Write , where is an integer and . The change of variables and the fact that is a periodic function giveSplit at , then substitute in the second piece:ThereforeThis proves translation invariance of an integral over one period without assuming that is differentiable.
First let . Substitute in the negative half of the integral. Since is an odd function,The two halves cancel, soFor both limits coincide. For , reverse the limits and apply the result with . Thus the identity holds for every real .
The real Fourier series of is writtenwhere the Fourier coefficients areBy part (a)(i), any other interval of length gives the same Fourier coefficients, because each integrand is a periodic function with period . The notation associates with its Fourier series; existence of the integrals alone does not assert pointwise convergence.
On the function is odd, so its mean and all its cosine Fourier coefficients vanish:The assigned endpoint value does not affect these integrals. The product of the two odd functions and is even, hence the sine Fourier coefficients areTwo applications of integration by parts giveThereforeThe periodic extension has a jump discontinuity at every odd multiple of : its left and right limits are and . Its assigned value at each such point is . Thus it is odd away from these points, but it is not a globally odd function pointwise. The Fourier series will take the midpoint value zero at these jumps.
By Dirichlet's theorem on Fourier series, a piecewise continuously differentiable periodic function has a Fourier series converging at each point to the average of its one-sided limits. In particular it converges to the function at every point of continuity. Our periodic extension satisfies these hypotheses, and is a point of continuity with .
At this point for even . For ,Substituting in the Fourier series from part (c) provesThe sum is taken in its displayed order. Discarding its zero even-indexed terms is valid and does not rearrange the remaining terms.
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