POLITECNICO DI TORINO - CERN

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POLITECNICO DI TORINOCorso di Laurea Magistrale in Ingegneria MeccanicaMaster Thesis01/04/2020CERN-THESIS-2020-019Quench Protection Heaters FE Analysis andThermal Conductivity Measurements of Nb3SnCables for High-Field Accelerator MagnetsSupervisor:Prof. Lorenzo PERONIAuthor:Carmelo BARBAGALLOCERN Supervisor:Susana IZQUIERDO BERMUDEZApril 2020

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Declaration of AuthorshipI, Carmelo BARBAGALLO, declare that this thesis titled, “Quench Protection Heaters FEAnalysis and Thermal Conductivity Measurements of Nb3Sn Cables for High-Field AcceleratorMagnets” and the work presented in it are my own. I confirm that: This work was done while in candidature for the Technical Student Programme atCERN (The European Organization for Nuclear Research). Where any part of this thesis has previously been submitted for a degree or any otherqualification at this University or any other institution, this has been clearly stated. Where I have consulted the published work of others, this is always clearly attributed. Where I have quoted from the work of others, the source is always given. With theexception of such quotations, this thesis is entirely my own work. I have acknowledged all main sources of help. Where the thesis is based on work done by myself jointly with others, I have made clearexactly what was done by others and what I have contributed myself.In Geneva, 06 February 2020Carmelo Barbagalloiii

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“Remember to look up at the stars and not down at your feet. Try to make sense of what yousee and wonder about what makes the universe exist. Be curious. And however difficult life mayseem, there is always something you can do and succeed at. It matters that you don’t just giveup”Prof. Stephen Hawkingv

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POLITECNICO DI TORINOAbstractMechanical EngineeringDepartment of Mechanical and Aerospace EngineeringMaster of ScienceQuench Protection Heaters FE Analysis and Thermal Conductivity Measurements ofNb3Sn Cables for High-Field Accelerator Magnetsby Carmelo BARBAGALLOThe Large Hadron Collider (LHC), the world’s largest and most powerful particle accelerator,represents a research instrument at CERN to improve our understanding of matter and the Universe. To date, scientists and engineers around the world are working hard to develop its upgrade, the High-Luminosity LHC (HL-LHC). More powerful superconducting accelerator magnets are being designed at CERN, allowing the peak magnetic field strength to be augmentedby around 50% than current LHC magnets. These magnets will permit to increase the HL-LHCintegrated luminosity - i.e. the total number of collisions – by a factor of ten beyond the LHC’sdesign value, allowing the scientific community to study the phenomena discovered at the LHCin greater detail.Due to the high peak field, in the range of 12 T to 13 T, magnets will use an innovativesuperconducting technology based on the use of Nb3Sn as a superconductor. From this perspective, quench protection is becoming a topic of very high interest. That means preventing damagein the case of an unexpected loss of superconductivity and the heat generation related to that.This procedure foresees the disconnection of the magnet current supply and the use of so-calledquench heaters. The heaters suppress the superconducting state in a large fraction of the windings and permit a uniform dissipation of the stored energy.In this thesis work, a numerical analysis on state-of-the-art quench protection heaters forhigh-field accelerators magnets is proposed, aiming to investigate on their performance andevaluate the prospects in high-field magnet protection. FE-analyses simulating the heat transferfrom protection heater to superconducting cables in Nb3Sn magnets were carried-out in COMSOL Multiphysics , in order to evaluate the heater efficiency from the time delay between theheater activation and normal zone initiation in the coil. Results from simulations were comparedwith measured data from R&D Nb3Sn quadrupoles and dipoles under development at CERNfor the HiLumi project. The thesis was also focused on the study of the thermal conductivity ofepoxy-impregnated coils, for having a better understanding of this thermal property which playsa key role in heat transfer phenomena during a quench. The thermal conductivity of differentinsulating materials used in Nb3Sn impregnated coils was studied. Finally, a multi-strand cablesFE-model was built in COMSOL to replicate the experimental procedure used at CERN Cryolab to measure the thermal conductivity of epoxy-impregnated Nb3Sn Rutherford cable stacks.vii

POLITECNICO DI TORINOSommarioIngegneria MeccanicaDipartimento di Ingegneria Meccanica e AerospazialeCorso di Laurea MagistraleQuench Protection Heaters FE Analysis and Thermal Conductivity Measurements ofNb3Sn Cables for High-Field Accelerator MagnetsA cura di Carmelo BARBAGALLOIl Large Hadron Collider (LHC), il più grande e potente acceleratore di particelle del mondo,rappresenta al CERN uno strumento di ricerca per migliorare la comprensione della materia edell’Universo. Ad oggi, scienziati e ingegneri di tutto il mondo stanno lavorando duramente perlo sviluppo del suo upgrade, l’High-Luminosity LHC (HL-LHC). Al CERN sono stati progettatimagneti superconduttori più potenti, che consentono di aumentare l’intensità di picco del campomagnetico di circa il 50% rispetto ai magneti dell’attuale LHC. Questi magneti permetterannodi aumentare la luminosità integrata dell’HL-LHC – cioè il numero totale di collisioni – di unfattore dieci oltre il valore di progetto dell’LHC, permettendo alla comunità scientifica distudiare in maggiore dettaglio i fenomeni scoperti con l’attuale acceleratore.A causa dell’alto campo magnetico, tra i 12 T e i 13 T, i magneti utilizzeranno un’innovativatecnologia superconduttiva basata sull’utilizzo del superconduttore Nb3Sn. In questo scenario,lo studio del sistema di protezione nel caso di quench sta diventando un argomento di notevoleinteresse. L’obiettivo è quello di prevenire eventuali danni al magnete nel caso di un’improvvisaperdita dello stato superconduttivo e della generazione di calore a essa correlata. In caso diquench, la procedura prevede la disconnessione dell’alimentazione elettrica del magnete el’utilizzo di riscaldatori, chiamati quench heater. Tali elementi sopprimono lo statosuperconduttivo in una grande frazione degli avvolgimenti del magnete e consentono unadissipazione uniforme dell’energia immagazzinata.Nel presente lavoro di tesi viene proposta un’analisi numerica sullo stato dell’arte deiquench heater usati in magneti ad alto campo magnetico per acceleratori di particelle, al fined’indagare sulle loro prestazioni e valutare nuove prospettive nella protezione di tali magneti.Analisi agli elementi finiti, che simulano lo scambio termico nei magneti tra gli heater e i cavisuperconduttori in Nb3Sn, sono state effettuate in COMSOL Multiphysics al fine dideterminare l’efficienza dell’heater tramite la valutazione dell’heater delay, ossia il tempo cheintercorre tra l’attivazione dell’heater e l’inizio dello stato resistivo nella bobina. I risultati dellesimulazioni sono stati confrontati con le misure sperimentali effettuate sui quadrupoli e dipolibasati su tecnologia Nb3Sn, in sviluppo al CERN per il progetto HiLumi. Il lavoro di tesi è statoanche incentrato sullo studio della conducibilità termica delle bobine impregnate con resinaepossidica, al fine di avere una migliore comprensione di questa proprietà termica che svolgeviii

un ruolo fondamentale nei fenomeni di scambio termico durante il quench. Infine, un modelloagli elementi finiti di un cavo multi-filamento è stato realizzato in COMSOL Multiphysics ,con lo scopo di replicare numericamente la procedura sperimentale utilizzata dal laboratorioCryolab al CERN per misurare la conducibilità termica di provini di cavi in Nb3Sn di tipoRutherford impregnati con resina epossidica.ix

AcknowledgmentsThis Master Thesis work was developed at CERN (The European Organization for NuclearResearch) while in candidature for the Technical Student Programme. I feel very grateful forthis exceptional experience I have had during this year at CERN, both professionally and personally. This opportunity allowed me to work in the one of the best research center in the world,in direct contact with the best scientists from all over the world. From a professional point ofview, I learned a lot about research world, in particular magnet technology development andnumerical modelling. From a personal point of view, I appreciated the possibility to know different cultures and people. That has allowed me to know better myself and to respect the others,as well as to enrich my person for a cultural point of view.One of the best parts of completing this thesis is to have the opportunity to formally thankthe people who have made this experience that what it was. First, I thank Susana IzquierdoBermudez, my supervisor at CERN, for her guidance on investigated topics and trust in myabilities. I thank Prof. Lorenzo Peroni, my supervisor at the Polytechnic University of Turin,for his academic supervision, support and trust since the early stage of this experience. I alsothank Tiina Salmi for her interest in my work, cooperation during tests in SM18 facility andguidance in quench modelling. I thank Patricia Tavares Coutinho Borges De Sousa, TorstenKoettig and Beatriz Del Valle Grande for their help in thermal conductivity activity. I thankMarco Morrone for his help, the interesting sharing on finite element simulations and for encouraging conversations. I also thank Nicola Cersullo for his friendship and for having sharedthis experience at CERN from the first day. I thank Fabrizio Niccoli for his suggestions and forfunny moments during lunches and coffee breaks in cafeteria. I thank all my colleagues ofMagnet Design & Technology section of CERN for all expertise shared. For their support, bigthanks to my friends Guglielmo Luca Bambino and Matteo Armando. I shared with them myuniversity experience in a way that they became very good friends. I want to thank my Familyto have trusted always in me, my “second family” in Turin, and my friends from Ramacca andGeneva.Last but not least, special thanks to my girlfriend Giuliana. She has always supported me inall decisions and strongly encouraged me with her unconditional love.x

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ContentsDeclaration of Authorship . iiiAbstract . viiSommario . viiiAcknowledgments . xList of Abbreviations . xviList of Symbols . xx1. Introduction . 241.2Scope of the thesis . 251.3Structure of the thesis. 252. The LHC and the HL-LHC . 262.1The Large Hadron Collider . 262.2The CERN accelerator complex . 272.3 The High-Luminosity Large Hadron Collider . 302.3.1 Luminosity . 302.3.2 Machine upgrade. 313. Superconducting accelerator magnets and their protection . 323.1 Superconducting accelerator magnets . 323.1.1 Particle accelerators and their physics . 323.1.2 The LHC main magnets and their general features. 333.1.3 Superconducting materials in accelerator magnets . 353.1.4 Practical wires and cables for magnets . 363.1.5 LHC dipole and quadrupole magnets. 383.1.6 Nb3Sn magnets for HiLumi upgrade . 423.2 Quench protection in superconducting magnets. 453.2.1 What is a quench? . 453.2.2 Quench detection and current supply disconnection. 463.2.3 Temperature rise and MIITs . 473.2.4 Quench protection strategies . 483.2.5 Heater designs . 494. Quench protection heater numerical simulation . 554.1Quench heater delay: from experimental procedure to numerical thermal model . 554.1.1 Quench heater delay experimental procedure . 554.1.2 Domain modelling . 564.1.3 Governing equation. 58xii

4.1.4 Boundary conditions . 594.1.5 Material properties . 604.1.6 Current sharing temperature. 624.1.7 Numerical solution . 634.2Quench heater delay analysis for MQXFS5 magnet . 644.2.1 Quench heater delay simulations results . 644.2.2 Heater temperature profile . 704.2.3 Heat diffusion in the coil. 714.3Quench heater analysis results for 11 T magnet . 714.3.1 Quench heater delay simulations results . 714.4Estimation of the heater adiabatic temperature . 824.4.1 Analytical approach . 824.4.2 FE heater model approach . 834.5Concluding remarks on quench heater analysis . 845. Steady-state measurements and numerical modelling of thermal conductivity ofimpregnated Nb3Sn cable stacks . 855.1Thermal conductivity of single components . 855.1.1 Evaluation of the interface resistance . 885.1.2 Epoxy resin thermal conductivity . 925.1.3 Impregnated S2-glass thermal conductivity . 925.1.4 Impregnated S2-glass with binder thermal conductivity . 935.1.5 Impregnated S2-glass-mica with binder thermal conductivity . 935.2Thermal conductivity measurements of coil segments and cable stacks components . 955.2.1 Steady-state measurement method . 985.2.2 Experimental setup description . 1005.2.3 Experimental results. 1015.3Numerical model of Nb3Sn cable stacks . 1055.3.1 Model implementation . 1055.3.2 Strand transposition effect modelling . 1115.3.3 Interfacial thermal contact resistance modelling. 1125.3.4 Numerical solution . 1165.4Results of thermal conductivity simulations on Nb3Sn cables stacks . 1165.4.1 Results of Case A: thermal conductivity of coil sample #3 . 1165.4.2 Results of Case B: strand transposition effect on thermal conductivity of coil sample#3 . 1205.4.3 Results of Case C: effect of interstand thermal resistance on thermal conductivity ofcoil sample #3 . 121xiii

5.4.4 Results of the analogy between thermal and electrical contact resistance . 1255.5Concluding remarks on cable stacks analysis . 1286. Conclusions . 130Annex 1 . 132Section 1: Real coil resistive voltage signals from tests of MBHSP106 magnet . 132Annex 2 . 134Section 1: Thermal conductivity measurements for single components . 134Section 2: Thermal conductivity measurements for coil segments . 141Reference

POLITECNICO DI TORINO Sommario Ingegneria Meccanica Dipartimento di Ingegneria Meccanica e Aerospaziale Corso di Laurea Magistrale Quench Protection Heaters FE Analysis and Thermal Conductivity Measurements of Nb 3Sn Cables for High-Field

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