1989
DOI: 10.1016/0011-2275(89)90086-6
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Superconducting current-leads made from high Tc superconductor and normal metal conductor

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Cited by 39 publications
(4 citation statements)
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“…Now, using a different parameterization, let us project the solution on the (j, Θ L ) plane along a curve with constant u, as presented in Figure 8. The bifurcation curves have an "S" form exhibiting two limit points determined by the roots of the equation dj/dΘ L u = 0 (27) as they separate the stable from the unstable solutions. The lower stable solutions correspond to the superconducting branch, whereas the upper ones correspond to the normal branch.…”
Section: Resultsmentioning
confidence: 99%
“…Now, using a different parameterization, let us project the solution on the (j, Θ L ) plane along a curve with constant u, as presented in Figure 8. The bifurcation curves have an "S" form exhibiting two limit points determined by the roots of the equation dj/dΘ L u = 0 (27) as they separate the stable from the unstable solutions. The lower stable solutions correspond to the superconducting branch, whereas the upper ones correspond to the normal branch.…”
Section: Resultsmentioning
confidence: 99%
“…The next significant progression in the CL development took place in the late 1980s after the discovery of HTS above the boiling temperature of liquid nitrogen (LN 2 ) in 1986. Shortly afterwards, in 1989, HTS applications into CLs as a lowtemperature (or second) stage took off as a field of study and the advantages were analysed by shorting out metallic conductor and eliminating Joule heat generation at cold ends [11,12], which opened up the possibility of a lower heat leak beyond the limitation of the WFL law. In the past three decades, different cooling concepts of HTS CLs have been studied [13], and they are generally classified into two categories according to the resistive part of the first stage.…”
Section: Cls With An Hts Sectionmentioning
confidence: 99%
“…Since high-temperature superconductors (HTSs) generate zero Joule loss under the superconducting state and have lower thermal conductivity than normal metals [1], they become an ideal material for current leads [2]. HTS binary current leads were first proposed by Mumford in 1989 [3]. In the past few years, HTS binary current leads have been widely applied, not only in large-scale systems, such as particle accelerators [4][5][6][7] and fusion devices [8][9][10][11][12][13], but also for smaller isolated magnets, such as superconducting magnetic resonance imaging (MRI) magnets [14,15], high-field magnet system [16][17][18][19][20][21] and other special test facilities [22][23][24][25][26][27][28][29][30].…”
Section: Introductionmentioning
confidence: 99%