Classical Electrodynamics |
From inside the book
Results 1-3 of 92
Page 193
93 ) , the tensor can be handled within the framework of vector operations by
introducing a corresponding dyadic . If a tensor in three dimensions is denoted by
Tij ( i , j = 1 , 2 , 3 ) , and e ; are the unit base vectors of the coordinate axes , the ...
93 ) , the tensor can be handled within the framework of vector operations by
introducing a corresponding dyadic . If a tensor in three dimensions is denoted by
Tij ( i , j = 1 , 2 , 3 ) , and e ; are the unit base vectors of the coordinate axes , the ...
Page 307
Make a sketch of I as a function of X for fixed Z . ( c ) Use the vector formula ( 9 .
82 ) to obtain a result equivalent to that of part ( a ) . Compare the two
expressions . A linearly polarized plane wave of amplitude E , and wave number
k is incident ...
Make a sketch of I as a function of X for fixed Z . ( c ) Use the vector formula ( 9 .
82 ) to obtain a result equivalent to that of part ( a ) . Compare the two
expressions . A linearly polarized plane wave of amplitude E , and wave number
k is incident ...
Page 640
Vector potential, for time-varying fields, 179 in magnetostatics, 139 f. in non-
cartesian coordinates, 141 of localized oscillating source, 269 f. of magnetic
dipole, 146 of oscillating electric dipole, 271 of oscillating electric quadrupole,
275 of ...
Vector potential, for time-varying fields, 179 in magnetostatics, 139 f. in non-
cartesian coordinates, 141 of localized oscillating source, 269 f. of magnetic
dipole, 146 of oscillating electric dipole, 271 of oscillating electric quadrupole,
275 of ...
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