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Progress in the Development of the Nb 3 Sn MQXFB Quadrupole for the HiLumi Upgrade of the LHC

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In this paper, the status of the development activities at CERN is described, in particular on the cold powering test of the first MQFXB prototype and on the construction of the second full scale prototype.
Abstract
The high-luminosity upgrade of the Large Hadron Collider (HL-LHC) requires new high field and large-aperture quadrupole magnets for the low-beta inner triplets (MQXF). With a nominal operating gradient of 132.2 T/m in a 150 mm aperture and a conductor peak field of 11.3 T, the new quadrupole magnets are based on Nb3Sn superconducting technology. After a series of short models constructed in close collaboration by LARP (LHC Accelerator Research Program) and CERN, the development program is entering in the series production phase with CERN on one side and the US Accelerator Upgrade Project (US-AUP) on the other side assembling and testing full-length magnets. This paper describes the status of the development activities at CERN, in particular on the cold powering test of the first MQFXB prototype and on the construction of the second full scale prototype. Critical operations such as reaction heat treatment, coil impregnation and magnet assembly are discussed. Finally, the plan towards the series production is described.

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Journal ArticleDOI

Power Test of the First Two HL-LHC Insertion Quadrupole Magnets Built at CERN

TL;DR: In this paper , the authors present the test and analysis results of two CERN-built prototypes of these two magnets, with emphasis on quenches and training, voltage-current measurements and the quench localization with voltage taps and a new quench antenna.
Journal ArticleDOI

Assembly and Pre-Loading Specifications for the Series Production of the Nb3Sn MQXFA Quadrupole Magnets for the HL-LHC

TL;DR: In this paper , a series of assembly and pre-load specifications have been defined with the goals of minimizing the risk of conductor degradation and providing the mechanical support required to reach the nominal current during powering.
Journal ArticleDOI

Status of the MQXFB Nb<sub>3</sub>Sn Quadrupoles for the HL-LHC

TL;DR: In this article , the authors outline the strategy that has been defined to address the possible sources of performance limitation, namely coil manufacturing, magnet assembly and integration in the cold mass, which can be found in the first two prototypes of the MQXFB quadrupoles.

Status of the MQXFB Nb3Sn Quadrupoles for the HL-LHC

TL;DR: In this article , the authors outline the strategy that has been defined to address the possible sources of performance limitation, namely coil manufacturing, magnet assembly and integration in the cold mass, and identify fractured Nb3Sn sub-elements in strands located at one specific position of the inner layer pole turn.
References
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Journal ArticleDOI

Magnet Design of the 150 mm Aperture Low- $\beta$ Quadrupoles for the High Luminosity LHC

TL;DR: In this article, the authors present the HL-LHC low-β quadrupole design, based on the experience gathered by the US LARP program, and describe the support structure components to preload the coils, withstand the electro-magnetic forces, provide alignment and LHe containment, and integrate the cold mass in the LHC IRs.
Journal Article

Magnet R&D for the US LHC Accelerator Research Program (LARP)

TL;DR: Sagourlay et al. as discussed by the authors reported that Fermilab National Accelerator Laboratory, Batavia, IL 3 M. Anerella, A. Ghosh,, R. Gupta, M. Harrison, J. Schmazle, and P. Wanderer are with Brookhaven National Laboratory, Upton, NY.
Journal ArticleDOI

Lumped-Element Dynamic Electro-Thermal model of a superconducting magnet

TL;DR: In this paper, a Lumped Element Dynamic Electro-Thermal (LEDET) model of a superconducting magnet is presented, which includes non-linear dynamic effects such as the dependence of the magnet's differential self-inductance on the presence of inter-filament and interstrand coupling currents in the conductor.
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Q1. What have the authors contributed in "Progress in the development of the nb3sn mqxfb quadrupole for the hilumi upgrade of the lhc" ?

After a series of short models constructed in close collaboration by LARP ( LHC Accelerator Research Program ) and CERN, the development program is entering in the series production phase with CERN on one side and the US Accelerator Upgrade Project ( US-AUP ) on the other side assembling and testing full-length magnets. This paper describes the status of the development activities at CERN, in particular on the cold powering test of the first MQFXB prototype and on the construction of the second full scale prototype. Critical operations such as reaction heat treatment, coil impregnation and magnet assembly are discussed. 

8. One 125 μm polyimide layer is wrapped around the coil, and two around the collars, with a total thickness of 375 μm which constitute the ground plane insulation. 

The pole is floating, and the maximum voltage drop during quench in the pole turns is 10 V meaning that 10 MΩ resistance between coil and pole is considered sufficient to assure safe operation. 

The longitudinal prestress at warm in MQXFBP1 was equal 0.6 MN, aiming at a total force of 1.2 MN after cooldown which corresponds to the longitudinal electromagnetic forces at nominal current. 

The target pre-stress in the SS shell is 75 MPa to assure that shell is still in contact with the magnet aluminum shell after cool-down. 

Thanks to the iteration on the cross section, increasing the pole insulation thickness and re-ducing the mid-plane shim thickness by 0.125 mm, b6 is close to the target in MQXFBP2. 

The production of MQXFB coils started in 2016 with two copper coils followed by two low performance Nb3Sn RRP conductor (CR001, CR002, CR101 and CR102) [14]. 

The expected impact of replacing the 13.8 mm key by the conical key is an increase of the stress in the shell of 18 MPa in the magnet extremities whereas the stress in the center remains constant. 

Before transferring the reacted coil in the impregnation mold, a flexible circuit which includes quench protection heaters is installed in the coil outer radius. 

The first prototype MQXFBP1 was limited in performance reaching a current of 15.1 kA, equivalent to 6.5 TeV operation in the LHC. 

Due to the impossibility to access the reverse side of the longitudinal weld of the shrinkage cylinders, a permanent backing strip has been chosen, in order to provide support for a fully penetrated root pass [31]. 

From September 2019, ten conformedcoils have been produced, one is on-hold and one was rejected due to a critical nonconformity during winding. 

Conductor procurement is close to completion and coil fabrication resumed after and in-depth review of the manufacturing process with a production rate of one coil per month. 

Quench propagation velocity at 15 kA is 15 m/s, similar to the typical quench propagation at this current level measured in short models and cable samples ([34],[35]), pointing to a local defect and not a global degradation of the coil. 

Figure 11 shows that the measured stress in the shell is 100 to 175 MPa, corresponding to an increase of azimuthal stress in the coil of 15 to 20 MPa which was considered adequate for MQXFB magnets. 

The azimuthal solution is in general preferred, as it allows to bring the four coils inner surface at the same radius, with beneficial effects on the field homogeneity [19]. 

The remaining quantity to fulfill the production, 1.7WDOI: 10.1109/TASC.2021.3061352 FERMILAB-PUB-21-126-TD (accepted)This manuscript has been authored by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the U.S. Department of Energy, Office of Science, Office of High Energy Physics.tons of RRP 108/127, are expected to be delivered by summer 2021 [9]. 

Thanks to an improvement on the leak-tightness of the reaction fixture, the difference in RRR among the connection and non-connection side decreased significantly in the last coils.