## 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 179

variation on the previous

neutral, and is no longer kept at a definite potential. In the presence of q, the

sphere ...

**Example**Point charge and an insulated uncharged conducting sphere. This is avariation on the previous

**example**. The sphere is assumed to be originallyneutral, and is no longer kept at a definite potential. In the presence of q, the

sphere ...

Page 326

Furthermore, if we have already solved the analogous electrostatic problem, we

can simply take over the solution by making the replacements e0E -* H, e0<//> -»

</>„,, P -» M, and so on. For

...

Furthermore, if we have already solved the analogous electrostatic problem, we

can simply take over the solution by making the replacements e0E -* H, e0<//> -»

</>„,, P -» M, and so on. For

**example**, we can write down the integral from which...

Page 402

As an

24-19) with the same values of k and <o, that is, they are traveling in the same

direction with the same velocity. Suppose, however, that they have different ...

As an

**example**, consider two plane waves i^, and \p2 tnat are each °& me form (24-19) with the same values of k and <o, that is, they are traveling in the same

direction with the same velocity. Suppose, however, that they have different ...

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angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conducting conductor const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux free charge function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz transformation magnetic magnitude Maxwell's equations normal component obtained origin parallel plate capacitor particle perpendicular point charge polarized position vector potential difference quadrupole quantities rectangular coordinates region result satisfy scalar potential shown in Figure situation solenoid solution sphere of radius spherical surface charge surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero