Time derivative of relativistic momentum help

AI Thread Summary
The discussion focuses on taking the time derivative of relativistic momentum, specifically the expression ϒmv. Participants initially struggle with separating gamma and mv, leading to confusion over the correct application of the product rule. The correct time derivative is clarified as involving terms for gamma, mass, and acceleration, with a crucial correction made regarding a dropped negative sign. The chain rule is emphasized for differentiating terms involving velocity, with the constant nature of c and c² noted. Overall, the conversation highlights the complexities of relativistic momentum derivatives and the importance of careful mathematical handling.
diewlasing
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How does one take the time derivative of ϒmv ?

I tried treating gamma and mv as separate functions but it just gets messy and ultimately wrong.
 
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diewlasing said:
How does one take the time derivative of ϒmv ?

I tried treating gamma and mv as separate functions but it just gets messy and ultimately wrong.

Well, the product rule simply gives:
\dot {\vec{p}} = \dot {\gamma} m \vec{v} + \gamma \dot {m} \vec{v} + \gamma m \dot {\vec{v}}

For systems that conserve mass, \dot m =0. While,
\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)

And so,

\dot {\vec{p}} = \gamma m \dot {\vec{v}} -\gamma ^3 m \left( \frac{v \dot {v}}{c^2} \right) \vec{v} =\gamma m {\vec{a}} -\gamma ^3 m \left( \frac{v a}{c^2} \right) \vec{v}
 
Why is \left( \frac{2v \dot {v} }{c^2} \right) not \left( \frac{-2v \dot {v} }{c^2} \right)? What happened to the minus sign?
 
snoopies622 said:
Why is \left( \frac{2v \dot {v} }{c^2} \right) not \left( \frac{-2v \dot {v} }{c^2} \right)? What happened to the minus sign?

OOps,. my bad:redface:. Yes I accidentally dropped a negative sign. The correct answer should be
\dot {\vec{p}} = \gamma m \dot {\vec{v}} +\gamma ^3 m \left( \frac{v \dot {v}}{c^2} \right) \vec{v} =\gamma m {\vec{a}} +\gamma ^3 m \left( \frac{v a}{c^2} \right) \vec{v}
 
Ah yes, thank you
 
i can't get (−2*v*v/c^2). what rule do we use on this? can anybody show a more detail step on this part?
 
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sgwayne said:
i can't get (−2*v*v/c^2). what rule do we use on this? can anybody show a more detail step on this part?

Chain rule. Since v is a function of t, the time derivative of 1-v^2/c^2 is -2v(dv/dt)/c^2.

https://www.physicsforums.com/showthread.php?t=343032
I posted a similar question a year after this one if you want a second angle.
 
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thanks master newbie, i was confused on the c^2 actually. so we just leave it as it is bcoz we want the derivative of v not c. correct me if I'm wrong.
 
It is left there because c (and c^2) is a constant.
 
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