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 66
Page 3
1-1 Definition of a Vector The properties of the displacement of a point provide us
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 l-l that the net effect ...
1-1 Definition of a Vector The properties of the displacement of a point provide us
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 l-l that the net effect ...
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
displacement. In order to understand the meaning of the gradient, let us consider
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 consider
Figure 1-18, ...
Page 35
The steady-state displacement of the electron will then be parallel to EP. The
problem then reduces to a one-dimensional one and if we let x be the
displacement, we can write (B-76) as dzx dx i :—u m,(F + 7 7; +wo2x) = — eEP=
— eEP0e U' ...
The steady-state displacement of the electron will then be parallel to EP. The
problem then reduces to a one-dimensional one and if we let x be the
displacement, we can write (B-76) as dzx dx i :—u m,(F + 7 7; +wo2x) = — eEP=
— eEP0e U' ...
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
Bibliographic information
| Title | Electromagnetic fields Wiley International editions |
| Author | Roald K. Wangsness |
| Edition | illustrated |
| Publisher | John Wiley & Sons Australia, Limited, 1979 |
| Original from | the University of California |
| Digitized | 24 Aug 2011 |
| ISBN | 0471041033, 9780471041030 |
| Length | 645 pages |
| Subjects | › › Science / Physics / Electromagnetism |
| Export Citation | BiBTeX EndNote RefMan |