2. Gauss’ Law and Applications
Let E be a simple solid region and S is the boundary surface of E with positive
orientation.Let F be a vector field whose components have continuous partial
derivatives,then
Coulomb’s Law
Inverse square law of force
In superposition, Linear superposition of forces due to all
other charges
3. Electric Field
Field lines give local direction of field
Field around positive charge directed
away from charge
Field around negative charge directed
towards charge
Principle of superposition used for field
due to a dipole (+ve –ve charge
combination).
qj +ve
qj -ve
4. Flux of a Vector Field
Normal component of vector field transports fluid across
element of surface area
Define surface area element as dS = da1 x da2
Magnitude of normal component of vector field V is
V.dS = |V||dS| cos(Y)
da1
da2
dS
dS = da1 x da2
|dS| = |da1| |da2|sin(p/2)
Y
dS`
5. Gauss’ Law to charge sheet AND
Plate
r (C m-3) is the 3D charge density, many applications make use
of the 2D density s (C m-2):
Uniform sheet of charge density s = Q/A
Same everywhere, outwards on both sides
Surface: cylinder sides
Inside fields from opposite faces cancel
+ + + + + +
+ + + + + +
+ + + + + +
+ + + + + +
E
EdA
++++++++++++++++++++++++
E
dA
6. Electrostatic energy of charges
In vacuum
Potential energy of a pair of point charges
Potential energy of a group of point charges
Potential energy of a charge distribution
In a dielectric (later)
Potential energy of free charges
Electrostatic energy of charge distribution
Energy in vacuum in terms
7. Stokes Theorem and
Applications
Let S be an oriented smooth surface that is bounded
by a simple, closed smooth boundary curve C with
positive orientation. Also let be a vector field then,
WORK :
- Boundary must be closed
- Transforms closed line integral into surface integral.
Stokes theorem combined with Gauss’s theorem can
be used for any surface and line integrals.
8. Green’s Theorem and
Applications
Let C be a positively oriented, piecewise smooth,
simple, closed curve and let D be the region
enclosed by the curve. If P and Q have
continuous first order partial derivatives on
D then,
Green's Theorem is in fact the special case of
Stokes Theorem in which the surface lies entirely
in the plane.
But with simpler forms. Especially, in a vector field
in the plane.
9. More of greens and Stokes
In terms of circulation Green's theorem
converts the line integral to a double integral
of the microscopic circulation.
Water turbines and cyclone may be a
example of stokes and green’s theorem.
Green’s theorem also used for calculating
mass/area and momenta, to prove kepler’s
law, measuring the energy of steady currents.
Electrodynamics is entirely based on green’s
theorem.