Classical Electrodynamics |
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Page 10
da (1.23) Another problem of interest is the potential due to a dipole-layer
distribution on a surface S. A dipole layer can be imagined as being formed by
letting the surface S have a surface-charge density of x) on it, and another
surface S", ...
da (1.23) Another problem of interest is the potential due to a dipole-layer
distribution on a surface S. A dipole layer can be imagined as being formed by
letting the surface S have a surface-charge density of x) on it, and another
surface S", ...
Page 132
The basic entity in magnetic studies was what we now know as a magnetic dipole
. In the presence of magnetic materials the dipole tends to align itself in a certain
direction. That direction is by definition the direction of the magnetic-flux density,
...
The basic entity in magnetic studies was what we now know as a magnetic dipole
. In the presence of magnetic materials the dipole tends to align itself in a certain
direction. That direction is by definition the direction of the magnetic-flux density,
...
Page 274
Considering only the magnetization term, we have the vector potential, ikor A(x) =
ik(n x m) o( - #) (9.33) r ikr where m is the magnetic dipole moment, in E so d°r = ;
se x J) doc (9.34) c The fields can be determined by noting that the vector ...
Considering only the magnetization term, we have the vector potential, ikor A(x) =
ik(n x m) o( - #) (9.33) r ikr where m is the magnetic dipole moment, in E so d°r = ;
se x J) doc (9.34) c The fields can be determined by noting that the vector ...
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Contents
Introduction to Electrostatics | 1 |
Nº 3 | 3 |
Greens theorem | 14 |
Copyright | |
30 other sections not shown
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angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Authors | John David Jackson, Patrick Thaddeus Jackson |
| Edition | 3 |
| Publisher | Wiley, 1962 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |