## 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 94

5-21

the x axis for which x = b>a to another point on the x axis for which x= —b, what is

the change in potential? 5-22 Express <f> for the charge distribution of Figure ...

5-21

**Consider**the charge distribution of Figure 5-7. If one moves from a point onthe x axis for which x = b>a to another point on the x axis for which x= —b, what is

the change in potential? 5-22 Express <f> for the charge distribution of Figure ...

Page 243

vacuum region just outside the wire and express it in terms of the quantities given

. (Overall, this portion of the wire is neutral.) 12-8

**Consider**a length / of the wire that has a resistance R. Find the electric field in thevacuum region just outside the wire and express it in terms of the quantities given

. (Overall, this portion of the wire is neutral.) 12-8

**Consider**a dielectric with a ...Page 287

[The expression (16-24) is an example of what is known as a gauge

transformation, and we

have completed the development of the general theory. The requirement (16-26),

and ...

[The expression (16-24) is an example of what is known as a gauge

transformation, and we

**consider**them again in more detail in Chapter 22 after wehave completed the development of the general theory. The requirement (16-26),

and ...

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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