Let each mass be and each spring constant be , with the denoting longitudinal displacements from equilibrium. The Lagrangian is
The inverse coordinate transformation is
Substitution gives
Thus the Euler-Lagrange equations separate into a symmetric pair,
and an antisymmetric pair,
The symmetric normal modes are:
  • , corresponding to and the translational frequency
  • , corresponding to and
For antisymmetric modes, the squared dimensionless frequencies are the eigenvalues of
namely . They give
and
In the original coordinates their mode shapes are respectively
and

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