As lurscher suggests in a comment, in the case of a closed curve, one could consider a periodic parametrization of the curve
f(θ) = f(θ+2π) ∈ R2,f(θ) = (x(θ),y(θ)).
Then define Fourier coefficients in the standard way
cn(f) := ∫2π0dθ2πe−inθ f(θ).
(The Fourier coefficients cn(f) are well-defined if the coordinate functions x,y are Lebesgue integrable x,y∈L1(R/2πZ).) The Fourier series for f is vector-valued
∑n∈Zcn(f) einθ.
A similar approached works also for a closed curve in higher dimensions. In the 2 dimensional case, one may identify the plane R2≅C with the complex plane, as Greg P, Mark Eichenlaub, and J.M. point out.
This post imported from StackExchange Mathematics at 2014-06-02 11:01 (UCT), posted by SE-user Qmechanic