## 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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Results 1-3 of 90

Page x

5-3 Uniform Line Charge Distribution 85 5-4 The Scalar Potential and Energy 91

6 Conductors in

Systems of Conductors 100 6-3 Capacitance 103 7

Energy ...

5-3 Uniform Line Charge Distribution 85 5-4 The Scalar Potential and Energy 91

6 Conductors in

**Electrostatic**Fields 95 6-1 Some General Results 95 6-2Systems of Conductors 100 6-3 Capacitance 103 7

**Electrostatic**Energy 111 7-1Energy ...

Page 78

Up to now, our description of

terms of the vector field E. By rewriting our expression for E, we will see that we

will be able to express substantially the same information in terms of a scalar field

...

Up to now, our description of

**electrostatic**effects has been done completely interms of the vector field E. By rewriting our expression for E, we will see that we

will be able to express substantially the same information in terms of a scalar field

...

Page 117

7-4

exert forces on each other and, in principle, these forces can be calculated from

Coulomb's law. It is often desirable to evaluate these forces in a different way.

7-4

**Electrostatic**Forces on Conductors In general, two charged conductors willexert forces on each other and, in principle, these forces can be calculated from

Coulomb's law. It is often desirable to evaluate these forces in a different way.

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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