Download presentation
Presentation is loading. Please wait.
Published byAlban Peters Modified over 9 years ago
1
C. Theis, D. Forkel-Wirth, S. Roesler, H. Vincke
2
Outline Ambient-dose-equivalent studies for An accident scenario (full beam-loss) Normal operation Calculation of field calibration coefficients for the IG5 ionization chambers RAMSES monitoring system. 2 C. Theis, SC/RP
3
Motivation Previous radiation studies by S. Roesler et al. date back >5 years already. Minimum requirements for openings were 3m in the lower & 2m for the upper shielding. Shielding layout has changed (new ducts, access maze, etc.) Check compliance with radiation limit of 20 mSv ambient-dose-equivalent for a full beam loss (~ 20 mSv effective-dose) 3 C. Theis, SC/RP
4
FLUKA geometry C. Theis, SC/RP 4 LHCb shielding wall Counting barracks Entrance maze Beam tunnel Barrack Access shaft PX84 Y Z X 2m Entrance maze (shown without roof) 4m Cable tray in the floor (1.1 x 0.17 m) 3m Side slit for cables (0.4 x 5.6m) Ventilation ducts Material passageway (blocked during operation) PAXL8501 PAXL8502 PAXL8511 PAXL8521 PAXL8512 PAXL8522 Front part of the counting barracks
5
Beam-loss scenario Full loss of 1 beam Protons at 7 TeV/c Loss at the worst location, giving the highest particle fluence in the cavern (5m upstream from the center of the cavern) 2 - step calculations 1 st step without the electromagnetic cascade 2 nd step including the electromagnetic cascade C. Theis, SC/RP 5
6
Beam-loss scenario C. Theis, SC/RP 6 Beam loss point Loss direction Beam loss point Loss direction Hadrons caused by the beam-loss :poss Beam loss point Loss direction Material passage is in the “shadow” at a full beam-loss Direction of the high-energetic particles
7
Beam-loss scenario C. Theis, SC/RP 7 Ground floor of the barracks Limits: (4.7 x 10 14 protons) Red arrow ~ 50 mSv Blue arrow ~ 20 mSv pSv/primary Y Z PAXL8501 PAXL8502 Front part of barracks pSv/proton No significant impact of the cable tray in the floor Avg. value for the front part of the barracks ~ 4mSv
8
Beam-loss scenario C. Theis, SC/RP 8 2 nd floor of the barracks Limits: (4.7 x 10 14 protons) Red arrow ~ 50 mSv Blue arrow ~ 20 mSv Y Z pSv/primary PAXL8521 PAXL8522 Front part of barracks pSv/proton Worst location 7.24 mSv
9
Beam-loss scenario C. Theis, SC/RP 9 Center of the cavern Y X pSv/primary Front part of barracks pSv/proton Limits: (4.7 x 10 14 protons) Red arrow ~ 50 mSv Blue arrow ~ 20 mSv Avg. value for the front part of the barracks ~ 4mSv
10
Normal operation DPMJET 3 for 7 TeV proton-proton collisions FLUKA 2006.3 for particle transport 2 step-method like for the beam-loss scenario Normalization parameters: Luminosity L = 2 x 10 32 cm -2 s -1 = 80 mbarn Beam-gas interactions (10 4 collisions/s) were neglected C. Theis, SC/RP 10 10 7 collisions/s
11
Normal operation C. Theis, SC/RP 11 Y Z Sv/hour PAXL8501 PAXL8502 Front part of barracks Sv/h Ground floor of the barracks Limits: Blue arrow ~ 3 Sv/h Average value for the front part of the barracks ~ 5.6 x 10 -2 Sv/h ± 2%
12
Normal operation C. Theis, SC/RP 12 2 nd floor of the barracks Limits: Blue arrow ~ 3 Sv/h Worst location ~ 0.1 Sv/h ± 7% Y Z PAXL8521 PAXL8522 Front part of barracks Sv/hour Sv/h
13
Normal operation C. Theis, SC/RP 13 Y X Sv/h our Front part of barracks Sv/h Center of the cavern Limits: Blue arrow ~ 3 Sv/h Average value for the front part of the barracks ~ 5.6 x 10 -2 Sv/h ± 2%
14
Field calibration studies Up to 6 IG5-H20 hydrogen filled ionization chambers will be installed. Usually calibrated with 238 PuBe source (neutrons up to 11 MeV) at LHCb there is a field calibration mixed field with much higher energies field calibration C. Theis, SC/RP 14 PAXL8501 PAXL8502 PAXL8511 PAXL8521 PAXL8512 PAXL8522 Front part of the counting barracks
15
Field calibration procedure C. Theis, SC/RP 15 1 Calculate monitor response function (charge per unit fluence) 2 Calculate particle fluence spectra at monitor location Calculate ambient-dose-equivalent (Sievert per unit fluence) 3 Convolve response and fluence spectra (total charge per unit fluence) 4 Field calibration factor = calculated Sievert / calculated total charge in the ionization chamber
16
Typical mixed field spectrum C. Theis, SC/RP 16 Average mixed field spectrum for the frontal barracks Spectrum for PAXL8522 Frontal barracks Individual factors would be the optimum solution.
17
Field calibration factors C. Theis, SC/RP 17 LocationCalibration factor [nSv/pC] Barrack8.11 ± 2% PAXL85016.30 ± 7% PAXL85027.40 ± 6% PAXL85118.15 ± 5% PAXL85127.41 ± 6% PAXL85218.74 ± 7% PAXL85227.94 ± 7% Individual values deviate from the one that was calculated as an average over the frontal barrack area by 20% individual values would be best.
18
Comparison to 238 Pu-Be calibration C. Theis, SC/RP 18
19
Field calibration vs. 238 PuBe Agreement within ~25% for fields that are comparable to LHCb or the CERF facility. However, the agreement comes from the integral compensation due to other particles. The charge due to neutrons only would underestimate the dose! C. Theis, SC/RP 19
20
Neutron response of the IG5-H20 chamber in a CERN-typical neutron spectrum C. Theis, SC/RP 20 238 PuBe has a mean energy of ~4.5 MeV. Compared to this the response to high- energy neutrons (>20 MeV) is much lower and thus, the contribution of these particles in a typical mixed field outside some concrete shielding, would be underestimated.
21
Summary & conclusions The final shielding design was found to be compliant with the old minimum shielding requirements. Neither the accident scenario nor the normal operation should not exceed the tolerable limits. C. Theis, SC/RP 21
22
IG5-H20 response functions C. Theis, SC/RP 22
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.