Charge distribution in a conductor (using maxwell's equations)

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SUMMARY

The discussion focuses on the time-dependent behavior of charge distribution in a conductor characterized by conductivity σ and relative permittivity κ. It establishes that the charge density ρ decays over time according to the equation ρ = ρ0exp(−t/ζ), where ζ = κǫ0/σ. Participants explore the application of Maxwell's equations, particularly the divergence of electric displacement D and current density Jfree, to derive this relationship. The conversation emphasizes the importance of substituting variables correctly to arrive at the exponential decay of charge density.

PREREQUISITES
  • Understanding of Maxwell's equations
  • Familiarity with Ohm's Law (J = σE)
  • Knowledge of electric displacement field (D) and its relation to electric field (E)
  • Basic concepts of ordinary differential equations
NEXT STEPS
  • Study the derivation of the continuity equation for free charge density
  • Learn about the relationship between electric displacement field (D) and electric field (E)
  • Explore the implications of charge distribution decay in conductors using differential equations
  • Investigate the role of bound currents in conductors and their relation to free charge density
USEFUL FOR

Students and professionals in electrical engineering, physicists studying electromagnetism, and anyone interested in the dynamics of charge distribution in conductive materials.

sweep123
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Homework Statement


Show that any charge distribution in a conductor of conductivity σ and relative
permittivity κ vanishes in time as ρ = ρ0exp(−t/ζ) where ζ = κǫ0
σ


Homework Equations


Maxwell's equation
∇ · D = ρfree

equation of continuity for a free charge density
∇ · Jfree = −∂(ρfree)/∂t


ohms law
J = σE



The Attempt at a Solution



I can see that ρ will get smaller and smaller as time 't' increases according to
ρ = ρ0exp(−t/ζ) and clearly some sort of substitution is required of the equations but I can't see how substitution will result in a exponential appearing. Basically I don't know where to start so any help would be appreciated or a push in the right direction.

Thanks
 
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Try expressing J in terms of D then combine your two maxwell's equation into a single DE for \rho
 
I could sub the first eq into the second to get the divergence of current density equals the negative differential of the divergence of the electric displacement field, or

∇ · Jfree = −∂(∇ · D)/∂t

Can Jfree and total J be considered to be the same thing in this example? Also I will lose ρ if i do this.
 
Is there ever any bound current in a conductor? If not, then Jfree and J are the same right?

And you don't want to combine the equations in that manner...start with expressing D in terms of E... there should be an equation for that
 
Okay so Jfree=J. also D=εE so E=D/ε
and therefore J=σD/ε

edit:
so

∇ · σD/ε = −∂(ρfree)/∂t
or
(∇σ/ε)· D + (σ/ε)(ρfree) = −∂(ρfree)/∂t

Doesn't feel like I am getting anyhere
 
Last edited:
Not sure if your allowed to bump threads on this forum...o:)
 
sweep123 said:
∇ · σD/ε = −∂(ρfree)/∂t
or
(∇σ/ε)· D + (σ/ε)(ρfree) = −∂(ρfree)/∂t

Doesn't feel like I am getting anyhere

σ/ε is a constant, so (∇σ/ε)=0 and therefor (σ/ε)(ρfree) = −∂(ρfree)/∂t

Also, is ρfree a function of any other variables besides time, inside a conductor?...if not, then−∂(ρfree)/∂t=−d(ρfree)/dt and you have a seperable ordinary differential equation for ρfree.
 
aha. I get it, Thanks a lot that's brilliant. Don't think I would have ever got that on my own:smile:
 

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