## 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 354

Although the boundary conditions at a surface of discontinuity can always be

obtained from

usual and convenient to list them separately. They are given by (10-42), (9-16)

and ...

Although the boundary conditions at a surface of discontinuity can always be

obtained from

**Maxwell's equations**and our general results from Chapter 9, it isusual and convenient to list them separately. They are given by (10-42), (9-16)

and ...

Page 355

In a similar manner, one can write the basic equations in terms of the pairs (E, H),

(D, B), and (D, H) if it is desirable and the terms that arise can be interpreted in

the same way. The so-called integral forms of

In a similar manner, one can write the basic equations in terms of the pairs (E, H),

(D, B), and (D, H) if it is desirable and the terms that arise can be interpreted in

the same way. The so-called integral forms of

**Maxwell's equations**are obtained ...Page 371

(23-11) Where they are applicable, the various constitutive equations are written

D = eE H = B//i Jf=oE P = X,E M = XmH ... The only one of

that is affected by this is Ampere's law, and then the equation of continuity, which

...

(23-11) Where they are applicable, the various constitutive equations are written

D = eE H = B//i Jf=oE P = X,E M = XmH ... The only one of

**Maxwell's equations**that is affected by this is Ampere's law, and then the equation of continuity, which

...

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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