Difference between revisions of "Linac Run Plan April 2018, Dr. McNulty"
Line 1: | Line 1: | ||
+ | =[[Absorbed Dose Information]]= | ||
+ | |||
==Calculations (1)== | ==Calculations (1)== | ||
Line 8: | Line 10: | ||
<math>10*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=6.2422*10^{10}\frac{e-}{pulse}</math> | <math>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. | Using a distance of 25cm for all simulations following. | ||
Line 62: | Line 60: | ||
<math>2.5*10^{-9}\frac{C}{pulse}*\frac{1\ e-}{1.602*10^{-19}}=1.56055*10^{10}\frac{e-}{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. | Using a distance of 25cm for all simulations following. | ||
Line 71: | Line 65: | ||
===OSL=== | ===OSL=== | ||
− | <math>\frac{1}{1000}</math> of a pulse. ~ | + | <math>\frac{1}{1000}</math> of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above. |
Deposited Energy: <math>4.46596*10^{6} MeV</math> | Deposited Energy: <math>4.46596*10^{6} MeV</math> | ||
Line 89: | Line 83: | ||
===Quartz=== | ===Quartz=== | ||
− | <math>\frac{1}{1000}</math> of a pulse. ~ | + | <math>\frac{1}{1000}</math> of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above. |
Deposited Energy: <math>4.71875*10^{8} MeV</math> | Deposited Energy: <math>4.71875*10^{8} MeV</math> |
Revision as of 16:51, 18 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 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