- #1
mmmboh
- 407
- 0
This isn't actually a homework question, but I have a midterm coming up and there is an example problem in the book that I don't quite get.
Basically there are two parallel conductors, each with charge Q on them, what is the electrostatic pressure on the places?
The answer is that there is no electric field between them, I imagine due to them canceling, but then on the other side of them the electric field is [tex]\sigma[/tex]/[tex]\epsilon[/tex]o (well that's not the full answer obviously, but that's the part I am having a bit of trouble with)...so there are a couple things that are bothering me...
1. I know that inside a conductor the field is zero, so because of the discontinuity it is [tex]\sigma[/tex]/[tex]\epsilon[/tex]o outside, but does this still apply if the plates don't have width? because then there is no inside the conductor, basically I am trying to figure out why it is [tex]\sigma[/tex]/[tex]\epsilon[/tex]o outside the conductors...
And, does the electric field from the bottom plate have the same field below the top plate as it does above the top plate? Basically if you have an electric field and put some metal plate in the way, I know the charges inside the plate will move around to cancel the field inside the plate, but what about on the other side of the plate? What is the field strength? Does the induced positive charge on the right side cause the same electric field...because I would say no because it takes the positive and negative charges inside the conductor to cancel off the electric field, but I'm not sure, or does the electric field sort of pass right through?
Basically, is the field outside the metal plate [tex]\sigma[/tex]/[tex]\epsilon[/tex]o because the discontinuity, or because of the influence of the other metal plate's electric field?
Thanks!
Basically there are two parallel conductors, each with charge Q on them, what is the electrostatic pressure on the places?
The answer is that there is no electric field between them, I imagine due to them canceling, but then on the other side of them the electric field is [tex]\sigma[/tex]/[tex]\epsilon[/tex]o (well that's not the full answer obviously, but that's the part I am having a bit of trouble with)...so there are a couple things that are bothering me...
1. I know that inside a conductor the field is zero, so because of the discontinuity it is [tex]\sigma[/tex]/[tex]\epsilon[/tex]o outside, but does this still apply if the plates don't have width? because then there is no inside the conductor, basically I am trying to figure out why it is [tex]\sigma[/tex]/[tex]\epsilon[/tex]o outside the conductors...
And, does the electric field from the bottom plate have the same field below the top plate as it does above the top plate? Basically if you have an electric field and put some metal plate in the way, I know the charges inside the plate will move around to cancel the field inside the plate, but what about on the other side of the plate? What is the field strength? Does the induced positive charge on the right side cause the same electric field...because I would say no because it takes the positive and negative charges inside the conductor to cancel off the electric field, but I'm not sure, or does the electric field sort of pass right through?
Basically, is the field outside the metal plate [tex]\sigma[/tex]/[tex]\epsilon[/tex]o because the discontinuity, or because of the influence of the other metal plate's electric field?
Thanks!
Last edited: