Classical Electrodynamics |
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Page 359
(11.23) J. p? co — —; cThe time t is the meson's lifetime t as observed in the
system K. Consequently T = − (11.24) U2 J-5 co When viewed from K the
moving meson lives longer than a meson at rest in K. The “clock” in motion is
observed to ...
(11.23) J. p? co — —; cThe time t is the meson's lifetime t as observed in the
system K. Consequently T = − (11.24) U2 J-5 co When viewed from K the
moving meson lives longer than a meson at rest in K. The “clock” in motion is
observed to ...
Page
Consequently we may neglect the parallel component of acceleration and
approximate the radiation intensity by that due to the perpendicular component
alone. In other words, the radiation emitted by a charged particle in arbitrary,
extreme ...
Consequently we may neglect the parallel component of acceleration and
approximate the radiation intensity by that due to the perpendicular component
alone. In other words, the radiation emitted by a charged particle in arbitrary,
extreme ...
Page
Consequently the plane containing the incident beam direction and the direction
of the radiation is a natural one with respect to which one specifies the state of
polarization of the radiation. For simplicity we consider a small angle deflection
so ...
Consequently the plane containing the incident beam direction and the direction
of the radiation is a natural one with respect to which one specifies the state of
polarization of the radiation. For simplicity we consider a small angle deflection
so ...
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
Copyright | |
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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 |