## 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 144

Origin of bound surface charges for a uniformly

Origin of bound volume charges in a "\^ dielectric with nonuniform

that pb = 0 in agreement with (10-10). However, there will be no such

cancellation ...

Origin of bound surface charges for a uniformly

**polarized**dielectric. Figure 10-4.Origin of bound volume charges in a "\^ dielectric with nonuniform

**polarization**.that pb = 0 in agreement with (10-10). However, there will be no such

cancellation ...

Page 168

is uniformly

spherical cavity of radius a is inside a very large dielectric that is uniformly

axis ...

is uniformly

**polarized**in the z direction. Find E at the center of the cube. 10-10 Aspherical cavity of radius a is inside a very large dielectric that is uniformly

**polarized**. Find E at the center of the cavity. 10-11 A cylinder of length 21. has itsaxis ...

Page 428

If the incident wave is linearly

transmitted electric field have in general? 25-6 Evaluate (S,) for the case of total

reflection and then show that (S,) . ft - 0 as required for T to be zero. 25-7 that tan(

<p,.

If the incident wave is linearly

**polarized**, what kind of**polarization**will thetransmitted electric field have in general? 25-6 Evaluate (S,) for the case of total

reflection and then show that (S,) . ft - 0 as required for T to be zero. 25-7 that tan(

<p,.

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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