Time derivative of relativistic momentum help

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SUMMARY

The discussion focuses on calculating the time derivative of relativistic momentum, specifically the expression ϒmv. The correct application of the product rule yields the derivative as 𝑝̇ = 𝛾m𝑎 + 𝛾³m(v𝑎/c²)𝑣, where 𝛾 is the Lorentz factor, m is mass, and v is velocity. A common error identified was the misplacement of a negative sign in the derivative calculation, which was clarified through the use of the chain rule. The final expression accurately reflects the dynamics of relativistic momentum under conditions of mass conservation.

PREREQUISITES
  • Understanding of relativistic physics concepts, particularly momentum.
  • Familiarity with the Lorentz factor (𝛾) and its implications in relativistic equations.
  • Knowledge of calculus, specifically the product and chain rules for differentiation.
  • Basic understanding of kinematics, including acceleration (a) and velocity (v).
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Students and professionals in physics, particularly those studying relativistic mechanics, as well as educators seeking to clarify concepts related to momentum and differentiation in a relativistic context.

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?
 
Last edited:
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.
 
Last edited:
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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