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 125
... quantities that depend on different details of the charge distribution , much as mechanical quantities such as the magnitude of the total mass and the moment of inertia of a set of mass points depend on different features of the mass ...
... quantities that depend on different details of the charge distribution , much as mechanical quantities such as the magnitude of the total mass and the moment of inertia of a set of mass points depend on different features of the mass ...
Page 305
... quantities which are referred to , and would be measured in , different systems . The primed quantities are those that would be observed by someone in the moving system and hence at rest with respect to it . On the other hand , the ...
... quantities which are referred to , and would be measured in , different systems . The primed quantities are those that would be observed by someone in the moving system and hence at rest with respect to it . On the other hand , the ...
Page 549
... quantities dx vx dr [ 1- ( v2 / c2 ) ] 1 / 2 D dr ̄ ̄ [ 1- ( v2 / c2 ) ] 1 / 2 dy dz Vz dt 1 dr - [ 1 − ( v2 / c2 ) ] 1 / 2 dr [ 1 − ( v2 / c2 ) ] 1 / 2 ( 28-54 ) transform in exactly the same way as do x , y , z , t . Therefore ...
... quantities dx vx dr [ 1- ( v2 / c2 ) ] 1 / 2 D dr ̄ ̄ [ 1- ( v2 / c2 ) ] 1 / 2 dy dz Vz dt 1 dr - [ 1 − ( v2 / c2 ) ] 1 / 2 dr [ 1 − ( v2 / c2 ) ] 1 / 2 ( 28-54 ) transform in exactly the same way as do x , y , z , t . Therefore ...
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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