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 390
... region 2 between the conductors is filled with a nonhomogeneous material such that Km K ( p / a ) where k = const . Find H and B within this region and the contribution L2 of a length / of this region to the self - inductance . 20-26 ...
... region 2 between the conductors is filled with a nonhomogeneous material such that Km K ( p / a ) where k = const . Find H and B within this region and the contribution L2 of a length / of this region to the self - inductance . 20-26 ...
Page 394
... regions shown in Figure 21-3 . Region 1 is the volume between the capacitor plates , and 2 is the remainder of that enclosed by the two parallel planes which coincide in part with the plates . Regions 3 and 4 are the rest of space ; I ...
... regions shown in Figure 21-3 . Region 1 is the volume between the capacitor plates , and 2 is the remainder of that enclosed by the two parallel planes which coincide in part with the plates . Regions 3 and 4 are the rest of space ; I ...
Page 486
... region as well as being solutions of Maxwell's equations . As soon as we start thinking about bounded regions , it is evident that there can be many possibilities , both in the shape of the region and in the materials comprising the ...
... region as well as being solutions of Maxwell's equations . As soon as we start thinking about bounded regions , it is evident that there can be many possibilities , both in the shape of the region and in the materials comprising the ...
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Ampère's law angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance E₁ electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point flux force free charge free currents frequency function given induction infinitely long integral integrand k₂ Laplace's equation located Lorentz transformation magnetic magnitude material Maxwell's equations normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector potential difference quadrupole quantities radiation radius rectangular region result satisfy scalar scalar potential shown in Figure solenoid sphere spherical tangential components unit vacuum vector potential velocity volume write written xy plane zero Απερ дх Мо