## 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 429

Then we see from the first two equations of (24-32) that we must have Ez = 0 and

Bz = 0. Thus both E and B have no component in the direction of

that is, both E and B are perpendicular to it; in other words, the electromagnetic ...

Then we see from the first two equations of (24-32) that we must have Ez = 0 and

Bz = 0. Thus both E and B have no component in the direction of

**propagation**,that is, both E and B are perpendicular to it; in other words, the electromagnetic ...

Page 443

In order to simplify our discussion somewhat, let us assume that our axes have

been chosen so that the positive z axis is the direction of

transverse plane is then the xy plane, but we will not assume any specific

orientation of ...

In order to simplify our discussion somewhat, let us assume that our axes have

been chosen so that the positive z axis is the direction of

**propagation**; thetransverse plane is then the xy plane, but we will not assume any specific

orientation of ...

Page 538

In other words, if the wave is traveling in the positive x' direction, it has the speed

c — V, while its speed is c + V for

results are therefore consistent with the particular case given by (28-5), and for a

...

In other words, if the wave is traveling in the positive x' direction, it has the speed

c — V, while its speed is c + V for

**propagation**in the negative x' direction. Theseresults are therefore consistent with the particular case given by (28-5), and for a

...

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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