How statement and proof provenance work
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Worked velocity transformation: collinear, transverse and null cases
Example
Let and be inertial charts related by a boost of parameter along the first axis (, The passive Lorentz boost with parameter beta, Inertial frames and inertial charts of the affine Minkowski model).
(a) Collinear case. A worldline with coordinate velocity in has, by clause (iv) of Coordinate formulas of a boost: clock rates, rod lengths, simultaneity and velocity transformation, , so ; the Galilean difference is not the transformed velocity.
(b) Transverse case. A worldline with has and , hence .
(c) Null limit. For the formula gives and : a null worldline is null in every inertial chart.
In each case take the affine coordinate curve on with the stated constant ; the first two are future timelike and the third future null. The three cases verify the velocity transformation and the subluminality statement of clause (iv) of Coordinate formulas of a boost: clock rates, rod lengths, simultaneity and velocity transformation.
Facts & Assumptions
Given: Two inertial charts , related by the boost of parameter along the first axis with , and the three coordinate velocities , , (The passive Lorentz boost with parameter beta, Inertial frames and inertial charts of the affine Minkowski model).
Clause (iv) of Coordinate formulas of a boost: clock rates, rod lengths, simultaneity and velocity transformation: for a future causal curve with coordinate velocity , , in the chart , the coordinate velocity in is and , with positive denominators, and for , with exactly when .
The boost parameter is and (The passive Lorentz boost with parameter beta).
Verification
Collinear case: with , , , the denominator of [L1] is and ; hence and because . The Galilean difference for this passive change of frame is , which is not the transformed velocity.
Transverse case: with , , the denominator is and [L1] gives and , so and because .
Null limit: with the denominator of [L1] is and , so and ; this is the equality case of the subluminality statement, consistent with .
Conclusion: steps 1.1-1.3 evaluate the transformation formula of [L1] in the three configurations and confirm for subluminal and in the null case; in particular the collinear case deviates from the Galilean difference by the relativistic denominator , and the transverse case exhibits the factor in the perpendicular component.
Depends on
Dependency tree · 2 levels
Sources
- B. Crowell, Special Relativity, revision 2020-12-10 (author-published undergraduate textbook, 246 PDF pages): Sections 1.1-1.3 pp. 12-28 (vector representation of observer motion, operational radar calibration, time dilation, length-contraction road-trip example), Sections 3.5 and 3.7 pp. 60-68 (four-velocity, acceleration, projection operator), Section 3.9.3 pp. 73-74 (local failure of accelerated simultaneity), Sections 7.1-7.3 pp. 147-151 (Rindler coordinates and nonuniform proper acceleration), Section 8.1 pp. 165-169 (rotating synchronization), Section 9.5 pp. 205-211 (congruences, expansion, Born rigidity); signature (+---) converted to (-+++) and c = 1 formulas converted to x^0 = c t
- H. S. Reall, Mathematical Tripos Part III General Relativity (Cambridge, October 12, 2022 revision): Sections 2.2-2.3 pp. 27-30 (Minkowski metric, causal classification, timelike proper time, observer measurements in an inertial chart, radar coordinates); Internet Archive copy of the original https://www.damtp.cam.ac.uk/user/hsr1000/part3_gr_lectures.pdf