pith. sign in

( 101), the last summand vanishes and we are left with δS = ∫ ϕ (¯t2) ϕ (¯t1)   ∂L ∂f − d dϕ   ∂L ∂ ( df dϕ )     δf dϕ

into δS = ∫ ϕ (¯t2) ϕ (¯t1) ∂L ∂f δf − d dϕ   ∂L ∂ ( df dϕ )   δf dϕ +   ∂L ∂ ( df dϕ )δf   ϕ (¯t2) ϕ (¯t1) (103) Because of the boundary condition defined in Eq

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Demystifying the Lagrangians of special relativity

physics.class-ph · 2021-07-04 · unverdicted · novelty 2.0

Derives Lagrangian mechanics for relativistic particles and fields from the postulates of special relativity, recovering E=mc² and Lorentz invariance of EM equations.

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  • Demystifying the Lagrangians of special relativity physics.class-ph · 2021-07-04 · unverdicted · none · ref 13

    Derives Lagrangian mechanics for relativistic particles and fields from the postulates of special relativity, recovering E=mc² and Lorentz invariance of EM equations.