In: Physics
W hat is polarization in dielectric? Derive the relation where symbols have their usual meaning.
Answer:
Polarization in dielectric medium:
If an external electric field is applied to a dielectric material then the electric field exerts a force on each charged particle in the material, pushes the positive charges along its own direction while the negative charge is displaced in opposite direction. Due to this effect, the centers of positive and negative charges of each atom are displaced from their equilibrium positions. Such a molecule or atom is then called as induced dielectric dipole and this process is known as dielectric polarization.
The induced dipole moment of an individual atom is proportional
to the applied electric field E and is given by p =
E,
where
is called
atomic polarizability. Its value depends on the detailed
structure of the atom.
A lot of little dipoles in the material pointing along the direction of the eternal electric field then the material becomes polarized. A convenient measure of this effect is P = dipole moment per unit volume, which is called Polarization.
Using Gauss's law in dielectric,
The total charge density in the dielectric is =
b +
f ,
where
b is the
bound charge density and
f is the
free charge density. Gauss's ;law states that ∇. E =
/
0
which implies that 0
∇. E =
=
b +
f = - ∇.
P +
f
Since bound charge density b = - ∇.
P
Therefore, ∇.(0E
+ P) =
f,
The expression in the parentheses, designated by the letter D.
D = (0E
+ P) is known as electric
displacement.
In terms of D, Gauss's law becomes ∇. D = f.
And polarization is proportional to the electric field , P =
0
eE,
where
e is
called the electric susceptibility of the medium.
In linear dielectric medium, D = 0E
+ P =
0E
+
0
eE =
0(1+
e)E
so D is also proportional to the electric field E, that means,
D = E
where, =
0(1+
e).
Here, the new constant
is called
the permittivity of the material
Finally. =
0(1+
e) =
0
r,
therefore the dimensionless quantity
r
=
/
0
= 1+
eand
it is known as relative permittivity or dielectric constant of the
material.