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Problems in Mathematical Analysis.pdf - pwp.net.ipl.pt

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Sec. 4] Fourier Series 319<br />

If a function / (x) is odd [i.e., /( x) = / (*)], then a n = Q t/i = 0, i, 2 ...)<br />

and IT<br />

b n = ~ \ / (x) s<strong>in</strong> nx dx (n = 1 , 2, . . .).<br />

JT J<br />

A function specified <strong>in</strong> an <strong>in</strong>terval (0, n) may, at our discretion, be cont<strong>in</strong>ued<br />

<strong>in</strong> the <strong>in</strong>terval ( Jt, 0) either as an even or an odd function; hence,<br />

it may be expanded <strong>in</strong> the <strong>in</strong>terval (0, Ji) <strong>in</strong> an <strong>in</strong>complete Fourier series<br />

of s<strong>in</strong>es or of cos<strong>in</strong>es of mult<strong>ipl</strong>e arcs.<br />

3. Fourier series of a period 21. If a function f (x) satisfies the Dirichlet<br />

conditions <strong>in</strong> some <strong>in</strong>terval ( /, /) of length 2/, then at the discont<strong>in</strong>uities<br />

of the function belong<strong>in</strong>g to this <strong>in</strong>terval the follow<strong>in</strong>g expansion holds:<br />

r, x a ,<br />

,<br />

ju<br />

= /(*) y + fli cos -J- + &! stay<br />

where<br />

.<br />

juc 2nx .<br />

, . . 2nx .<br />

,<br />

+a 2 cos<br />

j- + b2 sm+..,<br />

nnx ,<br />

. . nnx ,<br />

e / v flllX . .<br />

/-v t r v<br />

f (x) cos -- dx = (/i 0, 1, 2, ...),<br />

-M<br />

6 n = -L \f(x)sln^-dx(n=\, 2,<br />

'<br />

-i<br />

At the po<strong>in</strong>ts of discont<strong>in</strong>uity of the function f (x) and at the end-po<strong>in</strong>ts<br />

x-l of the <strong>in</strong>terval, the sum of the Fourier series is def<strong>in</strong>ed <strong>in</strong> a manner<br />

similar to that which we have <strong>in</strong> the expansion <strong>in</strong> the <strong>in</strong>terval ( Jt, n).<br />

In the case of an expansion of the function / (x) <strong>in</strong> a Fourier series <strong>in</strong><br />

an arbitrary <strong>in</strong>terval (a, a-f-2/) of length 2/, the limits of <strong>in</strong>tegration <strong>in</strong><br />

formulas (2) should be replaced respectively by a and a-|-2/<br />

Expand the follow<strong>in</strong>g functions <strong>in</strong> a Fourier series <strong>in</strong> the<br />

<strong>in</strong>terval ( ji, ji), determ<strong>in</strong>e the sum of the series at the po<strong>in</strong>ts<br />

of discont<strong>in</strong>uity and at the end-po<strong>in</strong>ts of the <strong>in</strong>terval (x = ic,<br />

X = JT), construct the graph of the function itself and of the sum<br />

of the correspond<strong>in</strong>g series [outside the <strong>in</strong>terval ( JT, ji) as well]:<br />

when ~~ n < x ^ Q ><br />

Consider the special case when c t =<br />

~ 1,<br />

9fi79 r<br />

2672. x = bx when<br />

Consider the special cases: a) a = b = l\ b) a = 1, 6=1;<br />

c) fl = 0, 6 = 1; d) a=l, 6 = 0.<br />

2673. f(x) = x 2<br />

. 2676. / (x) = cos ax.<br />

2674. f(x) = e ax . 2677. f(x) = smhax.<br />

2675. f(x) = slnax. 2678. f (x) = cosh ax.<br />

2679. Expand the function f(x) = -jr-<br />

the <strong>in</strong>terval (0, 2ji).<br />

(2)<br />

<strong>in</strong> a Fourier series <strong>in</strong>

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