Classical Electrodynamics |
From inside the book
Results 1-3 of 100
Page 9
If the path is closed, the line integral is zero, jeal-o (1.21) a result that can also be
obtained directly from Coulomb's law. Then application of Stokes's theorem [if A(x
) is a vector field, S is an open surface, and C is the closed curve bounding S, ...
If the path is closed, the line integral is zero, jeal-o (1.21) a result that can also be
obtained directly from Coulomb's law. Then application of Stokes's theorem [if A(x
) is a vector field, S is an open surface, and C is the closed curve bounding S, ...
Page 10
The tangential component of electric field can be shown to be continuous across
a boundary surface by using (1.21) for the line integral of E around a closed path.
It is only necessary to take a rectangular path with negligible ends and one side ...
The tangential component of electric field can be shown to be continuous across
a boundary surface by using (1.21) for the line integral of E around a closed path.
It is only necessary to take a rectangular path with negligible ends and one side ...
Page 240
167 This is the same rate of energy dissipation as given by the Poynting's vector
result (8.12). The current density J is confined to such a small thickness just
below the surface of the conductor that it is equivalent to an effective surface
current ...
167 This is the same rate of energy dissipation as given by the Poynting's vector
result (8.12). The current density J is confined to such a small thickness just
below the surface of the conductor that it is equivalent to an effective surface
current ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
16 other sections not shown
Other editions - View all
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 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 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written