## Electromagnetic fieldsThis revised edition provides patient guidance in its clear and organized presentation of problems. It is rich in variety, large in number and provides very careful treatment of relativity. One outstanding feature is the inclusion of simple, standard examples demonstrated in different methods that will allow students to enhance and understand their calculating abilities. There are over 145 worked examples; virtually all of the standard problems are included. |

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Page 83

Now let us consider the

the nearby vacuum region certainly can be different from zero. Suppose that E

made an angle with the surface as shown in Figure 6-la. We can imagine E ...

Now let us consider the

**situation**at the surface of a conductor. The electric field inthe nearby vacuum region certainly can be different from zero. Suppose that E

made an angle with the surface as shown in Figure 6-la. We can imagine E ...

Page 132

As soon as we consider the possibility of matter being present and subject to the

influence of other charges, we realize that we may need to consider a

which we have two kinds of matter meeting at a common boundary.

As soon as we consider the possibility of matter being present and subject to the

influence of other charges, we realize that we may need to consider a

**situation**inwhich we have two kinds of matter meeting at a common boundary.

Page 274

The

the same numerical value as the motional emf given by (17-33) for the previous

example, but now we are talking about a completely different concept.] What is ...

The

**situation**as seen by the observer moving with the rod. [We note that this hasthe same numerical value as the motional emf given by (17-33) for the previous

example, but now we are talking about a completely different concept.] What is ...

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### Common terms and phrases

angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conducting conductor const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux free charge function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz transformation magnetic magnitude Maxwell's equations normal component obtained origin parallel plate capacitor particle perpendicular point charge polarized position vector potential difference quadrupole quantities rectangular coordinates region result satisfy scalar potential shown in Figure situation solenoid solution sphere of radius spherical surface charge surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero