Recommended reading for Lecture 8: Chap. 25, pp661-680
Problem solving - Finding the electric field
We now have two methods for finding the electric field
due to either discrete charges or due to continuous
distribution of charges. The first is the direct
method where we carried out a vector sum of the
contributions due to point charges ie. a sum of
terms like
.
The second method is
to use Gauss' law. Here are some guidlines for the
best method to solve different types of charge
distribution:
Direct method Discrete charge distributions,
ring of charge, finite lines of charge, finite sheets
of charge.
Gauss' law Spherical shells of charge,
sphere's of charge, infinite sheets of charge, infinite
rods of charge. Electric field near the surface of
a conductor.
Gauss' law calculations
Infinite uniform rod of charge density
Assume the rod has radius a. Use Gauss' law.
Choose a cylindrical Gaussian surface, S, of radius
r>a and length L.
The electric flux is given by,
(1) |
(2) |
(3) |
Uniform sphere of charge
Consider a sphere of radius a which has uniform charge density throughout. Find the electric field inside and outside
of this sphere. Use Gauss' law. Choose the Gaussian
surface to be the surface of a sphere. For a surface
of radius r, the electric flux is given by,
(4) |
(5) |
(6) |
(7) |
(8) |
We also went through problem 24.26
Electric potential energy and electric potential
The electric potential energy (U) is the potential energy due to the electrostatic force. As always we use only differences in potential energy. However we define a reference potential energy and make calculate all differences in potential energy with respect to this reference. In electrostatics, the potential energy is defined to be zero when the charges are an infinite distance apart.
The difference in potential energy in moving a charge
between two positions a and b is defined in terms of the
work done in moving the charge between these two positions, so that,
(9) |
Instead of using the Coulomb force, we defined the electric field
which is the force per unit charge. In the same way we define
the electric potential, V, to be the potential
energy per unit charge, ie. U=qV.
The electric potential is so important it is given its
own unit, the volt (V). In terms of the electric potential,
equation (9) is,
(10) |