General Relativity: An Introduction for Physicists · Problem 1.12

The spacetime of special relativity — Hobson, Efstathiou & Lasenby

Physics · spacetime-diagrams

Problem

Draw a spacetime diagram illustrating the coordinate transformation corresponding to two inertial frames SS and S′S' in standard configuration (i.e. where S′S' moves at a speed vv along the positive xx-direction and the two frames coincide at t=t′=0t = t' = 0). Show that the angle between the xx- and x′x'- axes is the same as that between the tt- and t′t'- axes and has the value tan⁡−1(v/c)\tan^{-1}(v/c).
Intuitive explanation

A spacetime diagram reveals how moving observers carve up spacetime differently: events that are simultaneous in SS lie along horizontal lines, while events simultaneous in S′S' tilt at angle θ=tan⁡−1(v/c)\theta = \tan^{-1}(v/c). The key insight is that the x′x'-axis (where t′=0t'=0) and t′t'-axis (where x′=0x'=0) must satisfy the Lorentz transformation equations, and their symmetric tilt around the 45°45° light-cone bisector reflects the invariance of the spacetime interval. This geometric symmetry—equal angles for both axes—emerges directly from how relativity treats space and time as unified dimensions.

Intuitive explanation

A spacetime diagram reveals how moving observers carve up spacetime differently: events that are simultaneous in SS lie along horizontal lines, while events simultaneous in S′S' tilt at angle θ=tan⁡−1(v/c)\theta = \tan^{-1}(v/c). The key insight is that the x′x'-axis (where t′=0t'=0) and t′t'-axis (where x′=0x'=0) must satisfy the Lorentz transformation equations, and their symmetric tilt around the 45°45° light-cone bisector reflects the invariance of the spacetime interval. This geometric symmetry—equal angles for both axes—emerges directly from how relativity treats space and time as unified dimensions.

Related theory

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