The function is even, so each product with a sine is an odd function and all the Fourier coefficients vanish. Its constant coefficient is
For , part (a) gives the remaining Fourier coefficients:
Consequently the Fourier cosine series is
The periodic extension is continuous, including at , and piecewise continuously differentiable. Thus the Fourier series equals everywhere. Its coefficients are also bounded in magnitude by a constant times , which gives absolute convergence.

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