## 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 286

But when all of the components of a

continuous across the surface, and therefore we conclude that A2 = A, (16-22) in

complete analogy to the continuity of the scalar

29).

But when all of the components of a

**vector**are continuous, the**vector**itself iscontinuous across the surface, and therefore we conclude that A2 = A, (16-22) in

complete analogy to the continuity of the scalar

**potential**<f> as expressed in (9-29).

Page 288

Various

corresponding symmetry of the source distribution as would be found by direct

calculation from (16-12), for example. A very common and useful expression for

the vector ...

Various

**vector potentials**that describe the same uniform induction. thecorresponding symmetry of the source distribution as would be found by direct

calculation from (16-12), for example. A very common and useful expression for

the vector ...

Page 335

In Chapter 8, we saw how the scalar potential at a point outside of a finite charge

distribution could be described by the ... 19-1 The Multipole Expansion of the

In Chapter 8, we saw how the scalar potential at a point outside of a finite charge

distribution could be described by the ... 19-1 The Multipole Expansion of the

**Vector Potential**The general situation is illustrated in Figure 19-1; compare with ...### What people are saying - Write a review

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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