## 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 3

Such quantities are called vectors and it is well to consider their

general before we meet specific examples. Using the notation and terminology

that has been developed for this purpose enables us to state our results more ...

Such quantities are called vectors and it is well to consider their

**properties**ingeneral before we meet specific examples. Using the notation and terminology

that has been developed for this purpose enables us to state our results more ...

Page 151

We can also expect that these different kinds of matter will have different

electromagnetic "

cross the surface of separation. As a result, it is quite possible that our various

fields will ...

We can also expect that these different kinds of matter will have different

electromagnetic "

**properties**," so that these**properties**will change abruptly as wecross the surface of separation. As a result, it is quite possible that our various

fields will ...

Page 593

matter on electromagnetic fields in terms of parameters such as the electric

susceptibility x<- From a purely macroscopic point of view such parameters are ...

**Properties**. of. Matter. We have described the overall effects of the presence ofmatter on electromagnetic fields in terms of parameters such as the electric

susceptibility x<- From a purely macroscopic point of view such parameters are ...

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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