The well-known result for the frequency of a simple spring–masssystem may be combined with elementary concepts like speed = wavelength × frequency to obtain wave propagation speeds for an infinite chain of springs and masses (masses m held apart atequilibrium distance a by springs of stiffness γ). These propagation speeds are dependent on the wavelength of the wave. The dispersionis easily investigated by considering normal modes of increasing wavelength. Thisinvestigation also elegantly highlights how the dispersion physically arises in the form of effective spring constants due to the way in which neighbouring springs contribute tothe propagation of each of the normal modes. The resulting propagation speeds v(λ) are given by an expression , which in the limit of large λ becomes . This of course means that —the serendipitous emergence of what turns out to be Viète’s formula forπ in terms of nested roots of 2.
Read full abstract