Differentiating the relativistic charge wrt velocity

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SUMMARY

The discussion focuses on differentiating the relativistic charge \( Q' \) with respect to velocity \( v \) in the context of electromagnetic theory. The key equation derived is \( \frac{dQ'}{dv} = \frac{1}{c^{2}} \int d^{3}x \bigg[ x \big( \frac{\partial \rho}{\partial t} - \frac{v}{c^{2}} \frac{\partial j^{x}}{\partial t} \big) - j^{x} \bigg] \bigg|_{t = \frac{vx}{c^{2}}, x, y, z} \). The discussion emphasizes the application of the chain rule and product rule in differentiation, particularly for the terms involving charge density \( \rho \) and current density \( j^{x} \). Participants provided hints on utilizing these calculus techniques to solve the problem effectively.

PREREQUISITES
  • Understanding of relativistic charge concepts
  • Familiarity with electromagnetic theory
  • Proficiency in calculus, specifically differentiation techniques
  • Knowledge of the chain rule and product rule in calculus
NEXT STEPS
  • Study the application of the chain rule in physics problems
  • Review the principles of electromagnetic charge density and current density
  • Explore advanced topics in relativistic electrodynamics
  • Learn about the implications of \( c^{2} \) in relativistic equations
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Students and researchers in physics, particularly those focusing on electromagnetism and relativistic dynamics, will benefit from this discussion. It is also valuable for anyone looking to deepen their understanding of calculus applications in physical theories.

spaghetti3451
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Homework Statement



Given that ##Q' = \int d^{3}x \bigg[ \rho \big( \frac{vx}{c^{2}},x,y,z \big) - \frac{v}{c^{2}} j^{x} \big( \frac{vx}{c^{2}},x,y,z \big) \bigg]##, show the following:

##\frac{dQ'}{dv} = \frac{1}{c^{2}} \int d^{3}x \bigg[ x \big( \frac{\partial \rho}{\partial t} - \frac{v}{c^{2}} \frac{\partial j^{x}}{\partial t} \big) - j^{x} \bigg] \bigg|_{t = \frac{vx}{c^{2}}, x, y, z}##

Homework Equations



3. The Attempt at a Solution [/B]

I understand that the second term can be easily obtained by differentiating ##- \frac{v}{c^{2}} j^{x}## with respect to ##v##. However, I am having trouble differentiating the first term with respect to ##v##.

In essence, I need to show that ##\frac{\partial \rho}{\partial v} = \frac{1}{c^{2}} x \bigg( \frac{\partial \rho}{\partial t} - \frac{v}{c^{2}} \frac{\partial j^{x}}{\partial t} \bigg)##.

Any hints?
 
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You have ##\frac{\partial }{\partial v}\left( p(t(v),x,y,z) - \frac {v}{c^2}j^x(t(v),x,y,z)\right) ##
Using the chain rule and product rule, you should be able to work this out.
##\frac{\partial }{\partial v} p(t(v),x,y,z) = \frac{\partial p }{\partial t}\frac{\partial t }{\partial v} ##
Then start with the product rule for the second part,
##\frac{\partial }{\partial v}\frac {v}{c^2} j^x(t(v),x,y,z)=\left( \frac{\partial }{\partial v}\frac {v}{c^2}\right)j^x+\frac {v}{c^2}\frac{\partial j^x}{\partial v} ##
Notice that you will need the chain rule one more time for that last derivative.
 
Thanks! Got it!
 

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