Introduction to Classical Mechanics · Problem 11.27

Relativity (Kinematics) — Morin

Physics — Mechanics · successive-lorentz-transformations

Problem

Successive Lorentz transformations The Lorentz transformation in Eq. (11.58) may be written in matrix form as (xct)=(cosh⁡ϕsinh⁡ϕsinh⁡ϕcosh⁡ϕ)(x′ct′).(11.76)\begin{pmatrix} x \\ ct \end{pmatrix} = \begin{pmatrix} \cosh\phi & \sinh\phi \\ \sinh\phi & \cosh\phi \end{pmatrix} \begin{pmatrix} x' \\ ct' \end{pmatrix}. \tag{11.76} Show that if you apply an L.T. with v1=tanh⁡ϕ1v_1 = \tanh\phi_1, and then another one with v2=tanh⁡ϕ2v_2 = \tanh\phi_2, the result is an L.T. with v=tanh⁡(ϕ1+ϕ2)v = \tanh(\phi_1 + \phi_2).

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