mass energy

The equation explained

Pulse 1=12L γ (1−βcos⁡φ),Pulse 2=12L γ (1+βcos⁡φ)\begin{gathered}\text{Pulse 1} = \frac{1}{2}L\,\gamma\,(1 - \beta\cos\varphi), \\ \text{Pulse 2} = \frac{1}{2}L\,\gamma\,(1 + \beta\cos\varphi)\end{gathered}
In wordsEach pulse carries half of the energy the body gives off at rest, multiplied by the factor and by one less or one plus the speed ratio times the cosine of the angle the light leaves at.OverviewThe two pulses as the moving observer measures them: the one sent forward and the one sent back, each half the rest-frame energy with the same factor and opposite angle terms.Full explanationThe body gives off two equal pulses in opposite directions, each of energy 12L\frac{1}{2}L as measured where the body rests. The moving observer measures each one changed by the factor the display at the top of the page gives, and the two angles differ by a half turn, so where the first carries 1−βcos⁡φ1 - \beta\cos\varphi the second carries 1+βcos⁡φ1 + \beta\cos\varphi. Neither pulse alone has a simple energy in this frame: the forward one is diminished and the backward one increased, or the reverse, depending on which way the observer moves. What matters for the argument is that the two angle terms are equal and opposite, which the next display uses.Every step12L,12L\frac{1}{2}L, \qquad \frac{1}{2}LThe two pulses as measured where the body rests: equal, and opposite in direction, so that the body does not begin to move.12L γ (1−βcos⁡φ)\frac{1}{2}L\,\gamma\,(1 - \beta\cos\varphi)The first pulse as the moving observer measures it, by the transformation of light energy at the top of the page, with φ\varphi the angle between the light and the observer's motion.12L γ (1+βcos⁡φ)\frac{1}{2}L\,\gamma\,(1 + \beta\cos\varphi)The second pulse goes the opposite way, half a turn from the first, so the cosine of its angle is the negative of the first one's. Nothing else about it differs.Historian's marginSplitting the emission into two named pulses is this edition's way of setting out the step; the paper writes the two terms inside one bracket and never names them separately. Two pulses rather than one is Einstein's own condition and not a simplification: a body that gave off a single pulse would recoil, and the energy it then carried away in motion would have to be accounted for. The pair makes the body's own motion unchanged, which is what lets the argument compare only energies.Also

Open the laboratory