Calculation of magnetic/electric fields

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    Calculation Fields
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Discussion Overview

The discussion revolves around the calculation of magnetic and electric fields within conductors and dielectrics, particularly comparing ordinary conductors to superconductors. Participants explore the equations and principles that govern these fields, addressing both theoretical and practical aspects.

Discussion Character

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

Main Points Raised

  • One participant notes the equation for the magnetic field in superconductors and questions how to find the field inside an ordinary conductor when the external field is known.
  • Another participant explains that the Meissner effect minimizes electromagnetic free energy in superconductors, while ordinary conductors do not have a corresponding minimum.
  • It is mentioned that an ordinary conductor always has zero electric field inside, while for dielectrics, the internal charge distribution is dependent on how charge was initially deposited.
  • A participant expresses that calculating the magnetic field inside a conductor with an external field is poorly posed without specific assumptions about the conductor's properties.
  • One contribution states that if the material is non-magnetic, the field penetrates freely, but if it is magnetic, magnetization must be calculated, which involves the demagnetizing field.
  • Another participant raises the relevance of paramagnetism and diamagnetism in the context of the discussion.
  • References to textbooks are provided for further reading on the phenomena discussed, including both undergraduate and advanced levels.

Areas of Agreement / Disagreement

Participants express differing views on the behavior of electric and magnetic fields in conductors and dielectrics, with no consensus reached on the best approach to calculate the fields inside ordinary conductors. Multiple competing views remain regarding the effects of material properties on field behavior.

Contextual Notes

Limitations include the lack of consensus on the assumptions required for calculating fields in ordinary conductors and the complexity introduced by the material properties such as magnetic susceptibility.

daudaudaudau
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Hi.

For a superconductor we have the nice equation [itex]\nabla^2 \mathbf B=\frac{1}{\lambda^2}\mathbf B[/itex]. Using this equation we can find the B-field inside the superconductor if we have the boundary values. But what about an ordinary conductor(or dielectric) ? If I know what the field is outside the object, what is the equation I can solve to find the field inside?
 
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Your quoting the Meisner effect which shows the electromagnetic free energy in a superconductor is minimized when your equation is satisfied.

There is no corresponding "minimum" in everyday conductors...it's zero when there is no electric nor magnetic induction.

This "London equation" predicts the magnetic field in a superconductor decays exponentially from whatever value it possesses at the surface.

Or are you looking for the charge distribution inside an electrical conductor??
 
An ordinary conductor always has 0 electric field inside. For a dielectric, the charge inside depends on how the charge was deposited in the first place and can't be calculated from surface charge.
 
Naty1 said:
Your quoting the Meisner effect which shows the electromagnetic free energy in a superconductor is minimized when your equation is satisfied.

There is no corresponding "minimum" in everyday conductors...it's zero when there is no electric nor magnetic induction.

This "London equation" predicts the magnetic field in a superconductor decays exponentially from whatever value it possesses at the surface.

Or are you looking for the charge distribution inside an electrical conductor??

My problem arose because I wanted to calculate the magnetic field inside a conductor (not necessarily a perfect conductor) if there is a given constant field outside. This seems to be extremely easy for a superconductor, because we have that nice equation I quoted, but what about an ordinary conductor? How can I actually calculate the field?
 
daudaudaudau said:
My problem arose because I wanted to calculate the magnetic field inside a conductor (not necessarily a perfect conductor) if there is a given constant field outside. This seems to be extremely easy for a superconductor, because we have that nice equation I quoted, but what about an ordinary conductor? How can I actually calculate the field?

My recollection is that it's a fairly poorly posed problem. Without the assumptions of the superconductor's properties, I recall that the magnetic field inside the conductor, due to an externally applied static magnetic field, must be constant. Assuming that the permeability is the same as vacuum inside the conductor then I believe that the magnetic field is unaffected by the presence of the conductor. But again I think that when assuming perfect electrical conductors that this is not a mathematically pleasant problem to define.
 
If the material is non-magnetic (permeability mu=1) then the field penetrates freely as though through a vacuum. If not, you can calculate the magnetization M

[tex]\vec{M}=\chi\vec{H}=\vec{B}-\mu_0\vec{H}[/tex]

where chi is the magnetic susceptibility. It is a little involved because of the so-called demagnetizing field, which depends on the shape of the object and direction of applied field.
EDIT: Corrected sign above.
 
Last edited:
My problem arose because I wanted to calculate the magnetic field inside a conductor (not necessarily a perfect conductor) if there is a given constant field outside.

I wondered if this is what you are after...anyone have a reference that explains the phenomena a bit...

An ordinary conductor always has 0 electric field inside
for an ideal conductor...not a real world imperfect conductor...

I don't have the background to provide any concrete answer but I would think paramagnetism and diamagnetism of the material would be relevant:
http://en.wikipedia.org/wiki/Magnetic_permeability
 
Last edited:
Naty1 said:
I wondered if this is what you are after...anyone have a reference that explains the phenomena a bit...
If [tex]\mu=1[/tex] then the field penetrates as in a vacuum. If not, see the equation I gave above for B inside.
For references, see
Undergrad level:
Reitz and Milford, Foundations of Electromagnetic Theory, has a very nice treatment of magnetization (I have the 1st edition, in case it matters).
Griffiths is likely to be good based on reputation, though I don't own a copy.

Advanced level:
Jackson, Classical Electrodynamics
Stratton, Electromagnetic Theory
 

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