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 | |
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