For a plane wave with nonzero angular wavevector kk, its wavelength in the direction k/kk/|k| is

λ=2πk.\lambda=\frac{2\pi}{|k|}.

Advancing by this distance changes kxk\cdot x by 2π2\pi, leaving the exponential unchanged. The is the reciprocal length with the angular factor included.

Variable phase

Where Ψ0\nabla\Psi\ne0, 2π/Ψ2\pi/|\nabla\Psi| is a local wavelength from linearizing the phase. For a nonlinear phase it need not be an exact distance between successive crests over a finite interval. If the Fourier convention uses cycles per length ξ|\xi|, the corresponding wavelength is 1/ξ1/|\xi|.