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 471
... reflected from a surface of a dielectric at grazing incidence . ( You can verify this for yourself right now by looking at a light source by reflection from a rough sheet of paper and then gradually increasing the angle of incidence to ...
... reflected from a surface of a dielectric at grazing incidence . ( You can verify this for yourself right now by looking at a light source by reflection from a rough sheet of paper and then gradually increasing the angle of incidence to ...
Page 474
... reflected with different phase shifts and the resultant reflected wave will be elliptically polarized and can be analyzed by the methods we used in Section 24-7 . 25-5 Energy Relations Now we are in a position to see how the incoming ...
... reflected with different phase shifts and the resultant reflected wave will be elliptically polarized and can be analyzed by the methods we used in Section 24-7 . 25-5 Energy Relations Now we are in a position to see how the incoming ...
Page 485
... reflected wave will be zero when L equals an odd multiple of a quarter wavelength in medium 2 and Z2 = ( Z1Z3 ) 12 . ( c ) Find the corresponding conditions for zero reflected wave when Z1 = Z3 Z2 . ( d ) Light of wavelength 5 × 10-7 ...
... reflected wave will be zero when L equals an odd multiple of a quarter wavelength in medium 2 and Z2 = ( Z1Z3 ) 12 . ( c ) Find the corresponding conditions for zero reflected wave when Z1 = Z3 Z2 . ( d ) Light of wavelength 5 × 10-7 ...
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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