TY - JOUR
T1 - Pinning characteristics in multifilamentary NbTi superconducting wires with submicrometre filaments introduced artificial pinning centres
AU - Miura, O.
AU - Matsumoto, K.
AU - Tanaka, Y.
AU - Yamafuji, K.
AU - Harada, N.
AU - Iwakuma, M.
AU - Funaki, K.
AU - Matsushita, T.
N1 - Copyright:
Copyright 2014 Elsevier B.V., All rights reserved.
PY - 1992
Y1 - 1992
N2 - Multifilamentary NbTi superconducting wires for a.c. use were developed by introducing ultrafine Nb island-type artificial pinning centres. The maximum Jc value obtained for wire with a filament diameter of 0.4 μm reached as high as 1.07 × 1010 A m-2 at 1 T and 4.44 × 109 A m-2 at 3 T, which are more than twice the Jc values for conventional wires for a.c. use. For these wires, the constants of the scaling rule for global pinning force, Fp α bγ(1-b)δ, became γ = 0.8 and δ = 1.6. This indicates that the pinning characteristics of the present wires were shifted to the oversaturation-type by the introduction of artificial pinning centres, while they are of the saturation-type for conventional a.c. wires. As a result, the global pinning force at low and medium magnetic fields can be explained fairly well by the direct summation model which is available only for strong pins. A helpful guideline in designing Jc values for a.c. wires is also discussed.
AB - Multifilamentary NbTi superconducting wires for a.c. use were developed by introducing ultrafine Nb island-type artificial pinning centres. The maximum Jc value obtained for wire with a filament diameter of 0.4 μm reached as high as 1.07 × 1010 A m-2 at 1 T and 4.44 × 109 A m-2 at 3 T, which are more than twice the Jc values for conventional wires for a.c. use. For these wires, the constants of the scaling rule for global pinning force, Fp α bγ(1-b)δ, became γ = 0.8 and δ = 1.6. This indicates that the pinning characteristics of the present wires were shifted to the oversaturation-type by the introduction of artificial pinning centres, while they are of the saturation-type for conventional a.c. wires. As a result, the global pinning force at low and medium magnetic fields can be explained fairly well by the direct summation model which is available only for strong pins. A helpful guideline in designing Jc values for a.c. wires is also discussed.
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U2 - 10.1016/0011-2275(92)90371-G
DO - 10.1016/0011-2275(92)90371-G
M3 - Article
AN - SCOPUS:0000173124
SN - 0011-2275
VL - 32
SP - 315
EP - 322
JO - Cryogenics
JF - Cryogenics
IS - 3
ER -