Abstract

It is shown that given a Lagrangian for a system with a finite number of degrees of freedom, the existence of a variational symmetry is equivalent to the existence of coordinates in the extended configuration space such that one of the coordinates is ignorable. The proof given here, which only requires multivariable calculus, provides an elementary derivation of the partial differential equation that determines the variational symmetries of a given Lagrangian, which is obtained in treatises on the Lie theory of symmetries of differential equations or of variational calculus.

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