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. |
From inside the book
Results 1-3 of 95
Page 125
... distribution of charges at any field point of interest . Let us suppose that the charges are contained in a finite ... charge distribution . However , as we get farther and farther away , it seems clear that the finer details of the ...
... distribution of charges at any field point of interest . Let us suppose that the charges are contained in a finite ... charge distribution . However , as we get farther and farther away , it seems clear that the finer details of the ...
Page 129
... charge distribution . In other words , the monopole moment is that feature of the charge distribution which is important for the monopole term . If the charges are continuously distributed , then the sum can be replaced by an integral ...
... charge distribution . In other words , the monopole moment is that feature of the charge distribution which is important for the monopole term . If the charges are continuously distributed , then the sum can be replaced by an integral ...
Page 149
... charge distribution of Figure 8-5b leads to ( 8-40 ) and thus evaluate Qa for this case . 8-7 A line charge of constant charge density λ and of length L lies in the first quadrant of the xy plane with one end at the origin . It makes an ...
... charge distribution of Figure 8-5b leads to ( 8-40 ) and thus evaluate Qa for this case . 8-7 A line charge of constant charge density λ and of length L lies in the first quadrant of the xy plane with one end at the origin . It makes an ...
Other editions - View all
Common terms and phrases
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