## 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 231

In (12-6), S can be either an open surface or a closed surface. If, for some reason,

the moving charges can be thought of as being constrained to flow on a surface,

we can define a

In (12-6), S can be either an open surface or a closed surface. If, for some reason,

the moving charges can be thought of as being constrained to flow on a surface,

we can define a

**surface current**density K. Its direction is that of the direction of ...Page 266

14-9 An infinite plane current sheet coincides with the xy plane. Its

parallel to the xy plane and intersects the positive z axis at z = d. The second

current ...

14-9 An infinite plane current sheet coincides with the xy plane. Its

**surface****current**density is K' = K'y where K' = const. Another infinite plane current sheet isparallel to the xy plane and intersects the positive z axis at z = d. The second

current ...

Page 355

Origin of magnetization

circulating in the same sense as shown in an end-on view in Figure 20-3. If we

consider the immediate neighborhood of an interior point, as indicated by the

dashed ...

Origin of magnetization

**surface currents**for a uniform magnetization. that is,circulating in the same sense as shown in an end-on view in Figure 20-3. If we

consider the immediate neighborhood of an interior point, as indicated by the

dashed ...

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angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law cross section current density current element curve cylinder defined dielectric direction displacement distance electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge free currents frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz Lorentz transformation magnitude material Maxwell's equations molecule normal components obtained origin particle perpendicular plane wave point charge polarized position vector potential difference propagation properties quadrupole quantities radiation region relation result satisfy scalar potential shown in Figure situation solenoid spherical substitute surface current surface integral tangential components total charge unit vacuum vector potential velocity volume write written xy plane zero