Energy deposition studies in IR7 for HL-LHC

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Presentation transcript:

Energy deposition studies in IR7 for HL-LHC C. Bahamonde, A. Lechner thanking the contributions of A. Bertarelli, R. Bruce, P. Fessia, P. Hermes, A. Mereghetti, D. Mirarchi, S. Redaelli 7th HL-LHC Collaboration Meeting – Madrid – November 16th

Outline I. Long straight section (LSS): cells 4-7 Motivation: upgrade plans during LS2 Integrated dose: mitigation strategies Conclusions and outlooks II. Dispersion suppressor (DS): cells 8-11 Peak power density: quench risk evaluation C. Bahamonde - 7th HL-LHC Collaboration Meeting

Outline I. Long straight section (LSS): cells 4-7 Motivation: upgrade plans during LS2 Integrated dose: mitigation strategies Conclusions and outlooks II. Dispersion suppressor (DS): cells 8-11 Peak power density: quench risk evaluation C. Bahamonde - 7th HL-LHC Collaboration Meeting

Long Straight Section (LSS): cells 4-7 LSS upgrade plans in LS2 Long Straight Section (LSS): cells 4-7 MQWA.E5 removal Tungsten mask/inserts installation Coils Spacers Say that during LS2 all primary collimators and four secondaries will be changed to MoGr but they were not changed in our FLUKA model (CFC) 8.4 x 1016 protons lost in IR7 for the whole HL-LHC nominal operation Dose received by downstream MQWs during HL-LHC should remain as if MQWA.E5 stayed in place Integrated dose evaluation assuming 1 x 1018 protons lost in IR7 for whole HL-LHC period → potential overestimation factor 12* *R. Garcia Alia, 7th HL-LHC Collaboration Meeting, 15/11/17 C. Bahamonde - 7th HL-LHC Collaboration Meeting

Outline I. Long straight section (LSS): cells 4-7 Motivation: upgrade plans during LS2 Integrated dose: mitigation strategies Conclusions and outlooks II. Dispersion suppressor (DS): cells 8-11 Peak power density: quench risk evaluation C. Bahamonde - 7th HL-LHC Collaboration Meeting

Materials test results and dose limits P. Fessia, Radiation levels of MBW and MQW, 14th HL-LHC TCC, 01/09/16 After: heavily damaged Dose limits (MGy) to not be surpassed until the end of HL-LHC Coils <50 Spacers<10 C. Bahamonde - 7th HL-LHC Collaboration Meeting

Peak dose with/without MQWA.E5 (MGy) 3.6 COILS 2.4 3.6 SPACERS 4.8 3.6 4.8 4.2 7.1 4.8 44 7.1 45 Tungsten mask/inserts in all MQWs 2.4 4.8 2.4 Factor 4 5.4 3.6 6.6 7.1 29 7.7 27 Coils <50 Spacers<10 C. Bahamonde - 7th HL-LHC Collaboration Meeting

Passive protection: iron shielding Separated from beam pipes ~0.5 cm ~20 cm thick (each piece) 200 cm long (5x40cm) 55 cm high 100 cm are made of solid iron (5 sections of 20 cm each) and 100 cm are made iron fins to allow for air flow (10 sections of 10 cm each). Fins thickness 0.5cm with air gap between them of 1cm. C. Bahamonde - 7th HL-LHC Collaboration Meeting

Peak dose with shielding (MGy) 2.4 COILS 2.4 1.8 SPACERS 1.8 3.6 6.0 2.4 3.6 17.9 9.5 Coils <50 Spacers<10 3.6 Factor 2 in the coils 2.4 3.6 4.8 3.6 4.8 4.2 7.1 4.8 44 7.1 45 C. Bahamonde - 7th HL-LHC Collaboration Meeting

Shielding limitations Dose accumulated by most exposed magnet during all HL-LHC with improved passive protection installed (MGy) 13.1 9.5 17.9 7.1 4.8 6.0 3.6 2 MGy 1 MGy 0.5 MGy Coils Spacers 0.1 MGy Mention in the return coils the dose is also ~18 MGy in that area  initial hotspot covered but now moved to upper coil 0.01 MGy C. Bahamonde - 7th HL-LHC Collaboration Meeting

Outline I. Long straight section (LSS): cells 4-7 Motivation: upgrade plans during LS2 Integrated dose: mitigation strategies Conclusions and outlooks II. Dispersion suppressor (DS): cells 8-11 Peak power density: quench risk evaluation C. Bahamonde - 7th HL-LHC Collaboration Meeting

LSS conclusions and outlooks During HL-LHC in order to keep the integrated dose received by the MQWs of cell 5 as if the removed module stayed in, additional passive protection should be installed The latest design of this passive protection is still a factor of 2 less effective as a shielding than the removed MQW, barely allowing to comply with the material limits Further designs will be evaluated in the near future C. Bahamonde - 7th HL-LHC Collaboration Meeting

Outline I. Long straight section (LSS): cells 4-7 Motivation: upgrade plans during LS2 Integrated dose: mitigation strategies Conclusions and outlooks II. Dispersion suppressor (DS): cells 8-11 Peak power density: quench risk evaluation C. Bahamonde - 7th HL-LHC Collaboration Meeting

installation left and right of IP7 DS upgrade plans in LS2 Dispersion Suppressor (DS): cells 8-11 One TCLD + two 11T installation left and right of IP7 Collimator position should be optimized between cells 8 and 9 to obtain the best cleaning balance both in proton and ion runs In our FLUKA model all TCP, TCSG in CFC and TCLA, TCLD (when used) in inermet 180 Worst case HL-LHC parameters for ions (1248 bunches 2.1e8 ions/bunch) Protons: HL-LHC: 980kW (7.9e11 p/s) [assuming 2.3e11 p / bunch] Quench risk evaluation (energy deposition in the magnet coils) assuming losses of 7.9x1011 protons/s (1MW) lost in the collimation system and 3.64x108 ions/s for 12 min beam life time C. Bahamonde - 7th HL-LHC Collaboration Meeting

Outline I. Long straight section (LSS): cells 4-7 Motivation: upgrade plans during LS2 Integrated dose: mitigation strategies Conclusions and outlooks II. Dispersion suppressor (DS): cells 8-11 Peak power density: quench risk evaluation C. Bahamonde - 7th HL-LHC Collaboration Meeting

Peak power density profile in the DS 3.8 mW/cm3 2.4 mW/cm3 3.2 mW/cm3 2.6 mW/cm3 2 mW/cm3 C. Bahamonde - 7th HL-LHC Collaboration Meeting

Peak power density for HL-LHC (mW/cm3) TCLD position PROTONS IONS Cell 8/9 Cell 11 MB MQ 11T No TCLD 6.3 3.0 - 3.6 3.8 19.4 8.9 12.1 MBB.8 2.0 2.4 3.2 2.6 1.8 4.9 7.1 11.8 11.2 MBA.9 14.2 <0.1 2 1.2 <0.001 MBB.9 15.5 <0.01 4.5 3.9 27.8 If the quench limit of the 11T is found to be lower than other superconducting magnets, MBB.8 position would be better for ions C. Bahamonde - 7th HL-LHC Collaboration Meeting

Outline I. Long straight section (LSS): cells 4-7 Motivation: upgrade plans during LS2 Integrated dose: mitigation strategies Conclusions and outlooks II. Dispersion suppressor (DS): cells 8-11 Peak power density: quench risk evaluation C. Bahamonde - 7th HL-LHC Collaboration Meeting

DS conclusions and outlooks Proton runs The TCLD may only help if placed in MBB8 (50% reduction in Cell 8/9 and almost no reduction in Cell 11 compared to not having a TCLD). Ion runs TCP impact parameter can influence a lot the energy density in the DS. When the TCLD is in MBB8 position, a factor of 5 reduction could be achieved in cell 8/9 and a 30% reduction in cell 11. When in MBA9 position a 40% reduction shows in cell 9 and really good cleaning in cell 11. Both positions are eligible depending on 11T quench limit. Proton and ion runs TCLA settings can influence a lot the DS peak energy density in Cell 8/9. Previous benchmarks showed a factor 3 underestimation with respect to BLM measurements → certain margin should be taken into account. C. Bahamonde - 7th HL-LHC Collaboration Meeting

Thank you for your attention C. Bahamonde - 7th HL-LHC Collaboration Meeting

Back-up C. Bahamonde - 7th HL-LHC Collaboration Meeting

LSS simulation parameters Obtention of results Parameters of the study MQW section of cell 5 (most restrictive) Horizontal halo (comparable for vertical) Beam 1: left from IP7 (symmetric for B2) 7 TeV, 40 cm β*, 205 μrad crossing, in collision ~0.35 MGy C. Bahamonde - 7th HL-LHC Collaboration Meeting

LSS power load shielding Assuming 7.9 x 1011 protons lost per second in IR7 during HL-LHC (BLT of 12 minutes) Total power 58.3 kW 7.3 kW 6.5 kW Peak power 1.9 W/cm3 outer piece 1.8 W/cm3 middle piece

DS simulation parameters Protons and Pb ions - 7Z TeV, HL-LHC optics - B2, Horizontal case Collimator materials in FLUKA model TCP, TCSG in CFC TCLA, TCLD (when used) in inermet 180

DS collimator settings Proton studies TCP 5.7 sigma TCSG 7.7 sigma TCLA 10 sigma TCLD 14 sigma (when used) Ion studies TCP 6 sigma TCSG 7 sigma TCLA 10 sigma TCLD 14 sigma (when used) 2 sigma retraction 1 sigma retraction 4 sigma retraction 4.3 sigma retraction

Protons: no TCLD 6.3 mW/cm3 3.8 mW/cm3

Protons: TCLD in MBB.8 3.8 mW/cm3 3.2 mW/cm3 2.4 mW/cm3

Protons: TCLD in MBA.9 14.2 mW/cm3 5.7 mW/cm3 2.4 mW/cm3

Protons: TCLD in MBB.9 15.5 mW/cm3 6.5 mW/cm3

Ions: no TCLD 19.4 mW/cm3

Ions: TCLD in MBB.8 4.9 mW/cm3 7.1 mW/cm3 11.8 mW/cm3

Ions: TCLD in MBA.9 11.2 mW/cm3 2 mW/cm3

Ions: TCLD in MBB.9 27.8 mW/cm3 4.5 mW/cm3