Boundary Value and Separation of Variables.

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To solve problems without boundary conditions in the form of electric potential, one can utilize the equation V = - ∫ E · dl. Choosing an appropriate reference point is crucial for this method. A common approach is to make an educated guess for a simple potential V that meets the differential equation's requirements. After establishing a potential, the next step is to apply the given boundary conditions to refine the solution. This method effectively addresses the challenge of missing boundary conditions in electrostatic problems.
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Homework Statement
Consider a rectangular box with sides, ##0\leq x \leq a##, ##0\leq y \leq b##, ##0\leq z\leq c##
The potential is 0 on four sides of the box: ##x=0##, ##x=a##, ##y=0##, ##y=b##, except at ##z= 0## and ##z = c##, (top and bottom) with electric field ##E_0 = E_z = constant##
Relevant Equations
##\nabla^2 V = 0##
If the boundary condition is not provided in the form of electric potential, how do we solve such problem?
In this case, I want to use ##V = - \int \vec{E} \cdot{d\vec{l}}##, but I don't know how to choose an appropriate reference point.
 
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You have a second order differential equation with first order (##\vec E = \vec\nabla V\ ## given) boundary conditions.
Make a guess for a simple ##V## that satisfies the equation and fill in the boundary conditions.
 
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