## 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 347

netic with susceptibility \mJ < 0 while everything else is unchanged. Find H, B, M,

and Jn, for all points of

boundary conditions are satisfied at p - a. 20-25 Consider the same coaxial line ...

netic with susceptibility \mJ < 0 while everything else is unchanged. Find H, B, M,

and Jn, for all points of

**region**1 and plot your results. Verify that the appropriateboundary conditions are satisfied at p - a. 20-25 Consider the same coaxial line ...

Page 351

Figure 21 -2. The displacement current between the plates of a parallel plate

capacitor being charged. J- (21-8) becomes H^2mp as usual so that H9(p) = 2 "

no (21-13) It will be helpful to divide space into the four

21-3.

Figure 21 -2. The displacement current between the plates of a parallel plate

capacitor being charged. J- (21-8) becomes H^2mp as usual so that H9(p) = 2 "

no (21-13) It will be helpful to divide space into the four

**regions**shown in Figure21-3.

Page 430

In the two preceding chapters, we have considered time-dependent solutions of

Maxwell's equations in the form of plane waves of infinite extent so that they

necessarily exist in unbounded

there ...

In the two preceding chapters, we have considered time-dependent solutions of

Maxwell's equations in the form of plane waves of infinite extent so that they

necessarily exist in unbounded

**regions**. In more realistic cases, we can expectthere ...

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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