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Probability of burn-through of defective 13 kA splices at increased energy levels

In many 13 kA splices in the machine there is a lack of bonding between the superconducting cable and the stabilising copper along with a bad contact between the bus stabiliser and the splice stabiliser. In case of a quench of such a defective splice, the current cannot bypass the cable through the...

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Autor principal: Verweij, A
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:https://dx.doi.org/10.5170/CERN-2011-005.149
http://cds.cern.ch/record/1353848
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author Verweij, A
author_facet Verweij, A
author_sort Verweij, A
collection CERN
description In many 13 kA splices in the machine there is a lack of bonding between the superconducting cable and the stabilising copper along with a bad contact between the bus stabiliser and the splice stabiliser. In case of a quench of such a defective splice, the current cannot bypass the cable through the copper, hence leading to excessive local heating of the cable. This may result in a thermal runaway and burn-through of the cable in a time smaller than the time constant of the circuit. Since it is not possible to protect against this fast thermal run-away, one has to limit the current to a level that is small enough so that a burn-through cannot occur. Prompt quenching of the joint, and quenching due to heat propagation through the bus and through the helium are considered. Probabilities for joint burn-through are given for the RB circuit for beam energies of 3.5, 4 and 4.5 TeV, and a decay time constant of the RB circuit of 50 and 68 s.
id cern-1353848
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2011
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spelling cern-13538482022-08-10T20:25:23Zdoi:10.5170/CERN-2011-005.149http://cds.cern.ch/record/1353848engVerweij, AProbability of burn-through of defective 13 kA splices at increased energy levelsAccelerators and Storage RingsIn many 13 kA splices in the machine there is a lack of bonding between the superconducting cable and the stabilising copper along with a bad contact between the bus stabiliser and the splice stabiliser. In case of a quench of such a defective splice, the current cannot bypass the cable through the copper, hence leading to excessive local heating of the cable. This may result in a thermal runaway and burn-through of the cable in a time smaller than the time constant of the circuit. Since it is not possible to protect against this fast thermal run-away, one has to limit the current to a level that is small enough so that a burn-through cannot occur. Prompt quenching of the joint, and quenching due to heat propagation through the bus and through the helium are considered. Probabilities for joint burn-through are given for the RB circuit for beam energies of 3.5, 4 and 4.5 TeV, and a decay time constant of the RB circuit of 50 and 68 s.oai:cds.cern.ch:13538482011
spellingShingle Accelerators and Storage Rings
Verweij, A
Probability of burn-through of defective 13 kA splices at increased energy levels
title Probability of burn-through of defective 13 kA splices at increased energy levels
title_full Probability of burn-through of defective 13 kA splices at increased energy levels
title_fullStr Probability of burn-through of defective 13 kA splices at increased energy levels
title_full_unstemmed Probability of burn-through of defective 13 kA splices at increased energy levels
title_short Probability of burn-through of defective 13 kA splices at increased energy levels
title_sort probability of burn-through of defective 13 ka splices at increased energy levels
topic Accelerators and Storage Rings
url https://dx.doi.org/10.5170/CERN-2011-005.149
http://cds.cern.ch/record/1353848
work_keys_str_mv AT verweija probabilityofburnthroughofdefective13kasplicesatincreasedenergylevels