## 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 123

To what should your

the charge distribution of Exercise 5-17 by using (7-8). 7-6 Find the energy of a

length L of the coaxial cylinders of Figure 6-12 when they are used as a capacitor

...

To what should your

**result**reduce when n = 0? Does it? 7-5 Find the energy ofthe charge distribution of Exercise 5-17 by using (7-8). 7-6 Find the energy of a

length L of the coaxial cylinders of Figure 6-12 when they are used as a capacitor

...

Page 192

It is coaxial with a dielectric cylinder of radius a whose dielectric constant varies

along the axis according to Ke = a + fiz where a and /J are constants. Find D, E, P

, and pb at all points within the cylinder. Is your

It is coaxial with a dielectric cylinder of radius a whose dielectric constant varies

along the axis according to Ke = a + fiz where a and /J are constants. Find D, E, P

, and pb at all points within the cylinder. Is your

**result**for pb consistent with the ...Page 612

(The total number of electrons is Z, = Y.knk) Comparing this

see that they are the same if we recall that we are assuming the nuclear force

constants to be so very large that \/Kt^0. The derivation of (B-21) from (B-20) still ...

(The total number of electrons is Z, = Y.knk) Comparing this

**result**with (B-9), wesee that they are the same if we recall that we are assuming the nuclear force

constants to be so very large that \/Kt^0. The derivation of (B-21) from (B-20) still ...

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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