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RE: Help in MCNP5
Yes, put an "e" card with your "f" card when you perform your tally. The
"e" card (Tally Energy card) can score your results in energy bins. I'm
looking at page 3-72, but that's of the MCNP4B manual.
Mike
Michael G. Stabin, PhD, CHP
Assistant Professor of Radiology and Radiological Sciences
Department of Radiology and Radiological Sciences
Vanderbilt University
1161 21st Avenue South
Nashville, TN 37232-2675
Phone (615) 343-0068
Fax (615) 322-3764
Pager (615) 835-5153
e-mail michael.g.stabin@vanderbilt.edu
internet www.doseinfo-radar.com
-----Original Message-----
From: owner-radsafe@list.vanderbilt.edu
[mailto:owner-radsafe@list.vanderbilt.edu] On Behalf Of Pramoth CM
Sent: Tuesday, November 23, 2004 11:07 AM
To: radsafe@list.vanderbilt.edu
Subject: Help in MCNP5
Hi Group,
I am a student working with MCNP5 and using a very small code to
obtain a
tally of gamma ray spectrum of a particular gamma ray energy for a given
number of events or live time. I want to modify this code so that the
code
would generate spectrums at increments at10 kev interval for 0 - 1000
kev. The only option of doing this which I can think of is running the
original
code over and over at 10 kev increments - which would be time consuming.
Could anybody suggest the required change in the code, so that I could
run
the code only once and then obtain a single OUTPUT file with a 100
columns
( each column representing the spectrum at 10 kev intervals) . I am very
new to MCNP5 and read the required parts of the MCNP5 manual and could
not
figure out how to do this. I will be really grateful if anybody could
help.
I have provided the original code below.
c ************************** Cell definition cards
************************** c RightCircularCylinder Detector Assembly c
Sensor Cell Definition Cards c
1 117 -3.67 (-1 2 -3 ) imp:p 1 $ NaI Sensor
c
c End Cap
c
20 213 -2.70 (84 -85 -82) imp:p 1 $ Al EndCap
Window
21 444 -8.00 (82 -83 -85 81 ):(-80 81 -82 ) imp:p 1 $ SS EndCap
c
c Vacuum
c
32 0 (-84 1 -82) imp:p 1 $ Vacuum
c
c Everything else...
c
988 220 -0.0012 (-900 -901 902 )(-81: 83: 85) &
&
imp:p 1 $ Detector environment
999 0 (900: 901: -902) imp:p 0 $ Outside world
c ************************* Surface definition cards
************************* c c Sensor Surface Definition Cards c
1 pz 0.00 $ Top Face of sensor
2 pz -5.08 $ Bottom Face of sensor
3 cz 2.54 $ Outer Radius of sensor
c
c End Cap and End Cap Window
c
80 pz -5.08 $ Inside Lower bound of detector end cap
81 pz -5.3975 $ Outside Lower bound of detector end cap
82 cz 2.54 $ Inside radius of end cap
83 cz 2.8575 $ Outside radius of end cap
84 pz 0.5 $ Inside detector Face
85 pz 0.55 $ Outside detector face
c
c Bounding surfaces
900 cz 3.8575 $ Bounding cylinder
901 pz 12 $ Bounding top Surface
902 pz -6.3975 $ Bounding bottom Surface
c ******************************** Data cards
******************************** c Mode P c c Material Cards c
m220 6000.01p -0.000124 $ C Air, rho = -0.001205 g/cc
7000.01p -0.755267 $ N
8000.01p -0.231781 $ O
18000.01p -0.012827 $ Ar
c
m117 11000.01p 1 $ NaI, rho = -3.67 g/cc
53000.01p 1
c
m444 6000.01p -0.0024 $ Stainless Steel, rho = -8 g/cc
14000.01p -0.064
15000.01p -0.0028
16000.01p -0.0016
22000.01p -0.032
24000.01p -1.44
25000.01p -0.16
26000.01p -5.5
27000.01p -0.002
28000.01p -0.8
c
m213 13000.01p 1 $ Aluminum, rho = -2.7 g/cc
c
c Tally defination card(s)
c
f8:p (1) $ Pulse Height tally on cell 1
c Gaussian Energy Broadening Term
ft8 geb 0 0.05086 0.30486 $ for NAI
c
c Source definition cards
c
sdef pos= 0 0 10 erg=d3
c
c Remember! The calculated efficiency is per photon emitted, so if you
have
more
c than one photon energy, and they are all equally probable, multiply by
N c
# si3 sp3
L D
1.0000 1.565E+15
c
c Energy Range and bin width [in MeV!]
c
e0 0 1e-5 8e-3 512i 4.112 $ 8 KeV bins up to 4096 KeV
c
c Number of particles to follow
c
nps 67900000
c
c .OR. Minutes to run
c
c ctme 1
c
c Print & Dump Cycle card to create MCTAL output file
c
prdmp 2j 1
Thanks,
Pramoth
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