4.I.9A

Special Relativity | Part IB, 2003

Prove that the two-dimensional Lorentz transformation can be written in the form

x′=xcosh⁡ϕ−ctsinh⁡ϕct′=−xsinh⁡ϕ+ctcosh⁡ϕ\begin{aligned} x^{\prime} &=x \cosh \phi-c t \sinh \phi \\ c t^{\prime} &=-x \sinh \phi+c t \cosh \phi \end{aligned}

where tanh⁡ϕ=v/c\tanh \phi=v / c. Hence, show that

x′+ct′=e−ϕ(x+ct)x′−ct′=eϕ(x−ct)\begin{aligned} &x^{\prime}+c t^{\prime}=e^{-\phi}(x+c t) \\ &x^{\prime}-c t^{\prime}=e^{\phi}(x-c t) \end{aligned}

Given that frame S′S^{\prime} has speed vv with respect to SS and S′′S^{\prime \prime} has speed v′v^{\prime} with respect to S′S^{\prime}, use this formalism to find the speed v′′v^{\prime \prime} of S′′S^{\prime \prime} with respect to SS.

[Hint: rotation through a hyperbolic angle ϕ\phi, followed by rotation through ϕ′\phi^{\prime}, is equivalent to rotation through ϕ+ϕ′\phi+\phi^{\prime}.]

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