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 94
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 A 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 A 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 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