Confusion regarding continuity equation in electrodynamics

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SUMMARY

The continuity equation in electrodynamics can be applied to a system of two charged particles with distinct charge densities ρ1(r,t) and ρ2(r,t), each having their own velocity fields V1(r,t) and V2(r,t). While the charge densities can be summed to obtain a local charge density, the velocities cannot be combined directly due to their dependence on individual charge distributions. Instead, a charge-weighted velocity must be defined to accurately represent the system. The charge flux density vector, which is the product of charge density and velocity, can be superimposed, allowing for the continuity equation to hold true in this context.

PREREQUISITES
  • Understanding of the continuity equation in electrodynamics
  • Familiarity with charge density and velocity fields
  • Knowledge of charge flux density vector concepts
  • Basic principles of superposition in physics
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  • Study the derivation and applications of the continuity equation in electrodynamics
  • Learn about charge-weighted velocity definitions and their implications
  • Explore the mathematical formulation of charge flux density vectors
  • Investigate the superposition principle in the context of electromagnetic theory
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Physicists, electrical engineers, and students studying electrodynamics who seek to deepen their understanding of the continuity equation and its application to systems with multiple charge distributions.

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Suppose I have two charged particles with charge densities ρ1(r,t) and ρ2 (r,t) with corresponding velocity fields V1(r,t) and V2(r,t). Can I write continuity equation for the combined system? Wouldn't charges moving with different velocities would contribute differently to the current which will violate the continuity equation?
 
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The continuity equation is linear in the charge density-- that means the sum of any two solutions is also a solution.
 
Perhaps the key point to stress is that if two different charge distributions are associated with two different velocity distributions, you can add the charge densities to get the local charge density, but you don't add the velocities-- there is no local velocity, you'd have to define a charge-weighted velocity to be able to use it like an independent local quantity in the continuity equation. You can think in terms of the charge flux density vector, which is the product of the charge density and the velocity, and then that quantity can be superimposed if you have two separate solutions, but the velocities of the two separate components cannot be meaningfully added the way the charge densities can.
 

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