## 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 31

When this procedure is carried out for rectangular

course, (l-43). 1-16 Cylindrical

rectangular

are ...

When this procedure is carried out for rectangular

**coordinates**, the result is, ofcourse, (l-43). 1-16 Cylindrical

**Coordinates**Up to now, we have used onlyrectangular

**coordinates**with their constant unit vectors. However, many problemsare ...

Page 41

We see from (l-l3) that these combinations are simply the components of the

relative position vector R, hence the name “relative

on. Functions of this type have properties that will enable us to simplify much of

our ...

We see from (l-l3) that these combinations are simply the components of the

relative position vector R, hence the name “relative

**coordinates**” for x —x' and soon. Functions of this type have properties that will enable us to simplify much of

our ...

Page 149

If it is possible to find a different origin of

will vanish, where should this origin be located? 8-6 Show that the charge

distribution of Figure 8-5b leads to (8-40) and thus evaluate Q“ for this case. 8-7 A

line ...

If it is possible to find a different origin of

**coordinates**for which the dipole momentwill vanish, where should this origin be located? 8-6 Show that the charge

distribution of Figure 8-5b leads to (8-40) and thus evaluate Q“ for this case. 8-7 A

line ...

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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