Difference between revisions of "Linac Run Plan April 2018, Dr. McNulty"

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=Beam Line info=
 
=Beam Line info=
  
−
0 degree line
+
Machine: 25b Linac
  
−
Aluminum window = 0.5mm thick. Radius = 23.813mm
+
0<math>&deg;</math> port
 +
 
 +
Beam Energy: 8 MeV
  
−
Air gap between Aluminum window and glass slide = 45mm
+
Rep Rate: Max (150Hz?)
  
−
Glass slide Thickness = 1mm
+
Pulse Width: 100ns
  
 
=Run Plan=
 
=Run Plan=
  
−
Will use 15 OSLs from reproducibility study to find operating point of accelerator
+
==To find operating point==
  
−
85 Nanodot OSLs total
+
- Will use 15 OSLs from reproducibility study to make sure that dose is within acceptable range
−
 
 
−
Machine: 25b Linac
 
  
−
Beam Energy: 8 MeV
+
===Table===
  
−
Rep Rate: Max (150Hz)
+
'''Start at 7am'''
  
−
:{| border="2" style="text-align:center;" |cellpadding="20" cellspacing="0  
+
:{| border="2" style="text-align:center;" |cellpadding="20" cellspacing="0"
 +
! scope="col" style="width: 50px;" | Shot #
 +
! scope="col" style="width: 150px;" | Number of Pulses
 +
! scope="col" style="width: 150px;" | Number of OSLs
 +
! scope="col" style="width: 150px;" | Beam Current
 +
! scope="col" style="width: 150px;" | Dose/pulse
 +
! scope="col" style="width: 150px;" | Expected Dose/pulse
 +
|-
 +
| 1 || 80 || 1 ||50 mA || ||
 +
|-
 +
| 2 ||  || 1 || mA || ||
 
|-
 
|-
−
| Shot # ||Start Time || End Time || Number of Pulses || Number of OSLs || Distance to end of beampipe || Beam Current || Aluminum Brick
+
| 3 || || 1 || mA || ||
 
|-
 
|-
−
| 1 ||7:00am || 7:05am || 2 || 1 || 1m || 5 mA || Out
+
| 4  || || 1 || mA || ||
 
|-
 
|-
−
| 2 ||7:10am || 7:15am || 2 || 1 || 1m || 10 mA || Out
+
| 5  || || 1 || mA || ||
 
|-
 
|-
−
| 3 ||7:20am || 7:25am || 2 || 1 || 1m || 25 mA || Out
+
| 6  || || 1 || mA || ||
 
|-
 
|-
−
| 4 ||7:30am || 7:35am || 2 || 1 || 1m || 50 mA || Out
+
| 7 || || 1 || mA || ||
 
|-
 
|-
−
| 5 ||7:40am || 7:45am || 2 || 1 || 1m || 25 mA || Out
+
| 8  || || 1 || mA || ||
 
|-
 
|-
−
| 6 ||7:50am || 7:55am || 2 || 1 || 1m || 25 mA || Out
+
| 9  || || 1 || mA || ||
 
|-
 
|-
−
| 7 ||8:00am || 8:05am || 2 || 16 || 1m || 25 mA || In
+
| 10  || || 1 || mA || ||
 
|-
 
|-
−
| 8 ||8:10am || 8:15am || 2 || 16 || 1m || 25 mA || In
+
| 11  || || 1 || mA || ||
 
|-
 
|-
−
| 9 ||8:20am || 8:25am || 2 || 16 || 1m || 25 mA || Out
+
| 12  || || 1 || mA|| ||
 
|-
 
|-
−
| 10 ||8:30am || 8:35am || 2 || 16 || 1m || 25 mA || Out
+
| 13  || || 1 || mA|| ||
 
|-
 
|-
−
| 11 ||8:40am || 8:45am || 2 || 16 || 1m || 25 mA || Out
+
| 14  || || 1 || mA|| ||
 
|-
 
|-
 +
| 15  || || 1 || mA|| ||
 
|}
 
|}
  
−
=[[Absorbed Dose Information]]=
+
==Experiment==
  
−
==100mA, 100ns pulse width, 25cm from beam pipe==
+
85 Nanodot OSLs for use (dose not include OSLs from reproducibility study)
  
−
Assuming <math>100\frac{mA}{pulse}</math> and a pulse width of <math>100ns</math>
+
- upper limit of OSLs is 15Gy, want to be around 7.5Gy with multiple pulses
  
−
Then <math>100\frac{mA}{pulse}=100\frac{mC}{s*pulse}=0.1\frac{C}{s*pulse}</math>
+
Will talk to engineers about double pulsing and guaranteeing number of pulses and update.  
  
−
<math>0.1\frac{C}{s*pulse}(100ns)=10*10^{-9}\frac{C}{pulse}</math>
+
===Table===
  
−
<math>10*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=6.2422*10^{10}\frac{e-}{pulse}</math>
+
:{| border="2" style="text-align:center;" |cellpadding="20" cellspacing="0
 +
|-
 +
! scope="col" style="width: 50px;" | Shot #
 +
! scope="col" style="width: 120px;" | Number of Pulses
 +
! scope="col"| Number of OSLs
 +
! scope="col" style="width: 150px;" | Beam Current
 +
! scope="col" style="width: 150px;" | Aluminum Brick
 +
! scope="col" style="width: 150px;" | Dose/Pulse
 +
! scope="col" style="width: 150px;" | Expected Dose/Pulse
 +
|-
 +
| 1  ||  || 1 || mA || Out || ||
 +
|-
 +
| 2 ||  || 1 ||  mA || Out || || 
 +
|-
 +
| 3|| || 1 ||  mA || Out  || ||
 +
|-
 +
| 4 || || 1 ||  mA || Out  || ||
 +
|-
 +
| 5 || || 1 || mA || Out  || ||
 +
|-
 +
| 6 || || 1 ||  mA || Out  || ||
 +
|-
 +
| 7 || || 16 ||  mA || In || ||
 +
|-
 +
| 8 || || 16 ||  mA || In  || ||
 +
|-
 +
| 9 || || 16 || mA || Out || ||
 +
|-
 +
| 10 || || 16 || mA || Out || ||
 +
|-
 +
| 11 || || 16 || mA || Out || ||
 +
|-
 +
|}
  
−
Using a distance of 25cm for all simulations following.
+
=[[Absorbed Dose Information]]=
  
−
===OSL===
+
Titanium window = 0.5mm thick. Radius = 23.813mm
  
−
<math>\frac{1}{1000}</math> of a pulse. ~62mil e- simulated, ~62bil e- per pulse. With beam parameters given above.
+
Air gap between Titanium window and glass slide = 45mm
  
−
Deposited Energy: <math>4.46596*10^{6} MeV</math>
+
Glass slide Thickness = 1mm
  
−
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
+
==[[5mA, 100ns pulse width, 100cm from beam pipe with Titanium window]]==
  
−
OSL Crystal density<math>=3.9698\frac{g}{cm^{3}}</math>
+
==[[25mA, 100ns pulse width, 100cm from beam pipe, with Titanium window]]==
  
−
Mass of a single OSL crystal: <math>(\pi(0.2505)^{2}*(0.03))*(3.9698)=0.0234777g</math>
+
==[[10mA, 100ns pulse width, 100cm from beam pipe, with Titanium window]]==
  
−
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes <math>4.46596*10^{9} MeV</math>
+
==[[100mA, 100ns pulse width, 100cm from beam pipe, with Titanium window]]==
  
−
Converting to Joules for dose calculation: <math>4.46596*10^{9} MeV=7.15525*10^{-4}J</math>
+
==[[25mA, 100ns pulse width, 50cm from beam pipe, tungsten target with aluminum beamstop]]==
  
−
Average dose per pulse <math>\frac{7.15525*10^{-4}J}{0.0234777*10^{-3}\ Kg}=30.4768\ Gy=3047.68\ rad</math>
+
----
  
−
===Quartz===
+
==[[100mA, 100ns pulse width, 25cm from beam pipe]]==
  
−
<math>\frac{1}{1000}</math> of a pulse. ~62mil e- simulated, ~62bil e- per pulse. With beam parameters given above.
+
==[[25mA, 100ns pulse width, 25cm from beam pipe]]==
  
−
Deposited Energy: <math>4.71875*10^{8} MeV</math>
+
==[[25mA, 100ns pulse width, 50cm from beam pipe]]==
  
−
Quartz Geometry: 1 inch cylinder with electrons incident upon the base of the cylinder.
 
  
−
Quartz density<math>=2.32\frac{g}{cm^{3}}</math>
+
----
−
 
 
−
Mass of Quartz used in simulation: <math>(\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>4.71875*10^{11} MeV</math>
 
−
 
 
−
Converting to Joules for dose calculation: <math>4.71875*10^{11} MeV=0.0756027J</math>
 
  
−
Average dose per pulse <math>\frac{0.0756027\ J}{29.8593*10^{-3}\ Kg}=2.53196\ Gy=253.196\ rad</math>
+
Low Dose Line: Dose = (0.11 +/- 0.01)(PMT Counts) + (119.29 +/- 29.08)
  
−
==25mA, 100ns pulse width, 25cm from beam pipe==
+
High Dose Line: Dose = (1.54 +/- 0.06)(PMT Counts) + (1004.80 +/- 1006.24)
  
−
Cut current by a factor of 4. 100mA->25mA
 
  
−
Assuming <math>25\frac{mA}{pulse}</math> and a pulse width of <math>100ns</math>
+
Peak Current: <math>50\frac{mA}{pulse}</math>  
  
−
Then <math>25\frac{mA}{pulse}=25\frac{mC}{s*pulse}=0.025\frac{C}{s*pulse}</math>
+
Pulse Width: <math>500ns</math>
  
−
<math>0.025\frac{C}{s*pulse}(100ns)=2.5*10^{-9}\frac{C}{pulse}</math>
 
  
−
<math>2.5*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{10}\frac{e-}{pulse}</math>
+
<math>50\frac{mA}{pulse}=50\frac{mC}{s*pulse}=0.050\frac{C}{s*pulse}</math>
  
−
Using a distance of 25cm for all simulations following.  
+
<math>0.050\frac{C}{s*pulse}(500ns)=2.5*10^{-8}\frac{C}{pulse}</math>
  
−
===OSL===
+
<math>2.5*10^{-8}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{11}\frac{e-}{pulse}</math>
  
−
<math>\frac{1}{1000}</math> of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
 
−
 
−
Deposited Energy: <math>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>=3.9698\frac{g}{cm^{3}}</math>
 
−
 
−
Mass of a single OSL crystal: <math>(\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>1.11636*10^{9} MeV</math>
 
−
 
−
Converting to Joules for dose calculation: <math>1.11636*10^{9} MeV=1.78841*10^{-4}J</math>
 
−
 
−
Average dose per pulse <math>\frac{1.78841*10^{-4}J}{0.0234777*10^{-3}\ Kg}=7.61748\ Gy=761.748\ rad</math>
 
−
 
−
===Quartz===
 
−
 
−
<math>\frac{1}{1000}</math> of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
 
−
 
−
Deposited Energy: <math>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>=2.32\frac{g}{cm^{3}}</math>
 
−
 
−
Mass of Quartz used in simulation: <math>(\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>9.82027*10^{10} MeV</math>
 
−
 
−
Converting to Joules for dose calculation: <math>9.82027*10^{10} MeV=0.0157321J</math>
 
−
 
−
Average dose per pulse <math>\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>25\frac{mA}{pulse}</math> and a pulse width of <math>100ns</math>
 
−
 
−
Then <math>25\frac{mA}{pulse}=25\frac{mC}{s*pulse}=0.025\frac{C}{s*pulse}</math>
 
−
 
−
<math>0.025\frac{C}{s*pulse}(100ns)=2.5*10^{-9}\frac{C}{pulse}</math>
 
−
 
−
<math>2.5*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{10}\frac{e-}{pulse}</math>
 
−
 
−
===OSL===
 
−
 
−
<math>\frac{1}{1000}</math> of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
 
−
 
−
Deposited Energy: <math>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>=3.9698\frac{g}{cm^{3}}</math>
 
−
 
−
Mass of a single OSL crystal: <math>(\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>9.29701*10^{8} MeV</math>
 
−
 
−
Converting to Joules for dose calculation: <math>9.29701*10^{8} MeV=1.48938*10^{-4}J</math>
 
−
 
−
Average dose per pulse: <math>\frac{1.48938*10^{-4}J}{0.0234777*10^{-3}\ Kg}=6.34381\ Gy=634.381\ rad</math>
 
−
 
−
===Quartz===
 
−
 
−
<math>\frac{1}{1000}</math> of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
 
−
 
−
Deposited Energy: <math>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>=2.32\frac{g}{cm^{3}}</math>
 
−
 
−
Mass of Quartz used in simulation: <math>(\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>9.21601*10^{10} MeV</math>
 
−
 
−
Converting to Joules for dose calculation: <math>9.21601*10^{10} MeV=0.0147657J</math>
 
−
 
−
Average dose per pulse <math>\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:Radiator.png]]
 
−
 
−
Assuming <math>25\frac{mA}{pulse}</math> and a pulse width of <math>100ns</math>
 
−
 
−
Then <math>25\frac{mA}{pulse}=25\frac{mC}{s*pulse}=0.025\frac{C}{s*pulse}</math>
 
−
 
−
<math>0.025\frac{C}{s*pulse}(100ns)=2.5*10^{-9}\frac{C}{pulse}</math>
 
−
 
−
<math>2.5*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{10}\frac{e-}{pulse}</math>
 
−
 
−
===OSL (8MeV)===
 
−
 
−
<math>\frac{1}{1000}</math> of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
 
−
 
−
Deposited Energy: <math>19.1759 MeV</math>
 
−
 
−
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
 
−
 
−
OSL Crystal density<math>=3.9698\frac{g}{cm^{3}}</math>
 
−
 
−
Mass of a single OSL crystal: <math>(\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>9.29701*10^{8} MeV</math>
 
−
 
−
Converting to Joules for dose calculation: <math>19.1759*10^{3} MeV=3.0723177*10^{-9}J</math>
 
−
 
−
Average dose per pulse: <math>\frac{3.0723177*10^{-9}J}{0.0234777*10^{-3}\ Kg}=0.000130861\ Gy=0.0130861\ rad</math>
 
  
  
Line 235: Line 154:
 
----
 
----
 
[[Thesis]]
 
[[Thesis]]
 +
 +
[[May 31st 2018 - 25b 0 degree port]]

Latest revision as of 01:41, 27 June 2018

Beam Line info

Machine: 25b Linac

0[math]°[/math] port

Beam Energy: 8 MeV

Rep Rate: Max (150Hz?)

Pulse Width: 100ns

Run Plan

To find operating point

- Will use 15 OSLs from reproducibility study to make sure that dose is within acceptable range

Table

Start at 7am

Shot # Number of Pulses Number of OSLs Beam Current Dose/pulse Expected Dose/pulse
1 80 1 50 mA
2 1 mA
3 1 mA
4 1 mA
5 1 mA
6 1 mA
7 1 mA
8 1 mA
9 1 mA
10 1 mA
11 1 mA
12 1 mA
13 1 mA
14 1 mA
15 1 mA

Experiment

85 Nanodot OSLs for use (dose not include OSLs from reproducibility study)

- upper limit of OSLs is 15Gy, want to be around 7.5Gy with multiple pulses

Will talk to engineers about double pulsing and guaranteeing number of pulses and update.

Table

Shot # Number of Pulses Number of OSLs Beam Current Aluminum Brick Dose/Pulse Expected Dose/Pulse
1 1 mA Out
2 1 mA Out
3 1 mA Out
4 1 mA Out
5 1 mA Out
6 1 mA Out
7 16 mA In
8 16 mA In
9 16 mA Out
10 16 mA Out
11 16 mA Out

Absorbed Dose Information

Titanium window = 0.5mm thick. Radius = 23.813mm

Air gap between Titanium window and glass slide = 45mm

Glass slide Thickness = 1mm

5mA, 100ns pulse width, 100cm from beam pipe with Titanium window

25mA, 100ns pulse width, 100cm from beam pipe, with Titanium window

10mA, 100ns pulse width, 100cm from beam pipe, with Titanium window

100mA, 100ns pulse width, 100cm from beam pipe, with Titanium window

25mA, 100ns pulse width, 50cm from beam pipe, tungsten target with aluminum beamstop

100mA, 100ns pulse width, 25cm from beam pipe

25mA, 100ns pulse width, 25cm from beam pipe

25mA, 100ns pulse width, 50cm from beam pipe

Low Dose Line: Dose = (0.11 +/- 0.01)(PMT Counts) + (119.29 +/- 29.08)

High Dose Line: Dose = (1.54 +/- 0.06)(PMT Counts) + (1004.80 +/- 1006.24)


Peak Current: [math]50\frac{mA}{pulse}[/math]

Pulse Width: [math]500ns[/math]


[math]50\frac{mA}{pulse}=50\frac{mC}{s*pulse}=0.050\frac{C}{s*pulse}[/math]

[math]0.050\frac{C}{s*pulse}(500ns)=2.5*10^{-8}\frac{C}{pulse}[/math]

[math]2.5*10^{-8}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{11}\frac{e-}{pulse}[/math]



Thesis

May 31st 2018 - 25b 0 degree port

Retrieved from "https://wiki.iac.isu.edu/index.php?title=Linac_Run_Plan_April_2018,_Dr._McNulty&oldid=123674"