How Does Polarization Affect Electric Field Calculation in a Dielectric Disc?

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SUMMARY

The discussion focuses on calculating the electric field strength (E) at the center of a uniformly polarized dielectric disc with radius R. The polarization vector (P) lies in the plane of the disc, leading to a surface charge density (\sigma) on opposite halves of the disc. The correct relationship for surface charge density is given by \sigma = \epsilon_0 E P, where \epsilon_0 is the permittivity of free space. The electric field at the center can be determined using E = \frac{1}{4 \pi \epsilon_0}\frac{\sigma}{r^2}, where r is the distance from the center.

PREREQUISITES
  • Understanding of dielectric materials and polarization
  • Familiarity with the concept of electric field and charge density
  • Knowledge of the equations for surface charge density and electric field
  • Basic grasp of electrostatics and permittivity of free space
NEXT STEPS
  • Study the derivation of electric fields in polarized dielectrics
  • Learn about the relationship between polarization and charge density in dielectrics
  • Explore the implications of uniform polarization on electric field calculations
  • Investigate the effects of varying dielectric shapes on electric field distribution
USEFUL FOR

Students and educators in physics, electrical engineers, and anyone interested in the principles of electrostatics and dielectric materials.

Saketh
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I'm trying to teach myself polarization and dielectrics by doing problems, but it's not going as well as I'd hoped. Here's the first problem that I got stuck on:
A round dielectric disc of radius R is statically polarized so that it gains the uniform polarization P, with the vector P lying in the plane of the disc. Find the strength E of the electric field at the center of the disc if d << R.​
I thought that since the disc is polarized along its plane, there would be a charge density \sigma on one half of it, and a charge density of -\sigma on the other half of it. I wasn't sure if \sigma = P, but I set them equal anyway. I also wasn't sure if \sigma is uniform along each half-surface, but I did that anyway. Then I thought that a uniform polarization vector means that the whole surface is charged up unformly, which means no net electric field at the center.

I realize this is going to sound silly, but I have no idea how I'm supposed to solve this problem. Where am I supposed to start?
 
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The first thing you need to do is to determine the charge distribution on the dielectric disc. Since the polarization is uniform, this means that the same amount of charge will be distributed uniformly across the surface of the disc. To calculate this, you can use the equation \sigma = \epsilon_0 E P, where \epsilon_0 is the permittivity of free space and E is the electric field at the surface of the disc. Once you have this, you can then calculate the electric field at the center of the disc by using the equation E = \frac{1}{4 \pi \epsilon_0}\frac{\sigma}{r^2}, where r is the distance from the center of the disc to the point where the electric field is being measured.
 

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