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 38
Page 516
... particle energy . This shows that the linear momentum and energy of a particle should not be regarded as different entities , but simply as two aspects of the same attributes of the particle since they appear as separate components of ...
... particle energy . This shows that the linear momentum and energy of a particle should not be regarded as different entities , but simply as two aspects of the same attributes of the particle since they appear as separate components of ...
Page 536
... particle speed gets very large , the relativistic equation of motion ( 29-105 ) has to be used . If we interpret this as corresponding to an increase in the particle mass , we see from ( A - 13 ) that the cyclotron frequency will no ...
... particle speed gets very large , the relativistic equation of motion ( 29-105 ) has to be used . If we interpret this as corresponding to an increase in the particle mass , we see from ( A - 13 ) that the cyclotron frequency will no ...
Page 544
... particle position must always equal one half the average induction enclosed by the circular orbit . EXERCISES A - 1 At t = = 0 , a particle is at the origin with initial velocity = vox and enters a region of Vo uniform electric field E ...
... particle position must always equal one half the average induction enclosed by the circular orbit . EXERCISES A - 1 At t = = 0 , a particle is at the origin with initial velocity = vox and enters a region of Vo uniform electric field E ...
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