## 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 110

These

definition. These considerations will also be helpful to us when we face the

problem of describing the effects of matter in electrostatics, since, for our

purposes, we ...

These

**quantities**are called electric multipoles and we will give them a specificdefinition. These considerations will also be helpful to us when we face the

problem of describing the effects of matter in electrostatics, since, for our

purposes, we ...

Page 271

If we label these

)E' . ds = - ( — .d»+(f)(\XB) ds (17-26) Tc js dt *c which can be written with the use

of (1-67) as , , dB / V X (E' - v X B) . d& = - I —da (17-27) Js Js dt so that dB V X ...

If we label these

**quantities**with a prime, and use (1-23) again, we find that S ' = <f)E' . ds = - ( — .d»+(f)(\XB) ds (17-26) Tc js dt *c which can be written with the use

of (1-67) as , , dB / V X (E' - v X B) . d& = - I —da (17-27) Js Js dt so that dB V X ...

Page 371

This is most prevalent with respect to magnetic

is as follows: B, gauss; H, oersted; M, oersted (but see the next section); $, 1

gauss-(centimeter)2 = 1 maxwell. It also follows from (23-9) that in a vacuum, D =

E ...

This is most prevalent with respect to magnetic

**quantities**and the common usageis as follows: B, gauss; H, oersted; M, oersted (but see the next section); $, 1

gauss-(centimeter)2 = 1 maxwell. It also follows from (23-9) that in a vacuum, D =

E ...

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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