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 o . 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 o . 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 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