Classical Electrodynamics |
From inside the book
Results 1-3 of 88
Page 237
First we assume that just outside the conductor there exists only a normal electric
field E , and a tangential magnetic field H . , , as for a perfect conductor . The
values of these fields are assumed to have been obtained from the solution of an
...
First we assume that just outside the conductor there exists only a normal electric
field E , and a tangential magnetic field H . , , as for a perfect conductor . The
values of these fields are assumed to have been obtained from the solution of an
...
Page 241
For simplicity , the cross - sectional size and shape are assumed constant along
the cylinder axis . With a sinusoidal time dependence e - iwt for the fields inside
the cylinder , Maxwell ' s equations take the form : V E = i B D . B = 0 ( 8 . 16 ) V x
...
For simplicity , the cross - sectional size and shape are assumed constant along
the cylinder axis . With a sinusoidal time dependence e - iwt for the fields inside
the cylinder , Maxwell ' s equations take the form : V E = i B D . B = 0 ( 8 . 16 ) V x
...
Page 297
The dimensions of the hole are assumed to be very small compared to a
wavelength of the electromagnetic fields which are assumed to exist on one side
of the sheet . The problem is to calculate the diffracted fields on the other side of
the ...
The dimensions of the hole are assumed to be very small compared to a
wavelength of the electromagnetic fields which are assumed to exist on one side
of the sheet . The problem is to calculate the diffracted fields on the other side of
the ...
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 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
8 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 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