## 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 456

These cases correspond to XL being greater than, equal to, or less than Xc. For

given circuit parameters, we see from (27-23) that # = 0 for the

^ (27-26) LC Although this is not the same as the natural

These cases correspond to XL being greater than, equal to, or less than Xc. For

given circuit parameters, we see from (27-23) that # = 0 for the

**frequency**1 «„ = ^^ (27-26) LC Although this is not the same as the natural

**frequency**un that we ...Page 556

It turns out that the

values of Bm. As a result we can approximate w + «0 by 2<o0 and replace « by

w0 in the right-hand side; we therefore find that A« = <o - <o0 = ± ^—Bm (B-42) ...

It turns out that the

**frequency**change Aw = u - «0 is very small even for very largevalues of Bm. As a result we can approximate w + «0 by 2<o0 and replace « by

w0 in the right-hand side; we therefore find that A« = <o - <o0 = ± ^—Bm (B-42) ...

Page 568

As the

it becomes equal to at least some of the natural

electrons. Then their resonant contributions become important and comparable

to or ...

As the

**frequency**increases into the infrared and visible portions of the spectrum,it becomes equal to at least some of the natural

**frequencies**of the boundelectrons. Then their resonant contributions become important and comparable

to or ...

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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