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BOUNDARY VALUE PROBLEMS WITH LINEAR DIELECTRICS We have shown that the bound volume charge density bound is proportional to the free charge volume density
What happens at the boundary / interface between two Linear dielectrics?
We have the boundary condition
boundary condition
for linear dielectrics
And
(eq. 2.34)
Example
Consider a hemispherical linear dielectric of radius R placed in between two infinite conducting parallel plates
far away from the hemisphere (r>>R)
We want to know/determine the following quantities: Inside the dielectric (r < R): Outside the dielectric (r > R):
Since there is NO volume free charge density inside the dielectric, therefore
However, at r=R: i.e. a bound surface charge density will exist on/at the surface of the hemispherical dielectric. 1. Since
, then
2. Note also that this problem has azimuthal / axial symmetry, therefore V, E, D, P have NO ϕ -dependence Therefore, the general solution can be represented in terms of Legendré polynomials
boundary conditions
since
Now, we can solve this problem directly.
Example 4.7 A dielectric sphere is placed in a Uniform electric field, find the electric field inside the sphere.
Boundary conditions:
Example 4.7 (conti.) Solution of Laplace’s equation
Therefore
BC3
Example 4.7 (conti.) BC1
BC2
Example 4.7 (conti.) Therefore
Energy in dielectric systems As ρf is increased by an amount Δρf, the work done is
Since
integrating by parts
By divergence theorem, vanishes as →∞
Energy in dielectric systems (conti.) Therefore For linear dielectric material
compare
Forces on dielectrics w
L dielectric
x
Assume Q=constant
Forces on dielectrics (conti.) Therefore
In this case,
( Check it by yourself)