Classical Electrodynamics |
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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 Eo and wave number k is incident on
a ...
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 Eo and wave number k is incident on
a ...
Page
John David Jackson. below which our approximate result (13.2) must be
replaced by a more exact expression which tends to (13.5) as b → 0. It can be
shown (Problem 13.1) that a proper treatment gives the more accurate result, ...
John David Jackson. below which our approximate result (13.2) must be
replaced by a more exact expression which tends to (13.5) as b → 0. It can be
shown (Problem 13.1) that a proper treatment gives the more accurate result, ...
Page
14.3, then the power radiated can be written *~ _dP e” - + = — to sin” (9 - 14.21 d
() 4trc” ( ) This exhibits the characteristic sin” (9 angular dependence which is a
wellknown result. We note from (14.18) that the radiation is polarized in the plane
...
14.3, then the power radiated can be written *~ _dP e” - + = — to sin” (9 - 14.21 d
() 4trc” ( ) This exhibits the characteristic sin” (9 angular dependence which is a
wellknown result. We note from (14.18) that the radiation is polarized in the plane
...
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Contents
Introduction to Electrostatics | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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 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 shown in Fig shows side solution 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 |