The velocity with which the overall envelope shape of the wave's amplitudes is called as the velocity of a wave group. The individual wavelets of differing wavelengths traveling at different speeds form a wave group.
We consider a wave packet as a function of position x and time t: α(x,t).
Let A(k) be its Fourier transform at time t = 0,
"\u03b1(x,0)= \\int_{ -\u221e}^ {\u221e} dk A(k)e^{ ikx } (1)"where ω is implicitly a function of k.
By the superposition principle, the wavepacket at any time t is
where ω is implicitly a function of k.
After integrating (2) we got:
where ω is the wave's angular frequency (usually expressed in radians per second), and k is the angular wavenumber.
Phase velocity vp and group velocity vg are related through Rayleigh's formula,
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