How to Use Poisson's Equation to Find V Between Two Infinite Parallel Plates?

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Homework Help Overview

The problem involves using Poisson's equation to determine the electric potential V between two infinite parallel plates separated by a distance s, with specified boundary conditions and a varying space charge density. The context is rooted in electrostatics and potential theory.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to apply Poisson's equation but expresses uncertainty about their approach. Some participants suggest using differential equations, while others clarify the nature of the equation involved. There is a focus on integrating and considering boundary conditions.

Discussion Status

The discussion is ongoing, with participants providing feedback on attempts and suggesting corrections. There is an acknowledgment of the need for an integration constant in the solution process, indicating a productive direction in the exploration of the problem.

Contextual Notes

Participants are navigating the implications of boundary conditions and the specific form of the charge density, which may influence the potential calculation. The original poster's initial attempts have not yet led to a complete solution.

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Homework Statement



Two infinite parallel plates separated by a distance s are at potential 0 and V_0
a) Use Poisson's eqn to find potential V in the region between the plates where the space charge density is rho = rho_0(x/s). The distance x is measured from the plate at 0 potential.
b)What are the charge densities in the plate?

Homework Equations


[tex]\nabla[/tex][tex]^2{}[/tex] V = - rho/ epsilon_0


The Attempt at a Solution


For this problem, I started with number of ways but none of them seem to be working. What will be V in this case?
 
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Why don't you show me what you've tried?
 
V will be in only x direction and it won't be in y and z direction. double partial derivative of V along x will be equal to -rho/epsilon_0. I was thinking of using differential equation but I am not sure.
 
You will need to use a differential equation. Luckily if V is only a function of x, then

[tex]\frac{\partial ^2V}{\partial x^2}=\frac{d^2V}{dx^2}[/tex]

And so you will have an ordinary differential equation instead of a partial differential equation.

Give integrating it a shot and show me what you get.
 
i got V = -(rho_0 * x^3)/(s* epsilon_0*6) and for charge densities I got rho = 0 at the plate with V = 0 and rho = rho_0 for the plate with V = V_0. does this look right?
 
Your V looks close, but there is a small error. On your first integration, you must include an integration constant:

[tex]\frac{d^2V(x)}{dx^2}=\frac{-\rho_0x}{s \epsilon _0} \Rightarrow \int_{x'=0}^{x'=x} \frac{d^2V(x')}{dx'^2} dx'= \int_0^x \frac{-\rho_0x'}{s \epsilon _0}dx'[/tex]

[tex]\Rightarrow V'(x)-V'(0)=\frac{-\rho_0x^2}{2s \epsilon _0} \Rightarrow V'(x)=\frac{dV(x)}{dx}=\frac{-\rho_0x^2}{2s \epsilon _0}+C[/tex]

where [itex]C=V'(0)[/itex] is the constant of integration

What do you get for V(x) when you don't forget the constant?
 

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