From: Francis Russell Date: Tue, 29 Nov 2011 12:33:57 +0000 (+0000) Subject: Remove unnecessary overlines on a few square roots. X-Git-Url: https://git.unchartedbackwaters.co.uk/w/?a=commitdiff_plain;h=8cc6e9ef91c36133cbc00e725240abe4792c8907;p=francis%2Frelativity.git Remove unnecessary overlines on a few square roots. --- diff --git a/relat10.tex b/relat10.tex index 43ba937..ad8b591 100644 --- a/relat10.tex +++ b/relat10.tex @@ -1165,8 +1165,8 @@ of the first equation of the Lorentz transformation the values of these two points at the time $t = 0$ can be shown to be \begin{eqnarray*} -x_{\mbox{(begining of rod)}} &=& 0 \overline{\sqrt{I-\frac{v^2}{c^2}}} \\ -x_{\mbox{(end of rod)}} &=& 1 \overline{\sqrt{I-\frac{v^2}{c^2}}} +x_{\mbox{(begining of rod)}} &=& 0 \sqrt{I-\frac{v^2}{c^2}} \\ +x_{\mbox{(end of rod)}} &=& 1 \sqrt{I-\frac{v^2}{c^2}} \end{eqnarray*} ~ @@ -1621,7 +1621,7 @@ experiences a contraction in the direction of motion in consequence of that motion. the contracted length being proportional to the expression -$$\overline{\sqrt{I-\frac{v^2}{c^2}}}.$$ +$$\sqrt{I-\frac{v^2}{c^2}}.$$ This, hypothesis, which is not justifiable by any electrodynamical facts, supplies us then with that particular law of motion which has