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電流リード標準化　 三戸利行（核融合科学研究所）

平成 22 年度第１回超電導応用研究会シンポジウム 　「コンセンサス標準と超電導国際規格」 平成 22 年 7 月 16 日　住友電気工業　大阪製作所　研究講堂. 電流リード標準化　 三戸利行（核融合科学研究所）. 沿革 : １９４７年に１８ヶ国により発足 目的 国家間の製品やサービスの交換を助けるために、標準化活動の発展を促進すること 知的、科学的、技術的、そして経済的活動における国家間協力を発展させること 会員その他（ 2008.1 現在） 　 会員数：１５７ヶ国（正会員＋準会員） 規格数：１７，０４１規格 規格作成委員会数：専門委員会（ TC ）２０１

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電流リード標準化　 三戸利行（核融合科学研究所）

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  1. 平成22年度第１回超電導応用研究会シンポジウム　「コンセンサス標準と超電導国際規格」平成22年度第１回超電導応用研究会シンポジウム　「コンセンサス標準と超電導国際規格」 平成22年7月16日　住友電気工業　大阪製作所　研究講堂 電流リード標準化　三戸利行（核融合科学研究所）

  2. 沿革 :１９４７年に１８ヶ国により発足 • 目的 • 国家間の製品やサービスの交換を助けるために、標準化活動の発展を促進すること • 知的、科学的、技術的、そして経済的活動における国家間協力を発展させること • 会員その他（2008.1現在） 　 • 会員数：１５７ヶ国（正会員＋準会員） • 規格数：１７，０４１規格 • 規格作成委員会数：専門委員会（TC）２０１ • 分科委員会 （SC）５４２ • 作業グループ（WG）２２８７ 国際標準化機構:ISO(International Organization for Standardization)

  3. 沿革 :１９０６年に１３ヶ国により発足。 • 目的 • 電機及び電子の技術分野における標準化のすべての問題及び規格適合性評価のような関連事項に関する国際協力を促進し、これによって国際理解を促進すること。 • 会員その他（2010.1現在） 　 • 会員数：７６ヶ国（正会員＋準会員） • 規格数：６，０２７規格（２００８年末現在） • 規格作成委員会数：専門委員会（TC）９４ • 分科委員会 （SC）８０ • 作業グループ（WG）５０５（2008年末現在） 国際電気標準会議:IEC(International ElectrotechnicalCommission)

  4. ＩＥＣ規格は次の６つの段階を踏んで作成 • 新作業項目の提案が承認された後、３６ヶ月以内に国際規格の最終案がまとめられる • （1）新業務項目（ＮＰ）の提案 • （2）作業原案（ＷＤ）の作成 • （3）委員会原案（ＣＤ）の作成 • （4）国際規格原案（ＣＤＶ）の照会及び策定 • （5）最終国際規格案（ＦＤＩＳ）の策定 • （6）国際規格の発行 IEC規格の制定手順

  5. 各国加盟機関、ＴＣ（専門委員会）／ＳＣ（分科委員会）の幹事などが新たな規格の策定、現行規格の改定を提案各国加盟機関、ＴＣ（専門委員会）／ＳＣ（分科委員会）の幹事などが新たな規格の策定、現行規格の改定を提案 • 中央事務局は各国に提案に賛成か反対かを３ヶ月以内に投票するよう依頼 • 投票結果が次を満たす時に提案は承認 • 投票したＴＣ／ＳＣのＰ（積極的参加）メンバーの単純過半数が賛成すること • Ｐメンバーが16人以下のＴＣ／ＳＣでは4人以上、17人以上のＴＣ／ＳＣでは5人以上の投票に賛成したＰメンバーが審議に参加すること （1）新業務項目（ＮＰ）の提案

  6. 提案の承認後、ＴＣ／ＳＣのＷＧ（作業グループ）においてＷＤの策定に当たる専門家をＴＣ／ＳＣの幹事がＰメンバーと協議して任命提案の承認後、ＴＣ／ＳＣのＷＧ（作業グループ）においてＷＤの策定に当たる専門家をＴＣ／ＳＣの幹事がＰメンバーと協議して任命 幹事より任命された専門家はＷＧまたはPTにおいてＷＤを検討作成 その上で、専門家はＮＰ提案承認後６ヶ月以内にＴＣ／ＳＣにＷＤを提出 （2）作業原案（ＷＤ）の作成

  7. ＷＤはＣＤ案として登録されＴＣ／ＳＣの全てのＰメンバー及びＯメンバーに意見照会のため回付ＷＤはＣＤ案として登録されＴＣ／ＳＣの全てのＰメンバー及びＯメンバーに意見照会のため回付 回答期限終了後、幹事が中心にＣＤ案を検討、必要に応じて修正 TC/SCのＰメンバーの合意が得られた場合にCDが成立。 その上で、ＣＤは国際規格原案（ＣＤＶ）として登録（登録期限はＮＰ提案承認から１２ヶ月以内） （3）委員会原案（CD）の作成

  8. 登録されたＣＤＶはＴＣ／ＳＣメンバーだけでなく全てのメンバー国に投票のため回付（投票期間５ヶ月間）登録されたＣＤＶはＴＣ／ＳＣメンバーだけでなく全てのメンバー国に投票のため回付（投票期間５ヶ月間） • ＣＤＶは次を満たす時に承認 • 投票したＴＣ／ＳＣのＰメンバーの２／３以上が賛成 • 反対が投票総数の１／４以下（ＣＤＶが否決された場合、ＴＣ／ＳＣの幹事が中心となりＣＤＶを修正し再投 票にかける） • その上で、ＣＤＶは最終国際規格案（ＦＤＩＳ）として登録 （登録期限はNP提案承認から２４月以内） （4）国際規格原案（ＣＤＶ）の照会及び策定

  9. 中央事務局が登録されたＦＤＩＳを全てのメンバー国に投票のため回付（投票期間２ヶ月。この段階で規格内容の修正は認められず。）中央事務局が登録されたＦＤＩＳを全てのメンバー国に投票のため回付（投票期間２ヶ月。この段階で規格内容の修正は認められず。） • ＦＤＩＳは次を満たす時に承認され国際規格として成立 • 投票したＴＣ／ＳＣのＰメンバーの２／３以上が賛成 • 反対が投票総数の１／４以下 （登録期限はNP提案承認から３３ヶ月以内） （5）最終国際規格案（ＦＤＩＳ）の策定

  10. ＦＤＩＳの承認後、正式に国際規格として発行（発行期限は幹事による国際規格の印刷・校正終了後２ヶ月以内）ＦＤＩＳの承認後、正式に国際規格として発行（発行期限は幹事による国際規格の印刷・校正終了後２ヶ月以内） （6）国際規格の発行

  11. IEC/TC

  12. TC90: Superconductivity Chairman : Mr Loren F. Goodrich (US) Secretary : Mr Ken-ichi Sato (JP) Mr Jun Fujikami(JP) Number of Participating countries :11 Number of Observer countries :15 WG 1 - Terms and definitions WG 2 - Critical current measurement of Nb-Ti composite superconductors WG 3 - Critical current measurement method of oxide superconductors WG 4 - Test method for residual resistivity ratio of Cu/Nb-Ti and Nb3Sn composite superconductors WG 5 - Room temperature tensile tests of Cu/Nb-Ti composite superconductors WG 6 - Matrix composition ratio of Cu/Nb-Ti composite superconductors WG 7 - Critical current measurement method of Nb3Sn composite superconductors WG 8 - Electronic characteristic measurements WG 9 - Measurement method for AC losses in superconducting wires WG 10 - Measurement for bulk high temperature superconductors - Trapped flux density in large grain oxide superconductors WG 11 - Critical temperature measurement - Critical temperature of composite superconductors WG 12 - Current Leads

  13. TC90/WG12 Member List Prof. Toshiyuki MITO (JP): Convenor Mrs. Amalia BALLARINO(IT) Dr. Reihard HELLER (DE) Mr. Masayuki KONNNO (JP) Prof. Takakazu SHINTOMI (JP) Prof. Jacek SOSNOWSKI (PL) Prof. Yinshun WANG (CN) Dr. Huub WEIJERS (US)

  14. Schedule ofTC90/WG12 Start of a project in WG12= moving the IEC-standard clock: 2007-02-02 1st WD: 2007-08 (6-month rule) Final WD: 2008-02 (12-month rule after started) →CD Comments on CD: 2008-05 (3-month rule after submitted CD) Final CD: 2009-03 (12-month rule after submitted CD) →CDV Voting CDV: 2009-08 (5-month rule after submitted CDV) Submitting FDIS: 2010-3 (9-month rule after submitted CDV) →FDIS Finishing WG12’s duty on the stage Voting FDIS: 2010-5 (2-month rule after FDIS) Publishing IS: 2010-8 (3-month rule after submitted FDIS)［the 3-year (=36-month) IEC-rule after moving the standard clock］

  15. Proceedings for the IEC/WG12 (1) Ad-hoc group: －Establishment: done in 9th IEC/TC90 meeting held at ANL on Sept. 3, 2004 －Rapporteur: Prof. Dr. Kozo Osamura (Japan) －1st ad-hoc group meeting: hosted by IEEE Council of Superconductivity and IEC/TC90 on Oct. 6, 2004 during the period of ASC at Jacksonville －Japanese mission: visited FzK (Karlsruhe), EAS (Hanau), ATI (Wien) and THEVA (Munchen) and exchanged opinions dated on June 20 to 24, 2005 －2nd ad-hoc group meeting: held at Wien on Sept. 15, 2005, and discussed on the purpose and the content for a standard of the current leads －3rd ad-hoc group meeting: held at Genova on Sept. 21, 2005 during the period of MT-19, and discussed on the agreeable solution for the standardization －Final report of the ad-hoc group: reported by the rapporteur on June 1, 2006 at Kyoto, Japan

  16. Proceedings for the IEC/WG12 (2) 10th IEC/TC90 Kyoto Meeting: －Date: on June 1, 2006 at Kyoto, Japan －Final report of the ad-hoc group: mentioned above －Decision: All participated countries were in favor for submitting NWIP Result of Voting on NWIP: －Circulation date: 2006-09-02 －Closing date: 2006-12-22 －Result: Approved without any comments Establishment of the WG12: －Date: 2007-02-02 －Convenor: Prof. Dr. Toshiyuki Mito (Japan)－Member: 6 experts, after that 1 expert was joined

  17. Proceedings for the IEC/WG12 (3) 1stMeeting of WG12: －Date: on August 28, 2007 at Philadelphia, USA －Discussion on the first working draft prepared by the JNC 2ndMeeting of WG12 : －Date: on November 7, 2007 at Tsukuba, Japan －Discussion on each comments with the members on the 1st WD after the 1st WG12 meeting 11th IEC/TC90 Berlin Meeting, 3rdMeeting of WG12: －Date: on June 10, 2008 at Berlin, Germany －Discussion on the working draft for IEC 61788-14 Ed.1

  18. Proceedings for the IEC/WG12 (4) 4thMeeting of WG12: －Date: on August 20, 2008 at Chicago, USA －Discussion on the submitted 1st WD and preparation for CDV 5thMeeting of WG12 : －Date: on October 29, 2008 at Tsukuba, Japan －Discussion on the submitted 1st WD and preparation for CDV

  19. Results of Voting on CDV P-members voting: 9 P-members in favour: 9 = 100 % >= 67% APPROVED Total votes cast: 11 Total against: 0 = 0 % <= 25% APPROVED Final Decision: APPROVED

  20. Comment on CDV(1)

  21. Comment on CDV(2)

  22. Results of Voting on Fdis P-members voting: 10 P-members in favour: 10 = 100 % >= 67% APPROVED Total votes cast: 11 ] Total against: 0 = 0 % <= 25% APPROVED Final Decision: APPROVED

  23. FDIS INTERNATIONAL ELECTROTECHNICAL COMMISSION ____________ SUPERCONDUCTIVITY – Part 14: Superconducting power devices – General requirements for characteristic tests of current leads designed for powering superconducting devices

  24. FDIS CONTENTS FOREWARD 4 INTRODUCTION 6 1. Scope 7 2. Normative references 7 3. Terms and definitions 7 4. Principles 8 5. Characteristic test items 9 6. Characteristic test methods 10 7. Reporting 15 8. Precautions 15 Annex A (Informative) Supplementary Information Relating to Chapters 1 to 8 17 Annex B (Informative) Typical current leads 19 Annex C (Informative) Explanation figures to help understanding of test methods 23 Annex D (Informative) Test items and methods for HTS component 26 Bibliography 28

  25. Current leads are indispensable components of superconducting devices in practical uses such as MRI diagnostic equipments, NMR spectrometers, single crystal growth devices, SMES, particle accelerators such as Tevatron, HERA, RHIC and LHC, experimental test instruments for nuclear fusion reactors, such as ToreSupra, TRIAM, LHD, EAST, KSTAR, W7-X, JT-60SA and ITER, etc. and of advanced superconducting devices in the near future in practical uses such as magnetic levitated trains, superconducting fault current limiters, superconducting transformers, etc. INTRODUCTION(1)

  26. The major functions of current leads are to power high currents into superconducting devices and to minimize the overall heat load, including heat leakage from room temperature to cryogenic temperature and Joule heating through current leads. For this purpose, current leads are dramatically effective for lowering the overall heat load to use the high temperature superconducting component as a part of the current leads.  This sentence is not understandable. INTRODUCTION(2)

  27. On the other hand, the current lead technologies applied to superconducting devices depend on each application, as well as on the manufacturer's experience and accumulated know-how. Due to their use as component parts, it is difficult to judge the compatibility, flexibility between devices, convenience, overall economical efficiency, etc of current leads. This may impede progress in the growth and development of superconducting equipment technology and its application to commercial activities, which is a cause for concern. INTRODUCTION(3)

  28. Consequently, it is judged industrially effective to clarify the definition of current leads to be applied to superconducting devices and to standardize the common characteristic test methods in a series of general rules. INTRODUCTION(4)

  29. The powering of superconducting equipment is made via components that provide the electrical link between the room temperature environment and the cryogenic temperature of the powered equipment. These components are called current leads. Since they operate in a gradient of temperature and they transport current into the cryogenic environment, they are one of the major sources of a heat leakage into the cryostat. 4. Principles(1)

  30. The current leads can be classified into two types: • normal conducting current leads, made entirely from normal conducting section. These are usually joined at their cold end to a superconducting (SC) bus or link leading to the device being powered; • high temperature superconducting (HTS) current leads, which incorporate a section of HTS material. A normal conducting section is necessary to conduct the current from room temperature to the warm end of the HTS section. The latter must be maintained at a sufficiently low temperature to ensure that it remains superconducting for the maximum rated current of the lead. The cold end of the HTS section is usually joined to the device by a SC bus.. 4. Principles(2)

  31. Depending on the cooling method, the leads can be either non-gas-cooled or gas-cooled. Both types of cooling methods can be used if the lead is subdivided into two, hydraulically separated, sections. If the device being powered uses low temperature superconducting (LTS) material, the link to the lead is usually via LTS cable or wires. 4. Principles(3)

  32. Optimized, self-cooled normal conducting current leads conduct into the helium bath 1,1 W/kA [1]) to 1,2 W/kA [2]. This value can be reduced substantially by using HTS material. HTS current leads have been extensively studied, designed and tested, and are already being integrated into large scale systems [3] [4]. 4. Principles(4)

  33. The design of a current lead is uniquely linked to the system within which it has to operate. The choice of materials, the cooling method, the geometry, the electrical characteristics and the admissible cryogenic consumptions are strongly influenced by boundary conditions imposed by the whole system. System requirements are electrical, cryogenic, and mechanical, and include the following: 4. Principles(5)

  34. maximum operating current, operation mode, current ramp rate, insulation voltage, circuit time constant, ambient magnetic fields; • cryogen availability, cryogen inlet/outlet temperature and pressure, admissible heat loads, time duration when the lead shall operate safely in case of failure of cryogen supply; • the volume available for integration, including mechanical support, vacuum insulation, and connection to the hydraulic and electrical interfaces. • NOTE 1 The heat leakage for self-cooled current leads should make use of 1,2 W/kA in the case of large current capacities. • NOTE 2 Typical current leads based on these principles are shown in Annex B. 4. Principles(6)

  35. The following chapters describe the qualification tests that should be performed on a current lead at both room and cryogenic temperatures in order to verify its mechanical, electrical and thermal performance. It is assumed that the design of the current lead has been carried out in consideration of general versatility. Before application to an actual system, it is also necessary to do the optimization of the current lead according to the constraints imposed by each system. The characteristic test items shown in Table 1 should enable the user to verify if the current lead meets the specified requirements, and to judge if the test items meet the execution stage of the current lead. It is in the responsibility of the user of this standard to select the appropriate tests according to Table 1 considering the boundary conditions of the current leads. 5. Characteristic test items

  36. Table 1 – Characteristic test items and test execution stages for current leads

  37. 6.1 Structure inspection 6.1.1 Purpose This test shall inspect dimensions, applicable materials, structure, structural state and so on as well as the thermal insulation property and leak tightness of the container in the target system. 6.1.2 Methods The structure inspection test at room temperature shall inspect dimensions, applicable materials, structure, structural state and so on. The structure inspection test at low temperature shall inspect visually the state of frost forming on the surface of a cryostat filled with cryogen or connected to a refrigerator. As for cryostats with the vacuum thermal insulating layer, it shall be confirmed that there is no malfunction in the layer such as tears and/or collapsing. 6.1.3 Results Test results shall be collated with the specifications and fully reported. 6. Characteristic test methods

  38. The following data shall be reported: – the outline of current leads; – the test conditions; – characteristic test results collating to the specifications; – the findings acquired through them. 7. Reporting

  39. Prior to the characteristic tests, make sure that test designers and persons involved are reminded of the following. a) Electrical tests The preventive means and countermeasure for electrical hazards shall be taken with room-temperature electrical tests and low-temperature electrical tests in mind. b) Cryogen and generated gas On low-temperature tests, the preventive means and countermeasure for electrical hazards shall be taken relating to gas replacement, cryogen injection, cryogenic leakage, physical contact with cryogen, constantly-generated gas and intentionally-generated gas. The cryogenic tests shall be based on the local legal regional laws. 8. Precautions

  40. (informative) Supplementary information relating to Clauses 1 to 8 A.1 Scope As applicable materials for superconducting current leads, in addition to the high-temperature copper oxide superconductors specified in this standard, superconductors such as MgB2, Nb3Sn, Nb-Ti may be applicable depending on designed temperatures. A.2 Current lead structure A.2.1 Normal conducting current lead (conventional current lead) The conducting parts of this current lead are made of normal conducting material, including additional connecting terminals or reinforcing material at both ends. A.2.2 Superconducting current lead The conducting parts of this current lead are made of normal conducting material in the high temperature region. The conducting components in the intermediate and low temperature region are superconducting material, HTS or LTS, as required by the design temperature. NOTE There may be other definitions of terms of temperature ranges. Annex A

  41. Typical current leads B.1 General The schematic diagrams shown in the figures of this annex are provided to facilitate understanding of typical current leads. Because the current leads take various configurations according to the target system and the operational environment, these diagrams only cover a representative sample of possible designs. B.2 Gas cooled type current leads B.3 Non-gas-cooled type current lead Annex B

  42. B.2.1 Self-cooled normal conducting current leads

  43. B.2.2 Forced flow cooled normal conducting current leads

  44. B.2.3 Current leads composed of forced flow cooled normal conducting section and HTS section in vacuum environment

  45. B.2.4 Current leads composed of forced flow cooled normal conducting section and HTS section in GHe environment

  46. B.2.5 Current leads composed of LN2/GN2 cooled normal conducting section and self-sufficient evaporated helium cooled HTS section

  47. B.3.1 Current leads composed of conduction cooled normal conducting section and HTS section

  48. Annex C Explanation figures to facilitate understanding of test methods Annex D Test items and methods for a HTS component ANNEX C, D

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