Difference between revisions of "Multiple scattering Angle"
Jump to navigation
Jump to search
![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)
(19 intermediate revisions by the same user not shown) | |||
Line 1: | Line 1: | ||
− | Angle as a Function of Radiation Length | + | [http://wiki.iac.isu.edu/index.php/HRRL Go Back] |
− | [[Image:Theta vs Radiation Length.JPG]] | + | |
+ | |||
+ | =Multiple Scattering Angle= | ||
+ | |||
+ | <math>\theta_{0} = \frac{13.6 MeV}{\beta cp}z{\sqrt{x/X_{0}}}{[1+0.038ln{(x/X_{0})}]}</math> | ||
+ | |||
+ | p = momentum of the incident particle | ||
+ | |||
+ | <math>\beta</math>c = velocity of the incident particle | ||
+ | |||
+ | z = charge number of the incident particle | ||
+ | |||
+ | <math>x/X_{0}</math> = thickness of the scattering medium in radiation lengths | ||
+ | |||
+ | ==1.Angle as a Function of Radiation Length== | ||
+ | [[Image:Theta vs Radiation Length.JPG |400 px]] | ||
---- | ---- | ||
+ | ==2.Graphs of Angle vs. Radiator Thickness for various metals== | ||
Scattering Angle as a Function of Thickness | Scattering Angle as a Function of Thickness | ||
− | [[Image:Al,Ti, W, Fe.JPG]] | + | {| border="1" cellpadding="20" cellspacing="0" |
− | [[Image:ATi.JPG]] | + | |- |
− | [[Image:FeL.JPG]] | + | [[Image:Al,Ti, W, Fe.JPG | 400 px]] |
− | [[Image:WRL.JPG]] | + | |- |
− | + | [[Image:ATi.JPG | 400 px]] | |
+ | |- | ||
+ | [[Image:FeL.JPG | 400 px]] | ||
+ | |- | ||
+ | [[Image:WRL.JPG | 400 px]] | ||
+ | |}<br> | ||
---- | ---- | ||
+ | ==3.Table of Radiator thickness for specific scattering angles== | ||
Radiator Thickness given specific Scattering Angles: | Radiator Thickness given specific Scattering Angles: | ||
Line 32: | Line 54: | ||
|- | |- | ||
|-<br> | |-<br> | ||
+ | } | ||
+ | [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 |