Classical Electrodynamics |
From inside the book
Results 1-3 of 83
Page
We will content ourselves with the extreme relativistic limit (3 - 1). Furthermore ...
can approximate the Bessel functions by their small argument limits (3.103). Then
in the relativistic limit the Fermi expression (13.70) is (#) ~ 2Ge): Re | los !--
We will content ourselves with the extreme relativistic limit (3 - 1). Furthermore ...
can approximate the Bessel functions by their small argument limits (3.103). Then
in the relativistic limit the Fermi expression (13.70) is (#) ~ 2Ge): Re | los !--
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 ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
Introduction to Electrostatics | 1 |
Nș 3 | 3 |
Greens theorem | 14 |
Copyright | |
30 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 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 |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |