Potential in parallel plate system from charge density?

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Homework Help Overview

The discussion revolves around determining the potential in a parallel plate system influenced by charge density. The original poster considers using Poisson's equation and relates the problem to a parallel plate capacitor, expressing confusion over the application of boundary conditions and the role of dielectric materials.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of Poisson's equation and boundary conditions, with attempts to integrate and apply conditions for potential at specific points. Questions arise regarding the treatment of the coordinate system and the implications of dielectric materials.

Discussion Status

Some participants have offered guidance on interpreting the results and the relevance of the coordinate variable in the context of the problem. There is an acknowledgment of potential misunderstandings, but no explicit consensus on the resolution of the problem has been reached.

Contextual Notes

Participants express uncertainty about the appropriateness of using images for notation and the limitations of their mathematical expression capabilities. There is also mention of the need to substitute expressions for charge density, indicating a focus on the relationship between variables.

smileandbehappy
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Homework Statement



16987125673_015172f5f0_b.jpg


Note - I have used an image here. For the simple reason I don't want to confuse anyone by missing out subscripts. But if that is not acceptable let me know and I will attempt to write it out.

Homework Equations



I have considered using Poissons equation - but couldn't get that to work.

I have also attempted to consider this as a parallel plate capacitor, so: u = 0.5e(o)E^2

The Attempt at a Solution



I am getting stuck with this. Annoyingly I think it's probably quite simple - but it's confusing me.

I have drawn a diagram here to understand what is going on, but I don't think I am allowed to post too many photo's. And have no idea how to draw that on a computer.

So I thought I could find the E field magnitude. To do this I could use the boundary conditions. But I am not going from air into a dialectic medium. So I got a bit confused there. I don't think I can say the E=V/d because of the dialectic material - however I do think I can say: E = eV/d

Subsitituting this into the above equation I get:

u = 0.5e(0)(eV/d)^2

Now the change in V is going to be V(0) so:

u = 0.5e(0)e^2V(o)^2/d^2

And I know that charge density = charge/volume

therefore: charge/volume = p(0)/d

But here I get stuck... I am at a bit of a loss. As I've said I think it's probably simpler than I am making it. But some hints would be amazing.

Thanks

Sam
 
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smileandbehappy said:
I have considered using Poissons equation - but couldn't get that to work.

What were your thoughts on this exactly?
 
Well as the plates are infinitely long - you are only dealing with d^2x/dx^2 = -p/e

So I tried to integrate this twice to solve the equation - and then applied boundary condition are V(x=0)=0 and V(x=d) = V(o)

But I still have no idea where to go after this...
 
If you have done things correctly, you then have the potential and there should not be anywhere else to go ...
 
Orodruin said:
If you have done things correctly, you then have the potential and there should not be anywhere else to go ...

Here is my problem - I am not doing it properly, or not understanding the question then!

I've posted my work below. I can't type that out, as I don't know how to put the differentials in etc... Or the integral signs. But I am not sure how to do get rid of the x. I am failing to understand this badly.

17423993030_a83193ed1f_b.jpg


Basically - I am doing something awfully wrong. I though x=d, but when I do that all I get is V = V(o) which is clearly not what they are after.
 
Last edited:
Why do you want to put x = d? The coordinate x is perfectly fine as a parameter in your answer as it describes the potential at the point x. Since the problem asks for the potential at any point, the result will generally be a function of the point, in this case x. You have essentially solved the problem without realising that you already have the answer.
 
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Thanks on both making me see how stupid I am being - and pointing out how I can use latex. I think I am trying to make a lot of this stuff harder than it has to be... Either that or I'm just a bit thick. But I appreciate you helping me out. So all I need to do now is substitute in the expression for the charge density and I'm good to do.

Thanks again.
 
smileandbehappy said:
I think I am trying to make a lot of this stuff harder than it has to be...
Some of the most difficult problems are those whose answers are staring us in the face ... :smile:
smileandbehappy said:
So all I need to do now is substitute in the expression for the charge density and I'm good to do.
Yes.
 

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