Conductor in an External Electric Field

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Discussion Overview

The discussion revolves around the behavior of a conductor placed in an external electric field, particularly focusing on the movement of free electrons within the conductor and the resulting electric field configuration. Participants explore theoretical implications, potential models, and the nuances of charge distribution in various scenarios.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that while free electrons rearrange to cancel the external electric field, not all electrons would move to the surface, as this could create an internal electric field that exceeds what is necessary for cancellation.
  • Others argue that a complete movement of all free electrons to the surface would lead to a substantial electric field inside the conductor, which contradicts the condition of zero electric field in a conductor.
  • A participant visualizes the electron movement as a fluid-like behavior, suggesting that electrons are nudged to the surface while maintaining a balance that prevents significant internal fields.
  • Another viewpoint suggests that only a sufficient number of free charges would move to the surface to neutralize the external field, with the remaining charges distributed to maintain a net zero field inside.
  • Some participants reference Gauss' law to support the idea that if all free electrons moved to the surface, the charge density would not be zero, contradicting the condition for a perfect conductor.
  • One participant highlights that the effectiveness of charge compensation depends on the density of free electrons and the strength of the external field, indicating that in some cases, it may not be possible to fully compensate the field.
  • Another participant provides a mathematical example involving a copper plate to illustrate the implications of charge density and the resulting electric field strength, suggesting that the scenario is more complex than a simple yes/no answer.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the movement of electrons and the resulting electric field configuration within the conductor. There is no consensus on whether all free electrons move to the surface or how charge distribution occurs under varying conditions.

Contextual Notes

Limitations include assumptions about the uniformity of charge distribution, the specific properties of different conductors, and the dependence on external field strength and electron density. The discussion does not resolve these complexities.

Drakkith
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I just had a test question in my E&M class that asked what would happen to a conductor when placed in an external electric field. One of the "correct" answers was that all of the free electrons would move to the surface of the conductor. I understand that the free electrons would rearrange themselves to cancel out the external field, but would all of the free electrons move to the surface? Wouldn't that build up an electric field inside the conductor?
 
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Drakkith said:
Wouldn't that build up an electric field inside the conductor?
Wouldn't that be just enough to counteract the external field's "penetration"?
 
jerromyjon said:
Wouldn't that be just enough to counteract the external field's "penetration"?

That's what I thought, but if ALL of the free electrons moved to the surface wouldn't that build up a substantial electric field inside the conductor that is much more than required to counteract the external field?
 
I just picture it like a fluid fluctuating over the surface bouncing every which way. Way inside is like opposite to counter the external magnetic field and electrons are nudged more strongly to the surface to blend in where they like to all balance each other and they tend to stay near the lines is more realistic I think.
 
Drakkith said:
I just had a test question in my E&M class that asked what would happen to a conductor when placed in an external electric field. One of the "correct" answers was that all of the free electrons would move to the surface of the conductor. I understand that the free electrons would rearrange themselves to cancel out the external field, but would all of the free electrons move to the surface? Wouldn't that build up an electric field inside the conductor?
Although the answer does appear to be wrong, an explanation for it does come to mind.
First the number of free charges required to neutralize the external field go to the surface ( electrons on one side and +ve charges on the other). Then the remaining free charges arrange themselves all over the surface ( not on just one side) such that the net field inside would still be zero ( there will of course be some neutralization of charges)
.
I don't know this surely, just seems like a plausible idea.
 
Aniruddha@94 said:
First the number of free charges required to neutralize the external field go to the surface ( electrons on one side and +ve charges on the other). Then the remaining free charges arrange themselves all over the surface ( not on just one side) such that the net field inside would still be zero ( there will of course be some neutralization of charges)

Why would the net field inside be zero if all of the negative charges are on the outside of the conductor and all of the positive charges are on the inside?
 
Drakkith said:
I understand that the free electrons would rearrange themselves to cancel out the external field, but would all of the free electrons move to the surface?
I believe not all the electrons will move to the surface. Once the surface electrons have canceled the external field, their movement will stop. So, number of electrons just enough to cancel the external electric field will move on the surface. If the conductor is a thin metal plate, -ve charges will be on one of its two surfaces. If the conductor is cylindrical and the external field is along its axis , rings of charge will form on it's surface.
 
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You can see that just some of the free electrons will come to the surface and not all of them from Gauss' law: [itex]\nabla E=\frac{\rho}{\epsilon}[/itex] . We know that electric field is zero in a perfect conductor, so the right hand side of that equation also has to be zero, hence, [itex]\rho = 0[/itex] . Now, if all of the free electrons moved to the surface, [itex]\rho[/itex] certaintly wouldn't be zero. The simplest way you can imagine that is very thin cylindrical metal stick in a homogenus electric field pointing down its axis. Let's say field points in x direction, and stick is also in x direction. Since it's very thin, it can be imagined from left to right as surface-inside-surface. So the outer field moves every free electron to the left, and that one from the right surface comes a little bit left (leaving the right surface negative), the next one travels the same distance (but he came near the stationary positive ion situated inside, and now you have electron and positive ion=neutral in the inside just as we said from Gauss' law) and so on, and when we come to left surface,it is negatively charged.
 
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The answer should depend on how many free electrons are, to start with. And how strong is the field. You need less electrons to compensate a very weak field. It is not a general, yes/no answer.

If it is a very poor conductor, with very low density of free carriers, it may not be possible the compensate the external field, even if they all move to the best positions on the surface.

It may be a situation with the right electric field and the right electron density where all free electrons are on the surface but this would be very special case.
But in general there should be just a gradient of electron density, with higher density near the surface.

Assume a copper plate with 1 mm thickness. If all the free electrons would be crowded (uniformly) on one of the two surfaces, the charge density will be

σ=e n h

where e is the electron charge, n is the number density of electrons and h the thickness of the plate.

n is the order of 1028 m-3 for copper and other good conductors.

So σ would be of the order of 10-19 x1028 10-3 = 106 Q/m2
The field produced by this charge density alone will be of the order
σ/εo or 106/10-11 =1017 V/m.

The dielectric strength (dielectric breakdown) of most materials is of the order 106-107 V/m.
 
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Drakkith said:
Why would the net field inside be zero if all of the negative charges are on the outside of the conductor and all of the positive charges are on the inside?
Ugh! I made the stupid assumption that the +ve charges also move ( I'm embarrassed). Sorry
So what did you conclude? The given "correct" answer must be wrong?
 
  • #11
Aniruddha@94 said:
Ugh! I made the stupid assumption that the +ve charges also move ( I'm embarrassed). Sorry
So what did you conclude? The given "correct" answer must be wrong?

Given my own knowledge and that of the posters in this thread, yes.
 

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