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 ... wave traveling in 438 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 ... wave traveling in 438 PLANE WAVES 24-5 Plane Wave in an Arbitrary Direction.
Page 455
... plane wave that is a superposition of two independent orthogonal plane waves and has the form E = ⭑Ee ( kz − wt + da ) + ŷ Eßei ( kz¬ - wt + ) where k is real . Find ( S ) and show that it equals the sum of the average Poynting ...
... plane wave that is a superposition of two independent orthogonal plane waves and has the form E = ⭑Ee ( kz − wt + da ) + ŷ Eßei ( kz¬ - wt + ) where k is real . Find ( S ) and show that it equals the sum of the average Poynting ...
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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