## 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 152

"Property" 4/ layer l-#4 Transition x

layer between two media. "Property" 1 2 Surface of discontinuity

idealized surface of discon,, tinuity between two media. regarded as possibly ...

"Property" 4/ layer l-#4 Transition x

**Flgure**9-1. The physical origin of a transitionlayer between two media. "Property" 1 2 Surface of discontinuity

**Flgure**9-2. Theidealized surface of discon,, tinuity between two media. regarded as possibly ...

Page 259

(a)

use this expression to compare this present approach with that of the last chapter.

If we have an infinitely long current parallel to the z axis, which passes through ...

(a)

**Flgure**14-3. Calculation of B due to a straight current of finite length. We canuse this expression to compare this present approach with that of the last chapter.

If we have an infinitely long current parallel to the z axis, which passes through ...

Page 291

In Figure 16-5 we show an end-on view of the solenoid with the K ~

End-on view of a long ideal.

long straight currents. in (16-23) is a circle of radius p for which. INFINITELY ...

In Figure 16-5 we show an end-on view of the solenoid with the K ~

**Flgure**16-5.End-on view of a long ideal.

**Flgure**16-4. Lines of B produced by two antiparallellong straight currents. in (16-23) is a circle of radius p for which. INFINITELY ...

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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