Derives Lagrangian mechanics for relativistic particles and fields from the postulates of special relativity, recovering E=mc² and Lorentz invariance of EM equations.
In this section we take the coordinates to be of the form ( ct,x 1,x 2,x 3)
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Demystifying the Lagrangians of special relativity
Derives Lagrangian mechanics for relativistic particles and fields from the postulates of special relativity, recovering E=mc² and Lorentz invariance of EM equations.