## 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

When a procedure like this is carried out with a monotonically increasing H, the

result typically is a B versus H curve with the general appearance

also ...

When a procedure like this is carried out with a monotonically increasing H, the

result typically is a B versus H curve with the general appearance

**shown in****Figure**20-19. A curve such as this is called a magnetization curve; this name isalso ...

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