Curl of Polarization in a bar electret

In summary, Griffith's says that in a bar electret the curl of the polarization does not equal zero everywhere. This is because at the surface/air interface, the derivative of the polarization may diverge.
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Telis
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In Griffith's "Introduction to Electrodynamics" says that in a bar electret the curl of the polarization does not equal zero everywhere. Why is that ? Thanks in advance
 
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What comes to mind very quickly is the corresponding magnetostatics problem with a cylinder of uniform magnetization ## \vec{M} ##. In that case, ## \nabla \times \vec{M} =\vec{J}_m ## results in surface currents per unit length of ## \vec{K}_m=\vec{M} \times \hat{n} ## on the surface of the cylinder. ## \\ ## In the simplest case of uniform ## \vec{ P} ##, if you take ## \nabla \times \vec{P} ##, you will get places where ## \nabla \times \vec{P } ## diverges at parts of the surface/air interface. In general, if ## \vec{P} ## is uniform, the derivative ## \nabla \times \vec{P} ## vanishes, but this derivative can diverge when ## \vec{P} ## undergoes a discontinuity such as at the surface/air interface.
 
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Thank you, it is pretty clear for me now that at the surface/air interface will have ##\nabla \times \vec{P} \neq 0 ##. Then Griffiths continues and says that "if the problem exhibits spherical, cylindrical, or plane symmetry then evidently in such cases ##\nabla \times \vec{P} = 0 ##." So what does he mean about cylindrical symmetry and why a bar electret is not such a case ?
 
  • #4
Griffith's seems to be talking about the polarization ## \vec{P} ## in the material, and not considering edge effects. It is well known from E&M, that in the case of a dielectric sphere in a uniform electric field, the polarization inside the sphere is uniform. This also is the case for a cylinder that is transverse to the electric field. I'll see if I can find a couple of "links" to these very special cases. In general, for odd geometries, the resulting polarization ## \vec{P} ## is not uniform when the dielectric object is placed in uniform electric field, and consequently, the derivative ## \nabla \times \vec{P} ## does not vanish. Let me try to find a couple of "links" on the two special dielectric geometries: See: https://www.physicsforums.com/threads/electric-field-of-a-charged-dielectric-sphere.890319/ and https://www.physicsforums.com/threa...ormly-polarized-cylinder.941830/#post-5956930
 
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1. What is the curl of polarization in a bar electret?

The curl of polarization in a bar electret refers to the rotation of electric polarization within the electret material. This rotation is caused by the presence of an external magnetic field.

2. How is the curl of polarization measured in a bar electret?

The curl of polarization can be measured by observing the change in electric polarization within the electret material when exposed to a varying magnetic field. This change can be measured using specialized equipment such as a magnetometer.

3. What causes the curl of polarization in a bar electret?

The curl of polarization in a bar electret is caused by the alignment of electric dipoles within the material in response to an external magnetic field. This alignment results in a rotation of the electric polarization within the material.

4. What are the applications of the curl of polarization in a bar electret?

The curl of polarization in a bar electret has various applications in fields such as sensors, actuators, and data storage. It is also used in devices such as magnetic field sensors and magnetic recording heads.

5. Can the curl of polarization in a bar electret be controlled?

Yes, the curl of polarization in a bar electret can be controlled by varying the strength and direction of the external magnetic field. This allows for precise manipulation of the electric polarization within the material, making it useful for various applications.

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