2014
DOI: 10.1109/tasc.2013.2285093
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Design, Construction, and Test Arrangement of a Fast-Cycling HTS Accelerator Magnet

Abstract: Design, fabrication and assembly of a novel fastcycling accelerator magnet is presented. A short-sample magnet is powered with a single-turn HTS cable capable to carry 80 kA current at 20 K and generate 1.75 T field in a 40 mm magnet gap. The applied conventional leads and the power supply, however, allow only for a sin-wave 24 kA, 20 Hz current limiting test magnet to a B-field of 0.5 T and to a maximum cycling rate of 20 T/s. The critical aspects of the cable construction and the splicing connection to the p… Show more

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Cited by 11 publications
(9 citation statements)
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“…Similar work was pursued at CERN [173] and is the baseline for the NICA upgrade of the Nuclotron facility [174]. The use of HTS materials may offer additional advantages in terms of operating margin and energy efficiency [175].…”
Section: E Superferric Magnets Spectrometers and Other Applicationsmentioning
confidence: 87%
“…Similar work was pursued at CERN [173] and is the baseline for the NICA upgrade of the Nuclotron facility [174]. The use of HTS materials may offer additional advantages in terms of operating margin and energy efficiency [175].…”
Section: E Superferric Magnets Spectrometers and Other Applicationsmentioning
confidence: 87%
“…The former are more economical. In spite of a number of specific issues, such as AC loss, cooling, quench detection and protection, field quality and material fatigue [17], SC ramping rates of ~1000 T/s are believed to be achievable in HTS-conductor based super ferric magnets [18][19][20]. Table 1 also includes acceleration parameters of the 30-450 GeV accelerator option "SPS" located in the SPS tunnel that accelerates the muons to the injection energy of the LHC size ring.…”
Section: Accelerationmentioning
confidence: 99%
“…The solution is use a core design where the field crossing conductor is strongly suppressed. As discussed in [5,6,7] to achieve this goal the conductor has to be placed in the center of a wide cable gap, and its width should be no more than 20% of that gap, as illustrated in Fig. 2 The total required cable current to generate 1.8 T field in the 30 mm gap is 60 kA.…”
Section: Normal Conducting Magnetsmentioning
confidence: 99%
“…The conceptual design of the super-conducting magnet for the Muon Synchrotrons is based on the work presented in [5,6,7]. The main idea for using the HTS, as oppose to the LTS (NbTi), is the possibility of operating with a wide temperature margin, e.g.…”
Section: Superconducting Magnetsmentioning
confidence: 99%
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