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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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Detalles Bibliográficos
Autores principales: Beavan, S, Kadi, Y, Kain, V
Lenguaje:eng
Publicado: 2006
Materias:
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