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 19
Page 541
... transformation given by ( 28-2 ) and ( 28-4 ) . The necessary new concepts are provided by the postulates of special relativity . One should not get the idea ... LORENTZ TRANSFORMATION 541 28-2 The Postulates and the Lorentz Transformation.
... transformation given by ( 28-2 ) and ( 28-4 ) . The necessary new concepts are provided by the postulates of special relativity . One should not get the idea ... LORENTZ TRANSFORMATION 541 28-2 The Postulates and the Lorentz Transformation.
Page 549
... show us that we should be able to write the transformation formulas for certain quantities quite easily , provided that we know something about their general properties . This THE POSTULATES AND THE LORENTZ TRANSFORMATION 549.
... show us that we should be able to write the transformation formulas for certain quantities quite easily , provided that we know something about their general properties . This THE POSTULATES AND THE LORENTZ TRANSFORMATION 549.
Page 553
... transformation and ( 28-69 ) and ( 28-75 ) represent the conditions required by ( 28-66 ) . When the particular Lorentz transformation ( 28-28 ) which we have been using is written in the notation of ( 28-65 ) , it becomes x1 = yx1 + ...
... transformation and ( 28-69 ) and ( 28-75 ) represent the conditions required by ( 28-66 ) . When the particular Lorentz transformation ( 28-28 ) which we have been using is written in the notation of ( 28-65 ) , it becomes x1 = yx1 + ...
Other editions - View all
Common terms and phrases
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