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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Results 1-3 of 83
Page 31
When this procedure is carried out for rectangular coordinates, the result is, of
course, (l-43). 1-16 Cylindrical Coordinates Up to now, we have used only
rectangular coordinates with their constant unit vectors. However, many problems
are ...
When this procedure is carried out for rectangular coordinates, the result is, of
course, (l-43). 1-16 Cylindrical Coordinates Up to now, we have used only
rectangular coordinates with their constant unit vectors. However, many problems
are ...
Page 41
We see from (l-l3) that these combinations are simply the components of the
relative position vector R, hence the name “relative coordinates” for x —x' and so
on. Functions of this type have properties that will enable us to simplify much of
our ...
We see from (l-l3) that these combinations are simply the components of the
relative position vector R, hence the name “relative coordinates” for x —x' and so
on. Functions of this type have properties that will enable us to simplify much of
our ...
Page 149
If it is possible to find a different origin of coordinates for which the dipole moment
will vanish, where should this origin be located? 8-6 Show that the charge
distribution of Figure 8-5b leads to (8-40) and thus evaluate Q“ for this case. 8-7 A
line ...
If it is possible to find a different origin of coordinates for which the dipole moment
will vanish, where should this origin be located? 8-6 Show that the charge
distribution of Figure 8-5b leads to (8-40) and thus evaluate Q“ for this case. 8-7 A
line ...
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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 |