## 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 76

The surface of the

everywhere. What particular value of 0 will make E=0 for all points outside the

charged

The surface of the

**cylinder**carries a charge of constant surface density 0. Find Eeverywhere. What particular value of 0 will make E=0 for all points outside the

charged

**cylinder**? ls your answer reasonable? 4-4 A charge of constant volume ...Page 208

We can go even further with what we found for the complete system of Figure 5-7.

Suppose that one of the equipotential

conductor occupying the volume enclosed by the

conductor ...

We can go even further with what we found for the complete system of Figure 5-7.

Suppose that one of the equipotential

**cylinders**were replaced by a solidconductor occupying the volume enclosed by the

**cylinder**. The surface of theconductor ...

Page 358

The appropriate cavity is thus a thin right

perpendicular to the direction of B there as shown in Figure 20-6. Since, by

construction, only normal components are involved, we see that the value of B in

the ...

The appropriate cavity is thus a thin right

**cylinder**cut in the material with its baseperpendicular to the direction of B there as shown in Figure 20-6. Since, by

construction, only normal components are involved, we see that the value of B in

the ...

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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