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Common forms
In short, we could loosely say that if a function defined on [-l, l]
can be written as S(x)
below we call the formula Fourier series.
S(x)=\frac{a_0}{2}+\sum\limits_{n=1}^{\infty}(a_n·\cos\frac{n\pi}{l}x+b_n·\sin\frac{n\pi}{l}x)
a_n=\frac{1}{l}\int_{-l}^lf(x)·\cos\frac{n\pi}{l}xdx,n=0,1,2,\dots
b_n=\frac{1}{l}\int_{-l}^lf(x)·\sin\frac{n\pi}{l}xdx,n=1,2,\dots
And:
f(x)=S(x)
whenf(x)
is continuous onx
f(x)=\frac{1}{2}[f(x-0)+f(x+0)]
whenx
is a discontinuity pointf(x)=\frac{1}{2}[f(-l+0)+f(l-0)]
whenx=\pm l
The rules above are known as Dirichlet convergence theorem, though I couldn’t find it on wikipedia actually.
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