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 72
Page 3
... Figure 1-1 that the net effect of the motion is the same as if the point were moved directly along the straight line ... illustrated in Figure 1-2 . Because of the first two properties , we can represent a vector by a directed line such ...
... Figure 1-1 that the net effect of the motion is the same as if the point were moved directly along the straight line ... illustrated in Figure 1-2 . Because of the first two properties , we can represent a vector by a directed line such ...
Page 30
... illustrated in Figure 1-24 . We would divide S into surfaces . each bounded by a single curve by introducing as many pairs of coincident lines as we would need ; two such pairs are shown dashed in the figure . Then Stokes ' theorem can ...
... illustrated in Figure 1-24 . We would divide S into surfaces . each bounded by a single curve by introducing as many pairs of coincident lines as we would need ; two such pairs are shown dashed in the figure . Then Stokes ' theorem can ...
Page 80
... illustrated in Figure 1-22 : - 2 ƒ3E · ds = ƒ2 - Vo · ds = − [ 2do = − ( 92− ¢ 1 ) = − [ ø ( r2 ) − q ( r , ) ] - where we have used ( 5-3 ) and ( 1-38 ) . We can write this , using ( 5-5 ) , as Ap = o ( r2 ) —¿ ( r , ) = − ƒ ' E ...
... illustrated in Figure 1-22 : - 2 ƒ3E · ds = ƒ2 - Vo · ds = − [ 2do = − ( 92− ¢ 1 ) = − [ ø ( r2 ) − q ( r , ) ] - where we have used ( 5-3 ) and ( 1-38 ) . We can write this , using ( 5-5 ) , as Ap = o ( r2 ) —¿ ( r , ) = − ƒ ' E ...
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