## 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 204

connected to something from which it can obtain charge as was the case in the

last

the same image charge q' = — (a/d)q at the same position as the last

this ...

connected to something from which it can obtain charge as was the case in the

last

**examples**. It must also be an equipotential volume. We begin by introducingthe same image charge q' = — (a/d)q at the same position as the last

**example**;this ...

Page 364

fields. Since there is a vacuum everywhere else, M = 0 and H = B/ fi<>. Thus we

can use our previous results (15-25) and (15-26) and we see that H„=0 while ...

**Example**Infinitely long ideal solenoid. Here we have free currents producing thefields. Since there is a vacuum everywhere else, M = 0 and H = B/ fi<>. Thus we

can use our previous results (15-25) and (15-26) and we see that H„=0 while ...

Page 418

Finally, the Heaviside-Lorentz system is simply a rationalized Gaussian system;

when this is used, the effect is to replace every Air in the equations (23-8) through

(23-12) by unity; for

Finally, the Heaviside-Lorentz system is simply a rationalized Gaussian system;

when this is used, the effect is to replace every Air in the equations (23-8) through

(23-12) by unity; for

**example**, one gets V-D=p/ and D = E + P. The factors of c ...### What people are saying - Write a review

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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