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Energy Deposition in Adjacent LHC Superconducting Magnets from Beam Loss at LHC Transfer Line Collimators
Injection intensities for the LHC are over an order of magnitude above the damage threshold. The collimation system in the two transfer lines is designed to dilute the beam sufficiently to avoid damage in case of accidental beam loss or mis-steered beam. To maximise the protection for the LHC most o...
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Lenguaje: | eng |
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2006
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Acceso en línea: | http://cds.cern.ch/record/972695 |
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author | Beavan, S Kadi, Y Kain, V |
author_facet | Beavan, S Kadi, Y Kain, V |
author_sort | Beavan, S |
collection | CERN |
description | Injection intensities for the LHC are over an order of magnitude above the damage threshold. The collimation system in the two transfer lines is designed to dilute the beam sufficiently to avoid damage in case of accidental beam loss or mis-steered beam. To maximise the protection for the LHC most of the collimators are located in the last 300 m upstream of the injection point where the transfer lines approach the LHC machine. To study the issue of possible quenches following beam loss at the collimators part of the collimation section in one of the lines, TI 8, together with the adjacent part of the LHC has been modeled in FLUKA. The simulated energy deposition in the LHC for worst-case accidental losses and as well as for losses expected during a normal filling is presented. |
id | cern-972695 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2006 |
record_format | invenio |
spelling | cern-9726952023-05-31T13:24:32Zhttp://cds.cern.ch/record/972695engBeavan, SKadi, YKain, VEnergy Deposition in Adjacent LHC Superconducting Magnets from Beam Loss at LHC Transfer Line CollimatorsAccelerators and Storage RingsInjection intensities for the LHC are over an order of magnitude above the damage threshold. The collimation system in the two transfer lines is designed to dilute the beam sufficiently to avoid damage in case of accidental beam loss or mis-steered beam. To maximise the protection for the LHC most of the collimators are located in the last 300 m upstream of the injection point where the transfer lines approach the LHC machine. To study the issue of possible quenches following beam loss at the collimators part of the collimation section in one of the lines, TI 8, together with the adjacent part of the LHC has been modeled in FLUKA. The simulated energy deposition in the LHC for worst-case accidental losses and as well as for losses expected during a normal filling is presented.LHC-PROJECT-Report-947CERN-LHC-Project-Report-947oai:cds.cern.ch:9726952006-07-13 |
spellingShingle | Accelerators and Storage Rings Beavan, S Kadi, Y Kain, V Energy Deposition in Adjacent LHC Superconducting Magnets from Beam Loss at LHC Transfer Line Collimators |
title | Energy Deposition in Adjacent LHC Superconducting Magnets from Beam Loss at LHC Transfer Line Collimators |
title_full | Energy Deposition in Adjacent LHC Superconducting Magnets from Beam Loss at LHC Transfer Line Collimators |
title_fullStr | Energy Deposition in Adjacent LHC Superconducting Magnets from Beam Loss at LHC Transfer Line Collimators |
title_full_unstemmed | Energy Deposition in Adjacent LHC Superconducting Magnets from Beam Loss at LHC Transfer Line Collimators |
title_short | Energy Deposition in Adjacent LHC Superconducting Magnets from Beam Loss at LHC Transfer Line Collimators |
title_sort | energy deposition in adjacent lhc superconducting magnets from beam loss at lhc transfer line collimators |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/972695 |
work_keys_str_mv | AT beavans energydepositioninadjacentlhcsuperconductingmagnetsfrombeamlossatlhctransferlinecollimators AT kadiy energydepositioninadjacentlhcsuperconductingmagnetsfrombeamlossatlhctransferlinecollimators AT kainv energydepositioninadjacentlhcsuperconductingmagnetsfrombeamlossatlhctransferlinecollimators |