Chapter 24: Gauss's Law
Learning Goals
- Understand the concept of Electric Flux.
- Understand the formal definition of Gauss's Law
- Apply Gauss's law, and understand how to utilize symmetry.
- Understand how to use Gauss's law to determine important facts about
conductors.
Gauss's Law
The fact that we call this a law means that it is very
fundamental. In fact, it has the same relationship to
electromagnetic theory as Newtons laws do to mechanics:
it is one of Maxwell's equations.
In words, Gausss law states that the total outward electric
flux through a closed surface is proportional to the net
charge enclosed by the surface. In symbols:
Applications of Gausss Law
Although it is a powerful theoretical tool, Gausss law
is difficult to solve for all but the most symmetric
situations. When the charge distribution is very
symmetric, Gausss law becomes easy to apply. The steps
to follow when solving Gausss law for the electric field
due to a symmetric charge distribution are:
- Choose a Gaussian surface with the same symmetry
as your charge distribution.
- Evaluate the scalar product and field magnitude on
your surface and pull out any constants within the integrand.
- It should now be the case that the surface integral
evaluates to the area of a simple geometric surface.
- Evaluate the qin and solve for the
explicit form of the field magnitude.
You should be able to follow the above procedure to
solve for the electric field in the vicinity of spherical,
cylindrical, and plane distributions of charge.
Conductors
A conductor with excess charge carriers all at rest
(no currents) is said to be in electrostatic
equilibrium. Conductors in electrostatic equilibrium
have the following properties (which you should be able
to demonstrate):
- The electric field inside the conductor is zero
everywhere, regardless of any excess or
nearby electric charge.
- Any excess charge placed on the conductor resides
entirely on its surface.
- The electric field just outside the conductors
surface is perpendicular to that surface with
magnitude equal to
s/e0 ,
where s is the charge per
unit area at that point.
- On an irregularly shaped conductor, charge tends to
accumulate at sharp points and move away from
valleys.