Linac Run Plan April 2018, Dr. McNulty: Difference between revisions
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Added .254cm of Tungsten and 2.286cm of Aluminum to be used as converter and beam stop. | Added .254cm of Tungsten and 2.286cm of Aluminum to be used as converter and beam stop. | ||
[[File:https://wiki.iac.isu.edu/index.php/File:Radiator.png]] | |||
Assuming <math>25\frac{mA}{pulse}</math> and a pulse width of <math>100ns</math> | Assuming <math>25\frac{mA}{pulse}</math> and a pulse width of <math>100ns</math> | ||
Revision as of 21:58, 24 April 2018
Absorbed Dose Information
100mA, 100ns pulse width, 25cm from beam pipe
Assuming [math]\displaystyle{ 100\frac{mA}{pulse} }[/math] and a pulse width of [math]\displaystyle{ 100ns }[/math]
Then [math]\displaystyle{ 100\frac{mA}{pulse}=100\frac{mC}{s*pulse}=0.1\frac{C}{s*pulse} }[/math]
[math]\displaystyle{ 0.1\frac{C}{s*pulse}(100ns)=10*10^{-9}\frac{C}{pulse} }[/math]
[math]\displaystyle{ 10*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=6.2422*10^{10}\frac{e-}{pulse} }[/math]
Using a distance of 25cm for all simulations following.
OSL
[math]\displaystyle{ \frac{1}{1000} }[/math] of a pulse. ~62mil e- simulated, ~62bil e- per pulse. With beam parameters given above.
Deposited Energy: [math]\displaystyle{ 4.46596*10^{6} MeV }[/math]
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
OSL Crystal density[math]\displaystyle{ =3.9698\frac{g}{cm^{3}} }[/math]
Mass of a single OSL crystal: [math]\displaystyle{ (\pi(0.2505)^{2}*(0.03))*(3.9698)=0.0234777g }[/math]
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes [math]\displaystyle{ 4.46596*10^{9} MeV }[/math]
Converting to Joules for dose calculation: [math]\displaystyle{ 4.46596*10^{9} MeV=7.15525*10^{-4}J }[/math]
Average dose per pulse [math]\displaystyle{ \frac{7.15525*10^{-4}J}{0.0234777*10^{-3}\ Kg}=30.4768\ Gy=3047.68\ rad }[/math]
Quartz
[math]\displaystyle{ \frac{1}{1000} }[/math] of a pulse. ~62mil e- simulated, ~62bil e- per pulse. With beam parameters given above.
Deposited Energy: [math]\displaystyle{ 4.71875*10^{8} MeV }[/math]
Quartz Geometry: 1 inch cylinder with electrons incident upon the base of the cylinder.
Quartz density[math]\displaystyle{ =2.32\frac{g}{cm^{3}} }[/math]
Mass of Quartz used in simulation: [math]\displaystyle{ (\pi(1.27)^{2}*(2.54))*(2.32)=29.8593g }[/math]
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes [math]\displaystyle{ 4.71875*10^{11} MeV }[/math]
Converting to Joules for dose calculation: [math]\displaystyle{ 4.71875*10^{11} MeV=0.0756027J }[/math]
Average dose per pulse [math]\displaystyle{ \frac{0.0756027\ J}{29.8593*10^{-3}\ Kg}=2.53196\ Gy=253.196\ rad }[/math]
25mA, 100ns pulse width, 25cm from beam pipe
Cut current by a factor of 4. 100mA->25mA
Assuming [math]\displaystyle{ 25\frac{mA}{pulse} }[/math] and a pulse width of [math]\displaystyle{ 100ns }[/math]
Then [math]\displaystyle{ 25\frac{mA}{pulse}=25\frac{mC}{s*pulse}=0.025\frac{C}{s*pulse} }[/math]
[math]\displaystyle{ 0.025\frac{C}{s*pulse}(100ns)=2.5*10^{-9}\frac{C}{pulse} }[/math]
[math]\displaystyle{ 2.5*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{10}\frac{e-}{pulse} }[/math]
Using a distance of 25cm for all simulations following.
OSL
[math]\displaystyle{ \frac{1}{1000} }[/math] of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy: [math]\displaystyle{ 1.11636*10^{6} MeV }[/math]
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
OSL Crystal density[math]\displaystyle{ =3.9698\frac{g}{cm^{3}} }[/math]
Mass of a single OSL crystal: [math]\displaystyle{ (\pi(0.2505)^{2}*(0.03))*(3.9698)=0.0234777g }[/math]
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes [math]\displaystyle{ 1.11636*10^{9} MeV }[/math]
Converting to Joules for dose calculation: [math]\displaystyle{ 1.11636*10^{9} MeV=1.78841*10^{-4}J }[/math]
Average dose per pulse [math]\displaystyle{ \frac{1.78841*10^{-4}J}{0.0234777*10^{-3}\ Kg}=7.61748\ Gy=761.748\ rad }[/math]
Quartz
[math]\displaystyle{ \frac{1}{1000} }[/math] of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy: [math]\displaystyle{ 9.82027*10^{7} MeV }[/math]
Quartz Geometry: 1 inch diameter, 0.5 inch tall cylinder with electrons incident upon the base of the cylinder.
Quartz density[math]\displaystyle{ =2.32\frac{g}{cm^{3}} }[/math]
Mass of Quartz used in simulation: [math]\displaystyle{ (\pi(1.27)^{2}*(1.27))*(2.32)=14.9296g }[/math]
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes [math]\displaystyle{ 9.82027*10^{10} MeV }[/math]
Converting to Joules for dose calculation: [math]\displaystyle{ 9.82027*10^{10} MeV=0.0157321J }[/math]
Average dose per pulse [math]\displaystyle{ \frac{0.0157321\ J}{14.9296*10^{-3}\ Kg}=1.05375\ Gy=105.375\ rad }[/math]
25mA, 100ns pulse width, 50cm from beam pipe
Changed distance from end of beam pipe from 25cm to 50cm.
Cut current by a factor of 4. 100mA->25mA
Assuming [math]\displaystyle{ 25\frac{mA}{pulse} }[/math] and a pulse width of [math]\displaystyle{ 100ns }[/math]
Then [math]\displaystyle{ 25\frac{mA}{pulse}=25\frac{mC}{s*pulse}=0.025\frac{C}{s*pulse} }[/math]
[math]\displaystyle{ 0.025\frac{C}{s*pulse}(100ns)=2.5*10^{-9}\frac{C}{pulse} }[/math]
[math]\displaystyle{ 2.5*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{10}\frac{e-}{pulse} }[/math]
OSL
[math]\displaystyle{ \frac{1}{1000} }[/math] of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy: [math]\displaystyle{ 9.29701*10^{5} MeV }[/math]
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
OSL Crystal density[math]\displaystyle{ =3.9698\frac{g}{cm^{3}} }[/math]
Mass of a single OSL crystal: [math]\displaystyle{ (\pi(0.2505)^{2}*(0.03))*(3.9698)=0.0234777g }[/math]
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes [math]\displaystyle{ 9.29701*10^{8} MeV }[/math]
Converting to Joules for dose calculation: [math]\displaystyle{ 9.29701*10^{8} MeV=1.48938*10^{-4}J }[/math]
Average dose per pulse: [math]\displaystyle{ \frac{1.48938*10^{-4}J}{0.0234777*10^{-3}\ Kg}=6.34381\ Gy=634.381\ rad }[/math]
Quartz
[math]\displaystyle{ \frac{1}{1000} }[/math] of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy: [math]\displaystyle{ 9.21601*10^{7} MeV }[/math]
Quartz Geometry: 1 inch diameter, 0.5 inch tall cylinder with electrons incident upon the base of the cylinder.
Quartz density[math]\displaystyle{ =2.32\frac{g}{cm^{3}} }[/math]
Mass of Quartz used in simulation: [math]\displaystyle{ (\pi(1.27)^{2}*(1.27))*(2.32)=14.9296g }[/math]
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes [math]\displaystyle{ 9.21601*10^{10} MeV }[/math]
Converting to Joules for dose calculation: [math]\displaystyle{ 9.21601*10^{10} MeV=0.0147657J }[/math]
Average dose per pulse [math]\displaystyle{ \frac{0.0147657\ J}{14.9296*10^{-3}\ Kg}=0.98902\ Gy=98.902\ rad }[/math]
25mA, 100ns pulse width, 50cm from beam pipe, tungsten target with aluminum beamstop
Added .254cm of Tungsten and 2.286cm of Aluminum to be used as converter and beam stop.
File:Https://wiki.iac.isu.edu/index.php/File:Radiator.png
Assuming [math]\displaystyle{ 25\frac{mA}{pulse} }[/math] and a pulse width of [math]\displaystyle{ 100ns }[/math]
Then [math]\displaystyle{ 25\frac{mA}{pulse}=25\frac{mC}{s*pulse}=0.025\frac{C}{s*pulse} }[/math]
[math]\displaystyle{ 0.025\frac{C}{s*pulse}(100ns)=2.5*10^{-9}\frac{C}{pulse} }[/math]
[math]\displaystyle{ 2.5*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{10}\frac{e-}{pulse} }[/math]
OSL
[math]\displaystyle{ \frac{1}{1000} }[/math] of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy: [math]\displaystyle{ 9.29701*10^{5} MeV }[/math]
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
OSL Crystal density[math]\displaystyle{ =3.9698\frac{g}{cm^{3}} }[/math]
Mass of a single OSL crystal: [math]\displaystyle{ (\pi(0.2505)^{2}*(0.03))*(3.9698)=0.0234777g }[/math]
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes [math]\displaystyle{ 9.29701*10^{8} MeV }[/math]
Converting to Joules for dose calculation: [math]\displaystyle{ 9.29701*10^{8} MeV=1.48938*10^{-4}J }[/math]
Average dose per pulse: [math]\displaystyle{ \frac{1.48938*10^{-4}J}{0.0234777*10^{-3}\ Kg}=6.34381\ Gy=634.381\ rad }[/math]
Quartz
[math]\displaystyle{ \frac{1}{1000} }[/math] of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy: [math]\displaystyle{ 9.21601*10^{7} MeV }[/math]
Quartz Geometry: 1 inch diameter, 0.5 inch tall cylinder with electrons incident upon the base of the cylinder.
Quartz density[math]\displaystyle{ =2.32\frac{g}{cm^{3}} }[/math]
Mass of Quartz used in simulation: [math]\displaystyle{ (\pi(1.27)^{2}*(1.27))*(2.32)=14.9296g }[/math]
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes [math]\displaystyle{ 9.21601*10^{10} MeV }[/math]
Converting to Joules for dose calculation: [math]\displaystyle{ 9.21601*10^{10} MeV=0.0147657J }[/math]
Average dose per pulse [math]\displaystyle{ \frac{0.0147657\ J}{14.9296*10^{-3}\ Kg}=0.98902\ Gy=98.902\ rad }[/math]