Boundary, capacitance and Laplace Eqn Apr. 4, 2007
+
Boundary conditions at 2 different media:
tangential component:
normal component:
step: 1) identify normal to the boundary (
goes
from medium 2 to 1),
2) get the
or
at the boundary
by substituting equation of the boundary,
3) apply boundary conditions
component by component
+
Capacitance C=q/V (Sect. 3.9)
step: 1) Assume +q on one plate and -q on the other,
2) find
for the given charge distribution,
3) relative potential of 2
plates
and find C (F)
parallel capacitor =
series capacitor =
+
Electrostatic energy: (Sect. 3.10.1)
density
energy
+
Recap: capacitance C=q/V (pp. 116-126)
Boundary conditions (Sect. 3.8)
Polarization and dielectric (pp. 102-107)
+
Method of image (Sect. 3.11.5)
Charge in front of a grounded conductive planes is similar to an object
facing a mirror.
The whole system can be replaced by an
"equivalent charge diagram" with real and image charges.
Image charge has opposite charge of the real one and locates
behind the conductor.
Equivalent diagram is valid for the space occupied by the real charge(s),
i.e. in front of the conductor.
+
Poisson's equation (Sect. 3.11.1):
.
Relating (free volume) charge density and potential.
Apply to regions with uniform permittivity, e.g. semi-conductors (diode)
+ Laplace's equation:
For region without free charges, Laplace's equation
holds
e.g. capacitors.
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HW #17 (no late homework) Due 4/10/07
is unchanged for R>b.)
and
V, find a)
and
, b)
and
.
and
.
If we know that
in region 1 is
, what
are the expressions for
and
in region 2?
Can we apply these expressions to the whole region 2? Explain.
(modified Problem 3.18 on page 145)
(Note: This a boundary problem. Do not forget to substitute the equation
of the boundary.)
is placed in air with relative permittivity
.
The electric field intensity in air
.
i. Find the unit vector that is normal to the air-glass boundary;
ii. Find electric field intensity,
and electric flux
density,
inside the sphere at the air-glass boundary;
iii. Find the bound surface charge density at the air-glass boundary.