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 66
Page 197
... satisfy Laplace's equation ; we also see this explicitly from ( 1-146 ) . In other words , the sum of individual potentials from a set of point charges is automatically a solution of Laplace's equation . This fact is the basis for the ...
... satisfy Laplace's equation ; we also see this explicitly from ( 1-146 ) . In other words , the sum of individual potentials from a set of point charges is automatically a solution of Laplace's equation . This fact is the basis for the ...
Page 287
... satisfy the first two by taking A and A , to be both independent of z , while A , is at most a function of z ; however , if we keep ( 16-17 ) in mind it is probably simpler just to take A2 = const . Then we see that the remaining ...
... satisfy the first two by taking A and A , to be both independent of z , while A , is at most a function of z ; however , if we keep ( 16-17 ) in mind it is probably simpler just to take A2 = const . Then we see that the remaining ...
Page 423
... satisfy the same equation . Thus , if ¥ ( r , t ) is any of the six rectangular components of E and B , we find that ν ' ψ - μα αψ Ət - με 224 = 0 Ət2 so that , in effect , we have only one scalar equation to solve . ( 24-7 ) This last ...
... satisfy the same equation . Thus , if ¥ ( r , t ) is any of the six rectangular components of E and B , we find that ν ' ψ - μα αψ Ət - με 224 = 0 Ət2 so that , in effect , we have only one scalar equation to solve . ( 24-7 ) This last ...
Other editions - View all
Common terms and phrases
Ampère's law angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider constant 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 function given induction infinitely long integral integrand 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 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 Мо