Dieletric Boundary Conditions (Parallel Plate Capacitor)

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SUMMARY

The discussion centers on the dielectric boundary conditions for a parallel plate capacitor, specifically focusing on the equations derived from the boundary conditions for the electric displacement field, D. The user expresses confusion regarding the interpretation of surface charge densities labeled as ρs0, ρs1, ρs2, and ρs3, questioning their relation to the capacitor plates and dielectric material. The conservation of charge is highlighted, indicating that ρs0 equals -ρs3 and ρs1 equals -ρs2, although the user seeks clarification on the mathematical justification for these relationships.

PREREQUISITES
  • Understanding of electric displacement field (D) in electromagnetism
  • Familiarity with boundary conditions in electrostatics
  • Knowledge of surface charge density concepts
  • Basic principles of conservation of charge
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  • Review the derivation of boundary conditions for electric fields in dielectrics
  • Study the relationship between surface charge densities and electric fields in capacitors
  • Examine the mathematical proof of conservation of charge in electrostatics
  • Explore the implications of dielectric materials on capacitance and electric fields
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Students and professionals in electrical engineering, physics, and anyone studying electrostatics, particularly those focusing on capacitors and dielectric materials.

jegues
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Homework Statement



See figure attached for problem statement, as well the solution.

Homework Equations





The Attempt at a Solution



I'm confused as to how he is writing these equations from the boundary conditions.

What I understand as the boundary condition for D is,

\hat{n} \cdot \vec{D_{1}} - \hat{n} \cdot \vec{D_{2}} = \rho_{s}

With the normal vector directed from region 1 to region 2.

With this I only generated 2 equations, as there is only 2 boundarys; one being from d1 to d2 and the other from d2 to d3.

He labels,

\rho_{s0}, \rho_{s1}, \rho_{s2}, \rho_{s3}

I'm confused as to what these surface charge densities pertain to? Is the surface charge density with subscript 0 and 3 the charge on the plates of the capacitor? Are 1 and 2 the surface charge densities on the faces of the dielectric material?

He states by conservation of charge that,

\rho_{s0} = -\rho_{s3}, \quad \rho_{s1} = -\rho_{s2}

This doesn't seem obvious to me at all. Can someone show me how he is drawing such a conclusion? (Is there some math behind it?)
 

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Bump, still looking for some help on this confusion please!
 

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