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 vii
... written and organized so that , if desired , it can be taken up section by section at an appropriate intermediate ... written this chapter primarily in terms of the purely practical aspects of how to recognize an equation written in ...
... written and organized so that , if desired , it can be taken up section by section at an appropriate intermediate ... written this chapter primarily in terms of the purely practical aspects of how to recognize an equation written in ...
Page 13
... written in terms of its rectangular components in ( 1-37 ) is called the gradient of u and is also often written grad u . We can regard ( 1-38 ) as the general definition of Vu since it is written in a form that is independent of a ...
... written in terms of its rectangular components in ( 1-37 ) is called the gradient of u and is also often written grad u . We can regard ( 1-38 ) as the general definition of Vu since it is written in a form that is independent of a ...
Page 533
... written in the ER = Мо d2p dt2 * { [ 13 ] x + ) x + 4πr BR Мо d2p 4πсr dt2 Xf where the quantity in brackets is evaluated at the retarded time . 27-7 Show that the electric dipole fields in the radiation zone can be written in the form ...
... written in the ER = Мо d2p dt2 * { [ 13 ] x + ) x + 4πr BR Мо d2p 4πсr dt2 Xf where the quantity in brackets is evaluated at the retarded time . 27-7 Show that the electric dipole fields in the radiation zone can be written in the form ...
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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