Classical Electrodynamics |
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Page 111
The surface may be taken as the plane z = 0, as shown in Fig. 4.5. We must find
the appropriate solution to the equations: eIV - E = 4mp, z > 0 l e.V. E = 0, 2 < 0 (
4.47) and V x E = 0, everywhere subject to the boundary conditions at z = 0: | e1E
, ...
The surface may be taken as the plane z = 0, as shown in Fig. 4.5. We must find
the appropriate solution to the equations: eIV - E = 4mp, z > 0 l e.V. E = 0, 2 < 0 (
4.47) and V x E = 0, everywhere subject to the boundary conditions at z = 0: | e1E
, ...
Page 117
It is customary to consider the two parts separately by imagining a spherical
surface of size large microscopically but small macroscopically surrounding a
molecule, as shown in Fig. 4.11, and determining the field at the center due to the
...
It is customary to consider the two parts separately by imagining a spherical
surface of size large microscopically but small macroscopically surrounding a
molecule, as shown in Fig. 4.11, and determining the field at the center due to the
...
Page 155
pillbox is oriented so that its faces are in regions 1 and 2 and parallel to the
surface boundary, S, as shown in Fig. 5.9, Gauss's theorem can be applied to V.
B = 0 to yield (B2 - B). n = 0 (5.88) where n is the unit normal to the surface
directed ...
pillbox is oriented so that its faces are in regions 1 and 2 and parallel to the
surface boundary, S, as shown in Fig. 5.9, Gauss's theorem can be applied to V.
B = 0 to yield (B2 - B). n = 0 (5.88) where n is the unit normal to the surface
directed ...
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Contents
Introduction to Electrostatics | 1 |
Nš 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 |