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 70
... equipotential surface and in the sense of decreasing p . 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 p . 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 87
... equipotential surface whose potential o ' is greater than 4 ,, the potential of S ,, which is also an equipotential surface by ( 6-2 ) . Then , according to ( 5-11 ) and Figure 5-1 , there will be lines of E generally directed from S ...
... equipotential surface whose potential o ' is greater than 4 ,, the potential of S ,, which is also an equipotential surface by ( 6-2 ) . Then , according to ( 5-11 ) and Figure 5-1 , there will be lines of E generally directed from S ...
Page 184
... 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 ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
Electrostatic Forces | 103 |
Copyright | |
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Ampère's law angle assume axis becomes bound charge boundary conditions calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance divergence theorem E₁ electric field electromagnetic electrostatic energy equal equipotential evaluate example expression field point flux force function given induction infinitely long integral integrand line charge located Lorentz transformation magnetic magnitude Maxwell's equations obtained parallel particle perpendicular plane wave plates point charge polarized position vector quantities region result scalar potential Section shown in Figure solenoid sphere of radius spherical surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero Απερ μο