## 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 393

For simplicity, we

radius that the electric field E can be taken to be uniform and confined entirely to

the ...

For simplicity, we

**assume**a vacuum between the plates, and, as usual, we also**assume**that the separation between the plates is so small compared with theradius that the electric field E can be taken to be uniform and confined entirely to

the ...

Page 443

24-7 Polarization So far we have obtained many of our results from the

form (24-89) without being very specific about Eg and B0 other than that they are

constants, that they will be related by B0 = (A:/w)kXE0 as found from (24-92), ...

24-7 Polarization So far we have obtained many of our results from the

**assumed**form (24-89) without being very specific about Eg and B0 other than that they are

constants, that they will be related by B0 = (A:/w)kXE0 as found from (24-92), ...

Page 595

We can also get a crude estimate of its value in a somewhat different manner as

follows. Let us consider a single atom and

distribution is not only spherically symmetric but uniform throughout a sphere of

radius ...

We can also get a crude estimate of its value in a somewhat different manner as

follows. Let us consider a single atom and

**assume**that the electron chargedistribution is not only spherically symmetric but uniform throughout a sphere of

radius ...

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angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law cross section current density current element curve cylinder defined dielectric direction displacement distance electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge free currents frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz Lorentz transformation magnitude material Maxwell's equations molecule normal components obtained origin particle perpendicular plane wave point charge polarized position vector potential difference propagation properties quadrupole quantities radiation region relation result satisfy scalar potential shown in Figure situation solenoid spherical substitute surface current surface integral tangential components total charge unit vacuum vector potential velocity volume write written xy plane zero