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Page 304
9.14 Diffraction pattern for a conducting sphere , showing the forward peak due to
shadow scattering , the isotropic reflected contribution , and the interference
maxima and minima . 0.1 0 4 / ka isotropic value at certain angles , as shown in
Fig .
9.14 Diffraction pattern for a conducting sphere , showing the forward peak due to
shadow scattering , the isotropic reflected contribution , and the interference
maxima and minima . 0.1 0 4 / ka isotropic value at certain angles , as shown in
Fig .
Page 458
But for reasonable thicknesses such that the particle does not lose appreciable
energy , the Gaussian will still be peaked at very small forward angles . The
multiple - scattering distribution for the projected angle of scattering is 1 012 PM (
O ...
But for reasonable thicknesses such that the particle does not lose appreciable
energy , the Gaussian will still be peaked at very small forward angles . The
multiple - scattering distribution for the projected angle of scattering is 1 012 PM (
O ...
Page 459
13.8 Multiple and single scattering distributions of projected angle . In the region
of plural scattering ( a ~ 2–3 ) the dotted curve indicates the smooth transition
from the small - angle multiple scattering ( approximately Gaussian in shape ) to
the ...
13.8 Multiple and single scattering distributions of projected angle . In the region
of plural scattering ( a ~ 2–3 ) the dotted curve indicates the smooth transition
from the small - angle multiple scattering ( approximately Gaussian in shape ) to
the ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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