## 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 138

Calculation of electric field for a uniform sheet by using the

Example Uniform infinite plane sheet. As given by (3-12), the electric field has the

constant magnitude of E = a/2e0 and is directed away from the charged sheet ...

Calculation of electric field for a uniform sheet by using the

**boundary conditions**.Example Uniform infinite plane sheet. As given by (3-12), the electric field has the

constant magnitude of E = a/2e0 and is directed away from the charged sheet ...

Page 172

But, since </> = const. on the boundary, we see that <//> = const. everywhere (11-

8) Now it is easy to prove our uniqueness theorem. We let ^(r) be a solution of (11

-3) that satisfies the given

But, since </> = const. on the boundary, we see that <//> = const. everywhere (11-

8) Now it is easy to prove our uniqueness theorem. We let ^(r) be a solution of (11

-3) that satisfies the given

**boundary conditions**. We also assume that there is ...Page 405

We will find that we can solve this problem by using the

the field vectors have to satisfy at a surface of discontinuity in properties, and we

recall that these

We will find that we can solve this problem by using the

**boundary conditions**thatthe field vectors have to satisfy at a surface of discontinuity in properties, and we

recall that these

**boundary conditions**were obtained directly from Maxwell's ...### What people are saying - Write a review

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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