Difference between revisions of "Counts Rate (44 MeV LINAC)"
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==bremsstrahlung== | ==bremsstrahlung== | ||
− | from plot above in (10 | + | plot from Dale<br> |
+ | from plot above in (10,20) MeV region we have about<br> | ||
0.1 photons/electrons/MeV/r.l | 0.1 photons/electrons/MeV/r.l | ||
Line 24: | Line 25: | ||
<math>0.1 \frac{\gamma 's}{(e^-\ MeV\ r.l.)} \times 3.48 \cdot 10^{-4} r.l. \times 10\ MeV \times 0.47 \cdot 10^{13} \frac{e^-}{sec}=1.64 \cdot 10^{9} \frac{\gamma}{sec}</math><br><br> | <math>0.1 \frac{\gamma 's}{(e^-\ MeV\ r.l.)} \times 3.48 \cdot 10^{-4} r.l. \times 10\ MeV \times 0.47 \cdot 10^{13} \frac{e^-}{sec}=1.64 \cdot 10^{9} \frac{\gamma}{sec}</math><br><br> | ||
− | =number of neutrons in | + | =Collimation factor= |
+ | We take 4-6 % of total number of photons going through collimator(Alex, GEANT calculation)<br> | ||
+ | |||
+ | =Number of neutrons/sec= | ||
+ | plot from Berman<br> | ||
+ | From plot above the average cross section for <math>^{238}U</math> in (10,20) MeV region is: | ||
+ | 130 mb | ||
+ | |||
+ | |||
=geometrical factor, isotropic case= | =geometrical factor, isotropic case= |
Revision as of 21:04, 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
from plot above in (10,20) MeV region we have about
0.1 photons/electrons/MeV/r.l
radiation length
radiation length of Ti(Z=22) is 3.59 cm
Assume the radiator thickness is
steps together...
Collimation factor
We take 4-6 % of total number of photons going through collimator(Alex, GEANT calculation)
Number of neutrons/sec
plot from Berman
From plot above the average cross section for in (10,20) MeV region is:
130 mb