Need help with Special Relativity: Force and Energy

unam1292
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Homework Statement



I'm trying to show that

\frac{dE}{dT}= F x V where F is force and V is velocity

Can someone please help me out?


Homework Equations



F=\frac{dP}{dT}=M x V x \gamma


All of the other equations from special relativity (contraction, dilation, energy) are probably important as well.

The Attempt at a Solution



Honestly, I have no idea where to start. Can someone please point me in the right direction. I'm a high school junior and I have very little experience with relativity. I understand that I should show some work, but I truly don't have any but I have been trying for a while.

Please help me get started!
 
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You should know the formula for the relativistic energy E of an object. Try differentiating that with respect to time and see what you get.
 
The formulas for relativistic energy don't involve time (t) as far as I can tell.
I'm not sure how taking the derivative of that would help unless I'm
overlooking something.
 
It doesn't depend explicitly on time, but the energy depends on \gamma, which, in turn, depends on velocity, which does change with time.
 
gosh, now I'm even more stuck, thanks anyway.

so you meant that I should use \frac{x}{t} instead of v?

well after doing that, and taking the derivative, I can see no way for it to manipulate in F x V.
 
No, I think that'll make it more complicated. Keep it in terms of just the velocity v.

Start with this first. You know that

\gamma = \frac{1}{\sqrt{1-(v/c)^2}}

What do you get if you differentiate it with respect to time, remembering that v is a function of time?
 
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ok, this is what I have

\frac{dE}{dt}=mc^{2}\frac{-\gamma^{3}v}{c^{2}}\frac{dv}{dt}= F x V

am I doing this correctly? when equate the equation above with F x V (where F = gamma*mass*acceleration*v)
i get that -\gamma^{3}=\gamma so I get the feeling I messed up somewhere...

I really appreciate your help!
 
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Hmm, not sure how you came up with that. Can you show more steps?
 
Sure,

So here's the derivative of gamma
\dot {\gamma} = \frac{d}{dt} \left( 1- \frac{v^2}{c^2} \right) ^{-1/2} = \left( \frac{-1}{2} \right) \left( \frac{-2v \dot {v} }{c^2} \right) \left( 1- \frac{v^2}{c^2} \right) ^{-3/2} = \gamma ^3 \left( \frac{v \dot {v}}{c^2} \right)

hence
\frac{dE}{dt}=mc^{2}\frac{-\gamma^{3}v}{c^{2}}\frac{dv}{dt}

because E = mc^{2}\gamma.

F\bulletV=m\gamma\frac{dv}{dt}v = \frac{dE}{dt}=mc^{2}\frac{\gamma^{3}v}{c^{2}}\frac{dv}{dt}

and then I simplified this
 
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  • #10
You're getting there. You need to be a bit more careful when calculating F. You know that the momentum is given by p=\gamma mv. When you differentiate it, you need to use the product rule.
 
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