## 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 65

Page 191

10-5 Find the potential <t> and Ez on the axis produced by the uniformly

your answers are consistent with the results found for z >0 and with Figure 10-11.

1Q-45 ...

10-5 Find the potential <t> and Ez on the axis produced by the uniformly

**polarized**sphere discussed in Section 10-4 for negative values of z. Show thatyour answers are consistent with the results found for z >0 and with Figure 10-11.

1Q-45 ...

Page 445

This second-degree equation is generally that of an ellipse (since both Ex and Ey

stay finite) and the electric field is said to be elliptically

traced out by its tip could be like that shown in Figure 24-8. The magnetic ...

This second-degree equation is generally that of an ellipse (since both Ex and Ey

stay finite) and the electric field is said to be elliptically

**polarized**. Thus the pathtraced out by its tip could be like that shown in Figure 24-8. The magnetic ...

Page 483

25-3 Show for the case n, >n2 that the

angle. 25-4 The expression tan0p = n2/nl for the

) involved the assumption that ^ = y^. Consider the general case in which media

1 ...

25-3 Show for the case n, >n2 that the

**polarizing**angle is less than the criticalangle. 25-4 The expression tan0p = n2/nl for the

**polarizing**angle found in (25-52) involved the assumption that ^ = y^. Consider the general case in which media

1 ...

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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