## 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 93

field? If so, find the potential <f> from which E can be obtained. 5-2 Could the

vector A of

the ...

**Exercises**. 5-1 Can the vector E=(yz -2x)x + xzy + xyi be a possible electrostaticfield? If so, find the potential <f> from which E can be obtained. 5-2 Could the

vector A of

**Exercise**1-15 be interpreted as a conservative electric field? If so, findthe ...

Page 123

7-4 Find the energy of the charge distribution of

what should your result reduce when n = 0? Does it? 7-5 Find the energy of the

charge distribution of

length ...

7-4 Find the energy of the charge distribution of

**Exercise**5-9 by using (7-10). Towhat should your result reduce when n = 0? Does it? 7-5 Find the energy of the

charge distribution of

**Exercise**5-17 by using (7-8). 7-6 Find the energy of alength ...

Page 333

18-4 Use the fact that the energy of two circuits as given by (18-8) must be

positive to show that \MI2\ < V/-1/-2 as was discussed in another way in

17-26. 18-5 A self -inductance L, a resistance R, and a battery of emf &b are all ...

18-4 Use the fact that the energy of two circuits as given by (18-8) must be

positive to show that \MI2\ < V/-1/-2 as was discussed in another way in

**Exercise**17-26. 18-5 A self -inductance L, a resistance R, and a battery of emf &b are all ...

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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