## 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 125

If we are near such a volume, we can expect that the values of the potential at

different points can be quite sensitive to the details of the

However, as we get farther and farther away, it seems clear that the finer details

of the ...

If we are near such a volume, we can expect that the values of the potential at

different points can be quite sensitive to the details of the

**charge distribution**.However, as we get farther and farther away, it seems clear that the finer details

of the ...

Page 129

In this context, the net charge Q is called the monopole moment of the

continuously ...

In this context, the net charge Q is called the monopole moment of the

**charge****distribution**. In other words, the monopole moment is that feature of the**charge****distribution**which is important for the monopole term. If the charges arecontinuously ...

Page 149

8-6 Show that the

evaluate Q“ for this case. 8-7 A line charge of constant charge density A and of

length L lies in the first quadrant of the xy plane with one end at the origin. It

makes an ...

8-6 Show that the

**charge distribution**of Figure 8-5b leads to (8-40) and thusevaluate Q“ for this case. 8-7 A line charge of constant charge density A and of

length L lies in the first quadrant of the xy plane with one end at the origin. It

makes an ...

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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