Difference between revisions of "Counts Rate (44 MeV LINAC)"
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Line 13: | Line 13: | ||
==bremsstrahlung== | ==bremsstrahlung== | ||
− | plot from Dale | + | plot from Dale |
− | + | ||
+ | in (10,20) MeV region we have about | ||
+ | |||
0.1 photons/electrons/MeV/r.l | 0.1 photons/electrons/MeV/r.l | ||
==radiation length== | ==radiation length== | ||
− | + | r.l. Ti(Z=22) is 3.59 cm | |
− | + | ||
+ | take radiator thickness is <math>12.5 \mu m</math> | ||
+ | |||
<math>3.59 cm/12.5\mu m = 3.48 \cdot 10^{-4} \ r.l.</math><br> | <math>3.59 cm/12.5\mu m = 3.48 \cdot 10^{-4} \ r.l.</math><br> | ||
Revision as of 21:54, 17 May 2010
LINAC parameters used in calculations
1) pulse width 50 ns
2) pulse current 50 A
3) repetition rate 300 Hz
4) energy 44 MeV
Number of electrons/sec on radiator
Number of photons/sec from radiator
bremsstrahlung
plot from Dale
in (10,20) MeV region we have about
0.1 photons/electrons/MeV/r.l
radiation length
r.l. Ti(Z=22) is 3.59 cm
take radiator thickness is
steps together...
Collimation factor
We take 4-6 % of total number of photons going through collimator (Alex, GEANT calculation)
So, the flux incident on target is
Number of neutrons/sec (yields)
cross section
plot from Berman
From plot above the average cross section for in (10,20) MeV region is:
130 mb
target thickness,
Assume the target thickness is 1 cm ->
neutrons per fission
2.4 neutrons/fission
steps together...
Worst Case Isotropic Neutrons
Let's say we have:
radius detector = 1 cm
1 meter away
fractional solid angle =
<= geometrical acceptance