For the Fourier cosine series, first take the even extension on , and then its -periodic extension. Evenness eliminates the sine terms. With the constant term written as , the Fourier coefficients and series are
For the Fourier sine series, take the odd extension for and for , and extend with period . Values assigned at isolated endpoints do not change the Fourier coefficients. Oddness eliminates the constant and cosine terms, leaving
Both formulas follow by orthogonality on and the parity of the extensions.
Using the usual piecewise smooth interpretation of the derivative hypothesis, Dirichlet's theorem on Fourier series gives the average of the two one-sided limits of the appropriate periodic extension. The even extension is continuous at and at the identified endpoints , so the Fourier cosine series converges to
For the odd extension, the one-sided limits at zero are and , while at the periodic one-sided limits are and . Hence the Fourier sine series converges to
At an endpoint this equals precisely when is zero there. One can also see the zero endpoint values directly: every partial sum consists of sines that vanish at both endpoints.

Articles by others on the same topic (0)

There are currently no matching articles.