Classical Mechanics (Kibble & Berkshire) · Problem 13.13

Hamilton's equations and phase space — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · hamiltons-principle

Problem

By using Hamilton's principle, show that, if the Lagrangian L(q,q˙,t)L(\boldsymbol{q}, \dot{\boldsymbol{q}}, t) is modified to L′L' by any transformation of the form L′=L+ddt g(q,t),L' = L + \frac{d}{dt}\, g(\boldsymbol{q}, t), then the equations of motion are unchanged.

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