Electromagnetic linear momentum for a system of two moving charges

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The discussion revolves around the challenge of expressing the sum of forces between two moving charges as a total time derivative of electromagnetic momentum. The participant acknowledges that while the forces can be derived from the Lienard-Wiechert potentials, the complexity of the forces complicates the derivation of the desired expression. They explore the possibility of integrating the momentum density from the electric and magnetic fields generated by the charges but admit to difficulties with retarded functions. An important realization is made regarding electromagnetic radiation, which indicates that conservation of linear momentum and electromagnetic momentum is not upheld when charges are accelerated, contradicting earlier assumptions. This highlights the intricate relationship between electromagnetic phenomena and conservation laws.
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Homework Statement
I want to obtain the "total" EM linear momentum for a system of two moving charges
Relevant Equations
Lienard-Wiechert potentials, Lorentz force law
When you write out the equations of motion for a system of two isolated charges, you can add both of the equations and get the increase in the particles linear momentum on one side. On the other side, you get the sum of all the forces between the particles. I understand that this sum of forces could be written as the negative time derivative of the system's total electromagnetic momentum. But since the forces are quite complicated, I just can't seem to deduce the expression of this EM momentum

I guess that you could write the ##\mathbf{E}## and ##\mathbf{B}## fields due to both charges and integrate the momentum density ##\mathbf{D}\times\mathbf{B}## over all space to get the desired momentum, but I'm not too skilled with the integration of retarded functions. I have also tried to write the forces without deriving the potentials explicitly,
since
$$\mathbf{F}_{12} = -q_2\nabla_2V_{12} -q_2\partial_t(V_{12} \mathbf{v}_1/c^2) + q_2\mathbf{v}_2 \times \nabla_2 \times(V_{12} \mathbf{v}_1/c^2)$$
and
$$\mathbf{F}_{21} = -q_1\nabla_1V_{21} -q_1\partial_t(V_{21} \mathbf{v}_2/c^2) + q_1\mathbf{v}_1 \times \nabla_1\times(V_{21} \mathbf{v}_2/c^2)$$
but that doesn't seem to give an inspiring result

tl;dr I'm trying to write the sum of ##\mathbf{F}_{12}+\mathbf{F}_{21}## as a total time derivative. ##V_{12}## and ##V_{21}## refer to the Lienard-Wiechert potential
 
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I just realized that electromagnetic radiation contradicts my statement. As soon as the charges get accelerated, then the sum of linear momentum plus electromagnetic momentum is not conserved anymore because the momentum flux is non-zero at infinity. My initial approach doesn't make sense due to radiation phenomena This means that the Griffiths book chapter on conservation laws gets contradicted by the chapter on radiation.
 
At first, I derived that: $$\nabla \frac 1{\mu}=-\frac 1{{\mu}^3}\left((1-\beta^2)+\frac{\dot{\vec\beta}\cdot\vec R}c\right)\vec R$$ (dot means differentiation with respect to ##t'##). I assume this result is true because it gives valid result for magnetic field. To find electric field one should also derive partial derivative of ##\vec A## with respect to ##t##. I've used chain rule, substituted ##\vec A## and used derivative of product formula. $$\frac {\partial \vec A}{\partial t}=\frac...