What Causes the Electric Field Outside Parallel Conductors?

AI Thread Summary
The discussion centers on understanding the electric field around parallel conductors with charge Q. It is clarified that there is no electric field between the conductors due to charge cancellation, while the electric field outside is given by σ/ε₀, stemming from the conductor's properties and the charge distribution. The electric field below the top plate is equal in magnitude to that above it, but the direction differs. When a conductor is placed in a uniform electric field, charges redistribute, resulting in an internal field that cancels the external field within the conductor, leading to a net zero field inside. Ultimately, the external electric field is influenced by both the external field and the induced charges on the conductor's surface.
mmmboh
Messages
401
Reaction score
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 \sigma/\epsilono (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 \sigma/\epsilono 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 \sigma/\epsilono 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 \sigma/\epsilono because the discontinuity, or because of the influence of the other metal plate's electric field?

Thanks!
 
Last edited:
Physics news on Phys.org
>>I know that inside a conductor the field is zero
Yes if there is no current

>>so because of the discontinuity it is \sigma/e outside
Not because of continuity? Its because the material is a conductor, therefor the charges spread themselves as far away as possible from each other, creating the build up of charge on the edges of the material. That creates the field you mentioned, which you can prove using Gausses Law

>>And, does the electric field from the bottom plate have the same field below the top >>plate as it does above the top plateAnd, does the electric field from the bottom plate
The magnitudes are the same, the field direction is not.

Heres how you can solve:

\oint\vec{E}\bullet\vec{n}dA = \frac{Q}{\epsilon_{0}}

E*A = \frac{Q}{\epsilon_{0}}

\sigma = \frac{Q}{A}E = \sigma/\epsilon_{0}
 
Last edited:
I think I may have not been clear. I meant if you have an electric field, and you put a metal plate in the electric field, is the electric field on both sides of the plate the same, or do the charges inside the metal plate affect it?
 
If you put a conductor in a electric field, the charge will redistribute themselves. But after this process, the E field in the conductor is not zero. There is an E-field in the conductor that is equivalent but opposite direction to the one that is passing through the conductor. That inner E-field is what moves the charges to a different distribution which momentary creates a current in the conductor. But yes if the Electric field is uniform, than the E field at the end of this process is the same magnitude on both sides
 
Ok cool, thanks! Just one thing, if you have a uniform electric field, let's say pointing to the right, and then you put in a metal plate, then negative charges will accumulate on the left side and positive charges on the right side; so wouldn't the electric field on either side of the conductor increase because of this?
 
what it does is that it creates an electric field in the conductor that is equivalent to the E field going through it, Those E fields cancel each other and you are left with a Net E-Field in the conductor of Zero. Than on the outside you have an E-Field that is the vector sum of the E-field passing through and the E - Field created by the polarized conducting object. So yes, it does increase
 
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
I was thinking using 2 purple mattress samples, and taping them together, I do want other ideas though, the main guidelines are; Must have a volume LESS than 1600 cubic centimeters, and CAN'T exceed 25 cm in ANY direction. Must be LESS than 1 kg. NO parachutes. NO glue or Tape can touch the egg. MUST be able to take egg out in less than 1 minute. Grade A large eggs will be used.
Back
Top