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

Could the vector A of

? If so, find ...

**EXERCISES**5-1 Can the vector E = (yz - 2x)i + xzy + xyz be a possibleelectrostatic field? 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, find ...

Page 283

17-16 The previous two

conductors as a result of Faraday's law and they are given the name "eddy

currents." If they arise from a time varying induction, it is possible to obtain a

differential ...

17-16 The previous two

**exercises**involved currents that are produced inconductors as a result of Faraday's law and they are given the name "eddy

currents." If they arise from a time varying induction, it is possible to obtain a

differential ...

Page 296

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

positive to show that | A/, 2 1 < ]/LxL2 as was discussed in another way in

are all ...

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

positive to show that | A/, 2 1 < ]/LxL2 as was discussed in another way in

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

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