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 191
... polarized sphere discussed in Section 10-4 for negative values of z . Show that your answers are consistent with the results found for z > 0 and with Figure 10-11 . 10-6 10-7 A sphere of radius a has a radial polarization given by P ...
... polarized sphere discussed in Section 10-4 for negative values of z . Show that your answers are consistent with the results found for z > 0 and with Figure 10-11 . 10-6 10-7 A sphere of radius a has a radial polarization given by P ...
Page 445
... polarized . Thus the path traced out by its tip could be like that shown in Figure 24-8 . The magnetic induction B will also be elliptically polarized since B is always perpendicular to E ... polarized electric field with a POLARIZATION 445.
... polarized . Thus the path traced out by its tip could be like that shown in Figure 24-8 . The magnetic induction B will also be elliptically polarized since B is always perpendicular to E ... polarized electric field with a POLARIZATION 445.
Page 483
... polarized , what kind of polarization will the transmitted electric field have in general ? 25-6 Evaluate ( S , ) for the case of total reflection and then show that ( S , ) · ân = 0 as required for T to be zero . 25-7 ( a ) For the ...
... polarized , what kind of polarization will the transmitted electric field have in general ? 25-6 Evaluate ( S , ) for the case of total reflection and then show that ( S , ) · ân = 0 as required for T to be zero . 25-7 ( a ) For the ...
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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