## 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 95

We will not consider this problem all at once, but in this chapter we restrict

ourselves to the case in which a particular class of matter known as

present. Because of the special properties of

deduce ...

We will not consider this problem all at once, but in this chapter we restrict

ourselves to the case in which a particular class of matter known as

**conductors**ispresent. Because of the special properties of

**conductors**, we will be able todeduce ...

Page 100

The

will be an equipotential volume. In fact, the potential within the cavity will be the

same as ...

The

**conductor**C is in a cavity in the**conductor**C. within a cavity inside a**conductor**, the electric field will be always zero within the cavity, and the cavitywill be an equipotential volume. In fact, the potential within the cavity will be the

same as ...

Page 103

6-3 Capacitance One of the earliest uses of

the storage of electric charge; the

giving it a definite potential by means of a battery. For such an application, one ...

6-3 Capacitance One of the earliest uses of

**conductors**in electrostatics was forthe storage of electric charge; the

**conductor**could be charged, for example, bygiving it a definite potential by means of a battery. For such an application, one ...

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angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law cross section current density current element curve cylinder defined dielectric direction displacement distance electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge free currents frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz Lorentz transformation magnitude material Maxwell's equations molecule normal components obtained origin particle perpendicular plane wave point charge polarized position vector potential difference propagation properties quadrupole quantities radiation region relation result satisfy scalar potential shown in Figure situation solenoid spherical substitute surface current surface integral tangential components total charge unit vacuum vector potential velocity volume write written xy plane zero