Is there a relativistic version of the work-energy theorem?

jaketodd
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The work-energy theorem is stated here on Wikipedia. On the same page it says "regardless of the choice of reference frame, the work energy theorem remains valid and the work done on the object is equal to the change in kinetic energy."

I am wondering if there is a relativistic version of the work-energy theorem.

Thanks,

Jake
 
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jaketodd said:
I am wondering if there is a relativistic version of the work-energy theorem.

No. The classical version applies to relativity too. But the result is different.
 
W=\Delta E_k=(\gamma -1)mc^2

Just integrate force over some distance, starting from rest:

W=\int Fdx=\int \frac{dp~dx}{dt}=\int vdp=vp-\int pdv=\gamma mv^2-\int \gamma mvdv

What you end up with is:

W=\gamma mc^2+C

with some constant of integration C. If you set v=0, you take W=0 and γ=1, therefore C=-mc2. So what you get is:

W=\gamma mc^2-mc^2=(\gamma -1)mc^2=E_k
 
In general, W=\int F dx, but the Lorentz transformations tell you the relationship between dx in the two different inertial frames as dx = {{dx'}\over{\sqrt{1-{{v^2}\over{c^2}}}}}.
 
Pengwuino said:
In general, W=\int F dx, but the Lorentz transformations tell you the relationship between dx in the two different inertial frames as dx = {{dx'}\over{\sqrt{1-{{v^2}\over{c^2}}}}}.

Two different inertial frames?
 
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