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 85
... charge distribution ) . Figure 5-4 is a plot of the potential as a function of r ; the negative slope of this curve gives the electric field E , that we have previously shown in Figure 4-5 and it is ... LINE CHARGE DISTRIBUTION 85.
... charge distribution ) . Figure 5-4 is a plot of the potential as a function of r ; the negative slope of this curve gives the electric field E , that we have previously shown in Figure 4-5 and it is ... LINE CHARGE DISTRIBUTION 85.
Page 207
... line charge and a semiinfinite plate grounded conductor . We consider an infinitely long line charge of constant charge λ per unit length that is a distance a from and parallel to the A surface of a grounded conductor occupying half of ...
... line charge and a semiinfinite plate grounded conductor . We consider an infinitely long line charge of constant charge λ per unit length that is a distance a from and parallel to the A surface of a grounded conductor occupying half of ...
Page 225
... charge and the conductor . Find and E at this point . 11-7 Verify that ( 11-35 ) can also be obtained by using ( 11 ... line charge , and the force per unit length on the line charge . 11-12 Show that the attractive force on a length L ...
... charge and the conductor . Find and E at this point . 11-7 Verify that ( 11-35 ) can also be obtained by using ( 11 ... line charge , and the force per unit length on the line charge . 11-12 Show that the attractive force on a length L ...
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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