## 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 397

These differential source equations must of course be supplemented by the

defining equations (10-40) and (20-28), ... It is often convenient to have

.

These differential source equations must of course be supplemented by the

defining equations (10-40) and (20-28), ... It is often convenient to have

**Maxwell's****equations**expressed in terms of only two vectors—one electric and one magnetic.

Page 398

Two of these equations are unchanged from before and the other two are no

longer quite as compact since the properties of ... The so-called integral forms of

and ...

Two of these equations are unchanged from before and the other two are no

longer quite as compact since the properties of ... The so-called integral forms of

**Maxwell's equations**are obtained by combining the divergence theorem (1-59)and ...

Page 406

21-3 Express the general form of

each of the following pairs: (E,H), (D, B), and (D, H). In other words, find the

analogues of (21-30) through (21-33) for each of these pairs. 21-4 Express the

general ...

21-3 Express the general form of

**Maxwell's equations**completely in terms ofeach of the following pairs: (E,H), (D, B), and (D, H). In other words, find the

analogues of (21-30) through (21-33) for each of these pairs. 21-4 Express the

general ...

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amplitude angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb’s law cross section current density current element cylinder defined dielectric displacement distance electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point Flgure flux force free currents frequency function Galilean transformation given incident induction infinitely long integral integrand length located loop Lorentz Lorentz transformation magnetic dipole magnitude material Maxwell’s equations medium normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector produced quadrupole quantities radiation radius rectangular reﬂected region relation result rotation satisfy scalar potential shown in Figure solenoid sphere substitute surface charge surface current tangential components transformation unit vacuum vector potential velocity volume write written xy plane zero