Confusion on Continuity of Current and Free Charge in Conductor

Click For Summary

Discussion Overview

The discussion revolves around the continuity of current and free charge in conductors, particularly in the context of Maxwell's equations. Participants explore the implications of these equations for charge distribution and current behavior in conductive materials, addressing both static and dynamic scenarios.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a derivation based on Maxwell's equations that suggests a specific behavior of free charge in a conductor, leading to an exponential decay of free charge over time.
  • Another participant argues that the derivation conflates the behavior of conductors with that of dielectrics, stating that the dielectric displacement is not applicable in conductors.
  • Some participants assert that the equations correctly describe the movement of charges to the surface of a conductor, resulting in zero current and electric field in the interior at equilibrium.
  • There is a question about whether electric fields and currents can exist inside a conductor under time-dependent conditions, with references to eddy currents and the skin effect.
  • It is noted that while free charge may disappear inside a conductor, an electric field can still be present due to surface charge distributions, particularly when a battery is involved.
  • Participants discuss the behavior of current in relation to frequency, indicating that at higher frequencies, current tends to flow near the surface of the conductor.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of certain equations to conductors versus dielectrics, and whether the derived implications about free charge are valid. The discussion remains unresolved with multiple competing perspectives on the behavior of current and charge in conductors.

Contextual Notes

The discussion highlights limitations in the assumptions made regarding the behavior of free charge and current in conductors, particularly in relation to static versus dynamic conditions and the role of surface charge distributions.

wzy75
Messages
7
Reaction score
0
I know there must be something wrong with the following derivation based on Maxwell's equations but could not figure out what is wrong. The derivation deals with continuity of current and free charge in a conductor in general.

Continuity of current says that,

\nabla\cdot \textbf{J}=-\frac{\partial \rho_v}{\partial t}. (1)

However, for currents in conductor, the current density and the electric field is related as

\textbf{J}=\sigma\textbf{E}.

Using the relation between \textbf{E} and \textbf{D} ,

\textbf{E}=\textbf{D}/\epsilon,

we have

\nabla\cdot \textbf{J}=\sigma\nabla\cdot\textbf{E}=\frac{\sigma}{\epsilon} \nabla\cdot\textbf{D}=\frac{\sigma}{\epsilon}\rho_v. (2)

Comparing (1) and (2) gives an equation on free charge \rho_v,

-\frac{\partial \rho_v}{\partial t}=\frac{\sigma}{\epsilon} \rho_v

which means that

\rho_v=\rho_{v0}e^{-\frac{\sigma}{\epsilon}t}. (3)

Since we are talking about general cases of Maxwell's equations, (3) looks like an unreal restriction on free charge in a conductor and does not make sense at all.

What went wrong in the above derivations? Thanks in advance!
 
Last edited:
Physics news on Phys.org
Would really appreciate it if someone can help me out. Thanks a lot!
 
Hi,
You are mixing up equations describing conductors and dielectrics. The dielectric displacement makes no sense in a conductor.
 
The equations are correct. It describes the disappearance of charges inside a conductor. In the long-time limit you approach a stationary solution (electrostatics). In this situation there cannot be free charges inside a conductor, but those all move to its surface, leading to a distribution such that the interior of the conductor has 0 current and 0 electric field.
 
Thank you so much vanhees71 for the clarification!

Is it true that in the most general case, even if the unpaired free charge will disappear inside a conductor, there still might be electric field \textbf{E} and current (e.g. eddy currents induced by changing magnetic fields)?
 
For time-dependent fields/sources, there can be a field/current inside the conductor. However, also here the current flows more close to the surface. This is known as the skin effect, which is due to eddy currents due to induced electric fields from the time-varying magnetic field in the interior of the conductor counteracting the current due to the driving field:

http://en.wikipedia.org/wiki/Skin_effect
 
Is it true that in the most general case, even if the unpaired free charge will disappear inside a conductor, there still might be electric field E and current (e.g. eddy currents induced by changing magnetic fields)?

The electric field in metal is non-zero whenever the current flows through it - Ohm's law states that the current is proportional to the electric field. In the case the current is due to a battery, the electric field is due to charge distribution on the surface of the conductor and battery - this need not vanish.

If the current does not vary too fast, it flows roughly uniformly through the whole cross-section of the conductor, not just on the surface. As the frequency of the alternating current is increased, the distribution of current moves to the surface of the conductor.
 

Similar threads

Replies
5
Views
2K
  • · Replies 19 ·
Replies
19
Views
3K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 5 ·
Replies
5
Views
995
  • · Replies 1 ·
Replies
1
Views
973
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 10 ·
Replies
10
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K