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 80
... equipotential surface and in the sense of decreasing ø . This is illustrated in Figure 5-1 , in which the equipotential surfaces are shown as solid curves and the dashed lines are drawn to indicate the direction of E at each point for ...
... equipotential surface and in the sense of decreasing ø . This is illustrated in Figure 5-1 , in which the equipotential surfaces are shown as solid curves and the dashed lines are drawn to indicate the direction of E at each point for ...
Page 207
... equipotential surfaces are actually cylinders whose axes are parallel to the z axis and , in fact , these axes lie in the xz plane . ) As we noted in the discussion following ( 5-38 ) , the yz plane ( x = 0 ) is the equipotential ...
... equipotential surfaces are actually cylinders whose axes are parallel to the z axis and , in fact , these axes lie in the xz plane . ) As we noted in the discussion following ( 5-38 ) , the yz plane ( x = 0 ) is the equipotential ...
Page 208
... equipotential cylinders were replaced by a solid conductor occupying the volume enclosed by the cylinder . The surface of the conductor would be an equipotential as required and would have the potential corresponding to the surface it ...
... equipotential cylinders were replaced by a solid conductor occupying the volume enclosed by the cylinder . The surface of the conductor would be an equipotential as required and would have the potential corresponding to the surface it ...
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Common terms and phrases
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