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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Results 1-3 of 43
Page 75
... integrand is zero as long as R 0 , so that any contribution to ( 4-23 ) must come from the region corresponding to R = | r - r ' | = 0 , that is , from the immediate neighborhood of the field point . Thus , in order to evaluate ( 4-23 ) ...
... integrand is zero as long as R 0 , so that any contribution to ( 4-23 ) must come from the region corresponding to R = | r - r ' | = 0 , that is , from the immediate neighborhood of the field point . Thus , in order to evaluate ( 4-23 ) ...
Page 247
... integrand in ( 13-1 ) is more complicated from a directional point of view than is Coulomb's law as expressed by , say , ( 2-15 ) , since the integrand depends on the relative orientation of the three quantities Ids , I'ds ' , and R. We ...
... integrand in ( 13-1 ) is more complicated from a directional point of view than is Coulomb's law as expressed by , say , ( 2-15 ) , since the integrand depends on the relative orientation of the three quantities Ids , I'ds ' , and R. We ...
Page 383
... integrand in ( 20-98 ) by using ( 20-76 ) and this last result , and then proceed exactly as we did in going from ( 20-75 ) to ( 20-77 ) , we get = SU = SH - 8BdT Sum = ( 20-99 ) as a completely general result for the increment in ...
... integrand in ( 20-98 ) by using ( 20-76 ) and this last result , and then proceed exactly as we did in going from ( 20-75 ) to ( 20-77 ) , we get = SU = SH - 8BdT Sum = ( 20-99 ) as a completely general result for the increment in ...
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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