## 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 23

The volume V2 is now enclosed by a single surface composed of those portions

of S2 and Sl to the left of the plane plus the plane surfaces of intersection shown

by AB and CD; the outward normal to the new part of the

The volume V2 is now enclosed by a single surface composed of those portions

of S2 and Sl to the left of the plane plus the plane surfaces of intersection shown

by AB and CD; the outward normal to the new part of the

**bounding surface**is ...Page 86

distributed uniformly over the surface with a constant density a = Q/4ira2, and the

electric field at the surface will be ... The total

now has two parts: an outer surface S0, and an inner surface St. Again let us ...

distributed uniformly over the surface with a constant density a = Q/4ira2, and the

electric field at the surface will be ... The total

**bounding surface**of the conductornow has two parts: an outer surface S0, and an inner surface St. Again let us ...

Page 442

Therefore, if we take any solution of the appropriate two-dimensional electrostatic

potential problem that gives an electric field normal to the perfectly conducting

Therefore, if we take any solution of the appropriate two-dimensional electrostatic

potential problem that gives an electric field normal to the perfectly conducting

**bounding surface**, call this field S, and then find Jf from (26-67), we can use the ...### What people are saying - Write a review

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### Common terms and phrases

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