## 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 84

Page 58

Chapter 3 The

“action at a distance” law. It provides us with a straightforward way of calculating

the force on a given charge when the relative position with respect to the source ...

Chapter 3 The

**Electric Field**Coulomb's law is an example of what is known as an“action at a distance” law. It provides us with a straightforward way of calculating

the force on a given charge when the relative position with respect to the source ...

Page 169

Then we can assume the

plate to the negatively charged plate as in Figure 6-9, and when we calculate A<

1>,, by means of (6-38), we get A¢,, = [+7 ED-ds = 12,4 (11122) where E, is the ...

Then we can assume the

**electric field**to be directed from the positively chargedplate to the negatively charged plate as in Figure 6-9, and when we calculate A<

1>,, by means of (6-38), we get A¢,, = [+7 ED-ds = 12,4 (11122) where E, is the ...

Page 235

The battery is an example of a localized source of a nonconservative

En, in (12-23) is different from zero only when the path of the charge is within the

battery and

The battery is an example of a localized source of a nonconservative

**field**so thatEn, in (12-23) is different from zero only when the path of the charge is within the

battery and

**E**”, =0 elsewhere on the circuit. In this case, it is possible to speak of ...### 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

amplitude angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb’s law cross section current density current element cylinder defined dielectric displacement distance electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point Flgure flux force free currents frequency function Galilean transformation given incident induction infinitely long integral integrand length located loop Lorentz Lorentz transformation magnetic dipole magnitude material Maxwell’s equations medium normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector produced quadrupole quantities radiation radius rectangular reﬂected region relation result rotation satisfy scalar potential shown in Figure solenoid sphere substitute surface charge surface current tangential components transformation unit vacuum vector potential velocity volume write written xy plane zero