2006 Fiscal Year Final Research Report Summary
Development of a Conduction-Cooled Low Temperature Superconducting (LTS) Pulse Coil
| Project/Area Number |
16206028
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| Research Category |
Grant-in-Aid for Scientific Research (A)
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| Allocation Type | Single-year Grants |
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| Section | 一般 |
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| Research Field |
電力工学・電気機器工学
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| Research Institution | National Institute for Fusion Science |
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Principal Investigator |
MITO Toshiyuki National Institute for Fusion Science, Department of LHD Project, Professor (10166069)
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| Co-Investigator(Kenkyū-buntansha) |
CHIKARAISHI Hirotaka National Institute of Fusion Science, Dep. of LHD Project, A. Professor (60249969)
NAGATO Yanagi National Institute of Fusion Science, Dep. of LHD Project, A. Professor (70230258)
TAMURA Hitoshi National Institute of Fusion Science, Dep. of LHD Project, R. Associate (20236756)
MAEKAWA Ryuji National Institute of Fusion Science, Dep. of LHD Project, A. Professor (80280600)
IWAMOTO Akifumi National Institute of Fusion Science, Dep. of LHD Project, R. Associate (00260050)
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| Project Period (FY) |
2004 – 2006
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| Keywords | Superconducting / Conduction cooling / Cryogenic / Pulse coil / Momentary voltage drop / SMES / Power failure / AC loss |
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| Research Abstract |
A conduction-cooled LTS pulse coil has excellent characteristics, which are adequate for a short-time uninterruptible power supply (UPS). The conduction cooling has higher reliability and easier operation than the conventional cooling schemes such as pool boiling with liquid helium or forced flow of supercritical helium. A low AC loss and a high stability are required for the superconducting (SC) conductor. The SC conductor of a NbTi/Cu compacted strand cable extruded with an aluminum has been developed. The coil shape is a single solenoid of 183 turns x 14 layers wound on the GFRP bobbin. The Dyneema FRP (DFRP) spacers and the Litz wires (braided wires of insulated copper strands) are inserted in each layer. The DFRP spacers have a good thermal conductivity along with Dyneema filaments, which enhance the heat transfer from layer to layer in the windings. On the other hand, the Litz wires increase the heat transfer from turn to turn in the windings and enable conduction cooling of the
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coil by attaching the end of the Litz wires directly to the cold heads of the cryocoolers. The coil was connected with three GM cryocoolers which have cooling capacity of 4.5 W at 4 K and 240 W at 50 K. Whereas the coil cold mass is 1, 100 kg and the heat loads are 2.3 W at 4 K and 186 W at 65 K. It took approximately two weeks to cool-down the coil as exclusively utilizing cryocoolers. The spatial temperature distributions within the coil were negligible during the cool-down, which indicated good thermal properties of the coil. To evaluate the thermal performance of the coil, the coil current was reduced rapidly from the rated current of 1000 A with a time constant of 4 s. Due to the AC loss of 447 J, the temperature of the coil increased from 3.9 K to 4.4 K. However, the temperature increase of the coil was only 0.5 K. It means that the heat generated by the AC loss was well distributed within the coil winding and was also transferred to the cold heads of cryocoolers during a few second. Since the components of the coil have high thermal diffusivities at the cryogenic temperature below 10 K, the enhanced thermal diffusivity of the coil results in the rapid temperature stabilization. We have successfully developed the 1 MJ conduction-cooled LTS pulse coil. The high performance of the conduction-cooled coil has been demonstrated by the cooling and excitation tests and its applicability was also confirmed by the energy extraction tests as the UPS-SMES. Less
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Research Products
(16 results)
