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

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SUMMARY

The electric field at a point P in the presence of a dielectric material is indeed the sum of the external electric field \(\vec E_{ext}\) and the electric field \(\vec E_{P}\) generated by the polarization of the dielectric. This principle also applies to magnetic fields, where the magnetic field at point P is the sum of the external magnetic field \(\vec B_{ext}\) and the contribution from the magnetic material. In full electrodynamics, changes in polarization also affect the magnetic field, particularly in scenarios involving dynamic fields. The discussion confirms that both electric and magnetic fields at point P can be analyzed using these additive principles.

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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.
 
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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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