2017
DOI: 10.1103/physrevaccelbeams.20.091002
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Modeling of beam-induced damage of the LHC tertiary collimators

Abstract: Modern hadron machines with high beam intensity may suffer from material damage in the case of large beam losses and even beam-intercepting devices, such as collimators, can be harmed. A systematic method to evaluate thresholds of damage owing to the impact of high energy particles is therefore crucial for safe operation and for predicting possible limitations in the overall machine performance. For this, a three-step simulation approach is presented, based on tracking simulations followed by calculations of e… Show more

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Cited by 16 publications
(13 citation statements)
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“…The fact that the TCT setting is not constrained by beamhalo background does, however, not mean that it can be arbitrarily tight. Other constraints from protection of the triplet magnets and the TCT itself, in particular during accidental losses, are the present limitation at the LHC for further reductions of β Ã [34,59], although they have been relaxed through the use of a specially matched optics [3].…”
Section: Discussionmentioning
confidence: 99%
“…The fact that the TCT setting is not constrained by beamhalo background does, however, not mean that it can be arbitrarily tight. Other constraints from protection of the triplet magnets and the TCT itself, in particular during accidental losses, are the present limitation at the LHC for further reductions of β Ã [34,59], although they have been relaxed through the use of a specially matched optics [3].…”
Section: Discussionmentioning
confidence: 99%
“…If the deposited power density is sufficiently high, dynamic responses will be induced, principally because the thermal expansion of the impacted material is initially prevented by its inertia, giving rise to isochoric (constant-volume) heating [21]. This can be the case, for instance, of accidental beam impacts on collimators [10], as opposed to nominal operating conditions, which typically lead to slow transient or quasi-static responses. From a thermomechanical standpoint, the problem can be reduced to the study of a body subjected to a non-uniform, quasi-instantaneous heat generation lasting the time of the beam interaction τ: this deposition time is of the order of few microseconds, thus generally much shorter than both the period T of the waves generated by the impact and the heat diffusion time t d [22].…”
Section: Dynamic Response Of Materials Subject To Quasi-instantaneousmentioning
confidence: 99%
“…The experiment profited of the experience of previous tests carried out at the CERN HiRadMat facility. In HRMT09 [9], carried out in 2012, a full LHC collimator, with a tungsten alloy as absorbing material, was tested to observe the effects of accidental direct beam impacts, benchmark simulations and derive acceptable limits for this absorbing material [10]. In HRMT14 [11], also performed in 2012, specimens of simple geometry, extensively instrumented, were impacted with particle beams to benchmark the numerical results obtained with different FE codes (namely, ANSYS [12], Autodyn [13] and LS-Dyna [14]).…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, these rotatable collimators would be installed in these locations in the LHC. This scenario has been revised since then (see e.g., [6][7][8]) by more realistic models, but is still relevant for design specifications of IR7 collimators.…”
Section: Introductionmentioning
confidence: 99%