With the standard unweighted inner product on real square-integrable functions, orthogonality on meansMultiplying this inner product by a common nonzero normalising constant does not change orthogonality.
The Fourier coefficients follow by multiplying the expansion by , by the appropriate cosine, or by the appropriate sine, then using orthogonality. In the convention with constant term ,The factor comes from the squared norms of the nonconstant sine and cosine functions: the integral of each square over is . The constant function has squared norm .
For , the even function has , because is an odd function. Its constant coefficient is . The remaining Fourier coefficients areTwo applications of integration by parts give the antiderivative, with ,Its endpoint difference is , so . ThereforeThe periodic extension is continuous and piecewise smooth, so pointwise convergence of a piecewise smooth Fourier series gives equality, including at the endpoints.
Termwise differentiation of a Fourier series, applied to the continuous periodic extension in part (c), gives for Hence the required Fourier sine series isThe endpoint deserves care: at every term is zero, so the Fourier series sums to , the average of the periodic one-sided limits and . It therefore does not reproduce the specified endpoint value . Changing a value at one point does not change any Fourier coefficient, so this is still the Fourier series of the stated function on .
Evaluate the Fourier sine series of part (d) at the interior point . Only odd indices remain, with alternating signs:Thus .
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