Sunday, December 31, 2017

calculus - How to find the closed form of the integralintinfty0f(x)fracsinnxxmdx

Where f(x) is an even function,and also is a periodic functions,the period is π,and n,mN,and n+m is odd number.
When n+m is even, I already have a solution.But when n+m is odd, I don't know how to solve it.I'd appreciate it if someone could help me with it.




When n+m is even,my answer is as follows:



If f (x) is an even function, and the period is π,we have:
0f(x)sinnxxmdx=π20f(x)gm(x)sinnxdx(1)



n,mN,
Where the n+m is an even,and gm(x) in (1) is as follows:
gm(x)={(1)m1(m1)!dm1dxm1(cscx),for n is odd and(1)m1(m1)!dm1dxm1(cotx), for n is even .

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Proof:
0f(x)sinnxxmdx=k=0(2k+1)π2kπf(x)(sinnxxm)dx+k=1kπ(2k1)π2f(x)(sinnxxm)dx=k=0π20f(x+kπ)(sinn(x+kπ)(x+kπ)m)dx+k=10π2f(x+kπ)(sinn(x+kπ)(x+kπ)m)dx=k=0(1)nkπ20f(x)(sinnx(x+kπ)m)dx+k=1(1)nk+n+mπ20f(x)(sinnx(xkπ)m)dx=π20f(x)sinnx(1xm+k=1(1)nk[1(x+kπ)m+(1)n+m(xkπ)m])dx=π20f(x)sinnxgm(x)dx
When n+m is an even,and we know by the Fourier series

cscx=1x+k=1(1)k(1x+kπ+1xkπ)
and
cotx=1x+k=1(1x+kπ+1xkπ)
Take the m-1 order derivative,thus we obtain gm(x).
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Example:

(1.)0sin3xxdx=π20sin2xg1(x)sinxdx=π20sin2x1sinxsinxdx=π20sin2xdx=π4
(2.)0(1+cos2x)sin2xx2dx=π20(1+cos2x)g2(x)sin2xdx=π20(1+cos2x)(ddxcotx)sin2xdx=π20(1+cos2x)(1sin2x)sin2xdx=π20(1+cos2x)dx=π2+π4=3π4
(3.)01(1+cos2x)sin3xx3dx=π20sin3x(1+cos2x)g3(x)dx=π20sin3x(1+cos2x)(12d2dx2(cscx))dx=π20sin3x(1+cos2x)(1+cos2x)2sin3xdx=π2012dx=π4

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