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 88
Page 179
... Example - Point charge and an insulated uncharged conducting sphere . This is a variation on the previous example . The sphere is assumed to be originally neutral , and is no longer kept at a definite potential . In the presence of q ...
... Example - Point charge and an insulated uncharged conducting sphere . This is a variation on the previous example . The sphere is assumed to be originally neutral , and is no longer kept at a definite potential . In the presence of q ...
Page 326
... Example = · Uniformly magnetized sphere . Let us reconsider this example from this new point of view . Since M = Mî = const . , Pm - v M = 0 and there is no volume pole density . However , since în in ( 20-42 ) is the ŵ = î ' of Figure ...
... Example = · Uniformly magnetized sphere . Let us reconsider this example from this new point of view . Since M = Mî = const . , Pm - v M = 0 and there is no volume pole density . However , since în in ( 20-42 ) is the ŵ = î ' of Figure ...
Page 402
... example of interference , sup- pose that of the previous exercise is now propagating in the negative z direction . Show that if the waves have equal real positive ampli- tudes that Re = 24 cos kz cos wt . This is an example of a ...
... example of interference , sup- pose that of the previous exercise is now propagating in the negative z direction . Show that if the waves have equal real positive ampli- tudes that Re = 24 cos kz cos wt . This is an example of a ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
19 other sections not shown
Other editions - View all
Common terms and phrases
Ampère's law angle assume axes axis bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction distance divergence theorem E₁ electric field electromagnetic electrostatic energy equipotential evaluate example expression field point free charge function given induction infinitely long integral integrand Laplace's equation line charge line integral located magnetic magnitude Maxwell's equations obtained origin P₁ perpendicular point charge polarized position vector potential difference quadrupole R₁ region result scalar potential Section shown in Figure sphere of radius spherical surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume wave write written xy plane zero Απερ μο дх