Classical Electrodynamics |
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The detailed calculations for all energies with some explicit expression such as (
13.74) for e(a)) are quite complicated and not particularly informative. We will
content ourselves with the extreme relativistic limit (3 - 1). Furthermore, since the
...
The detailed calculations for all energies with some explicit expression such as (
13.74) for e(a)) are quite complicated and not particularly informative. We will
content ourselves with the extreme relativistic limit (3 - 1). Furthermore, since the
...
Page
angles such that 2ka sin-1 (14.112) If the frequency is low enough so that ka o 1,
then the limit qa & 1 will apply at all angles. But for frequencies where ka » 1,
there will be a region of forward angles less than 0.-4 (14.113) ka where the limit
qa ...
angles such that 2ka sin-1 (14.112) If the frequency is low enough so that ka o 1,
then the limit qa & 1 will apply at all angles. But for frequencies where ka » 1,
there will be a region of forward angles less than 0.-4 (14.113) ka where the limit
qa ...
Page
15.5 Radiation cross section So in the complete screening limit. The constant
value is the semiclassical result. The curve marked O (4) “Bethe-Heitler” is the
quantummax (A) mechanical Born approximation. For extremely relativistic
particles ...
15.5 Radiation cross section So in the complete screening limit. The constant
value is the semiclassical result. The curve marked O (4) “Bethe-Heitler” is the
quantummax (A) mechanical Born approximation. For extremely relativistic
particles ...
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Contents
Introduction to Electrostatics | 1 |
Nș 3 | 3 |
Greens theorem | 14 |
Copyright | |
30 other sections not shown
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Common terms and phrases
angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Authors | John David Jackson, Patrick Thaddeus Jackson |
| Edition | 3 |
| Publisher | Wiley, 1962 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |