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 110
... 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 113
... charge q . It will be convenient to look at the terms in ( 8-8 ) one by one . 1. The Monopole Term The sum in the ... distribution will act as if it were a point charge as we have already concluded . In this context , the net charge Q is ...
... charge q . It will be convenient to look at the terms in ( 8-8 ) one by one . 1. The Monopole Term The sum in the ... distribution will act as if it were a point charge as we have already concluded . In this context , the net charge Q is ...
Page 131
... 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 ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
12 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 curve cylinder dielectric dipole direction distance divergence theorem E₁ electric field electromagnetic electrostatic energy equation 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 surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume wave write written xy plane zero Απερ дх