Publication | Closed Access
Characteristics of Round and Extracted Strands of ${\hbox{Nb}}_{3}\hbox{Al}$ Rutherford Cable
24
Citations
10
References
2007
Year
Materials ScienceMaterials EngineeringMagnetic PropertiesMagnetismN ValueEngineeringPhysicsMagnetic MaterialsRutherford CableNatural SciencesApplied PhysicsSuperconductivityCu StabilizerCopper StabilizerCrystallographyParticle AcceleratorAccelerator Technology
Long Nb <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> Al strands with copper stabilizer are promising for future high field accelerator magnets. A 1.2 kilometer Nb <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> Al strand with Cu stabilizer was fabricated at the National Institute for Materials Science in Japan. Using this strand a 30 meter Cu stabilized Nb <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> Al Rutherford cable was made for the first time by a collaboration of NIMS and Fermilab. The Nb <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> Al strands extracted from cable with a relatively low packing factor showed almost no J <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c</sub> degradation. But the extracted strands from the highly compacted cable showed some degradation in both J <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c</sub> and n value, which may be caused by local separation of the copper stabilizer. Still, its J <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c</sub> degradation is lower than that of typical Nb3Sn strands. The current limit due to magnetic instability in low field is about 500 A at 4.2 K. The magnetization of the strands, which was measured with balanced coils at 4.2 K, showed large flux jumps, usually around 1.5 T. This value is much larger than the B <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c2</sub> (4.2 K) of the Nb matrix, which is around 0.4 Tesla. The magnetic instability of the Nb <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> Al strand at low field is not completely understood, but it might be explained by the superconducting coupling current through the Nb matrix.
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