## 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 390

Find H, B, M, and J,,, for all points of

appropriate boundary conditions are satisfied at p=a. 20-25 Consider the same

coaxial line as discussed at the end of Section 20-5, except that

between ...

Find H, B, M, and J,,, for all points of

**region**1 and plot your results. Verify that theappropriate boundary conditions are satisfied at p=a. 20-25 Consider the same

coaxial line as discussed at the end of Section 20-5, except that

**region**2between ...

Page 394

Thus we have the equivalent of a uniform current density between the plates as

shown in Figure 21-2; we use the word “equivalent” because there is no transfer

of real charge in the vacuum

...

Thus we have the equivalent of a uniform current density between the plates as

shown in Figure 21-2; we use the word “equivalent” because there is no transfer

of real charge in the vacuum

**region**between the plates, but, by (21-7), there is a...

Page 486

Chapter Fields in Bounded

considered time-dependent solutions of Maxwell's equations in the form of plane

waves of infinite extent so that they necessarily exist in unbounded

more ...

Chapter Fields in Bounded

**Regions**In the two preceding chapters, we haveconsidered time-dependent solutions of Maxwell's equations in the form of plane

waves of infinite extent so that they necessarily exist in unbounded

**regions**. Inmore ...

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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