Electric field inside a conductor

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Homework Help Overview

The discussion revolves around the behavior of electric fields within a conductor, particularly in the context of an ideal circuit with a voltage source, resistor, and wire. Participants explore the implications of Ohm's law and the conditions under which electric fields and current densities exist in a conductor.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants examine the relationship between voltage, electric field, and current density in a conductor, questioning the assumptions made about resistance and conductivity. They discuss the implications of infinite conductivity and the resulting behavior of electric fields.

Discussion Status

The discussion is active, with participants raising questions about the validity of assumptions and the nature of electric fields in ideal conditions. Some guidance has been offered regarding the limits of conductivity and the behavior of electric fields, but no consensus has been reached on the underlying principles.

Contextual Notes

Participants are navigating the complexities of ideal versus real conditions in conductors, particularly regarding the assumptions of zero resistance and infinite conductivity. The implications of these assumptions on electric field behavior are under scrutiny.

anhnha
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I need help to understand what is going on in this simple circuit. Consider all voltage source, resistor and wire are ideal. And also assume that the wire has the same cross-section area along its length (A = const (m^2)).
attachment.php?attachmentid=59350&stc=1&d=1370610004.jpg


The voltage between two points A and B is defined as path integral from A to B of electric field.
[tex]V_{AB} = \int ^B_A \overrightarrow {E}.\overrightarrow {dl}[/tex]

The current is equal to each other everywhere in the wire and the wire has the same cross-section area => the current density is also the same everywhere.
Acoording to Ohm's law:
[tex]\overrightarrow {J}=\sigma \overrightarrow {E}[/tex]

Because J ≠ 0, σ ≠ 0 => E ≠ 0 (1) everywhere in the wire (also very point from A to B)
But I also know that: [tex]V_{AB} = 0[/tex]
[tex]V_{AB} = E\int ^B_A \overrightarrow {r0}.\overrightarrow {dl} = 0[/tex]
If I choose the path is the straight line from A to B => integral from A to B of dl ≠ 0
[tex]\int ^B_A \overrightarrow {r0}.\overrightarrow {dl} ≠ 0[/tex]=> E = 0 (2)
(1) and (2) can't exist simultaneously. Can you point out what I am wrong?
 

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I think that when you say

[tex]V_{AB} = 0[/tex]

You make the assumption that the resistance of the conductor is zero. This is only justified when the conductivity of the conductor is infinity. As J is finite then the value of E should tend to zero making the equations consistent and removing the contradiction.
 
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Thanks, but the product ∞.0 is undefined.
J ≠ 0, σ = ∞ then can we say E = 0?
 
anhnha said:
Thanks, but the product ∞.0 is undefined.
J ≠ 0, σ = ∞ then can we say E = 0?

Are you familiar with limits? The product isn't undefined it tends to J. We can say that E tends to zero but σ.E tends to J. The contradictions are from mixing ideal conditions like "potential difference inside a wire is zero!" and real conditions with wire having some finite resistance.
 
I know the limit but not sure.
J = σE
J is a constant larger than zero.
Is there any rule to say that when σ approaches to infinity (∞) E has to approach to zero?
 
If ## \sigma \rightarrow \infty ##, then what about ## E = \frac {J} {\sigma} ##?
 
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anhnha said:
I know the limit but not sure.
J = σE
J is a constant larger than zero.
Is there any rule to say that when σ approaches to infinity (∞) E has to approach to zero?

Yes because (tending to infinity)*(something other than tending to zero) is always infinity it isn't any finite number.

On a side note your question raises some interesting questions like "in an ideal wire with no resistance there is no potential difference between two points on the wire so why do the electrons move?" I am not too sure about the answer except to say that they are moving towards the positive terminal of the battery.
 
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voko said:
If ## \sigma \rightarrow \infty ##, then what about ## E = \frac {J} {\sigma} ##?

Ah, that is simple. I thought about it as J = σE and it makes more difficult!
 
On a side note your question raises some interesting questions like "in an ideal wire with no resistance there is no potential difference between two points on the wire so why do the electrons move?" I am not too sure about the answer except to say that they are moving towards the positive terminal of the battery.
yes, that is also what I am confused. I asked this question in another thread but still not understand.
Hope someone can help.
 
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consciousness said:
On a side note your question raises some interesting questions like "in an ideal wire with no resistance there is no potential difference between two points on the wire so why do the electrons move?" I am not too sure about the answer except to say that they are moving towards the positive terminal of the battery.

In an ideal wire, a.k.a. a superconductor, electrons are not subject to any force, so they just keep going steadily. Simple inertial motion. All it takes is just a little push.
 
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In an ideal wire, a.k.a. a superconductor, electrons are not subject to any force, so they just keep going steadily. Simple inertial motion. All it takes is just a little push.
Well, it makes sense.:smile:
 
  • #12
voko said:
In an ideal wire, a.k.a. a superconductor, electrons are not subject to any force, so they just keep going steadily. Simple inertial motion. All it takes is just a little push.

Cant say no to that! :smile:
 

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