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 151
Roald K. Wangsness. Chapter 9 Boundary Conditions at a Surface of Discontinuity As soon as we consider the possibility of matter being present and subject to the influence of other charges , we realize that we may need to consider a ...
Roald K. Wangsness. Chapter 9 Boundary Conditions at a Surface of Discontinuity As soon as we consider the possibility of matter being present and subject to the influence of other charges , we realize that we may need to consider a ...
Page 196
... boundary conditions . We also assume that there is another distinct solution 2 ( r ) satisfying these same boundary conditions . We want to prove that o , and 2 are identical . We let = 1 − 2 . Then V2 = V2 , - V22 = 0 because of ( 11 ...
... boundary conditions . We also assume that there is another distinct solution 2 ( r ) satisfying these same boundary conditions . We want to prove that o , and 2 are identical . We let = 1 − 2 . Then V2 = V2 , - V22 = 0 because of ( 11 ...
Page 457
... boundary conditions that the field vectors have to satisfy at a surface of discontinuity in properties , and we recall that these boundary conditions were obtained directly from Maxwell's equations . 25-1 The Laws of Reflection and ...
... boundary conditions that the field vectors have to satisfy at a surface of discontinuity in properties , and we recall that these boundary conditions were obtained directly from Maxwell's equations . 25-1 The Laws of Reflection and ...
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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