## 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 95

If p is the perpendicular distance from the axis of the cylinder, show that the

potential outside the cylinder can be written i <Mp) 2irt0 \ p J (p>fl) ... 6-6 A

capacitor C, is charged resulting in a

. Another ...

If p is the perpendicular distance from the axis of the cylinder, show that the

potential outside the cylinder can be written i <Mp) 2irt0 \ p J (p>fl) ... 6-6 A

capacitor C, is charged resulting in a

**potential difference**A</J> between its plates. Another ...

Page 109

7-16 A battery is used to charge a parallel plate capacitor to a

A</> and is then disconnected. The separation between the plates is now

increased from d to ad where a is a spring $tretched)or compressed? ^ '"' r t*\ ' f 7-

15 A ...

7-16 A battery is used to charge a parallel plate capacitor to a

**potential difference**A</> and is then disconnected. The separation between the plates is now

increased from d to ad where a is a spring $tretched)or compressed? ^ '"' r t*\ ' f 7-

15 A ...

Page 147

We do this only qualitatively now, but we will be able to give a quantitative

discussion in Section 10-7. We consider two simple experiments. We charge a

capacitor to some charge Q, and measure the

there is a ...

We do this only qualitatively now, but we will be able to give a quantitative

discussion in Section 10-7. We consider two simple experiments. We charge a

capacitor to some charge Q, and measure the

**potential difference**A<//>0 whenthere is a ...

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angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitance capacitor cavity charge density charge distribution charge q circuit conductor const constant convenient corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge line integral located Lorentz transformation magnetic magnitude Maxwell's equations obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector potential difference quantities rectangular coordinates region result scalar potential shown in Figure solenoid sphere of radius spherical surface integral tangential components theorem total charge unit vectors vacuum vector potential velocity volume write written xy plane zero