Current density in a conductor at DC

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Discussion Overview

The discussion centers on the concept of current density in a conductor under direct current (DC) conditions. Participants explore the behavior of charge distribution within conductors, the implications of electrostatics, and the relationship between current density and electric fields in various configurations, including cylindrical wires and transmission lines.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why current density is uniform in a conductor at DC, noting that charges repel each other and typically reside on the surface of conductors in static situations.
  • Another participant explains that while excess charges may reside on the surface, the bulk of the conductor contains a uniform distribution of electrons and positive ions, allowing current to flow throughout the material when an electric field is present.
  • A different participant elaborates that in electrostatics, only excess charges move to the surface, while the electrons that balance the positive nuclei remain distributed within the conductor, contributing to current without being pushed to the surface.
  • One participant raises a question about the treatment of conductors as lines of charge in electromagnetic theory, suggesting that a wire with current should not appear as a line of charge due to the presence of equal positive and negative charges.
  • Another participant mentions that while DC current does create surface charge on the wire, the charge density is not uniform and decreases along the length of the wire from high to low potential.
  • A participant references a textbook example of a transmission line, expressing confusion about why it would appear as a line of charge despite having equal positive and negative charges, and questions the implications for current density at the surface of the conductor.
  • One participant discusses the relationship between electric field and current density, indicating that they expect current density to be constant throughout the conductor based on circuit theory.

Areas of Agreement / Disagreement

Participants express varying viewpoints regarding the distribution of charge within conductors and the implications for current density. There is no consensus on whether a wire with current should be treated as a line of charge or how charge density varies along the conductor.

Contextual Notes

Participants reference concepts from electromagnetic theory and electrostatics, indicating potential limitations in their understanding of how these theories apply to current density in conductors. Some assumptions about charge distribution and the implications for electric fields remain unresolved.

FrankJ777
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Why is there a uniform current density in a conductor at DC. It’s my understanding that generally in a conductor, a sphere for instance, in a static situation, all charge is at the surface of the conductor because it the charges repel each other. So in a cylindrical conductive wire even though there is an electric field that is causing the charges to flow longitudinally with respect to the wire, why don't the electric fields of the charges themselves repel each other and cause the current to be confined to the surface of the conductor?
 
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A conductor like copper has a large amount of movable negative charge carriers (electrons) and nearly the same amount of positive charges (copper ions). Any excess or deficit of electrons will be at the surface, but the material will always be filled a much larger amount of electrons and copper ions, and this will result in a current wherever there's an electric field.
 
Very good question.

The short answer may be that in electrostatics, only the superfluous charges get to the surface. The negative electrons that cancel the positive nuclei are still inside the metal. They form negative charge density, which is canceled by the positive charge density of the nuclei. In statics, these densities are uniform.

These distributed electrons later form the DC current. The electrons do repel each other, but this is balanced by the positive nuclei, so the electrons are not pushed out to the surface, but can stay distributed in the volume.
 
Thanks for the explanation. That brings up another question though. In Electromagnetics we often used the concept of a line of charge to find an electric field and to derrive the E&M field in a cable. To find the E&M fields in the cable it seems we treated the positive conductor as positive line of charge and the negitive cable as a negitive line of charge. I'd assumed at the time that a wire with a current would appear as a line of charge, but thinking about your guys' explanation about current density this doesn't seem to be the case. I gather from your explanations that there is an equal positive and negitive charge in the conductors, so as to be a net zero charge. So as viewed from outside of a wire, no matter what the current flowing through it, it would not appear as a line of charge? Is that correct?
 
Was your example about the coaxial cable?

Anyway, when DC current flows through wire, the wire will be charged on its surface, in order to produce electric field inside the wire that pushes the charges inside. The charge density will not be uniform though, but will decrease as one advances from the end of higher potential to the end of lower potential.
 
In my EM book, Wentorth, he used the example of a transmission line. The book states "...a test charge placed a couple of centimeters from an elevated transmission line will see what appears to be an infinite length line (of charge)." I'm confused why this would appear to be a line of charge if there is an equal amount of positive and negative charges inside the transmission line or conductor. It would seem to me that it would appear as an infinite line of current.

Also i was a bit confused about your explanation about how the current density at the surface of the conductor would be greater. By surface do you mean where the potential is applied?

I've attached a diagram similar to one in my EM textbook. It depicts a conductor with a voltage applied to both ends. According to the book the E field in the conductor is E = V_{ab}/L . Because current density, J = σE , I would expect the current density to be constant through the length of the conductor, which I would expect from circuit theory as well.

Sorry for the lengthy questions. I took EM quite a while ago. It seems like I spent a lot of time doing vector calculus, and just now trying to ferret out what it all means.
 

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