 4k=5; ...<br />

and the corresponding. Fourier series is<br />

4k<br />

<br />

<br />

sin x ‡ 1 3 sin 3x ‡ 1 <br />

sin 5x ‡ :<br />

5<br />

For the special case k ˆ =2, the Fourier series becomes<br />

2 sin x ‡ 2 3 sin 3x ‡ 2 sin 5x ‡:<br />

5<br />

The ®rst two terms are shown in Fig. 4.4, the solid curve is their sum. We will see<br />

that as more and more terms in the Fourier series expansion are included, the sum<br />

more and more nearly approaches the shape of f …x†. This will be further demonstrated<br />

by next example.<br />

Example 4.3<br />

Find the Fourier series that represents the function de®ned by<br />

0;

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