## 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. |

### From inside the book

Results 1-3 of 37

Page 396

21-2

knowledge of macroscopic descriptive electro- magnetism is complete and can

be summarized by the equations (2l-l) as extended in (21 -7): V-D=P/ (21-19)

VXE=-^ ...

21-2

**Maxwell's Equations**In General Form At this point, finally, our presentknowledge of macroscopic descriptive electro- magnetism is complete and can

be summarized by the equations (2l-l) as extended in (21 -7): V-D=P/ (21-19)

VXE=-^ ...

Page 538

Since (28-6) is a consequence of

there can be only one frame of reference in which

form in which we have been writing them and in which electromagnetic waves ...

Since (28-6) is a consequence of

**Maxwell's equations**, these results imply thatthere can be only one frame of reference in which

**Maxwell's equations**have theform in which we have been writing them and in which electromagnetic waves ...

Page 562

28-5 Electromagnetlsm in Vacuum In contrast to mechanics, we will see that

electromagnetism as described by

covariant with respect to Lorentz transformations. We did not require this directly,

...

28-5 Electromagnetlsm in Vacuum In contrast to mechanics, we will see that

electromagnetism as described by

**Maxwell's equations**for a vacuum is alreadycovariant with respect to Lorentz transformations. We did not require this directly,

...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Other editions - View all

### Common terms and phrases

angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law cross section current density current element curve cylinder defined dielectric direction displacement distance electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge free currents frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz Lorentz transformation magnitude material Maxwell's equations molecule normal components obtained origin particle perpendicular plane wave point charge polarized position vector potential difference propagation properties quadrupole quantities radiation region relation result satisfy scalar potential shown in Figure situation solenoid spherical substitute surface current surface integral tangential components total charge unit vacuum vector potential velocity volume write written xy plane zero