## 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 354

Although the boundary conditions at a surface of discontinuity can always be

obtained from

usual and convenient to list them separately. They are given by (10-42), (9-16)

and ...

Although the boundary conditions at a surface of discontinuity can always be

obtained from

**Maxwell's equations**and our general results from Chapter 9, it isusual and convenient to list them separately. They are given by (10-42), (9-16)

and ...

Page 355

In a similar manner, one can write the basic equations in terms of the pairs (E, H),

(D, B), and (D, H) if it is desirable and the terms that arise can be interpreted in

the same way. The so-called integral forms of

In a similar manner, one can write the basic equations in terms of the pairs (E, H),

(D, B), and (D, H) if it is desirable and the terms that arise can be interpreted in

the same way. The so-called integral forms of

**Maxwell's equations**are obtained ...Page 362

21-5 Starting with the Lorentz force (21-29) and

derive Coulomb's law (2-3). 21-6 Assume that a certain distribution of free

charges and currents (p{,Ji) results in an electromagnetic field Eu Bu H,, and D,,

that is, ...

21-5 Starting with the Lorentz force (21-29) and

**Maxwell's equations**for vacuum,derive Coulomb's law (2-3). 21-6 Assume that a certain distribution of free

charges and currents (p{,Ji) results in an electromagnetic field Eu Bu H,, and D,,

that is, ...

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