Title: FLUKA for accelerator radiation protection –Indian perspective
1FLUKA for accelerator radiation protection
Indian perspective
- Sunil C
- Accelerator Radiation Safety Section
- Radiation Safety Systems Division,
- Bhabha Atomic Research Centre
2Accelerator Radiation Safety Section
- Operational radiation protection
- Associated RD
- Heavy Ion Accelerators (TIFR Bombay and VECC,
Calcutta - 5-7 MeV/amu Pelletron
- 10 MeV/amu with a superconducting linac booster
- 100 MeV/amu superconducting cyclotron
- Electron accelerators (RRCAT Indore)
- 20 MeV Microtron to 2.5 GeV electron synchrotron
- High current industrial accelerators
3Future plans
- ADSS
- Proton accelerators
- 20 MeV to 1 GeV
- Swimming poll critical reactor that can also be
operated in sub critical mode with 600 MeV
protons incident on LBE - 14 MeV neutron generators
- Bare
- Injectors for sub critical assemblies
4Uses of FLUKA
- Routine accelerator radiation protection
- Source term calculations
- Shielding
- Induced activity
- Synchrotron hutch shielding
- Photoneutron estimation
- ADSS
- Proton accelerators
- Secondary particle dose from heavy Ion reactions
- Muon Transport and dose estimation
- Spallation yields comparison with JQMD
5Heavy Ion accelerators
- Neutron source term calculations
- EMPIRE, PACE (heavy ions) ALICE, PRECO (protons)
- Transport using the source.f
- BME!
- 10 MeV/amu to 100 MeV/amu
- Hauser-Feshbach for compound nucleus?
- Induced activity calculations
- Neutron spectrometry using passive techniques
- ECR ion sources
- Simulate electric fields?
620 MeV proton on Be
7Electron Accelerators
- Photon (Bremsstrahlung) spectrometry
- High energy
- Detector response studies
- neutrons and photons
- Photoneutron spectrometry and dosimetry
- Synchrotron dosimetry
- Low energy (lt 10 keV)
8Photoneutrons
- Contribution to the exposure in electron
accelerators - A new technique to predict the neutron spectra
using empirical relations - Spectra from FLUKA fitted to a Maxwellian
- Temperature
- Yield
- Form a couple equation to predict the GDR part of
the photoneutron spectrum
9Check
10The procedure
Sunil C, Sarkar P K, Empirical estimation of
photoneutron energy distribution in high energy
electron accelerators, Nuclear Instruments and
Methods A 581, (2007), 844-849.
11Independent FLUKA Calculation
Experiment
Our Calculation
12Neutrons gt 50 MeV
- Experimental verification using Bi fission foils,
track etch membranes shows higher values when
compared to FLUKA calculations. - How much is photon induced fission?
- The cross section is 1 of neutron fission (?gt200
MeV) - But at the experimental area, the photon fluence
is expected to be several times higher than
neutrons! - Calculate photon induced fission using FLUKA?
13Photon Transmission
- 30 cm diameter and 30 cm long cylindrical
detector (approximating the upper trunk of a
human body) is used to count the photons. - USRTRACK estimator tallies the photon fluence.
- Deq99 (FLUSUW) subroutine used to fold the
fluence with the dose conversion coefficients to
obtain ambient dose equivalent
14Transmitted dose
15Unshielded Dose rate
16Variation with detector size
17Effect of detector size
18Variation with detector size
19Residual activity
- 2.5 GeV electron incident on 10 X0 -1Xm targets.
- DPMJET activated using PHYSICS
- LAM-BIAS at 100
- Photon transport cut off to 10 MeV
20Residual Activity (Bq/g)
SS
212.5 GeV e-, 1mA, 24 hours
22Residual Nuclei
- In SS, 51Cr was reported by Fasso with a higher
neutron cutoff energy. - Swansons technique and present calculation agree
within a factor of 2 for example 57Co in Ni
target, 63, 65Cu from Cu target. - 59Fe in SS (58Fe(n,?)) target in this calculation
was found to be four orders less compared to that
obtained by Sato and Fasso - Most of the important nuclides formed are in the
range of 200 -500 MBqW-1.
23Synchrotron Hutch Shielding
- Hutch design in INDUS (2.5 GeV, 1 mA)
- Bremsstrahlung mixed with SR
- Experiments claim existence of SR
- Transportation tough - low energy at the edge of
FLUKA capabilities. - Can it be simulated using FLUKA?
24Heavy Ion reactions
- Work done at PTB Germany
- 200 MeV 12C ions on water phantom
- Score neutron fluence and dose inside 5.7 cm
spheres at different angles. - Compare with measurements done at GSI
- Spectra from TOF (GSI measurements)
- Dose using a TEPC (PTB measurements)
- Dose using WENDI (GSI measurements)
25Neutron Spectra
200 MeV/amu 12C incident on 15 cm diameter
cylindrical water phantom
26Neutron and charged particles
27Charged particles
Apply coincidence measurements
28Response Matrices
- Neutron attenuation through a target of finite
thickness. - Response of Bonner sphere type passive
techniques. - Response of liquid scintillators
- Bismuth fission detectors
- Neutron induced fission
- Photon induced fission
29ADSS
- A sub critical assembly driven by 14 MeV neutrons
- 256 nat.U rods inside water column, beam tube at
center. - Analog mode
- 36 hours for 106 histories !
- And still large errors (10-30)
30Proton accelerators for ADSS
- Plans to couple a sub critical reactor to a
proton accelerator - Source term for lateral shielding of the
accelerator tunnel, reactor pool top - Residual activity in LBE loop
- Activation of magnets concrete wall
- LBE window rupture due to heat load
31ADSS problems
- High beam current 1-5 mA!
- Proton energies varying from 100 MeV to 1GeV
- Shielding calculations
- Reduce dose by 9 orders- 7 meters!
- Induced activity after several meters of water
- Explicit Transport !? Or calculate neutrons at
intermediate thicknesses? - Induced activity in magnets, concrete walls.
- Induced activity in LBE after several
combinations of irradiations.
32Shielding
- Attenuation length from IAEA 283
- n/p ratio from FLUKA
- Multiply end result by the n/p ratio to get the
transmitted dose after shield - Biasing!
33Simplified view
concrete
7 m
water
Window
34Further work
- Establish attenuation curves for different shield
configurations. - Different types of concrete
- Transport neutrons through several meters of
water and calculate induced activity. - Irradiation profile, raddecay, dcytimes, usrbin
35Thank you