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. |
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Page 184
... axes are parallel . For simplicity , we assume that they have the same radius A ; their axes are separated by a distance D as shown in Figure 11-10 . If we identify these cylinders with the appropriate equipotentials of Figure 5-8 ...
... axes are parallel . For simplicity , we assume that they have the same radius A ; their axes are separated by a distance D as shown in Figure 11-10 . If we identify these cylinders with the appropriate equipotentials of Figure 5-8 ...
Page 508
... axes while its coordinates are x ' , y ' , z ' in the other set . Both of these different sets of numbers locate the ... axes . It is also evident that these aj cannot all be independent because the transforma- tion equations ( 29-60 ) ...
... axes while its coordinates are x ' , y ' , z ' in the other set . Both of these different sets of numbers locate the ... axes . It is also evident that these aj cannot all be independent because the transforma- tion equations ( 29-60 ) ...
Page 510
... axes in three - dimensional space will also keep the expression x2 + y2 + z2 - c22 invariant because of ( 29-57 ) and its independence of the time . Thus such a physical rotation of axes should also be included in the group of general ...
... axes in three - dimensional space will also keep the expression x2 + y2 + z2 - c22 invariant because of ( 29-57 ) and its independence of the time . Thus such a physical rotation of axes should also be included in the group of general ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
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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