Difference between revisions of "Linac Run Plan April 2018, Dr. McNulty"
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Average dose per pulse <math>\frac{0.0157321\ J}{29.8593*10^{-3}\ Kg}=0.526873\ Gy=52.6873\ rad</math> | Average dose per pulse <math>\frac{0.0157321\ J}{29.8593*10^{-3}\ Kg}=0.526873\ Gy=52.6873\ rad</math> | ||
+ | |||
+ | ==Calculations (3)== | ||
+ | |||
+ | 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> | ||
+ | |||
+ | Using a distance of 25cm for all simulations following. | ||
+ | |||
+ | ===OSL=== | ||
+ | |||
+ | <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}*(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>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}{29.8593*10^{-3}\ Kg}=0.526873\ Gy=52.6873\ rad</math> | ||
+ | |||
+ | |||
+ | |||
---- | ---- | ||
[[Thesis]] | [[Thesis]] |
Revision as of 19:05, 23 April 2018
Absorbed Dose Information
Calculations (1)
Assuming
and a pulse width ofThen
Using a distance of 25cm for all simulations following.
OSL
of a pulse. ~62mil e- simulated, ~62bil e- per pulse. With beam parameters given above.
Deposited Energy:
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
OSL Crystal density
Mass of a single OSL crystal:
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes
Converting to Joules for dose calculation:
Average dose per pulse
Quartz
of a pulse. ~62mil e- simulated, ~62bil e- per pulse. With beam parameters given above.
Deposited Energy:
Quartz Geometry: 1 inch cylinder with electrons incident upon the base of the cylinder.
Quartz density
Mass of Quartz used in simulation:
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes
Converting to Joules for dose calculation:
Average dose per pulse
Calculations (2)
Cut current by a factor of 4. 100mA->25mA
Assuming
and a pulse width ofThen
Using a distance of 25cm for all simulations following.
OSL
of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy:
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
OSL Crystal density
Mass of a single OSL crystal:
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes
Converting to Joules for dose calculation:
Average dose per pulse
Quartz
of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy:
Quartz Geometry: 1 inch diameter, 0.5 inch tall cylinder with electrons incident upon the base of the cylinder.
Quartz density
Mass of Quartz used in simulation:
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes
Converting to Joules for dose calculation:
Average dose per pulse
Calculations (3)
Cut current by a factor of 4. 100mA->25mA
Assuming
and a pulse width ofThen
Using a distance of 25cm for all simulations following.
OSL
of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy:
OSL geometry: 0.501cm diameter cylinder of 0.03cm thickness with beam incident on flat face.
OSL Crystal density
Mass of a single OSL crystal:
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes
Converting to Joules for dose calculation:
Average dose per pulse
Quartz
of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy:
Quartz Geometry: 1 inch diameter, 0.5 inch tall cylinder with electrons incident upon the base of the cylinder.
Quartz density
Mass of Quartz used in simulation:
Scaling deposited energy by 1000 to account for only shooting a 1000th of a pulse, the deposited energy becomes
Converting to Joules for dose calculation:
Average dose per pulse