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 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 538
... particle moves into a region of larger B ,, its longitudinal kinetic energy will decrease , and if mB , becomes equal to & , the particle will reverse its direction and move back into the region of weaker field ; this is in agreement ...
... particle moves into a region of larger B ,, its longitudinal kinetic energy will decrease , and if mB , becomes equal to & , the particle will reverse its direction and move back into the region of weaker field ; this is in agreement ...
Page 545
... particle of charge q is produced at rest and then accel- erated through a potential difference Ap . It then enters a region of uniform B , which is perpendic- ular to its velocity . After traveling a semicircle , the particle strikes a ...
... particle of charge q is produced at rest and then accel- erated through a potential difference Ap . It then enters a region of uniform B , which is perpendic- ular to its velocity . After traveling a semicircle , the particle strikes a ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
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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