Let each mass be and each spring constant be , with the denoting longitudinal displacements from equilibrium. The Lagrangian isThe inverse coordinate transformation isSubstitution givesThus the Euler-Lagrange equations separate into a symmetric pair,and an antisymmetric pair,
The symmetric normal modes are:
For antisymmetric modes, the squared dimensionless frequencies are the eigenvalues ofnamely . They giveandIn the original coordinates their mode shapes are respectivelyand
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