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 109
... capacitor of Figure 6-8 and verify that they give the same result ( 6-37 ) for the capacitance . A capacitor C , is charged resulting in a potential difference Ap between its plates . Another capacitor C2 is uncharged . One plate of C2 ...
... capacitor of Figure 6-8 and verify that they give the same result ( 6-37 ) for the capacitance . A capacitor C , is charged resulting in a potential difference Ap between its plates . Another capacitor C2 is uncharged . One plate of C2 ...
Page 188
... capacitor in general . We have already seen the effect of a dielectric on a capacitor in the special case by which we obtained ( 10-86 ) . Let us now briefly look at the general case . The energy in general is given by ( 7-21 ) . In ...
... capacitor in general . We have already seen the effect of a dielectric on a capacitor in the special case by which we obtained ( 10-86 ) . Let us now briefly look at the general case . The energy in general is given by ( 7-21 ) . In ...
Page 193
... Capacitor in Exercise 10-28 . 10-28 The region between the plates of the spherical capacitor of Figure 10-20 is filled with two 1. i . h . dielectrics with permittivities shown . The total volume is divided exactly into halves by a ...
... Capacitor in Exercise 10-28 . 10-28 The region between the plates of the spherical capacitor of Figure 10-20 is filled with two 1. i . h . dielectrics with permittivities shown . The total volume is divided exactly into halves by 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