A bunch of L.T.'s
Using the results from the "Passing trains" examples in Sections 11.5.1 and 11.6, the relative speeds and the associated γ factors for the six pairs of frames are
AB AC AD BC BD CD
v 5c/13 4c/5 c/5 3c/5 c/5 5c/7γ 13/12 5/3 5/2 5/4 5/27/2
From the example in Section 11.6, the separations between the two events in the four frames are
A B C D
Δx −L L 5L 0
Δt 5L/c 5L/c 7L/c 26L/c
The Lorentz transformations are
Δx = γ(Δx' + vΔt'), (11.84)
Δt = γ(Δt' + vΔx'/c²).
For each of the six pairs, we'll transform from the faster frame to the slower frame. This means that the coordinates of the faster frame will be on the right-hand side of the L.T.'s. The sign on the right-hand side of the L.T.'s will therefore always be a "+." In the AB case, for example, we'll write "Frames B and A," in that order, to signify that the B coordinates are on the left-hand side and the A coordinates are on the right-hand side. We'll simply list the L.T.'s for the six cases, and you can check that they do indeed all work out.
Frames B and A: L = 1213(-L + 135c · c5L),
c5L = 1213(c5L + 13c25c(−L)).
Frames C and A: 5L = 35(-L + 54c · c5L),
c7L = 35(c5L + 5c24c(−L)).
Frames D and A: 0 = 25(-L + 5c · c5L),
c26L = 25(c5L + 5c2c(−L)).
Frames C and B: 5L = 45(L + 53c · c5L), (11.85)
c7L = 45(c5L + 5c23cL).
11.13 Solutions 571
Frames B and D: L = 25(0 + 5c · c26L),
c5L = 25(c26L + 5c2c(0)).
Frames C and D: 5L = 27(0 + 75c · c26L),
c7L = 27(c26L + 7c25c(0)).