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 473
... reflected electric field . Using ( 25-56 ) , we find that ( 25-31 ) and ( 25-45 ) can be written as E , E ( 특 ) ... reflected wave has the same amplitude as the incident wave . As we will see in the next section , AMA . v2x 2 1 Figure 25 ...
... reflected electric field . Using ( 25-56 ) , we find that ( 25-31 ) and ( 25-45 ) can be written as E , E ( 특 ) ... reflected wave has the same amplitude as the incident wave . As we will see in the next section , AMA . v2x 2 1 Figure 25 ...
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 bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb's law current density cylinder defined dielectric dipole direction displacement distance E₁ electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge function given incident induction infinitely long integral integrand k₁ Laplace's equation located Lorentz transformation magnetic magnitude material Maxwell's equations medium molecule n₂ normal components obtained origin parallel plate capacitor particle perpendicular plane wave point charge polarized position vector potential difference quantities radiation rectangular refraction region result satisfy scalar scalar potential shown in Figure solenoid spherical surface charge density tangential components total charge vacuum vector potential velocity volume write written xy plane Z₂ zero Απερ дх