Status of FLUKA Simulations for Collimation BLM Thresholds 6 th BLM Threshold Working Group 10/02/2015 E.Skordis On behalf of the FLUKA team Sixtrack input.

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Presentation transcript:

Status of FLUKA Simulations for Collimation BLM Thresholds 6 th BLM Threshold Working Group 10/02/2015 E.Skordis On behalf of the FLUKA team Sixtrack input provided from the Collimation team

Overview Ideal strategy Present request Concerns Available results BLM matrices Disclaimer 6 th BLM Threshold Working Group 10/02/2015 E.Skordis

Run FLUKA simulations Run tracking studies Run Thermomechanical studies Ideal Strategy Collimator (Type, material, BLM position etc…) Parameters ( Collimator orientation, opening etc…) Scenario (Accident, Nominal cleaning etc…) Run tracking (SixTrack) studies to provide FLUKA with the distribution of protons (ions) impacting the collimator. Run shower simulations and provide: energy deposition distribution and BLM signal per incident proton Attention: The relevant energy deposition and BLM signal could very well be at a collimator other than the one considered in the scenario Run thermomechanical studies to identify the intensity rate limit Calculate BLM Thresholds: translate the above limit into BLM signal using the FLUKA ratio Identify scenario parameters Calculate BLM Thresholds 6 th BLM Threshold Working Group 10/02/2015 E.Skordis

Present request BLM signal per proton lost (BLM Matrices) for 4 families:  TCP (carbon)  TCSG (carbon)  TCLA (Inermet)  TCT (Inermet) Use primary collimator lossmap for all cases (scenario: considered collimator acting as primary).  Pre-defined intensity rate limits to be translated into BLM thresholds by the above matrices for 2 orientations:  Horizontal  Vertical for 3 energies: o 450 GeV o 3.5 TeV o 7 TeV 6 th BLM Threshold Working Group 10/02/2015 E.Skordis

Concerns How was the max number of protons into the collimators estimated? What is the uncertainty of that calculation? What level of accuracy are we looking for in the present study? No 450 GeV primary collimator lossmap available in order to provide results for that energy 6 th BLM Threshold Working Group 10/02/2015 E.Skordis

Concerns Depending on the level of accuracy required each case can be unique The complexity is increased by the BLM signal Crosstalk which plays a major role LHC Collimation Working Group 6/5/ th BLM Threshold Working Group 10/02/2015 E.Skordis

Available Results Various unpresented studies with artificial sources on different collimators e.g.:  Tertiary collimators with a BLM at the TCLA position.  Tertiary collimators with x, x’, y, y’ coordinates of TCP losses 6 th BLM Threshold Working Group 10/02/2015 E.Skordis

BLM matrices Available extrapolations for 2 families:  Carbon  Inermet Use primary collimator lossmap for all cases (scenario: considered collimator acting as primary). The minimum computed BLM signal is given for each case based on multiple simulations A possible underestimation (overprotection) factor is given for each BLM signal ( maximum expected BLM signal = min BLM signal * factor ) Results are normalised to the horizontal TCP primary response ( Gy/p taken as 1) for 2 orientations:  Horizontal  Vertical for 2 energies: o 3.5 TeV o 7 TeV 6 th BLM Threshold Working Group 10/02/2015 E.Skordis

BLM Responses matrices (Values are normalised to the BLM_TCP.C response for horizontal losses at 3.5 TeV which corresponds to Gy/p) 6 th BLM Threshold Working Group 10/02/2015 E.Skordis 3.5 TeV Orientation Collimator material HorizontalVertical Minimum BLM signal Possible overprotection factor Minimum BLM signal Possible overprotection factor Carbon Inermet TeV Orientation Collimator material HorizontalVertical Minimum BLM signal Possible overprotection factor Minimum BLM signal Possible overprotection factor Carbon Inermet This defines a variation interval from 0.5 up to ~20, reduced inside a specific family (C vs W) scenario: considered collimator acting as primary

Disclaimer The BLM signals presented in this study are a guess for the “worst” possible case, meaning the lowest possible signal per case – just considering the impacted collimator and its BLM - Cross-talk totally neglected! For a more meaningful evaluation, we propose the strategy suggested in slide 3 6 th BLM Threshold Working Group 10/02/2015 E.Skordis