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 397
... equations must of course be supplemented by the defining equations ( 10-40 ) and ( 20-28 ) , which relate pairs of the field vectors along with the ... equations are unchanged from before and the MAXWELL'S EQUATIONS IN GENERAL FORM 397.
... equations must of course be supplemented by the defining equations ( 10-40 ) and ( 20-28 ) , which relate pairs of the field vectors along with the ... equations are unchanged from before and the MAXWELL'S EQUATIONS IN GENERAL FORM 397.
Page 398
... equations in that we still have the possibility that P = P ( E ) and M = M ( B ) and until these functional relationships are known , these equations will be of limited utility . The ... Maxwell's equations are 398 MAXWELL'S EQUATIONS.
... equations in that we still have the possibility that P = P ( E ) and M = M ( B ) and until these functional relationships are known , these equations will be of limited utility . The ... Maxwell's equations are 398 MAXWELL'S EQUATIONS.
Page 406
... cross section of the line equals & 2 / R and interpret . Will the direction of energy flow change if the connections to the battery are interchanged ? 21-11 Consider a l.i.h. medium where of and J , 406 MAXWELL'S EQUATIONS.
... cross section of the line equals & 2 / R and interpret . Will the direction of energy flow change if the connections to the battery are interchanged ? 21-11 Consider a l.i.h. medium where of and J , 406 MAXWELL'S EQUATIONS.
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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