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 449
... frequency of light waves . The atomic nature of matter is the ultimate reason for this variation with frequency ; the atomic charges that are polarized by the fields possess inertia that makes their response to the electromagnetic ...
... frequency of light waves . The atomic nature of matter is the ultimate reason for this variation with frequency ; the atomic charges that are polarized by the fields possess inertia that makes their response to the electromagnetic ...
Page 603
... frequency change Aww - wo is very small even for very large values of Bm- As a result we can approximate w + wo by 2w 。 and replace w by wo in the right hand side ; we therefore find that ( B - 42 ) e Aw = w - wo = = + Bm 2me so that ...
... frequency change Aww - wo is very small even for very large values of Bm- As a result we can approximate w + wo by 2w 。 and replace w by wo in the right hand side ; we therefore find that ( B - 42 ) e Aw = w - wo = = + Bm 2me so that ...
Page 609
... frequency w rather than as simply constants . We also discussed the conductivity from a microscopic point of view and found in ( 24-130 ) that o was a complex function of frequency . The conductivity expression involved both the inertia ...
... frequency w rather than as simply constants . We also discussed the conductivity from a microscopic point of view and found in ( 24-130 ) that o was a complex function of frequency . The conductivity expression involved both the inertia ...
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Common terms and phrases
Ampère's law angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance E₁ electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point flux force free charge free currents frequency function given induction infinitely long integral integrand k₂ Laplace's equation located Lorentz transformation magnetic magnitude material Maxwell's equations normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector potential difference quadrupole quantities radiation radius rectangular region result satisfy scalar scalar potential shown in Figure solenoid sphere spherical tangential components unit vacuum vector potential velocity volume write written xy plane zero Απερ дх Мо