## 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 393

24-7 POLARIZATION So far we have obtained many of our results from the

that they are constants, that they will be related by B0 = (k/u)k X E0 as found from

(24-92) ...

24-7 POLARIZATION So far we have obtained many of our results from the

**assumed**form (24-89) without being very specific about E0 and B0 other thanthat they are constants, that they will be related by B0 = (k/u)k X E0 as found from

(24-92) ...

Page 405

25-1 THE LAWS OF REFLECTION AND REFRACTION We

boundary between the two media is an infinite plane surface. We further

that there are no free charges or free surface currents on the boundary surface.

25-1 THE LAWS OF REFLECTION AND REFRACTION We

**assume**that theboundary between the two media is an infinite plane surface. We further

**assume**that there are no free charges or free surface currents on the boundary surface.

Page 563

Comparing (B-73) and (B-72), we see that n + i'ij = lO 1/2 (B-74) For simplicity, we

nonconducting, a = 0 as well and (B-74) reduces to n + it) = y/icj (B-75) We are ...

Comparing (B-73) and (B-72), we see that n + i'ij = lO 1/2 (B-74) For simplicity, we

**assume**the material to be nonmagnetic and set Km = 1. If, in addition, it isnonconducting, a = 0 as well and (B-74) reduces to n + it) = y/icj (B-75) We are ...

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