Classical Electrodynamics · Problem 12.2

Radiating Systems, Multipole Fields and Radiation — John David Jackson

Physics — E&M · gauge-invariance-lagrangian

Problem

(a) Show from Hamilton's principle that Lagrangians that differ only by a total time derivative of some function of the coordinates and time are equivalent in the sense that they yield the same Euler--Lagrange equations of motion. (b) Show explicitly that the gauge transformation Aα→Aα+∂αΛA^\alpha \to A^\alpha + \partial^\alpha \Lambda of the potentials in the charged-particle Lagrangian (12.12) merely generates another equivalent Lagrangian.

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