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 504
... frequency given by ( 26-88 ) . This property is known as degeneracy and is a fundamental and important feature of electromagnetic standing waves . If a , b , c are all different , then the various frequencies given by ( 26-88 ) will ...
... frequency given by ( 26-88 ) . This property is known as degeneracy and is a fundamental and important feature of electromagnetic standing waves . If a , b , c are all different , then the various frequencies given by ( 26-88 ) will ...
Page 27
... frequency change Aw = w - wo is very small even for very large values of B , As a result we can approximate w + wo by 2w 。 and replace w by wo in the right hand side ; we therefore find that e Aw = w - wo = = Bm 2me ( B - 42 ) so that ...
... frequency change Aw = w - wo is very small even for very large values of B , As a result we can approximate w + wo by 2w 。 and replace w by wo in the right hand side ; we therefore find that e Aw = w - wo = = Bm 2me ( B - 42 ) so that ...
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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