## 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 64

3-3 Consider a cube of edge a with the location and orientation of the figure in

Figure l-41. ... I G 3-10 The circular arc of radius a

xy plane and has a constant linear charge density A and center of curvature at

the ...

3-3 Consider a cube of edge a with the location and orientation of the figure in

Figure l-41. ... I G 3-10 The circular arc of radius a

**shown in Figure**3-7 lies in thexy plane and has a constant linear charge density A and center of curvature at

the ...

Page 290

Then the situation will correspond exactly to that

symbol )1 replaced by I, and we can use (5-34) to write down the vector potential

for this case as _ 1101 2+ 2+2 ,1(,,,.,,)=,T1,,(a2_P%2˘fl (M5) 'F a +p —2apcos<p

...

Then the situation will correspond exactly to that

**shown in Figure**5-7 with thesymbol )1 replaced by I, and we can use (5-34) to write down the vector potential

for this case as _ 1101 2+ 2+2 ,1(,,,.,,)=,T1,,(a2_P%2˘fl (M5) 'F a +p —2apcos<p

...

Page 358

The appropriate cavity is thus a thin right cylinder cut in the material with its base

perpendicular to the direction of B there as

construction, only normal components are involved, we see that the value of B in

the ...

The appropriate cavity is thus a thin right cylinder cut in the material with its base

perpendicular to the direction of B there as

**shown in Figure**20-6. Since, byconstruction, only normal components are involved, we see that the value of B in

the ...

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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