Understanding the Relationship Between Electric Fields and Conductors

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Discussion Overview

The discussion revolves around the relationship between electric fields and conductors, particularly focusing on the conditions under which electric fields exist in conductors, the implications of static versus time-varying fields, and the behavior of currents in these scenarios. Participants explore theoretical aspects, boundary conditions, and the application of concepts such as Ohm's law and the Lorentz force law.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that E=0 for a conductor applies only under static conditions, questioning why boundary conditions state that the tangential component of the electric field must be zero.
  • Others clarify that the electrostatic condition requires both static fields and zero currents, suggesting that tangential electric fields would lead to surface currents, thus violating electrostatic conditions.
  • There is a discussion about the nature of the electric field produced by a DC voltage source, with some asserting that a constant potential difference does not imply a zero electric field due to spatial derivatives.
  • Participants express confusion about how a static electric field can produce a current, with references to the Lorentz force law indicating that charges in a conductor respond to static electric fields.
  • Some propose that in ideal conductors, electrons rearrange instantly to maintain zero tangential electric fields, while others question the validity of this assumption.
  • There are inquiries about the setup of spatial voltage distributions, with examples like batteries being mentioned as a simple case.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and disagreement, particularly regarding the implications of static versus time-varying electric fields and their effects on current flow. No consensus is reached on the validity of certain assumptions or the interpretation of boundary conditions.

Contextual Notes

Limitations include the dependence on definitions of electrostatic and magnetostatic conditions, as well as unresolved questions about the behavior of electric fields in non-ideal conductors.

vig
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There are some very basic questions about conductors that are bugging me:
1. I know that E=0 for a conductor is only if the fields remain static, If there was a time varying field, the electrons would be in constant motion across the conductor, meaning that at any point of time, a net tangential field does exist causing the electrons to move. So why is it that we keep applying boundary conditions that the tangential component of E field on a conductor MUST be 0?..

2. What kind of a field does a DC voltage source provide in a wire that causes a constant flow of current? I ask this because if the potential difference remains constant, the electric field must be zero (E=-delV) and if E is indeed zero, no current can flow...

I guess the answers to both are interlinked.
Would be grateful for any help.
Thanks in advance :)
 
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vig said:
1. I know that E=0 for a conductor is only if the fields remain static, If there was a time varying field, the electrons would be in constant motion across the conductor, meaning that at any point of time, a net tangential field does exist causing the electrons to move. So why is it that we keep applying boundary conditions that the tangential component of E field on a conductor MUST be 0?..
Actually, the electrostatic condition is a little stronger than just the fields remain static. Not only do the fields need to remain static, but the currents must also be 0. You can have scenarios where the fields are static, but there is a non-zero current. Such scenarios are called "magnetostatic" so as to distinguish them from electrostatic ones.

In any scenario where there is a tangential E-field on the surface of a conductor then you get a current along the surface of the conductor. Since the electrostatic condition is defined as having no currents it implies that there is no tangential E-field, essentially by definition. I.e. you certainly can have tangential E-fields on the surface of a conductor, but then it is not electrostatic.

vig said:
2. What kind of a field does a DC voltage source provide in a wire that causes a constant flow of current? I ask this because if the potential difference remains constant, the electric field must be zero (E=-delV) and if E is indeed zero, no current can flow...
It is an E field. Your comment about the potential difference is incorrect. The gradient consists of spatial derivatives, so the time derivative of the potential can be zero and still have non-zero spatial derivatives, and therefore a non-zero E-field.
 
DaleSpam said:
Actually, the electrostatic condition is a little stronger than just the fields remain static. Not only do the fields need to remain static, but the currents must also be 0. You can have scenarios where the fields are static, but there is a non-zero current. Such scenarios are called "magnetostatic" so as to distinguish them from electrostatic ones.

In any scenario where there is a tangential E-field on the surface of a conductor then you get a current along the surface of the conductor. Since the electrostatic condition is defined as having no currents it implies that there is no tangential E-field, essentially by definition. I.e. you certainly can have tangential E-fields on the surface of a conductor, but then it is not electrostatic.

forgive my ignorance, but how can a STATIC field produce a current in the first place?..All that i can decipher is that if the E field changes at a constant rate, the current through the conductor must be constant.
If the tangential field is 0 only in the electrostatic case, why do we apply the condition on, say, reflection of an EM wave from a dielectric? There doesn't seem to be anything static here..
One theory i could think of is that in an ideal conductor, maybe we can assume that the moment the field is applied, the electrons rearrange themselves without any delay, implying that at any instant of time, the tangential field is 0..i don't know about the validity of this theory though..

DaleSpam said:
It is an E field. Your comment about the potential difference is incorrect. The gradient consists of spatial derivatives, so the time derivative of the potential can be zero and still have non-zero spatial derivatives, and therefore a non-zero E-field.

could you pls enumerate on how exactly a spatial distribution of voltage is set up?
 
vig said:
forgive my ignorance, but how can a STATIC field produce a current in the first place?
According to the Lorentz force law, a static E-field means that there is a steady force on charges. In a conductor, the charges are not stuck firmly to their atoms, so they will move in response to that force. That is the defining characteristic of a conductor.

vig said:
All that i can decipher is that if the E field changes at a constant rate, the current through the conductor must be constant.
No, if the E-field changes at a constant rate then the current will also change at a constant rate. The current in a conductor is proportional to the E-field, not the time derivative of the E-field. This is called Ohm's law.

vig said:
If the tangential field is 0 only in the electrostatic case, why do we apply the condition on, say, reflection of an EM wave from a dielectric? There doesn't seem to be anything static here..
I don't know for sure, do you have a reference?

vig said:
could you pls enumerate on how exactly a spatial distribution of voltage is set up?
Well, the simplest example is a battery. The + terminal has a higher voltage than the - terminal, and they are located at different locations in space, so there is a spatial distribution of voltage.
 
DaleSpam said:
According to the Lorentz force law, a static E-field means that there is a steady force on charges. In a conductor, the charges are not stuck firmly to their atoms, so they will move in response to that force. That is the defining characteristic of a conductor.



DaleSpam said:
No, if the E-field changes at a constant rate then the current will also change at a constant rate. The current in a conductor is proportional to the E-field, not the time derivative of the E-field. This is called Ohm's law.

Yea..so a static field will cause the electrons to move until a point is reached where it completely cancels out the external fields, so the net E field becomes zero.
However, if the field were time varying, the electrons would have to keep moving in an attempt to cancel out the electric field (but it never happens), causing a current.
Now if the field were to vary at a constant rate, the rate at which the electrons would move would also be constant, which is a constant current.
So in a non ideal situation, there would always be a net tangential E field on the conductor at any point.
The only thing that i can make out is, that if it were an ideal conductor (σ=∞), then there would be no time taken for the electrons to drift and cancel, so that at any point of time, the E(tan) must be zero. Is this correct?

DaleSpam said:
I don't know for sure, do you have a reference?
That's the reason, also, why we carry put analysis using the methods of images for a currentcarrying element above a ground plane.
 
vig said:
Yea..so a static field will cause the electrons to move until a point is reached where it completely cancels out the external fields, so the net E field becomes zero.
The E field is what you are calling the "net" E field. So this is already a time varying E field and therefore a time varying current. Again, the current is proportional to the E field, not the change (time derivative) of the E field.
 

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