I love the fourier series as the functions are simply mind boggli ng.
The fourier series of the function f(x)
a(0) / 2 + (k=1..) (a(k) cos kx + b(k) sin kx)
a(k) = 1/PI f(x) cos kx dx
b(k) = 1/PI f(x) sin kx dx
Remainder of fourier series. Sn(x) = sum of first n+1 terms at x.
Sn(x) = 1/PI f(x+t) Dn(t) dt
Dn(x) = Dirichlet kernel = 1/2 + cos x + cos 2x + .. + cos nx = [ sin(n + 1/2)x ] / [ 2sin(x/2) ]
Riemann's Theorem. If f(x) is continuous except for a finite # of finite jumps in every finite interval then:
lim(k->) f(t) cos kt dt = lim(k->)f(t) sin kt dt = 0
The fourier series of the function f(x) in an arbitrary interval.
A(0) / 2 + (k=1..) [ A(k) cos (k(PI)x / m) + B(k) (sin k(PI)x / m) ]
a(k) = 1/m f(x) cos (k(PI)x / m) dx
b(k) = 1/m f(x) sin (k(PI)x / m) dx
Parseval's Theorem. If f(x) is continuous; f(-PI) = f(PI) then
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