I Resultant of Different Permittivity substances

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In a scenario with two regions of different permittivity, e1 and e2, the force experienced by a charge q1 due to another charge q2 can be determined by calculating the electric field generated by each charge. This involves solving Maxwell's Equations, specifically focusing on the electric field and scalar potential in each region. The equations indicate that the electric field can be expressed as the negative gradient of the scalar potential, leading to the conclusion that the charge density is zero in most areas. The solution requires addressing the boundary conditions at the interface between the two media. This problem is similar to examples found in Griffiths and Jackson's electrodynamics texts.
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Say the space is divided into two parts: one has permittivity e1 and other e2. A charge q1 is placed at a distance d1 from the interface of two media in region in permittivity e1 and another charge q2 is placed at a distance d2 in region of permittivity e2. What is the force experienced by a charge due to the field of the other charge? How to calculate it?
 
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Solve Maxwell's Equations, to find electric field due to charges. Finding the force is then trivial.

Electrostatics is fine for this problem, so (##\vec{E}## - electric field, ##\phi## - scalar potential, ##\rho## - charge density)

##\vec{\nabla}.\vec{E}=\rho/\epsilon##
##\vec{\nabla}\times\vec{E}=\vec{0}##

Which is satisfied if ##\vec{E}=-\vec{\nabla}\phi## and ##\epsilon\nabla^2\phi=-\rho##. Since you have point-charges, the charge density is zero almost everywhere, so begin by solving ##\nabla^2\phi=0## in both domains and then determine how to stitch the solution at the boundary.
 
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Problem (or something very similar) is treated in

Griffiths "Introduction to Electrodynamics", Example 4.8 (Ch4)
Jackson "Classical Electrodynamics", Section 4.4
 
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