Abstract

The magnetizations of eight high-gradient quadrupole cables designated HQ and QXF and a pair of strands, identical in architecture but with different effective strand diameters extracted from an HQ and a related QXF cable, were measured. In the service of field quality assessment, the cable magnetizations and losses were measured by pickup coil magnetometry at 4.2 K in face-on fields, Bm, of ± 400 mT at frequencies, f, of up to 60 mHz. Based on the coupling component of loss, Qcoup, the coupling magnetization Mcoup = Qcoup/4Bm was derived for a ramp rate of 7.5 mT/s. Persistent current (shielding) magnetization and loss (Msh and Qh,strand) were measured on short pieces of extracted strand by vibrating sample magnetometry at 4.2 K. Unpenetrated M-B loops to ± 400 mT and fully penetrated loops to ± 14 T were obtained. Mcoup can be easily controlled and reduced to relatively small values by introducing cores and adjusting the preparation conditions. But in low fields near injection Nb3Sn’s high Jc and correspondingly high Msh,cable may call for magnetic compensation to preserve field quality. The suitably adjusted cable and strand fully penetrated M-B loops were in reasonable accord leading to the conclusion that strand magnetization is a useful measure of cable magnetization, and that when suitably manipulated can provide input to magnet field error calculations.

Highlights

  • 1.1 High Field Nb3Sn Magnets Rutherford cables wound with Nb3Sn strands will be used in all the high field superconducting magnets required for ongoing and planned upgrades to the large hadron collider (LHC), viz. the high luminosity LHC (High Lumi LHC, HL-LHC, 11 and 12 T), a higher energy LHC (HE-LHC, 16 T), and a very high energy future circular collider (FCC, 16 T) [1]

  • As a contribution to this topic, and indirectly to the US LHC Accelerator Research Program (LARP), we report on the magnetizations of: (i) LARP high gradient quadrupole cables designated HQ and QXF [18], (ii) a pair of strands, identical in architecture but with different deffs, that had been extracted from a LARP HQ and a related LARP QXF cable

  • As a contribution to this topic, and indirectly to the US LHC Accelerator Research Program (LARP), we have measured the magnetizations of: (i) eight LARP high gradient quadrupole cables designated HQ and QXF, (ii) a pair of strands, identical in architecture but with different deffs, that had been extracted from a LARP HQ and a related LARP QXF cable

Read more

Summary

Introduction

1.1 High Field Nb3Sn Magnets Rutherford cables wound with Nb3Sn strands will be used in all the high field superconducting magnets required for ongoing and planned upgrades to the large hadron collider (LHC), viz. the high luminosity LHC (High Lumi LHC, HL-LHC, 11 and 12 T), a higher energy LHC (HE-LHC, 16 T), and a very high energy future circular collider (FCC, 16 T) [1]. Reported elsewhere are the effects of core type, placement, and width and heat treatment condition on interstrand coupling properties of Nb3Sn cables[17][18]; important properties of strands are the field dependent critical current density, Jc(B), and the effective filament diameter, deff. As a contribution to this topic, and indirectly to the US LHC Accelerator Research Program (LARP), we report on the magnetizations of: (i) LARP high gradient quadrupole cables designated HQ and QXF [18], (ii) a pair of strands, identical in architecture but with different deffs, that had been extracted from a LARP HQ and a related LARP QXF cable. Several coils of the stainless-steel-cored HQ- and QXF-type Nb3Sn Rutherford cables wound at LBNL were supplied for measurement to the Ohio State University’s Center for Superconducting and Magnetic Materials (OSU-CSMM).

Strand Measurement
Cable Loss and Magnetization
Strand Loss and Magnetization
Cable and Strand Magnetizations
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call