The function is even and continuous, with period . On it is , so it rises from zero to one at , crosses zero at , reaches minus one at , and returns to zero at . Reflect this curve about the vertical axis and repeat periodically. The joins at integer multiples of have corners, but no jumps.
Figure 1.
Even periodic extension of a sine mode and its Fourier approximation
. Original plot over two periods. The dashed approximation uses the first twelve nonzero cosine coefficients; the exact function is continuous with corners at integer multiples of . Details.
Because the function is even, all sine Fourier coefficients vanish. Its average is zero, so . The Fourier cosine coefficients of a sine mode follow from the product-to-sum identity:
For , the integral is directly zero rather than an undefined substitution into a denominator. Thus
The Fourier series equals the continuous function at every point, including the corners. Its coefficients decay quadratically, so the series is also absolutely convergent.
At , the Fourier series equals . Isolating the first term gives
Changing the sign of the remaining denominators proves
The absolute convergence justifies the evaluation and rearrangement.

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