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 xii
... Plane Waves 422 24-1 Separate Equations for E and B 422 24-2 Plane Waves in a Nonconducting Medium 423 24-3 Plane Waves in a Conducting Medium 430 24-4 Plane Waves in a Charged Medium 437 24-5 Plane Wave in an Arbitrary Direction 438 24 ...
... Plane Waves 422 24-1 Separate Equations for E and B 422 24-2 Plane Waves in a Nonconducting Medium 423 24-3 Plane Waves in a Conducting Medium 430 24-4 Plane Waves in a Charged Medium 437 24-5 Plane Wave in an Arbitrary Direction 438 24 ...
Page 438
... wave . The other part represents a static field that can be a function of position ; while this is a possibility , it is of no interest for a study of wave propagation and , rather ... PLANE WAVES 24-5 Plane Wave in an Arbitrary Direction.
... wave . The other part represents a static field that can be a function of position ; while this is a possibility , it is of no interest for a study of wave propagation and , rather ... PLANE WAVES 24-5 Plane Wave in an Arbitrary Direction.
Page 473
... wave is W с V2x = = = k1 sin 0 n , sin 0 ( c / n2 ) ( n1 / n2 ) sin 0 , = sin 0 V2 sin 0 , ( 25-58 ) where V2 is the normal speed of a wave in this medium . Since 0 ; > 0c , v2x < v2 and this wave travels more slowly than a usual plane wave ...
... wave is W с V2x = = = k1 sin 0 n , sin 0 ( c / n2 ) ( n1 / n2 ) sin 0 , = sin 0 V2 sin 0 , ( 25-58 ) where V2 is the normal speed of a wave in this medium . Since 0 ; > 0c , v2x < v2 and this wave travels more slowly than a usual plane wave ...
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Ampère's law angle assume axis bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb's law current density cylinder defined dielectric dipole direction displacement distance E₁ electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge function given incident induction infinitely long integral integrand k₁ Laplace's equation located Lorentz transformation magnetic magnitude material Maxwell's equations medium molecule n₂ normal components obtained origin parallel plate capacitor particle perpendicular plane wave point charge polarized position vector potential difference quantities radiation rectangular refraction region result satisfy scalar scalar potential shown in Figure solenoid spherical surface charge density tangential components total charge vacuum vector potential velocity volume write written xy plane Z₂ zero Απερ дх