For a nonzero integer , direct integration gives
whereas . The product-to-sum formulas
therefore establish Fourier orthogonality: for positive integers ,
Here is the Kronecker delta. In particular the constant function is orthogonal to every nonconstant sine and cosine in this system. Integrating the given Fourier series, then multiplying it by or and integrating, isolates its Fourier coefficients. Using the permitted interchange of the sum and integral gives
If is an even function, then is an odd function, while is an even function. Thus
The Fourier series consequently reduces to a Fourier cosine series.
The function is an even function, so every Fourier sine coefficient is zero. Introduce the auxiliary integral
For a nonzero integer , integration by parts gives
Consequently
For , a product-to-sum formula yields
If , this becomes
The exceptional Fourier coefficient at must be evaluated before dividing by :
Thus the full Fourier series is
This equality holds on and by periodicity everywhere. Indeed the periodic extension is continuous at the joined endpoints, since both endpoint values are zero, and is piecewise smooth. The theorem on pointwise convergence of a piecewise smooth Fourier series therefore applies, including at the endpoints. The Fourier coefficients also decay as , making the resulting series absolutely and uniformly convergent.
Set and in the Fourier series from b. Since the function is continuous there, pointwise convergence of a piecewise smooth Fourier series gives
It follows that
The and terms are and , respectively. Subtracting them gives the required absolutely convergent series:

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