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If we begin with the equation for time dilation:

$$ \Delta t^\prime = \frac{\Delta t}{\sqrt{1-\frac{v^2}{c^2}}} $$

Now, for a particle moving in space with no potential energy,

$$ E = \frac{1}{2} mv^2 $$

So

$$ v^2 = \frac{2E}{m} $$

Then

$$ \Delta t^\prime = \frac{\Delta t}{\sqrt{1-\frac{2E}{mc^2}}} $$

$$ = \frac{\Delta t}{\sqrt{1-2}} $$

$$ = \frac{\Delta t}{\sqrt{-1}} $$

Explain please?

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    $\begingroup$ This $E = \frac{1}{2}mv^2$ is only correct in the limit of $v \ll c$ (the Newtonian or non-relativistic limit). The generally correct expression is $E = \sqrt{(mc^2)^2 + (pc)^2}$. It follows that rest of your work is also incorrect except in that limit. Never mix relativistically correct and Newtonian math. Unless you really know what you are doing, of course. $\endgroup$ Commented Aug 5, 2013 at 2:52
  • $\begingroup$ @dmckee that could probably be an answer $\endgroup$
    – David Z
    Commented Aug 5, 2013 at 2:55
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    $\begingroup$ After enough comment edits I'll even get the units right. ::sigh:: That's why particle physicists work in $c = 1$ units: because we're too dumb to handle SI units. $\endgroup$ Commented Aug 5, 2013 at 2:56

2 Answers 2

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This $E = \frac{1}{2}mv^2$ is only correct in the limit of $v \ll c$ (the Newtonian or non-relativistic limit). The generally correct expression is $$E = \sqrt{(mc^2)^2 + (pc)^2}\,.$$ It follows that rest of your work is also incorrect.


Never mix relativistically correct and Newtonian math. Unless you really know what you are doing, of course.

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Generally, $E = \gamma mc^2$ which becomes $E = \frac 1 2 mv^2 + mc^2$ for $v$ << $c$.

You've gone wrong by equating $E$ to just kinetic energy, and then using $E$ equal to just the rest energy $mc^2$.

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  • $\begingroup$ You could taylor expand if you want to not use the slow-motion approximation, (contd $\endgroup$ Commented Aug 5, 2013 at 12:23

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