## 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 83

Page 159

agrees exactly with (10-67), which we found by other means, and verifies our

previous analysis which led to the form E = E0- Eb given in (10-25). This field Eb

is ...

**result**(3-12) along with (10-68), and we find that Eb = ^ + ^ = — = - (10-70) Thisagrees exactly with (10-67), which we found by other means, and verifies our

previous analysis which led to the form E = E0- Eb given in (10-25). This field Eb

is ...

Page 163

In (7-21), we found that the energy of a capacitor is equal to Q2/2C. This

was obtained by using very general properties of the charge distributions on

conductors, and thus is generally true whether there are dielectrics present or not

...

In (7-21), we found that the energy of a capacitor is equal to Q2/2C. This

**result**was obtained by using very general properties of the charge distributions on

conductors, and thus is generally true whether there are dielectrics present or not

...

Page 339

The latter quantity can be measured by wrapping another coil about the torus and

finding the total charge A<2c that passes through it as a

current. If Rc is the resistance of this circuit, we find from (12-2) and (17-3) that the

...

The latter quantity can be measured by wrapping another coil about the torus and

finding the total charge A<2c that passes through it as a

**result**of the inducedcurrent. If Rc is the resistance of this circuit, we find from (12-2) and (17-3) that the

...

### 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 axes axis becomes bound charge boundary conditions bounding surface calculate capacitance capacitor cavity charge density charge distribution charge q circuit conductor const constant convenient corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge line integral located Lorentz transformation magnetic magnitude Maxwell's equations obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector potential difference quantities rectangular coordinates region result scalar potential shown in Figure solenoid sphere of radius spherical surface integral tangential components theorem total charge unit vectors vacuum vector potential velocity volume write written xy plane zero