The propagation of harmonic waves in a linear chain consisting of equally spaced
masses m connected by linear springs of stiffness k has been studied extensively. The
chain behaves as a low pass filter so that waves can propagate without attenuation
below the frequency "\\omega_0=2\\sqrt{\\frac{k}{m}}" . Above this frequency, the amplitude decays
exponentially and those waves are called evanescent waves. The "[0,\\omega_0]" frequency range is called a pass-band and in that range the dispersion relation is given by "\\omega=\\omega_0 \\sin{0.5ka}", where k is the wave number, and a is the distance between two consecutive masses. In that range, waves with different phase velocities "c=\\frac{\\omega}{k}" and group velocities "c_g=\\frac{d\\omega}{dk}".
For long waves "(k\\to 0)" , the chain behaves as a rod governed by the classical wave
equation. Several higher order continuum models are derived from the dispersion
relation.
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