Solution

ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2004/ib/paper-3/8b/solution

Take to move along at velocity , with the origins coincident at zero time. The Lorentz transformation is
Differentiating along the particle trajectory gives the relativistic velocity-addition formula
For a timelike particle, and . Direct algebra gives
so , in particular . Strictness requires a massive, subluminal particle; for a photon with , the transformation preserves instead.

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