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 14
... perpendicular to such a surface . words , the gradient is that quantity that will give the change in the scalar when ... perpendicular ; thus Vu is perpendicular to a surface of constant u , as is also shown in Figure 1-18 . Now let us ...
... perpendicular to such a surface . words , the gradient is that quantity that will give the change in the scalar when ... perpendicular ; thus Vu is perpendicular to a surface of constant u , as is also shown in Figure 1-18 . Now let us ...
Page 32
... perpendicular to both of these and in the direction shown . We see that is perpendicular to the semiinfinite plane = const . , and its direction is therefore in the sense of increasing p . These unit vectors are shown at the location of ...
... perpendicular to both of these and in the direction shown . We see that is perpendicular to the semiinfinite plane = const . , and its direction is therefore in the sense of increasing p . These unit vectors are shown at the location of ...
Page 463
... perpendicular to k , and therefore contains E ;; this plane is also perpendicular to the plane of incidence defined by k , and în . We see that E , can be written as the vector sum E1 = E11 + E ; ll ( 25-22 ) ill where E is the ...
... perpendicular to k , and therefore contains E ;; this plane is also perpendicular to the plane of incidence defined by k , and în . We see that E , can be written as the vector sum E1 = E11 + E ; ll ( 25-22 ) ill where E is the ...
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Common terms and phrases
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