## 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 239

The path C does not link the circuit C. In this case, the relative orientations are

like those

to P after completing the loop C, the final solid angle has the same value that it

had ...

The path C does not link the circuit C. In this case, the relative orientations are

like those

**shown in Figure**15-2. Here, if we start at P, then when we come backto P after completing the loop C, the final solid angle has the same value that it

had ...

Page 319

20-3 UNIFORMLY MAGNETIZED SPHERE Let us now consider a sphere of

radius a that has a constant magnetization M. We choose the z axis in the

direction of M and the origin at the center of the sphere as

thus M = Mi ...

20-3 UNIFORMLY MAGNETIZED SPHERE Let us now consider a sphere of

radius a that has a constant magnetization M. We choose the z axis in the

direction of M and the origin at the center of the sphere as

**shown in Figure**20-8;thus M = Mi ...

Page 339

We see at once that the relationship shown is very nonlinear. Eventually, as H, -»

oo, M approaches a constant ... When n is found from a curve like Figure 20-19,

the result is like that

We see at once that the relationship shown is very nonlinear. Eventually, as H, -»

oo, M approaches a constant ... When n is found from a curve like Figure 20-19,

the result is like that

**shown in Figure**20-20. The maximum is generally of the ...### 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