Classical Electrodynamics |
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Page 299
9.10 Scattering by a Conducting Sphere in the Short-Wavelength Limit Another
type of problem which is essentially diffraction is the scattering of waves by an
obstacle. We will consider the scattering of a plane electromagnetic wave by a ...
9.10 Scattering by a Conducting Sphere in the Short-Wavelength Limit Another
type of problem which is essentially diffraction is the scattering of waves by an
obstacle. We will consider the scattering of a plane electromagnetic wave by a ...
Page 447
We will content ourselves with the extreme relativistic limit (3 - 1). Furthermore,
since the important ... we can approximate the Bessel functions by their small
argument limits (3.103). Then in the relativistic limit the Fermi expression (13.70)
is ...
We will content ourselves with the extreme relativistic limit (3 - 1). Furthermore,
since the important ... we can approximate the Bessel functions by their small
argument limits (3.103). Then in the relativistic limit the Fermi expression (13.70)
is ...
Page 598
The first integral is therefore et/7 C r mW(t) = “s e-"F(t') dt' (17.50) T J t The minus
sign of the preceding line has been absorbed by making the lower limit of the
integral the indefinite one. The constant of integration C is to be determined on ...
The first integral is therefore et/7 C r mW(t) = “s e-"F(t') dt' (17.50) T J t The minus
sign of the preceding line has been absorbed by making the lower limit of the
integral the indefinite one. The constant of integration C is to be determined on ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
BoundaryValue Problems in Electrostatics II | 54 |
Copyright | |
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge 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 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written