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 457
... medium . Eventually in any real situation , the wave will encounter another medium with different electromagnetic properties ; for example , a light wave in air may impinge on a piece of glass . The incident wave will generally be able ...
... medium . Eventually in any real situation , the wave will encounter another medium with different electromagnetic properties ; for example , a light wave in air may impinge on a piece of glass . The incident wave will generally be able ...
Page 483
... medium of index of refraction 4.5 . The second medium is a nonmagnetic glass of index 1.5 . The incident wave is linearly polarized such that the components of Eo perpendicular and parallel to the plane of incidence are equal . Find ...
... medium of index of refraction 4.5 . The second medium is a nonmagnetic glass of index 1.5 . The incident wave is linearly polarized such that the components of Eo perpendicular and parallel to the plane of incidence are equal . Find ...
Page 484
... medium . For the remainder of this exercise , assume a perfect conductor ( 02 → ∞ ) . Assume Eo ; to be real for simplicity , and find E1 real , that is , the total physical electric field in the incident medium and show that it is a ...
... medium . For the remainder of this exercise , assume a perfect conductor ( 02 → ∞ ) . Assume Eo ; to be real for simplicity , and find E1 real , that is , the total physical electric field in the incident medium and show that it is a ...
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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