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 190
... function of position on these conducting surfaces . 11-5 SEPARATION OF VARIABLES IN SPHERICAL COORDINATES If we use ... function of r alone to that for ℗ alone , we get 1 d dR 1 d = sin 0 R dr dr T sin 0 de dT do = const . = K ( 11-89 ) ...
... function of position on these conducting surfaces . 11-5 SEPARATION OF VARIABLES IN SPHERICAL COORDINATES If we use ... function of r alone to that for ℗ alone , we get 1 d dR 1 d = sin 0 R dr dr T sin 0 de dT do = const . = K ( 11-89 ) ...
Page 332
... function of p in Figure 20-17 . We see that M has discontinuities at both a and b , and therefore this must result ... function of P distance from the axis . Figure 20-17 . Magnetization from coaxial line as a function of distance from ...
... function of p in Figure 20-17 . We see that M has discontinuities at both a and b , and therefore this must result ... function of P distance from the axis . Figure 20-17 . Magnetization from coaxial line as a function of distance from ...
Page 552
... function and measures the ratio of the actual average component of po to its maximum value Po . The function L ( y ) is shown as a function of y in Figure B - 3 . We see that L ( y ) → 1 as y becomes very large , that is , for large ...
... function and measures the ratio of the actual average component of po to its maximum value Po . The function L ( y ) is shown as a function of y in Figure B - 3 . We see that L ( y ) → 1 as y becomes very large , that is , for large ...
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