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 286
... vector are continuous , the vector itself is continuous across the surface , and therefore we conclude that A2 = A1 ( 16-22 ) in complete analogy to the continuity of the scalar potential as expressed in ( 9-29 ) . The magnetic flux Þ ...
... vector are continuous , the vector itself is continuous across the surface , and therefore we conclude that A2 = A1 ( 16-22 ) in complete analogy to the continuity of the scalar potential as expressed in ( 9-29 ) . The magnetic flux Þ ...
Page 335
... potential at a point outside of a finite charge distribution could be described by the various multipole moments of the system . Each multipole ... VECTOR POTENTIAL 335 Magnetic Multipoles 19-1 The Multipole Expansion of the Vector Potential.
... potential at a point outside of a finite charge distribution could be described by the various multipole moments of the system . Each multipole ... VECTOR POTENTIAL 335 Magnetic Multipoles 19-1 The Multipole Expansion of the Vector Potential.
Page 630
... vector potential of , 284 Point dipole , 136 Poisson's equation , 82 , 179 , 195 , 285 , 366 uniformly charged ... potential , 413 Polarizing angle , 471 , 483 Polarizing field , 594 Polar molecule , 162 Pole , magnetic , 366 , 389 ...
... vector potential of , 284 Point dipole , 136 Poisson's equation , 82 , 179 , 195 , 285 , 366 uniformly charged ... potential , 413 Polarizing angle , 471 , 483 Polarizing field , 594 Polar molecule , 162 Pole , magnetic , 366 , 389 ...
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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