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Worked collinear composition and rapidity addition at beta = 3/5
Example
Worked computation. Let be a unit spatial direction of an inertial frame and let be the passive boost with parameter (The passive Lorentz boost with parameter beta), so and, in the ordered pair of directions , the boost has the matrix and is the identity on , the -orthogonal complement of (Rapidity parametrization of collinear boosts). Then:
(i) , because and . This is the velocity-addition law , with .
(ii) The rapidities are and , so the rapidities add under composition: .
(iii) The two boosts commute: the reversed product equals the square computed in (i), and this is the instance of the commutativity of collinear boosts.
Facts & Assumptions
Given: A unit spatial direction of an inertial frame, the passive boost , and the collinear family , .
For the boost acts in the frame coordinates by , on the plane, with and the coefficient of the unit direction; the matrix on the ordered pair is and the map is the identity on (The passive Lorentz boost with parameter beta).
For a unit spatial direction and , the boost has on the matrix ; in particular, with , and (Rapidity parametrization of collinear boosts).
For unit and one has with and , and collinear boosts commute (Collinear boost composition and the relativistic velocity-addition law).
For the rapidity is , a strictly increasing bijection of onto with ; for a fixed unit direction, rapidities add: (Rapidity parametrization of collinear boosts, The natural logarithm as the inverse of the exponential function).
For one has and (Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm); the exponential satisfies and the hyperbolic functions are , (The real exponential function and the number by a power series).
The Euclidean norm of a vector of satisfies for a unit direction (The Euclidean inner product on ).
Proof
With and by [L6], [L1] gives , so the matrix of on the ordered pair is , and the map is the identity on the -orthogonal complement of . This is the matrix form recorded in [L2], with the rapidity fixed by ; the numerical value of that rapidity is computed below.
By the commutativity clause of [L3], , i.e. the reversed order gives back the same product; clause (iii) is this instance, and no separate computation is needed.
Squaring the matrix of step 1.1 in the block, on the diagonal and off the diagonal, while the identity block on the complement squares to itself; hence has matrix on and is the identity on the complement. By [L3], with , and . For this , and ; by [L1] the matrix of is therefore on , matching the square. This proves clause (i) and the velocity-addition law.
By [L4] and [L5], , and by the product law, so ; similarly and , so . With this gives : the rapidity of the composed boost in step 2.1 is the sum of the two equal rapidities, in agreement with the addition statement of [L4].
Steps 1.1-2.1 prove clauses (i) and (iii) and step 3.1 proves clause (ii); every entry is an exact rational or logarithmic identity justified by the displayed suppliers.
Depends on
The passive Lorentz boost with parameter beta
Collinear boost composition and the relativistic velocity-addition law
Rapidity parametrization of collinear boosts
The Euclidean inner product on
The natural logarithm as the inverse of the exponential function
The real exponential function and the number by a power series
Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm
Dependency tree · 2 levels
Sources
- B. Crowell, Special Relativity, revision 2020-12-10 (author-published undergraduate textbook), Section 1.4 'The Lorentz transformation' pp. 30-32 including Examples 11-14, Sections 2.3-2.4 'Additional postulates'/'Other axiomatizations' pp. 46-49, and Section 8.3 'Boosts and rotations' pp. 174-176; signature (+---) converted to (-+++) with x^0 = ct restored
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997), Chapter 1 'Special relativity and flat spacetime' pp. 3-7 (PDF pp. 10-14), equations (1.3)-(1.21)