Magnetization in superconducting corrector magnets and impact on luminosity-calibration scans in the Large Hadron Collider (original) (raw)
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IEEE Transactions on Appiled Superconductivity, 1995
Dynamic Magnetic Mé'surements of Superconducting Magnets for the LHC M we 3 S 93 LHC Note 294 CERN AT/94-2.9 g (MA) / CERN'AT'94'39 llllllllllllllllllllllllllllllllllllll CERN LIBRARIES, GENEVA EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH constant rate. the shaft rotation rate is constant and the same OCR Output revolution and averaged. The current changes with a By + iBx = Blzfbn + ia,_)(z/r0)" measurements are performed with both directions of eliminate to first order these disturbances. The B1 of the magnet at x = ro: Two characteristics of the measuring device are used to The field B(B,,B,) is expanded relative to the main field errors on the harmonics, mainly the lowest ones. measured as a function of the angle, non-linearity's seen as H. DEFNITION OFFHDERRORS coils assemblies introduces, in the integrated voltage during the several seconds needed for a revolution of the wider superconducting cable used. sweeps brings another complication. The change of the field
Performance of the superconducting corrector magnet circuits during the commissioning of the LHC
2008
The LHC is a complex machine requiring more than 7400 superconducting corrector magnets distributed along a circumference of 26.7 km. These magnets are powered in 1446 different electrical circuits at currents ranging from 60 A up to 600 A. Among the corrector circuits the 600 A corrector magnets form the most diverse and differentiated group. All together, about 60000 high current connections had to be made. A fault in a circuit or one of the superconducting connections would have severe consequences for the accelerator operation. All magnets are wound from various types of Nb-Ti superconducting strands, and many contain parallel protection resistors to by-pass the current still flowing in the other magnets of the same circuit when they quench. In this paper the performance of these magnet circuits is presented, focussing on the quench behaviour of the magnets. Quench detection and the performance of the electrical interconnects will be dealt with. The results as measured on the entire circuits are compared to the test results obtained at the reception of the individual magnets.
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IEEE Transactions on Applied Superconductivity, 2014
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Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2011
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IEEE Transactions on Appiled Superconductivity, 1999
Abstra-When using superconducting magnets in particle accelerators like the LHC, persistent currents in the superconductor. often determine the field quality at injection, where the magnetic field is low. This paper describes magnetization measurements made on LHC cable strands at the Technical University of Vienna and the Institute of Physics of the Polish Academy of Sciences in collaboration with CERN. Measurements were performed at T=2K and T=4.2K on more than 50 strands of 7 different manufacturers with NbTi filament diameter between 5 and 7 micrometer. Two different measurement set-ups were used: vibrating sample magnetometer, with a sample length of about 8mm, and an integrating coil magnetometer, with sample length of about lm. The two methods were compared by measuring the same sample. Low field evidence of proximity effect is discussed. Statistics like ratio of the width of the magnetization loop at 4.2K and 2K, and the initial slope dM/dB after cooldown are presented. Decrease of the magnetization with time, of the order of 2% per hour, was observed in some samples.
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IEEE Transactions on Appiled Superconductivity, 2004
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Quench-back Management for Fast Decaying Currents in SHMS Superconducting Magnets at Jefferson Lab
IEEE Transactions on Applied Superconductivity, 2019
The Super High Momentum Spectrometer (SHMS) of Hall C, part of the 12 GeV Upgrade at Jefferson Lab, was successfully commissioned in 2017. Early operation shows that fast dumps of the SHMS Q2/Q3 and Dipole superconducting magnets triggered quenches, causing some level of operational difficulty. Tests and detailed analyses indicate that a fast discharge produces a fast current decay, which results in substantial AC loss in the conductor and subsequently triggers a quench-back effect. The OPERA/ELECTRA software package was used to calculate the amount of heat deposited in the copper stabilizer from a fast current decay. The magnets' external protection dump resistor values were lowered to slow the fast dumping of the magnet's current, which therefore reduces or eliminates the quench-back effects. A worst-case adiabatic quench scenario was analyzed, assuming no external dump resistor and no liquid helium surrounding the coil, to ensure the safety of the magnets. The stress levels in the coil imposed by winding, collaring preload, Lorentz force, and temperature gradient during a quench, were also examined. The Tsai-Wu material failure criterion was used to determine the acceptable combined stress level. Linear orthotropic analysis of the coil indicates that the magnets can be operated safely with appropriately sized dump resistors. Fast dump tests with the modified dump resistors have been planned to verify the performance and suitability. Index Terms-Magnet, fast discharge, superconducting, AC loss, quench-back, dump resistor, Tsai-Wu criterion I. INTRODUCTION Jefferson Lab's 11 GeV Super High Momentum Spectrometer (SHMS), consisting of Horizontal Bend (HB), Q1, Q2, Q3, and Dipole magnets has been commissioned successfully [1]-[5] with all magnets achieving the required 11 GeV specifications. Fig. 1 indicates the layout of all five superconducting magnets in experimental Hall C [5]. Table 1 summarizes the key design parameters for the magnets. The magnet design employs 36-strand NbTi-Rutherford cable, originally manufactured for the dipoles of the now abandoned Superconducting Super Collider (SSC) [5]. The HB and Q1 used bare SSC cable while the Q2, Q3, and the Cos θ Dipole used copper stabilized SSC cable. During pre-commissioning, the HB experienced a series of training quenches, starting at 2640 A, before reaching 4000 A (3900 A is required for 11 The Manuscript received XXXXXX.