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 xi
... Induction 255 14-1 Definition of the Magnetic Induction 255 14-2 14-3 Straight Current of Finite Length Axial Induction of a Circular Current 258 260 14-4 14-5 Infinite Plane Uniform Current Sheet Moving Point Charges 262 263 15 The ...
... Induction 255 14-1 Definition of the Magnetic Induction 255 14-2 14-3 Straight Current of Finite Length Axial Induction of a Circular Current 258 260 14-4 14-5 Infinite Plane Uniform Current Sheet Moving Point Charges 262 263 15 The ...
Page 255
... induction " ; the term “ magnetic field " is generally used for a different vector field that we define later when we include the effects of matter . 14-1 ... INDUCTION 255 The Magnetic Induction 14-1 Definition of the Magnetic Induction.
... induction " ; the term “ magnetic field " is generally used for a different vector field that we define later when we include the effects of matter . 14-1 ... INDUCTION 255 The Magnetic Induction 14-1 Definition of the Magnetic Induction.
Page 296
... induction : др Ət V.J + = 0 F = q ( E + vXB ) ( 17-2 ) The equations ( 17-1 ) form two completely independent sets , one for E and one B , thereby implying no connection between the ... INDUCTION Faraday's Law of Induction 17-1 Faraday's Law.
... induction : др Ət V.J + = 0 F = q ( E + vXB ) ( 17-2 ) The equations ( 17-1 ) form two completely independent sets , one for E and one B , thereby implying no connection between the ... INDUCTION Faraday's Law of Induction 17-1 Faraday's Law.
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Ampère's law angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance E₁ electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point flux force free charge free currents frequency function given induction infinitely long integral integrand k₂ Laplace's equation located Lorentz transformation magnetic magnitude material Maxwell's equations normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector potential difference quadrupole quantities radiation radius rectangular region result satisfy scalar scalar potential shown in Figure solenoid sphere spherical tangential components unit vacuum vector potential velocity volume write written xy plane zero Απερ дх Мо