Difference between revisions of "100mA, 100ns pulse width, 100cm from beam pipe, with Titanium window"
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<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> | ||
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===OSL=== | ===OSL=== | ||
Revision as of 18:09, 30 May 2018
Assuming
and a pulse width ofThen
OSL
of a pulse. 624219 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. ~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
Plastic
of a pulse. ~15mil e- simulated, ~15bil e- per pulse. With beam parameters given above.
Deposited Energy:
Plastic Geometry: 1 inch diameter, 0.5 inch tall cylinder with electrons incident upon the base of the cylinder.
Plastic density
Mass of Plastic 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