New Magnets for the IR How far are we from the HL-LHC Target?

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Presentation transcript:

New Magnets for the IR How far are we from the HL-LHC Target? BNL - FNAL - LBNL - SLAC New Magnets for the IR How far are we from the HL-LHC Target? GianLuca Sabbi for the US LHC Accelerator Research Program LHC Performance Workshop – Chamonix 2012

New Magnets for the IR How far are we from the HL-LHC Target? BNL - FNAL - LBNL - SLAC New Magnets for the IR How far are we from the HL-LHC Target? close GianLuca Sabbi for the US LHC Accelerator Research Program LHC Performance Workshop – Chamonix 2012

Presentation Outline Topics/guidelines: Summary of LARP magnet program components and achievements Focus on remaining challenges, both technical and programmatic Selecting a conductor design and developing it for production Managing stress/strain in the final design and during production Incorporating design elements for accelerator integration Project organization and timelines for prototyping/production …and wait, how far from what? Converging on targets for HL-LHC Build on collaboration meeting discussion, minimize repetitions LARP program goals and organization Details of conductor development, magnet designs, test results https://indico.cern.ch/conferenceDisplay.py?confId=150474

US LHC Accelerator Research Program Started by DOE in 2003, expected to be completed around 2014 Progression from the US LHC Accelerator Research Project Collaboration of four national Labs: BNL, FNAL, LBNL, SLAC General goals: Extend and improve the performance of LHC Maximize scientific output in support of the experiments Maintain and develop US Labs capabilities Prepare for a leadership role in future projects Research and training for US accelerator physicists and engineers Advance international collaboration on large accelerator projects Major focus: development of Nb3Sn IR Quadrupoles for HL-LHC

Nb3Sn Technology Challenges Brittleness: React coils after winding Epoxy impregnation Strain sensitivity: Mechanical design and analysis to prevent degradation under high stress Transverse Stress (MPa) Cable Critical Current (kA) Material NbTi Nb3Sn Dipole Limit ~ 10 T ~ 17 T Reaction Ductile ~ 6750C Insulation Polymide S/E Glass Coil parts G-10 Stainless Axial Strain N/A ~ 0.3 % Transverse stress ~ 200 MPa

LARP Magnet Development Chart Ongoing Completed

LARP Magnets SQ SM TQS LR LQS-4m HQ TQC

Program Achievements - Timeline (1/2) Mar. 2006 SQ02 reaches 97% of SSL at both 4.5K and 1.9K Demonstrates MJR 54/61conductor performance for TQ Jun. 2007 TQS02a surpasses 220 T/m at both 4.5K and 1.9K (*) Achieved 200 T/m goal with RRP 54/61 conductor Jan. 2008 LRS02 reaches 96% of SSL at 4.5K with RRP 54/61 Coil & shell structure scale-up from 0.3 m to 4 m July 2009 TQS03a achieves 240 T/m (1.9K) with RRP 108/127 (*) Increased stability with smaller filament size Dec. 2009 TQS03b operates at 200 MPa (average) coil stress (*) Widens Nb3Sn design space (as required…) (*) Tests performed at CERN

Program Achievements - Timeline (2/2) Dec. 2009 LQS01a reaches 200 T/m at both 4.5K and 1.9K LARP meets its “defining” milestone Feb. 2010 TQS03d shows no degradation after 1000 cycles (*) Comparable to operational lifetime in HL-LHC July 2010 LQS01b achieves 220 T/m with RRP 54/61 Same TQS02 level at 4.5K, but no degradation at 1.9K Apr. 2011 HQ01d achieves 170 T/m in 120 mm aperture at 4.5 K At HL-LHC operational level with good field quality Oct. 2011 HQM02 achieves ~90% of SSL at both 4.6 K and 2.2 K Reduced compaction results in best HQ coil to date (*) Test performed at CERN

TQ Studies: Stress Limits Coil layer 1 stress evolution - sq Calculated peak stresses in TQS03c 260 MPa @ 4.5K Systematic investigation in TQS03: TQS03a: 120 MPa at pole, 93% SSL TQS03b: 160 MPa at pole, 91% SSL TQS03c: 200 MPa at pole, 88% SSL Peak stresses are considerably higher Considerably widens design window 255 MPa @ SSL

TQS03d Cycling Test Reduced coil stress to TQS03b levels (160 MPa average) Pre-loading operation and test performed at CERN Did not recover TQS03b quench current (permanent degradation) Performed 1000 cycles with control quenches every ~150 cycles No change in mechanical parameters or quench levels

Long Quadrupole (LQ) TQ length scale-up from 1 m to 4 m (2) D1 (1) S2 (4) S3 S4 D2 D3 TQ length scale-up from 1 m to 4 m Coil Fabrication: FNAL+BNL+LBNL Mechanical structure and assembly: LBNL Test: FNAL Target gradient 200 T/m LQS01 assembly at LBNL LQSD test at FNAL

LQS01 & LQS01b Quench Performance 200 T/m 200 T/m 4.5 K ~3 K 1.9 K

Conductor – Technical Issues Two leading processes: Internal tin (US-OST-RRP) and powder in tube (EU-Bruker-PIT) A quasi-continuous range of “stacks” using fewer or more sub-elements Mainly exercised for RRP, for programmatic and historical reasons Low range: High range: 169 Better developed (high/controlled Jc/RRR; long pieces Larger filament size (magnetization effects, flux-jumps) Smaller magnetization effects and in principle more stable (only if tolerance to cabling and reaction can be preserved) Less developed: control of properties, piece length

Conductor – Programmatic Issues Multiple applications with different requirements, priorities, time scales IR Quads, 11 T dipoles, cable testing and HE-LHC dipoles Developing a single conductor suitable for all applications is difficult Pursuing parallel routes & incremental improvements is inefficient Need to define a clear strategy for the HL-LHC IR Quads. Examples: Focus on “middle range” 108/127 (moderate improvement from 54/61, close to production readiness) Select/push a more ambitious target (RRP 217 and/or PIT 192) and analyze/qualify a fall back option using RRP 54/61 Perform cost/benefits analysis for accelerator, materials, magnet Move from R&D approach to project-type organization Engage the DOE-HEP materials R&D community, which appears to be primarily focused on very long term developments (HTS)

HQM02 Temperature Dependence RRP 54/61 Performance in HQ Mirror #2 Training at 4.5K: HQM02 vs. HQM01, HQ01a, HQ01d HQM02 Temperature Dependence The best performing HQ coil to date was built with RRP 54/61 a production-ready conductor

Handling High Stress in Magnet Coils 1. Understand limits 2. Optimize structure and coil for minimum stress TQ (90 mm, ~12 T) LQ (90 mm, ~12 T) HQ (120 mm, ~15 T) Titanium pole Key location Coil geometry 180 MPa 170 MPa 4.5K, 0T/m SSL preload 4.5K, 0T/m SSL preload 4.5K, 0T/m SSL preload 200 MPa 170 MPa 190 MPa

Mechanical Design Space in HQ models Pole quenches (HQ01d) Pole stress during ramp to quench (HQ01d) Pole quenches and strain gauge data indicate insufficient pre-load Mid-plane quenches indicate excessive pre-load Narrow design and assembly window: ok for an R&D model designed to explore stress limits, may require optimization for production, in particular if the aperture is further increased Mid-plane Quenches (HQ01d)

HQ Coil Design – Lessons Learned HQ design assumed less space for inter-turn insulation than TQ/LQ Based on measurements, but limits expansion during reaction As a result, coils were over sized and over compressed Also, insufficient pole gaps led to excessive longitudinal strain  Analyzed, understood and fixed in second generation coils We do not yet control this technology sufficiently well to scale to a larger aperture or full length coils without experimental verification 

Accelerator Integration Issues Pre-load optimization for high gradient with minimal training Alignment, quench protection, radiation hardness, cooling system Field quality: cross-section iteration; cored cable for eddy current control Structure and assembly features for magnet production and installation

Accelerator Quality in LARP Models Design Features LR SQ TQS/LQS TQC HQ LHQ (Goals) Geometric field quality √ Structure alignment Coil alignment Saturation effects Persistent/eddy currents End optimization Cooling channels Helium containment Radiation hardness

Coil Aperture and Length Two design choices will have significant implications on the project: Quadrupole aperture (120 mm vs. 140-150 mm) Production coil length: full (8-10 m) or half (4-5 m) If the final design uses 120 mm aperture and half length coils: LHQ can be considered as a pre-prototype The coil fabrication infrastructure is (mostly) available Simple transition from technology demonstration to production Otherwise, experimental verification of the final design will be required: Larger aperture will require short model development Full length coils will require infrastructure and a prototype Change of aperture and full length coils will require both (in series)

R&D and Construction Schedule As of June 2011 (DOE review) Significant contributions from CERN will be required to implement this plan, in particular if the larger aperture and/or the full length coil option is selected

Summary Acknowledgement A large knowledge base is available after 7 years of fully integrated effort involving three US Labs and CERN Demonstrated all fundamental aspects of Nb3Sn technology: - Steady progress in understanding and addressing R&D issues The remaining challenges have an increasingly programmatic flavor: design integration, production organization and processes HL-LHC IR Quads are a key step for future high-field applications Next few years will be critical and much work is still left to do - Integrate effort with CERN, EuCARD, KEK, US core programs Acknowledgement