How to Determine Electric Displacement in a Linear Dielectric Capacitor?

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SUMMARY

The discussion focuses on determining the electric displacement field (D) in a parallel-plate capacitor filled with two linear dielectric slabs. Slab 1 has a dielectric constant of 2, while slab 2 has a dielectric constant of 1.5, with a total separation of 2a between the plates. The electric displacement D is established as equal to the free charge density sigma for each slab, directed downward when fringing effects are neglected. The relationship between D and the electric field E is clarified, emphasizing that inside the dielectric, D equals epsilon times E.

PREREQUISITES
  • Understanding of Gauss's Law for dielectrics
  • Familiarity with dielectric constants and their implications
  • Knowledge of electric displacement field (D) and electric field (E) relationships
  • Basic concepts of parallel-plate capacitors
NEXT STEPS
  • Study the application of Gauss's Law in different dielectric materials
  • Learn about the effects of fringing fields in capacitors
  • Explore the differences between electric displacement (D) and electric field (E) in SI and Gaussian units
  • Investigate the behavior of electric displacement in capacitors with varying charge distributions
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Students and professionals in electrical engineering, particularly those studying electromagnetism, capacitor design, and dielectric materials.

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Homework Statement


Griffith's Problem 4.18
The space between the plates of a parallel-plate capacitor (in the figure) is filled
with two slabs of linear dielectric material. Each slab has thickness a, so the total distance between the plates is 2a. Slab 1 has a dielectric constant of 2, and slab 2 has a dielectric constant of 1.5. The free charge density on the top plate is sigma and on the bottom plate -sigma.Find the electric displacement D in each slab.


Homework Equations


Gauss law for dielectrics
\int D \cdot dA = Q_{f,enc}

The Attempt at a Solution



In the diagram i have posted, the top and bottom 'gaps' are the metal slabs that make up this capacitor.
For the electric displacement in the top slab where epsilon = 2
The free charge on the upper boundary of this slab is +sigma. But there is some charge going to be present within the slab as well... but that's bound charge right... so we need not worry?
The electric displacement is just +sigma for this slab. but what is the direction? I am tempted to say that it points downward because it only seems natural (positive to negative) but what if there were no negative charge involved in the question? What then?

What if in the question the bottom slab was of some charge +sigma? The free charge on the top slab is still sigma but would the direction of D be pointing downward?

Thanks for your help and input.
 

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D=\sigma, and D_n is continuous.
D is straight down if fringing is neglected.
If both plates had +Q, everything is different.
D would flare out on each side.
By Gauss's law, D would have to be large outside.
 
clem said:
D=\sigma, and D_n is continuous.
D is straight down if fringing is neglected.
If both plates had +Q, everything is different.
D would flare out on each side.
By Gauss's law, D would have to be large outside.

so D is just like an electric field ... but how is it different??
 
Outside the dielectric D and E should be the same, and are in gaussian units.
In SI, they are given different units for some reason.
Inside the dielectric D=epsilon E.
 

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