## 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 64

Page 3

1-1 Definition of a Vector The properties of the

the essentials required for our definition. If we start at some point P, and move in

some arbitrary way to another point P2, we see from Figure 1-1 that the net ...

1-1 Definition of a Vector The properties of the

**displacement**of a point provide usthe essentials required for our definition. If we start at some point P, and move in

some arbitrary way to another point P2, we see from Figure 1-1 that the net ...

Page 14

The gradient is perpendicular to such a surface. words, the gradient is that

quantity that will give the change in the scalar when it is dotted with the

Figure 1-18, ...

The gradient is perpendicular to such a surface. words, the gradient is that

quantity that will give the change in the scalar when it is dotted with the

**displacement**. In order to understand the meaning of the gradient, let us considerFigure 1-18, ...

Page 611

*"elec eEp and we can simplify (B-76) even further by neglecting the term vXBm.

The steady-state

problem then reduces to a one-dimensional one and if we let x be the

*"elec eEp and we can simplify (B-76) even further by neglecting the term vXBm.

The steady-state

**displacement**of the electron will then be parallel to E,. Theproblem then reduces to a one-dimensional one and if we let x be the

**displacement**, ...### 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