Potential in the three regions of an infinite slab

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SUMMARY

The discussion focuses on the boundary conditions for electric fields and potentials in the context of an infinite slab. It establishes that the electric field and electric potential must remain continuous across boundaries, with the potential having the flexibility of a reference point. The confusion arises regarding the justification for the condition ##E_{\text{at} \, z = 0} = 0##, which is derived from the symmetrical nature of the charge distribution. The importance of using LaTeX for clarity in mathematical expressions is also emphasized.

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Homework Statement
The charge density in the region
-z’<z<z’
depends only on z; that is,
p=p’cos(pi z/z’)
where p’ and z’ are constants. Determine the potential in all regions of space
Relevant Equations
Poisons equation, laplace equation
for the boundary conditions for this problem I understand that Electric field and Electric potential will be continuous on the boundaries.
I also know that I can set the reference point for Electric potential, wherever it is convenient. This gives me the fifth boundary condition. I am confused at where I find the last boundary condition.

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You cannot arbitrarily choose a "zero point" for the electric field like you can with the potential. However, can you justify the condition ##E_{\text{at} \, z = 0} = 0## from the symmetrical nature of the charge distribution in this problem?
 
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