Ideal conductor and charge movement

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Discussion Overview

The discussion centers around the movement of charge in an ideal conductor, particularly addressing the conditions under which current flows and the implications of Maxwell's equations. Participants explore the relationship between electric fields and current density, as well as the assumptions made in the literature regarding ideal conductors.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions why charge moves in an ideal conductor, noting that if the electric field is zero, then according to Ohm's law, the current density should also be zero.
  • Another participant clarifies that the electric field being zero applies only in the electrostatic case and that a non-zero field exists when current is flowing.
  • A participant emphasizes that the assumption of zero electric field in ideal conductors is not universally applicable and requests references to support this claim.
  • Further clarification is provided that in electrodynamics, an ideal conductor can have a zero electric field under specific conditions, but this leads to implications of infinite current, which raises physical concerns.
  • One participant draws an analogy between the movement of electrons in a conductor and gas molecules, discussing the role of temperature and probability in charge movement, while also referencing historical figures like Max Planck and Boltzmann.

Areas of Agreement / Disagreement

Participants express disagreement regarding the conditions under which the electric field is zero in ideal conductors, with some asserting that it only applies in electrostatics, while others challenge this view. The discussion remains unresolved with multiple competing perspectives on the topic.

Contextual Notes

Participants highlight limitations in understanding the behavior of ideal conductors, particularly regarding the assumptions made in literature and the implications of infinite conductivity. There are also references to the complexities of superconductivity and its relation to Ohm's law.

Paul20
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Hi

This question really matters me and I would like to someone to point me out (rigorously if possible) why and what makes charge move in ideal conductor.
All good conductors are modeled as being ideal so that the Maxwell equations inside the conductor needs not to be solved. So as electric field is zero in the conductor and that the tangential component of electric field on the surface needs to be zero why does current really flow? According to Ohm's law J the current density is proportional to the electrif field which is zero this implies that current density is zero and there is no charge movement as far as I know?

So what is the flaw I am my reasoning?

Thanks!
 
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Paul20 said:
So as electric field is zero in the conductor...
That's only true in the electrostatic case. If there's current flowing, there's a non-zero field within the conductor.
 
Hi and thanks for your reply

I still don't get it...What I have understood is that it is the electric field which gets the charge moving. And everywhere in literature when they are speaking of ideal conductors it is always assumed that the electric field inside the conductor is zero.

Can you point more specificly from the Maxwell's equation what you mean?
 
Paul20 said:
What I have understood is that it is the electric field which gets the charge moving.
True.
And everywhere in literature when they are speaking of ideal conductors it is always assumed that the electric field inside the conductor is zero.
Not true. That's only true in the electrostatic case (no moving charges). If you think you've read otherwise, provide a reference.
 
Doc Al said:
Not true. That's only true in the electrostatic case (no moving charges). If you think you've read otherwise, provide a reference.

One comment: There *is* one case in electrodymanics where the electric field inside the conductor is zero, and that it for the case of an ideal conductor; ideal in the meaning of infinite conductivity.

In that case Ohm's law would imply infinite current for anything else than zero field in the conductor, which would be intolerant from a physical point of view. Hence, once you have gotten a current going in an infinitely conducting wire, no futher electromotive force is needed to sustain the current.

The example is of course rather artificial, save for superconductors, but I'm not sure the obey Ohm's law in the first place, and my course in quantum electronics and supercoductivity is scheduled a year from now :)
 
Last edited:
Why current flows in a conductor

Paul20 said:
Hi

This question really matters me and I would like to someone to point me out (rigorously if possible) why and what makes charge move in ideal conductor.
All good conductors are modeled as being ideal so that the Maxwell equations inside the conductor needs not to be solved. So as electric field is zero in the conductor and that the tangential component of electric field on the surface needs to be zero why does current really flow? According to Ohm's law J the current density is proportional to the electrif field which is zero this implies that current density is zero and there is no charge movement as far as I know?

So what is the flaw I am my reasoning?

Thanks!

The movement of electric charges (electrons) in a conductor is similar to the movements of gas molecules. This assertion was made by Professor Max Planck over 100 years ago. The molecular movements is related to temperature and probability. The movement of molecules was defined by Boltzmann a few decades earlier. At a given temperature, various states of equilibrium exist within the material. The number of states and the degrees of movement are related by probability theory. Planck noted the similarity to atomic states and derived his famous Blackbody Radiation equation, partly on the basis of Boltzmann's probability calculations. These energy state equation shows that the energy level is proportional to kT. Similarly, the electron mobility of a conductor is inversely proportional to the square root of kT (proportional to an inherent actuating voltage). The electrons move in various directions, sideways, forwards and backwards, so there is no net movement to speak of in any direction (only low-level noise spikes). These moving electrons are sometimes referred to as "free electrons", although there has been some confusion, in the past, of the concept of a free electron.
 

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