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 181
... Vacuum between the plates . ( b ) Dielectric between the plates . Now Q , and of are kept constant when the dielectric is put between the plates , so that D will not be changed and will equal the vacuum value : D = Do = 0f ( 10-61 ) ...
... Vacuum between the plates . ( b ) Dielectric between the plates . Now Q , and of are kept constant when the dielectric is put between the plates , so that D will not be changed and will equal the vacuum value : D = Do = 0f ( 10-61 ) ...
Page 505
... vacuum . If one wanted to build the dielectric filled guide to operate in the same manner at a given frequency as the vacuum case , that is , to keep the cutoff frequencies the same , should it be made larger or smaller and by what ...
... vacuum . If one wanted to build the dielectric filled guide to operate in the same manner at a given frequency as the vacuum case , that is , to keep the cutoff frequencies the same , should it be made larger or smaller and by what ...
Page 562
... Vacuum In contrast to mechanics , we will see that electromagnetism as described by Maxwell's equations for a vacuum is already covariant with respect to Lorentz transformations . We did not require this directly , although the second ...
... Vacuum In contrast to mechanics , we will see that electromagnetism as described by Maxwell's equations for a vacuum is already covariant with respect to Lorentz transformations . We did not require this directly , although the second ...
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Common terms and phrases
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