## 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 225

11-12 Show that the attractive force on a

ll-10 is given by F = _ '"'¢oL(-'3¢)2 ' 2[cosh_'(D/2A)]2(D2—4A2)'/2 11-13 A long

wire of circular cross section of radius A is strung on poles at a height h above ...

11-12 Show that the attractive force on a

**length**L of one of the cylinders of Figurell-10 is given by F = _ '"'¢oL(-'3¢)2 ' 2[cosh_'(D/2A)]2(D2—4A2)'/2 11-13 A long

wire of circular cross section of radius A is strung on poles at a height h above ...

Page 275

Geometry used to verify the 1 "1 boundary conditions on B. rectangular path of

integration shown dashed, with two horizontal sides each of

same distance D from the sheet; these are connected by two vertical sides of ...

Geometry used to verify the 1 "1 boundary conditions on B. rectangular path of

integration shown dashed, with two horizontal sides each of

**length**I and each thesame distance D from the sheet; these are connected by two vertical sides of ...

Page 545

In principle, we measure a

to be measured and then finding the difference between the scale marks that

simultaneously coincide with the ends of the

In principle, we measure a

**length**by placing a measuring rod along the distanceto be measured and then finding the difference between the scale marks that

simultaneously coincide with the ends of the

**length**of interest. Although such a ...### What people are saying - Write a review

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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