Classical Electrodynamics · Problem 11.2
Radiating Systems, Multipole Fields and Radiation — John David Jackson
Physics — E&M · lorentz-transformation-group-property
Problem
Consider three inertial frames and coordinates , , and . Frame moves in the direction with speed relative to ; frame moves with speed relative to , and speed relative to . By considering the group property of the transformations of Problem 11.1 (including the results of parts a and b), and directly, show that is a universal constant with the dimensions of an inverse speed squared. This approach obtains the Lorentz transformation without reference to electromagnetism or the second postulate, but requires experiment to show that . Reference: Y. P. Terletskii, Paradoxes in the Theory of Relativity, Plenum Press, New York (1968), pp. 17--25.Intuitive explanation
The key insight is that the group structure of inertial transformations—composing two successive boosts must equal a single direct boost—imposes a powerful algebraic constraint. By comparing the composition with the direct transformation , you'll find that the transformation's functional form must satisfy a consistency condition that forces the ratio to be independent of velocity. This ratio must have dimensions of inverse speed squared to make the algebra work out dimensionally, revealing that relativity's structure emerges purely from the requirement that boosts form a closed group—no light-speed postulate needed yet.
Intuitive explanation
The key insight is that the group structure of inertial transformations—composing two successive boosts must equal a single direct boost—imposes a powerful algebraic constraint. By comparing the composition with the direct transformation , you'll find that the transformation's functional form must satisfy a consistency condition that forces the ratio to be independent of velocity. This ratio must have dimensions of inverse speed squared to make the algebra work out dimensionally, revealing that relativity's structure emerges purely from the requirement that boosts form a closed group—no light-speed postulate needed yet.