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 155
... tangential components of F : Ô × ( F2 , — F1 , ) = lim ( he ) h → 0 ( 9-16 ) We can , in fact , write our result even more explicitly in terms of the tangential components . With the use of ( 1-23 ) , THE CURL AND THE TANGENTIAL COMPONENTS ...
... tangential components of F : Ô × ( F2 , — F1 , ) = lim ( he ) h → 0 ( 9-16 ) We can , in fact , write our result even more explicitly in terms of the tangential components . With the use of ( 1-23 ) , THE CURL AND THE TANGENTIAL COMPONENTS ...
Page 156
... tangential components of F. If we combine these results with those of the last section , we see that we have ... tangential components Fin and F1 ,. We can find the normal component of F2 from ( 9-7 ) , and its tangential component from ...
... tangential components of F. If we combine these results with those of the last section , we see that we have ... tangential components Fin and F1 ,. We can find the normal component of F2 from ( 9-7 ) , and its tangential component from ...
Page 363
... tangential components of H only if there is a free ( e.g. , conduction ) surface current density . This is in contrast to B whose tangential components will be discontinuous if there is a surface current density of any kind as we saw in ...
... tangential components of H only if there is a free ( e.g. , conduction ) surface current density . This is in contrast to B whose tangential components will be discontinuous if there is a surface current density of any kind as we saw in ...
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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