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Page 456
13.7 Mean Square Angle of Scattering and the Angular Distribution of Multiple
Scattering Rutherford scattering is confined to very small angles even for a point
Coulomb field , and for fast particles Omax is small compared to unity . Thus there
...
13.7 Mean Square Angle of Scattering and the Angular Distribution of Multiple
Scattering Rutherford scattering is confined to very small angles even for a point
Coulomb field , and for fast particles Omax is small compared to unity . Thus there
...
Page 458
( O2 ) – 40N In ( 13.111 ) pv The mean square angle increases linearly with the
thickness t . But for reasonable thicknesses such that the particle does not lose
appreciable energy , the Gaussian will still be peaked at very small forward
angles .
( O2 ) – 40N In ( 13.111 ) pv The mean square angle increases linearly with the
thickness t . But for reasonable thicknesses such that the particle does not lose
appreciable energy , the Gaussian will still be peaked at very small forward
angles .
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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