## 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

5-3 Uniform

potential, let us consider the uniform infinite

found the field as given by (3-9) to be E=(7\/ 21rq,p)p. Since E has only a p ...

5-3 Uniform

**Line Charge**Distribution As an example of the use of (5-ll) to find thepotential, let us consider the uniform infinite

**line charge**for which we previouslyfound the field as given by (3-9) to be E=(7\/ 21rq,p)p. Since E has only a p ...

Page 207

By comparing (11-17) and (ll-18) with (ll-48), we see that the total bound charge

induced on the dielectric surface will again equal the image ... We consider an

infinitely long

By comparing (11-17) and (ll-18) with (ll-48), we see that the total bound charge

induced on the dielectric surface will again equal the image ... We consider an

infinitely long

**line charge**of constant charge A per unit length that is a distance ...Page 225

11-8 Using the spherical coordinate system of Figure ll-3, find q> at all points

outside the sphere for the charge ... 11-14 Show that the potential produced by

an infinite

of a ...

11-8 Using the spherical coordinate system of Figure ll-3, find q> at all points

outside the sphere for the charge ... 11-14 Show that the potential produced by

an infinite

**line charge**of constant density A at a distance D from the parallel axisof a ...

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amplitude angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb’s law cross section current density current element cylinder defined dielectric displacement distance electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point Flgure flux force free currents frequency function Galilean transformation given incident induction infinitely long integral integrand length located loop Lorentz Lorentz transformation magnetic dipole magnitude material Maxwell’s equations medium normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector produced quadrupole quantities radiation radius rectangular reﬂected region relation result rotation satisfy scalar potential shown in Figure solenoid sphere substitute surface charge surface current tangential components transformation unit vacuum vector potential velocity volume write written xy plane zero