E-Field in Hollow Polarized Dielectric

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Homework Help Overview

The discussion revolves around determining the electric field intensity at the center of a spherical cavity within a polarized dielectric material. The original poster is grappling with the complexities of non-uniform charge distributions due to polarization.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to calculate surface charge density using polarization and is uncertain about integrating over a non-uniform surface. Some participants question the existence of surface charge in this context, while others clarify that surface charge does exist due to the polarization direction.

Discussion Status

The discussion is active, with participants exploring different interpretations of the polarization effects on surface charge. There is mention of a potential solution being provided by the professor, indicating a productive direction in the conversation.

Contextual Notes

Participants are navigating the complexities of dielectric materials and polarization, with specific focus on the implications of a spherical cavity. There is an acknowledgment of the original poster's assumptions regarding charge distribution and the challenges posed by the geometry of the problem.

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Homework Statement


Determine the electric field intensity at the center of a small spherical cavity cut out of a large block of dielectric in which a polarization P exists.

The Attempt at a Solution


charge densitysurface = P(dot)n --> charge densitysurface = P(dot)r

This is about as far as I've gotten... My problem is I've never dealt with a non-uniform charge distribution before. My first goal was to find the surface charge around the sphere, but the polarization makes it such that it's non-uniform. I've assumed that the dielectric is polarized in the positive-z direction, which puts a concentration of negative charges at the top of the sphere and a concentration of positive charges at the bottom. My professor recommended using a sin() function to integrate over the sphere (positive->neutral->negative->neutral->repeat), but I don't really know how to fit this into a surface integral. Any thoughts?

Thanks,
Spencer
 
Last edited:
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The material is a dialectric. I don't think it's to be supposed that there is surface charge.
 
There actually i s surface charge - picture a surface of thin dielectric in the xy-plane. If you polarize the whole thing with an e-field in the z-direction, the dipoles at the top of the plane will have their positive charges pointing up (giving a positive surface charge). Likewise, the bottom will have a negative surface charge. This case is tricky, because it's a sphere, so there's a smooth transition around the surface that goes sinusoidally. The professor has actually solved the problem since I first posted the problem, so I'll post a solution later for anybody who's interested.
 
I'd love to see that solution.
 
Haha - so, I've graduated since I originally posted this problem a couple years ago, but I actually just pulled out a box of old schoolwork to sort through. If I can find the solution, I'll post it.
 

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