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Mathematical Methods for Physicists: A concise introduction - Site Map

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FOURIER SERIES AND INTEGRALS<br />

Figure 4.17.<br />

Fourier trans<strong>for</strong>m of e ikx ; jxj a:<br />

Fourier sine and cosine trans<strong>for</strong>ms<br />

If f …x† is an odd function, the Fourier trans<strong>for</strong>ms reduce to<br />

r<br />

Z r<br />

2 1<br />

Z<br />

g…!† ˆ f …x 0 † sin !x 0 dx 0 2 1<br />

; f …x† ˆ g…!† sin !xd!:<br />

<br />

<br />

0<br />

0<br />

…4:33a†<br />

Similarly, if f …x† is an even function, then we have Fourier cosine trans<strong>for</strong>mations:<br />

r<br />

Z r<br />

2 1<br />

Z<br />

g…!† ˆ f …x 0 † cos !x 0 dx 0 2 1<br />

; f …x† ˆ g…!† cos !xd!: …4:33b†<br />

<br />

<br />

0<br />

To demonstrate these results, we ®rst expand the exponential function on the<br />

right hand side of Eq. (4.30)<br />

g…!† ˆp<br />

1<br />

2<br />

ˆ p 1<br />

2<br />

Z 1<br />

1<br />

Z 1<br />

1<br />

f …x 0 †e i!x 0 dx 0<br />

f …x 0 † cos !x 0 dx 0 p<br />

i <br />

2<br />

0<br />

Z 1<br />

1<br />

f …x 0 † sin !x 0 dx 0 :<br />

If f …x† is even, then f …x† cos !x is even and f …x† sin !x is odd. Thus the second<br />

integral on the right hand side of the last equation is zero and we have<br />

g…!† ˆ 1 Z r<br />

1<br />

Z<br />

p f …x 0 † cos !x 0 dx 0 2 1<br />

ˆ f …x 0 † cos !x 0 dx 0 ;<br />

2<br />

<br />

1<br />

g…!† is an even function, since g…!† ˆg…!†. Next from Eq. (4.31) we have<br />

f …x† ˆp<br />

1<br />

2<br />

ˆ p 1<br />

2<br />

Z 1<br />

1<br />

Z 1<br />

1<br />

g…!†e i!x d!<br />

g…!† cos !xd! ‡ p<br />

172<br />

i <br />

2<br />

0<br />

Z 1<br />

1<br />

g…!† sin !xd!:

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