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

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SUMMARY

This discussion focuses on solving Poisson's equation to determine the electric potential V between two infinite parallel plates separated by a distance s, with a space charge density defined as ρ = ρ₀(x/s). The equation used is ∇²V = -ρ/ε₀, leading to the ordinary differential equation d²V/dx² = -ρ₀x/(sε₀). The potential V is derived as V(x) = -(ρ₀x³)/(6sε₀) + C, where C is the integration constant. The charge densities at the plates are confirmed as ρ = 0 at V = 0 and ρ = ρ₀ at V = V₀.

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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


\nabla^2{} 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

\frac{\partial ^2V}{\partial x^2}=\frac{d^2V}{dx^2}

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:

\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'

\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

where C=V'(0) is the constant of integration

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

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