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 96
Page 56
... point charge q located at an arbitrary point in the xy plane . 2-2 Four equal point charges q ' are located at the corners of a square of side a . The square lies in the yz plane with one corner at the origin and its sides parallel to ...
... point charge q located at an arbitrary point in the xy plane . 2-2 Four equal point charges q ' are located at the corners of a square of side a . The square lies in the yz plane with one corner at the origin and its sides parallel to ...
Page 264
... point charge , so that ( 14-28 ) gives the magnetic induction produced by a moving point charge . By comparing ( 14-28 ) with ( 14-6 ) , we see that this value of B is just the same as that produced by a current element I'ds ' = q'v ...
... point charge , so that ( 14-28 ) gives the magnetic induction produced by a moving point charge . By comparing ( 14-28 ) with ( 14-6 ) , we see that this value of B is just the same as that produced by a current element I'ds ' = q'v ...
Page 575
... point charge , q ( E + vXB ) , the right - hand side becomes q { E + vXB - [ ( v · E ) / c2 ] v } . 28-23 Show that the equation of motion of a particle of charge q in an electromagnetic field where the force is given by f = q ( E + v ...
... point charge , q ( E + vXB ) , the right - hand side becomes q { E + vXB - [ ( v · E ) / c2 ] v } . 28-23 Show that the equation of motion of a particle of charge q in an electromagnetic field where the force is given by f = q ( E + v ...
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