Difference between revisions of "Multiple scattering Angle"
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![Al,Ti, W, Fe.JPG](/./images/thumb/7/74/Al%2CTi%2C_W%2C_Fe.JPG/400px-Al%2CTi%2C_W%2C_Fe.JPG)
![ATi.JPG](/./images/thumb/6/6c/ATi.JPG/400px-ATi.JPG)
![FeL.JPG](/./images/thumb/0/05/FeL.JPG/400px-FeL.JPG)
![WRL.JPG](/./images/thumb/3/3e/WRL.JPG/400px-WRL.JPG)
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=Multiple Scattering Angle= | =Multiple Scattering Angle= | ||
− | <math>theta_{0} = 13.6 MeV | + | |
− | + | <math>\theta_{0} = \frac{13.6 MeV}{\beta cp}z{\sqrt{x/X_{0}}}{[1+0.038ln{(x/X_{0})}]}</math> | |
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+ | p = momentum of the incident particle | ||
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+ | <math>\beta</math>c = velocity of the incident particle | ||
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+ | z = charge number of the incident particle | ||
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+ | <math>x/X_{0}</math> = thickness of the scattering medium in radiation lengths | ||
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==1.Angle as a Function of Radiation Length== | ==1.Angle as a Function of Radiation Length== | ||
[[Image:Theta vs Radiation Length.JPG |400 px]] | [[Image:Theta vs Radiation Length.JPG |400 px]] | ||
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+ | [http://wiki.iac.isu.edu/index.php/HRRL Go Back] |
Latest revision as of 16:30, 10 June 2010
Multiple Scattering Angle
p = momentum of the incident particle
c = velocity of the incident particle
z = charge number of the incident particle
= thickness of the scattering medium in radiation lengths
1.Angle as a Function of Radiation Length
2.Graphs of Angle vs. Radiator Thickness for various metals
Scattering Angle as a Function of Thickness
3.Table of Radiator thickness for specific scattering angles
Radiator Thickness given specific Scattering Angles:
} Go BackRadiator | 0.2 degrees | 0.3 degrees | 0.4 degrees | 0.5 degrees | 0.6 degrees |
W | 0.15 microns | 0.3 microns | 0.5 microns | 0.7 microns | 1 micron |
Fe | 0.7 microns | 1.4 microns | 2.5 microns | 3.6 microns | 5 microns |
Ti | 1.4 microns | 2.8 microns | 4.8 microns | 7.2 microns | 10 microns |
Al | 3.5 microns | 7.1 microns | 12 microns | 18 microns | 25 microns |
Radiation Length | 3.9 E-5 | 8 E-5 | 1.35 E-4 | 2 E-4 | 2.8 E-4 |