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Worked velocity transformation: collinear, transverse and null cases

Example

Let x and x′ be inertial charts related by a boost of parameter v=3c/5 along the first axis (γ=5/4, 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 w=(4c/5,0,0) in x has, by clause (iv) of Coordinate formulas of a boost: clock rates, rod lengths, simultaneity and velocity transformation, w1′=(4c/5−3c/5)/(1−(3/5)(4/5))=(c/5)/(13/25)=5c/13, so ∣w′∣=5c/13<c; the Galilean difference c/5 is not the transformed velocity.

(b) Transverse case. A worldline with w=(0,c/2,0) has w1′=(0−3c/5)/(1−0)=−3c/5 and w2′=(c/2)/((5/4)(1−0))=2c/5, hence ∣w′∣=9/25+4/25 c=(13/5)c<c.

(c) Null limit. For w=(c,0,0) the formula gives w1′=(c−3c/5)/(1−3/5)=c and ∣w′∣=c: a null worldline is null in every inertial chart.

In each case take the affine coordinate curve t↦(ct,wt) on R with the stated constant w; 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 x, x′ related by the boost of parameter v=3c/5 along the first axis with γ=5/4, and the three coordinate velocities w=(4c/5,0,0), w=(0,c/2,0), w=(c,0,0) (The passive Lorentz boost with parameter beta, Inertial frames and inertial charts of the affine Minkowski model).

[L1]

Clause (iv) of Coordinate formulas of a boost: clock rates, rod lengths, simultaneity and velocity transformation: for a C1 future causal curve with coordinate velocity w, ∣w∣≤c, in the chart x, the coordinate velocity in x′ is w1′=(w1−v)/(1−vw1/c2) and w⊥′=w⊥/(γ(1−vw1/c2)), with positive denominators, and ∣w′∣<c for ∣w∣<c, with ∣w′∣=c exactly when ∣w∣=c.

[L2]

The boost parameter is β=v/c=3/5 and γ=(1−β2)−1/2=5/4 (The passive Lorentz boost with parameter beta).

Verification

technique · direct
1.1L1L2algebra

Collinear case: with w1=4c/5, w⊥=0, v=3c/5, the denominator of [L1] is 1−35⋅45=1−1225=1325>0 and w1′=c/513/25=5c13; hence w′=(5c/13,0,0) and ∣w′∣=5c/13<c because 5/13<1. The Galilean difference for this passive change of frame is 4c/5−3c/5=c/5, which is not the transformed velocity.

1.2L1L2algebra

Transverse case: with w1=0, w⊥=(c/2,0), the denominator is 1 and [L1] gives w1′=(0−3c/5)/1=−3c/5 and w2′=(c/2)/(γ⋅1)=2c/5, so ∣w′∣2=(9/25+4/25)c2=13c2/25 and ∣w′∣=(13/5)c<c because 13<5.

1.3L1L2algebra

Null limit: with w1=c the denominator of [L1] is 1−3/5=2/5>0 and w1′=(c−3c/5)/(2/5)=(2c/5)/(2/5)=c, so w′=(c,0,0) and ∣w′∣=c; this is the equality case of the subluminality statement, consistent with ∣w∣=c.

2.1step 1.1step 1.2step 1.3∎

Conclusion: steps 1.1-1.3 evaluate the transformation formula of [L1] in the three configurations and confirm ∣w′∣<c for subluminal w and ∣w′∣=c in the null case; in particular the collinear case deviates from the Galilean difference by the relativistic denominator 1−vw1/c2, and the transverse case exhibits the factor 1/γ in the perpendicular component.

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