Classical Electrodynamics |
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Page 52
7 A line charge with linear charge density T is placed parallel to , and a distance
R away from , the axis of a conducting cylinder of radius b held at fixed voltage
such that the potential vanishes at infinity . Find ( a ) the magnitude and position
of ...
7 A line charge with linear charge density T is placed parallel to , and a distance
R away from , the axis of a conducting cylinder of radius b held at fixed voltage
such that the potential vanishes at infinity . Find ( a ) the magnitude and position
of ...
Page 259
5 we considered wave guides made of hollow metal cylinders with fields only
inside the hollow . ... however , characteristic differences which arise because of
the very different boundary conditions to be satisfied at the surface of the cylinder
.
5 we considered wave guides made of hollow metal cylinders with fields only
inside the hollow . ... however , characteristic 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 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence 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 light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written