Electric & Magnetic Fields at Point P with Dielectric/Magnetic Material

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Discussion Overview

The discussion revolves around the behavior of electric and magnetic fields at a point P in the presence of dielectric and magnetic materials. Participants explore the relationship between external fields and the fields generated by these materials due to polarization effects, with a focus on theoretical implications and clarifications of concepts.

Discussion Character

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

Main Points Raised

  • Some participants propose that the electric field at point P in an external electric field is the sum of the external field and the field due to polarization from the dielectric material.
  • Others argue that this relationship holds true for magnetic fields as well, with similar contributions from magnetic materials.
  • A participant questions whether the polarization field itself can cause secondary polarization effects.
  • There is mention of the complexities in full electrodynamics, where changes in polarization can also affect the magnetic field.
  • Some participants clarify that the polarization need not be caused by the external field, especially in ferromagnetic cases.
  • There is discussion about the implications of point P being a reference point in space, as opposed to being located in a conducting material.
  • Concerns are raised regarding the interpretation of point P in relation to dipole densities and their contribution to magnetic fields.

Areas of Agreement / Disagreement

Participants express varying degrees of agreement on the relationship between external fields and fields due to materials, but there is no consensus on the implications of polarization and the role of point P in different contexts.

Contextual Notes

Limitations in the discussion include assumptions about the nature of polarization, the conditions under which fields are summed, and the specific scenarios being considered (e.g., static vs. dynamic fields).

yungman
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Electric/magnetic field at point P in presence of dielectric/magnetic material.

I want to confirm either the electric field at a point P in space in an \vec E_{ext} field with the presence of a dielectric material is the sum of the \vec E_{ext} and electric field \vec E_{p} from the dielectric material due to polarization cause by the \vec E_{ext}.

And this is also true of the magnetic field at a point P in space with \vec B_{ext} and magnetic material.

Thanks
 
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whats your question?
 


granpa said:
whats your question?

I just want to verify my assertion. Books are not very clear on this.
 


yungman said:
I want to confirm either the electric field at a point P in space in an \vec E_{ext} field with the presence of a dielectric material is the sum of the \vec E_{ext} and electric field \vec E_{p} from the dielectric material due to polarization cause by the \vec E_{ext}[/color]

And this is also true of the magnetic field at a point P in space with \vec B_{ext} and magnetic material.

Thanks

you are asking if the field due to the polarization due to the external field itself causes secondary polarization?
 
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Yes, yungman, that's true, at least for the electric field and/ or in magnetostatics. In full electrodynamics, there is also a contribution of the change of P to the magnetic field. In fact, in optics one sets often M=0, so that all effects of the medium are due to P alone.
 


granpa said:
you are asking if the field due to the polarization due to the external field itself causes secondary polarization?

No, I just want to verify that the field experienced at a point P with a piece of dielectric material close by, is the sum of the \vec E_{ext} + \vec E_{P} where \vec E_{P} is the field from polarizing of the dielectric sitting somewhere in space( somewhere close to P but not touching P).

Same as in the case of magnetic with a piece of magnetic material close by.
 


DrDu said:
Yes, yungman, that's true, at least for the electric field and/ or in magnetostatics. In full electrodynamics, there is also a contribution of the change of P to the magnetic field. In fact, in optics one sets often M=0, so that all effects of the medium are due to P alone.

Thanks

Do you mean if P is at some conducting material where very small free current density \vec J_{free} created by even static magnetic field. But if P is just a point in space ( empty space) there should be no more changes.
 


yungman said:
I want to confirm either the electric field at a point P in space in an \vec E_{ext} field with the presence of a dielectric material is the sum of the \vec E_{ext} and electric field \vec E_{p} from the dielectric material due to polarization cause by the \vec E_{ext}.

And this is also true of the magnetic field at a point P in space with \vec B_{ext} and magnetic material.

Thanks
Yes to both cases, but the polarization need not be "caused" by the field. In ferro cases, there mayi not even be an external field.
 


yungman said:
Thanks

Do you mean if P is at some conducting material where very small free current density \vec J_{free} created by even static magnetic field. But if P is just a point in space ( empty space) there should be no more changes.
I don't know what you mean with P being just a point in space. In the simplest cases, P corresponds to a dipole density and, e.g. a rotating dipole will lead to a magnetic field. Hence the \partial P/\partial t term on the rhs of Ampere's law.
 
  • #10


DrDu said:
I don't know what you mean with P being just a point in space. In the simplest cases, P corresponds to a dipole density and, e.g. a rotating dipole will lead to a magnetic field. Hence the \partial P/\partial t term on the rhs of Ampere's law.

What I meant P is just a reference point in space. It is like books always talk about fields experienced at a point from a source some distance away.


Anyway, thanks for all the replies to confirm my understanding.

Alan
 

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