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 26
... surface , but we can easily extend the proof to a region bounded by several surfaces , such as a hollow ball ... bounding surface is shown as în1⁄2 . Similar remarks apply to V1 ; its corresponding outward normal is în ,. Applying ( 1-59 ) ...
... surface , but we can easily extend the proof to a region bounded by several surfaces , such as a hollow ball ... bounding surface is shown as în1⁄2 . Similar remarks apply to V1 ; its corresponding outward normal is în ,. Applying ( 1-59 ) ...
Page 164
... surface charge density σ on the bounding surface where Pb = -V'.P = P · ĥ ' = P2 n ( 10-7 ) ( 10-8 ) for then we would have 1 ( ( r ) = are √ Poet ' + 4 = $ 3 da Sv Απερ R ATTEO D .. o da ' JS ' R ( 10-9 ) as we would expect . [ In ...
... surface charge density σ on the bounding surface where Pb = -V'.P = P · ĥ ' = P2 n ( 10-7 ) ( 10-8 ) for then we would have 1 ( ( r ) = are √ Poet ' + 4 = $ 3 da Sv Απερ R ATTEO D .. o da ' JS ' R ( 10-9 ) as we would expect . [ In ...
Page 499
... bounding surface , call this field & , and then find K from ( 26-67 ) , we can use the results in ( 26-14 ) and ( 26-15 ) to give a possible TEM mode for the system . The two - dimensional field pattern obtained in this way will then ...
... bounding surface , call this field & , and then find K from ( 26-67 ) , we can use the results in ( 26-14 ) and ( 26-15 ) to give a possible TEM mode for the system . The two - dimensional field pattern obtained in this way will then ...
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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