## 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 107

If we also integrate from the positive

direction so that ds= dri, then (6-38) becomes 1;----1:.2.::- ass)-4 which gives us

the same result for C as we found before in (6-37); this time the result has been ...

If we also integrate from the positive

**plate**to the negative**plate**in the radialdirection so that ds= dri, then (6-38) becomes 1;----1:.2.::- ass)-4 which gives us

the same result for C as we found before in (6-37); this time the result has been ...

Page 193

10-28 The region between the

filled with two_l. i. h. dielectrics with permittivities shown. The total volume is

divided exactly into halves by a plane that passes through the common center of

the ...

10-28 The region between the

**plates**of the spherical capacitor of Figure 10-20 isfilled with two_l. i. h. dielectrics with permittivities shown. The total volume is

divided exactly into halves by a plane that passes through the common center of

the ...

Page 393

Example Charging capacitor. In Figure 21-1, we have a side view of a parallel

vacuum between the

between ...

Example Charging capacitor. In Figure 21-1, we have a side view of a parallel

**plate**capacitor with circular**plates**of radius a. For simplicity, we assume avacuum between the

**plates**, and, as usual, we also assume that the separationbetween ...

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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