Griffiths (electrodynamics) problem 4.19, part b

So, to find P, we need to use the E-field in the air portion rather than the dielectric portion. The surface charge density over the air segment is equal to the total surface charge density because the air segment has no free charges, so all of the surface charge comes from the bound charges in the dielectric.
  • #1
phrankle
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When finding the polarization of the dielectric portion between the two plates using P=[tex]\epsilon_{0}[/tex] [tex]X_{e}[/tex]E, why would we use the E-field in the air portion (as is done in the solutions manual and here: http://www.getofftheinternet.net/s_10077.pdf ) instead of solving for the E-field in the dielectric portion and using that to find P?

Also, why is the surface charge density over the air segment equal to the TOTAL surface charge density? Isn't it the free charge density in this problem? I'm pretty confused, so any help will be massively appreciated.
 
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  • #2
P and E0 contribute to E in the material by vector summing. P is the part of E that is due to the charge separation, and E0 is the reason for the charge separation.
 

1. What is Griffiths problem 4.19, part b?

Griffiths problem 4.19, part b is a question from the textbook "Introduction to Electrodynamics" by David J. Griffiths. It involves solving for the electric potential inside and outside of a spherical shell with a non-uniform charge distribution.

2. How do I approach solving this problem?

To solve this problem, you should first review the concepts of electric potential and Gauss's law, as well as the equations for the electric potential for different charge distributions. Then, you can use these equations and the given information to determine the electric potential in and out of the spherical shell.

3. What are the key equations needed to solve this problem?

The key equations needed to solve this problem are Gauss's law, the equation for the electric potential due to a point charge, and the equation for the electric potential due to a uniformly charged spherical shell.

4. Are there any special considerations to keep in mind while solving this problem?

One important consideration is that the electric potential is continuous at the boundary between the inside and outside of the spherical shell. This means that the potential inside and outside must be equal at the boundary. Additionally, the electric field inside the shell is zero due to the charge distribution.

5. How can I check my solution to this problem?

You can check your solution by calculating the electric field inside and outside of the spherical shell using the electric potential you found. The electric field should be zero inside the shell and follow the expected behavior outside the shell. Additionally, you can check your solution using the given boundary conditions and by ensuring that the electric potential is continuous at the boundary.

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