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Modelling of helium-mediated quench propagation in the LHC prototype test string-1

机译:LHC原型测试线1中氦介导的猝灭传播的建模

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The Large Hadron Collider (LHC) prototype test string-1, hereafter referred to as the string, is composed of three 10-m long prototype dipole magnets and one 6-m long prototype quadrupole manget. The magnets are immersed in a pressurized static bath of superfluid helium that is maintained at a pressure of about 1 bar and at a temperature of about 1.9 K. This helium bath constitutes one single hydraulic unit. extending along 42.5 m of the string length. We have measured the triggering of quenches of the string magnets due to the quenching of a single dipole magnet located at the string's extremity, i.e., "quench propagation". Previously reported measurements enabled to establish that in this configuration the quench propagation is mediated by the helium and not by the inter-magnet bus bar connections (L. Coull, D. Hagedorn, G. Krainz, F. Rodriguez-Mateos, R. Schmidt, Quench propagation tests on the LHC superconducting magnet string, in: S. Myers, A. Pacheco, R. Pascual, C. Petit-Jean-Genaz, J. Poole (Eds.), Fifth European Particle Accelerator Conference EPAC '96, Sitges, Barcelona, Spain, 10-14 June 1996, IOP, Bristol, 1996; F. Rodriguez-Mateos, R. Schmidt, L. Serio, Thermo-hydraulic quench propagation at the LHC superconducting magnet string, in: D. Dew-Hughes, R.G. Scurlock, J.H.P. Watson (Eds), 17th International Cryogenic Engineering Conference (ICEC-17), Bournemouth, UK, 14-17 July 1998, IOP, Bristol, 1998). We present a model of helium-mediated quench propagation based on the qualitative conclusions of these two previous papers, and on additional information gained from a dedicated series of quench propagation measurements that were not previously reported. We will discuss the specific mechanisms and their main parameters involved at different timescales of the propagation process, and apply the model to make quantitative predictions.
机译:大型强子对撞机(LHC)原型测试弦1(以下称为弦)由三个10米长的原型偶极磁体和一个6米长的原型四极座子组成。将磁铁浸入超流体氦的静压浴中,该静浴保持在约1 bar的压力和约1.9 K的温度下。该氦浴构成一个单独的液压单元。沿弦长的42.5 m延伸。我们已经测量了由于位于弦的末端处的单个偶极磁体的猝灭引起的弦磁体的猝灭的触发,即“猝灭传播”。先前报道的测量结果可以确定,在这种配置下,淬灭传播是由氦介导的,而不是由磁体间母线连接引起的(L. Coull,D。Hagedorn,G。Krainz,F。Rodriguez-Mateos,R。Schmidt ,在LHC超导磁体弦上的猝灭传播测试,见:S. Myers,A。Pacheco,R。Pascual,C。Petit-Jean-Genaz,J。Poole(编辑),第五届欧洲粒子加速器会议EPAC '96, 1996年6月10日至14日,西班牙巴塞罗那锡切斯,1996年,布里斯托尔,IOP; F。Rodriguez-Mateos,R。Schmidt,L。Serio,在LHC超导磁体弦上的热液猝灭传播,在:D. Dew- Hughes,RG Scurlock,JHP Watson(编辑),第17届国际低温工程会议(ICEC-17),英国伯恩茅斯,1998年7月14日至17日,IOP,布里斯托尔,1998年。我们基于前两篇论文的定性结论,以及从先前未报道的一系列专门的猝灭传播测量中获得的其他信息,提出了一种氦介导的猝灭传播模型。我们将讨论在传播过程的不同时间尺度上涉及的特定机制及其主要参数,并应用该模型进行定量预测。

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