special relativity

The equation explained

x′V−v=t.\frac{x'}{V-v} = t .
In wordsThe distance along the motion divided by the velocity of light less the speed of the moving system is the stationary time.OverviewWhere the same ray has got to, told in the stationary system. It gains on the moving origin at the difference of the two speeds, so the time it has taken is the distance divided by that difference.Full explanationThe previous display left a stationary time and a stationary distance both standing in the expression for ξ\xi. This removes one of them. In the stationary system the ray travels at VV and the origin of kk travels at vv in the same direction, so the ray draws away from that origin at V−vV - v. The distance it has drawn away, measured in the stationary system, is what the paper calls x′x'. The two together give the elapsed stationary time. The step uses the stationary system's own measurements only, where VV was assumed at the outset; the moving system's claim about the same ray was used in the previous display, and the two claims are what the section is holding together.Every stepgap=(V−v)×stationary time\text{gap} = (V - v) \times \text{stationary time}The ray goes at VV and the origin of kk at vv, both measured in the stationary system, so the gap between them opens at V−vV - v.x′=(V−v)tx' = (V - v) tThat gap is the distance from kk's origin measured in the stationary system, which is x′x'; the ray and the origin were together at t=0t = 0.x′V−v=t\frac{x'}{V - v} = tDivide by V−vV - v, which is the line as printed.Historian's marginThe closing speed V−vV - v is a difference of two speeds in one system, not a velocity of light for anyone: no observer here measures light at V−vV - v, and the paper's own § 2 used the same difference for the rod (p. 896). Reading it as a slower light is the mistake the section exists to avert.Also

Read it in the paper