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 1
... electromagnetic effects . At that time , it had been only slightly more than 50 years since Oersted and Ampère had shown the relation between electricity and magnetism - subjects that had been studied and developed completely separately ...
... electromagnetic effects . At that time , it had been only slightly more than 50 years since Oersted and Ampère had shown the relation between electricity and magnetism - subjects that had been studied and developed completely separately ...
Page 2
... Electromagnetic Theory , Third Edition , Addison - Wesley , Reading , Mass . , 1979 . A. Shadowitz , The Electromagnetic Field , McGraw - Hill , New York , 1975 . The following books discuss electromagnetism at a more advanced level ...
... Electromagnetic Theory , Third Edition , Addison - Wesley , Reading , Mass . , 1979 . A. Shadowitz , The Electromagnetic Field , McGraw - Hill , New York , 1975 . The following books discuss electromagnetism at a more advanced level ...
Page 546
Roald K. Wangsness. B ELECTROMAGNETIC PROPERTIES OF MATTER We have described the overall effects of the presence of matter on electromagnetic fields in terms of parameters such as the electric susceptibility xe . From a purely ...
Roald K. Wangsness. B ELECTROMAGNETIC PROPERTIES OF MATTER We have described the overall effects of the presence of matter on electromagnetic fields in terms of parameters such as the electric susceptibility xe . From a purely ...
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