Free surface charge density (not bound density)

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SUMMARY

The discussion focuses on calculating the free surface charge density in a parallel plate capacitor with a dielectric of relative permittivity 5.0, separated by 0.20 mm and subjected to a potential difference of 500V. The boundary conditions for electric displacement, D1 and D2, are confirmed to be equal, leading to the conclusion that the free surface charge density is zero. The polarization of the dielectric material is calculated as 3.54 x 10-9 Cm-2, and the relationship between electric field (E), displacement (D), and surface charge density is established. Fringing effects are noted as a consideration for practical applications.

PREREQUISITES
  • Understanding of parallel plate capacitors
  • Familiarity with electric displacement (D) and polarization (P)
  • Knowledge of boundary conditions in electrostatics
  • Basic principles of dielectrics and their properties
NEXT STEPS
  • Study the derivation of electric displacement in dielectrics
  • Learn about the effects of fringing fields in capacitor design
  • Explore the relationship between electric field strength and potential difference in capacitors
  • Investigate advanced topics in electrostatics, such as boundary value problems
USEFUL FOR

Students in electrical engineering, physicists studying electrostatics, and anyone involved in capacitor design and analysis will benefit from this discussion.

Roodles01
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Homework Statement


a parallel plate capacitor has 2 plates separated by a dielectric of rel. permittivity 5.0 are separated by 0.20mm and have area of 5.0 cm2.
Potential difference between the plates is 500V.

I need to be able to calculate the free surface charge density.




Homework Equations


I'm assuming Dout = Din

From boundary conditions D1 ┴ = D2
and D2 ┴ - D1 ┴ = σf

Could someone just confirm what the boundary conditions are so I can say that the free surface charge density is zero or not!


The Attempt at a Solution



I have Dout = Din = ε0Ein + P
so from calculations
P = 4.43x10-9 - (8.85x10-12 x 100)
P = 3.54x10-9 Cm-2

Could I just say;
D1 ┴ = D2 ┴ so there is zero free surface charge density!
 
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Sorry, I should have said.
D1 ┴ is the electric displacement in media 1 perpendicular to a boundary with a different media
D2 ┴ is the electric displacement in media 1 perpendicular to a boundary with a different media

They form the boundary condition
Roodles01 said:
Dout = Din
could have been
D1 = D2.

and P is the polarization of the material.
 
I don't know what you mean by "different media" or "Dout" vs. "Din". There is only one medium, the dielectric of epsilon_relative = 5.

D is continuous from one medium to another along the plates' normal even if there were two or more media, but there aren't.

So V = E x d, d = 0.2mm so you know E.
Then, D = epsilon x E.
And if you know D you know the surface charge density, right?

This ignores fringing effects of course which you have to do since they didn't give you the dimensions of the plates.
 

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