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JPH0534291B2 - - Google Patents
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JPH0534291B2 - - Google Patents

Info

Publication number
JPH0534291B2
JPH0534291B2 JP62331101A JP33110187A JPH0534291B2 JP H0534291 B2 JPH0534291 B2 JP H0534291B2 JP 62331101 A JP62331101 A JP 62331101A JP 33110187 A JP33110187 A JP 33110187A JP H0534291 B2 JPH0534291 B2 JP H0534291B2
Authority
JP
Japan
Prior art keywords
superconducting
superconducting material
film
superconducting film
particles
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP62331101A
Other languages
Japanese (ja)
Other versions
JPH01172219A (en
Inventor
Kyoji Tachikawa
Yukio Shinho
Minoru Matsuda
Makoto Kabasawa
Shigechika Kosuge
Itaru Watanabe
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Tokai University
JFE Engineering Corp
Original Assignee
Tokai University
Nippon Kokan Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Tokai University, Nippon Kokan Ltd filed Critical Tokai University
Priority to JP62331101A priority Critical patent/JPH01172219A/en
Publication of JPH01172219A publication Critical patent/JPH01172219A/en
Publication of JPH0534291B2 publication Critical patent/JPH0534291B2/ja
Granted legal-status Critical Current

Links

Classifications

    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Landscapes

  • Inorganic Compounds Of Heavy Metals (AREA)
  • Coating By Spraying Or Casting (AREA)
  • Superconductor Devices And Manufacturing Methods Thereof (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、超電導材の製造方法に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a method for manufacturing a superconducting material.

〔従来技術及びその問題点〕[Prior art and its problems]

超電導物質は、既に高エネルギー粒子加速器、
医療診断用MRI−CT物性研究装置等において、
超電導マグネツトの形で実用化されている。ま
た、発電機、エネルギーの貯蔵や変換、リニアモ
ーターカー、資源回収用磁気分離装置、核融合
炉、送電ケーブル、磁気シールド材等への応用、
さらには、ジヨセフソン効果を用いた超電導素子
は、超高速コンピユーター、赤外線検出器、低雑
音の増幅器等への応用が期待されており、これら
が本格的に実用化された場合の産業的、社会的イ
ンパクトの大きさは、未だ測りがたい。
Superconducting materials are already used in high-energy particle accelerators,
In MRI-CT physical property research equipment for medical diagnosis, etc.
It has been put into practical use in the form of superconducting magnets. Applications include generators, energy storage and conversion, linear motor cars, magnetic separation devices for resource recovery, nuclear fusion reactors, power transmission cables, magnetic shielding materials, etc.
Furthermore, superconducting elements using the Josephson effect are expected to be applied to ultra-high-speed computers, infrared detectors, low-noise amplifiers, etc., and if these are put into full-scale practical use, they will have significant industrial and social impact. The magnitude of the impact is still difficult to measure.

これまでに開発された超電導物質の代表的なも
のとして、Nb−Ti合金があり、これは、現在9T
までの磁界発生用線材として広く使用されてい
る。Nb−Ti合金のTc(超電導状態が存在する臨
界温度)は、9Kである。また、Nb−Ti合金より
も格段に高いTcを有する材料として化合物系超
電導物質が開発され、現在Nb3Sn(Tc:18K)V3
Ga(Te:15K)が線材化され実用に供せられてい
る。さらに、Nb3Geでは23KのTcが得られてい
る。
A typical superconducting material developed so far is Nb-Ti alloy, which is currently 9T
It is widely used as a wire for generating magnetic fields. The Tc (critical temperature at which a superconducting state exists) of the Nb-Ti alloy is 9K. In addition, compound-based superconducting materials have been developed as materials with Tc much higher than Nb-Ti alloys, and currently Nb 3 Sn (Tc: 18K) V 3
Ga (Te: 15K) has been made into wire and put into practical use. Furthermore, a Tc of 23K has been obtained with Nb 3 Ge.

このように長年に亘つて高Tc超電導物質を得
るための努力がなされてきたが、従来の合金系お
よび化合物系超電導物質においては、Tc 23Kが
大きな壁になつている。Tcが23K以下の超電導
物質の冷却には、高価な液体ヘリウムが必要であ
り、このことが超電導物質の広範な応用を阻害し
ている。このTcの壁を打破する材料として、
1986年にIBMチユーリツヒのMu¨ller氏等が、Ba
−La−Cu−O系の酸化物で超電導の徴候が認め
られたと発表して以来、酸化物系超電導物質の開
発競争に拍車がかかつた。1986年にはTc 40Kで
あつたものが、1987年の初には、早くも77Kの液
体窒素温度を超えるY−Ba−Cu−O系超電導物
質が開発され、Tcは約93Kに達した。さらに、
その後も精力的な開発が続けられており、今のと
ころ安全性等に問題はあるものの室温で超電導現
象を示す超電導物質の開発も報告されている。液
体窒素温度で使用可能な高温超電導物質の発見
は、前述した応用分野への期待度を増々高めるも
のであるが、Jc(臨界電流密度)の値が高い超電
導材を容易に製造することができる方法は、まだ
提案されていない。
As described above, efforts have been made for many years to obtain high Tc superconducting materials, but Tc 23K has become a major barrier in conventional alloy-based and compound-based superconducting materials. Cooling superconducting materials with Tc below 23 K requires expensive liquid helium, which hinders their widespread application. As a material to break down this Tc wall,
In 1986, Mr. Mu¨ller of IBM Zurich et al.
Since the announcement that signs of superconductivity were observed in -La-Cu-O-based oxides, the race to develop oxide-based superconducting materials has accelerated. In 1986, the Tc was 40K, but in early 1987, Y-Ba-Cu-O superconducting materials were developed that exceeded the liquid nitrogen temperature of 77K, and the Tc reached approximately 93K. moreover,
Since then, vigorous development has continued, and the development of superconducting materials that exhibit superconductivity at room temperature has been reported, although there are currently safety issues. The discovery of high-temperature superconducting materials that can be used at liquid nitrogen temperatures has raised expectations for the aforementioned application fields, and superconducting materials with high Jc (critical current density) values can be easily manufactured. No method has yet been proposed.

従つて、この発明の目的は、Jcの値が高い超電
導材を容易に製造することができる方法を提供す
ることにある。
Therefore, an object of the present invention is to provide a method by which a superconducting material having a high Jc value can be easily produced.

〔問題点を解決するための手段〕[Means for solving problems]

この発明は、基材の表面上に、CuxOy基を含む
複合酸化物超電導物質からなる粒子を溶射して、
前記表面上に超電導皮膜を形成し、このようにし
て得た超電導素材を加熱しながらこれに圧下力を
付与し、かくして、前記超電導皮膜の粒子の結晶
面のうち通電性に優れた結晶面を、前記超電導皮
膜の面と平行に揃えることに特徴を有するもので
ある。
This invention involves thermally spraying particles made of a composite oxide superconducting material containing Cu x O y groups onto the surface of a base material.
A superconducting film is formed on the surface, and a rolling force is applied to the thus obtained superconducting material while heating it, and in this way, among the crystal planes of the particles of the superconducting film, the crystal planes having excellent electrical conductivity are , is characterized in that it is aligned parallel to the surface of the superconducting film.

次に、この発明の一実施態様の、超電導材の製
造方法を図面を参照しながら説明する。
Next, a method for manufacturing a superconducting material according to an embodiment of the present invention will be described with reference to the drawings.

第1図は、基材の表面上に超電導皮膜を形成す
るためのプラズマ溶射装置の断面図、第2図は、
この発明の方法の一実施態様を示す正面図であ
る。
FIG. 1 is a cross-sectional view of a plasma spraying apparatus for forming a superconducting film on the surface of a base material, and FIG.
FIG. 1 is a front view showing one embodiment of the method of the present invention.

この発明は、先ず、第1図に示すプラズマ溶射
装置によつてCu等からなる基材1の表面上に、
CuxOy基を含む複合酸化物超電導物質からなる粉
末を溶射する。プラズマ溶射装置は、真空容器2
と、真空容器2内に設けられた溶射ノズル3と、
溶射ノズル3内に設けられた電極4と、溶射ノズ
ル3と電極4との間に接続された電源5とからな
つている。
This invention first involves spraying onto the surface of a base material 1 made of Cu or the like using a plasma spraying apparatus shown in FIG.
A powder made of a composite oxide superconducting material containing Cu x O y groups is thermally sprayed. The plasma spraying equipment is a vacuum vessel 2
and a thermal spray nozzle 3 provided in the vacuum container 2,
It consists of an electrode 4 provided within the thermal spray nozzle 3 and a power source 5 connected between the thermal spray nozzle 3 and the electrode 4.

真空容器2内に基材1を、溶射ノズル3と対向
して取り付け、真空容器2内を減圧し、溶射ノズ
ル3の後端部内にアルゴン、ヘリウム等の作動ガ
スを供給し、溶射ノズル3の先端部内に、CuxOy
基を含む複合酸化物超電導物質からなる粉末を供
給し、そして、電源5を作動させて、溶射ノズル
3と電極4との間にプラズマアークを発生させ
る。これによつて、基材1の表面上に、CuxOy
を含む複合酸化物超電導物質からなる超電導皮膜
6が形成される。
The base material 1 is installed in a vacuum vessel 2 facing the thermal spray nozzle 3, the pressure inside the vacuum vessel 2 is reduced, and a working gas such as argon or helium is supplied into the rear end of the thermal spray nozzle 3. Inside the tip, Cu x O y
A powder made of a composite oxide superconducting material containing a group of 100% is supplied, and a power source 5 is activated to generate a plasma arc between the thermal spray nozzle 3 and the electrode 4. As a result, a superconducting film 6 made of a composite oxide superconducting material containing Cu x O y groups is formed on the surface of the base material 1 .

次に、このようにして、基材1と超電導皮膜6
とからなる超電導素材7を得たら、第2図に示す
ように、超電導素材7を加熱しながら、これに圧
下ロール8によつて圧下力を付与する。これによ
つて、圧下力を付与する前、即ち、溶射ままの状
態では、ランダムに入り組んでいた超電導皮膜6
の粒子の特定の結晶面が、超電導皮膜6と平行に
揃う。即ち、第3図に示すように、通電性が他の
面に比べて大幅に優れたab結晶面が、超電導皮
膜6の面と平行に揃う。これを粒子に配向性が付
与されたと云う。この結果、超電導皮膜7のJcの
値が増大する。
Next, in this way, the base material 1 and the superconducting film 6
Once the superconducting material 7 is obtained, as shown in FIG. 2, a rolling force is applied to the superconducting material 7 by a rolling roll 8 while heating the superconducting material 7. As a result, the superconducting film 6, which was randomly convoluted before applying the rolling force, that is, in the as-sprayed state,
The specific crystal planes of the particles are aligned parallel to the superconducting film 6. That is, as shown in FIG. 3, the ab crystal plane, which has much better electrical conductivity than other planes, is aligned parallel to the plane of the superconducting film 6. This is said to have imparted orientation to the particles. As a result, the value of Jc of the superconducting film 7 increases.

〔実施例〕〔Example〕

次に、この発明の実施例について説明する。 Next, embodiments of the invention will be described.

第1図に示すプラズマ溶射装置によつて、Ni
基合金からなる基材1(厚み1.0mm、縦20mm、横
30mm)の表面上に、Y0.3Ba0.7Cu1O3-yからなる厚
み150μmの超電導皮膜6を形成した。即ち、第1
図に示すプラズマ溶射装置の真空容器2内に、
Cu製の板状基板1を設置し、作動ガスとしてア
ルゴンガスとヘリウムガスとの混合ガス(Ar:
20/min、He:40/min)を溶射ノズル3の
後端部内に連続的に供給し、プラズマ電源5から
溶射ノズル3と電極4との間に25KWの電力を供
給し、溶射ノズル3の前端部内に、粒径10から
100μmのY0.3Ba0.7Cu1O3-yからなる超電導物質の
粒子を供給し、そして、真空容器2内の気圧を80
ミリバールに減圧して、基材1の表面上に厚み
150μmの超電導皮膜6を形成した。
Using the plasma spraying equipment shown in Figure 1, Ni
Base material 1 made of base alloy (thickness 1.0 mm, length 20 mm, width
30 mm), a superconducting film 6 made of Y 0.3 Ba 0.7 Cu 1 O 3-y and having a thickness of 150 μm was formed. That is, the first
In the vacuum vessel 2 of the plasma spraying apparatus shown in the figure,
A plate-shaped substrate 1 made of Cu is installed, and a mixed gas of argon gas and helium gas (Ar:
20/min, He: 40/min) into the rear end of the thermal spray nozzle 3, and 25 KW of power is supplied from the plasma power source 5 between the thermal spray nozzle 3 and the electrode 4 to In the front end, from grain size 10
Particles of superconducting material consisting of Y 0.3 Ba 0.7 Cu 1 O 3-y with a diameter of 100 μm are supplied, and the atmospheric pressure inside the vacuum vessel 2 is set to 80 μm.
Apply a reduced pressure to millibar and deposit a thickness on the surface of substrate 1.
A superconducting film 6 of 150 μm was formed.

このようにして得た超電導素材7を800℃に加
熱しながら、第2図に示すように、圧下ロール8
によつて、超電導皮膜7の膜厚が75μmになるま
で超電導素材7に圧下を加えた。次いで、超電導
素材7を930℃の温度に30分間加熱した。
While heating the superconducting material 7 obtained in this way to 800°C, as shown in FIG.
The superconducting material 7 was compressed by the following steps until the thickness of the superconducting film 7 became 75 μm. Next, the superconducting material 7 was heated to a temperature of 930° C. for 30 minutes.

このようにして製造した超電導材をX線回折に
供して、超電導皮膜の粒子の配向性について調べ
た。この結果、溶射ままでは、超電導皮膜の粒子
の結晶面003のピークが、他の結晶面001,
002,004,005のピークに比べて非常に
高いのに対して、この発明の方法により製造した
超電導材においては、これら結晶面のピークはほ
ぼ同等であつた。このことは、超電導皮膜に粒子
配向性が生じたこと、即ち、超電導皮膜の粒子
の、通電性に優れたab形晶面が超電導材の面と
平行に揃つたことを意味する。
The superconducting material thus produced was subjected to X-ray diffraction to examine the orientation of particles in the superconducting film. As a result, the peak of the crystal plane 003 of the particles of the superconducting film is different from that of other crystal planes 001,
The peaks of these crystal planes were much higher than those of 002, 004, and 005, whereas in the superconducting material produced by the method of the present invention, the peaks of these crystal planes were almost the same. This means that particle orientation has occurred in the superconducting film, that is, the a-b crystal planes of the particles of the superconducting film, which have excellent electrical conductivity, are aligned parallel to the plane of the superconducting material.

次に、この発明の方法により製造した超電導材
のTcおよびJcについて調べた。この結果、本発
明超電導材のJcの値は、8000A/cm2であつたのに
対して、超電導素材に圧下を付与しない比較超電
導材のJcの値は、150A/cm2であり、Tcの値は、
何れも90.5Kであつた。
Next, the Tc and Jc of the superconducting material produced by the method of this invention were investigated. As a result, the value of Jc of the superconducting material of the present invention was 8000 A/cm 2 , whereas the value of Jc of the comparative superconducting material, which did not apply any reduction to the superconducting material, was 150 A/cm 2 . value is,
Both were 90.5K.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、この発明によれば、超電
導皮膜に圧下を加えることによつて、超電導皮膜
の粒子の、通電性に優れたab結晶面の方向が、
超電導皮膜の面と平行に揃うので、Jcの値が著し
く増大する。
As explained above, according to the present invention, by applying pressure to the superconducting film, the direction of the ab crystal plane of the particles of the superconducting film, which has excellent electrical conductivity, can be changed.
Since it is aligned parallel to the surface of the superconducting film, the value of Jc increases significantly.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、プラズマ溶射装置の断面図、第2図
は、この発明の方法の一実施態様を示す正面図、
第3図は、超電導皮膜の粒子の結晶面を示す説明
図である。図面において、 1……基材、2……真空容器、3……溶射ノズ
ル、4……電極、5……電源、6……超電導皮
膜、7……超電導素材、8……圧下ロール。
FIG. 1 is a sectional view of a plasma spraying apparatus, FIG. 2 is a front view showing an embodiment of the method of the present invention,
FIG. 3 is an explanatory diagram showing crystal planes of particles of a superconducting film. In the drawings, 1... Base material, 2... Vacuum container, 3... Thermal spray nozzle, 4... Electrode, 5... Power source, 6... Superconducting film, 7... Superconducting material, 8... Rolling down roll.

Claims (1)

【特許請求の範囲】[Claims] 1 基材の表面上に、CuxOy基を含む複合酸化物
超電導物質からなる粉末を溶射して、前記表面上
に超電導皮膜を形成し、このようにして得た超電
導素材を加熱しながらこれに圧下力を付与し、か
くして、前記超電導皮膜の粒子の結晶面のうち通
電性に優れた結晶面を、前記超電導皮膜の面と平
行に揃えることを特徴とする、超電導材の製造方
法。
1. On the surface of a base material, a powder made of a composite oxide superconducting material containing a Cu x O y group is thermally sprayed to form a superconducting film on the surface, and the superconducting material thus obtained is heated. A method for producing a superconducting material, which comprises applying a rolling force to the superconducting material, thereby aligning crystal planes with excellent electrical conductivity among the crystal planes of the particles of the superconducting film parallel to the plane of the superconducting film.
JP62331101A 1987-12-26 1987-12-26 Production of superconducting material Granted JPH01172219A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62331101A JPH01172219A (en) 1987-12-26 1987-12-26 Production of superconducting material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62331101A JPH01172219A (en) 1987-12-26 1987-12-26 Production of superconducting material

Publications (2)

Publication Number Publication Date
JPH01172219A JPH01172219A (en) 1989-07-07
JPH0534291B2 true JPH0534291B2 (en) 1993-05-21

Family

ID=18239870

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62331101A Granted JPH01172219A (en) 1987-12-26 1987-12-26 Production of superconducting material

Country Status (1)

Country Link
JP (1) JPH01172219A (en)

Also Published As

Publication number Publication date
JPH01172219A (en) 1989-07-07

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