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 347
... region 2 between the conductors is filled with a nonhomogeneous material such that K ,, = K ( p / a ) where x = 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 K ,, = K ( p / a ) where x = 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 351
... 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 430
... 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 ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
Electrostatic Forces | 103 |
Copyright | |
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Ampère's law angle assume axis becomes bound charge boundary conditions calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance divergence theorem E₁ electric field electromagnetic electrostatic energy equal equipotential evaluate example expression field point flux force function given induction infinitely long integral integrand line charge located Lorentz transformation magnetic magnitude Maxwell's equations obtained parallel particle perpendicular plane wave plates point charge polarized position vector quantities region result scalar potential Section shown in Figure solenoid sphere of radius spherical surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero Απερ μο