Classical Electrodynamics |
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Page 52
A line charge with linear charge density r is placed parallel to, and a distance R
away from, the axis of a conducting cylinder of radius b held at zero potential. By
the method of images, find (a) the magnitude and position of the image charge(s);
...
A line charge with linear charge density r is placed parallel to, and a distance R
away from, the axis of a conducting cylinder of radius b held at zero potential. By
the method of images, find (a) the magnitude and position of the image charge(s);
...
Page 259
8.8 Dielectric Wave Guides In Sections 8.2–8.5 we considered wave guides
made of hollow metal cylinders with fields ... differences which arise because of
the very different boundary conditions to be satisfied at the surface of the cylinder.
8.8 Dielectric Wave Guides In Sections 8.2–8.5 we considered wave guides
made of hollow metal cylinders with fields ... differences which arise because of
the very different boundary conditions to be satisfied at the surface of the cylinder.
Page 260
The axial propagation constant k must be the same inside and outside the
cylinder in order to satisfy boundary conditions at all points on the surface at all
times. In the usual way, inside the dielectric cylinder the transverse Laplacian of
the ...
The axial propagation constant k must be the same inside and outside the
cylinder in order to satisfy boundary conditions at all points on the surface at all
times. In the usual way, inside the dielectric cylinder the transverse Laplacian of
the ...
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
Copyright | |
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Common terms and phrases
acceleration 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 |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |