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JPH0531490B2 - - Google Patents
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JPH0531490B2 - - Google Patents

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Publication number
JPH0531490B2
JPH0531490B2 JP62200926A JP20092687A JPH0531490B2 JP H0531490 B2 JPH0531490 B2 JP H0531490B2 JP 62200926 A JP62200926 A JP 62200926A JP 20092687 A JP20092687 A JP 20092687A JP H0531490 B2 JPH0531490 B2 JP H0531490B2
Authority
JP
Japan
Prior art keywords
film
superconducting
superconducting material
base material
temperature
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
JP62200926A
Other languages
Japanese (ja)
Other versions
JPS6445013A (en
Inventor
Kyoji Tachikawa
Minoru Matsuda
Yukio Shinho
Teruo Suzuki
Makoto Kabasawa
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 JP62200926A priority Critical patent/JPS6445013A/en
Publication of JPS6445013A publication Critical patent/JPS6445013A/en
Publication of JPH0531490B2 publication Critical patent/JPH0531490B2/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)
  • Superconductor Devices And Manufacturing Methods Thereof (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔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。 〔従来の技術およびその問題点〕 超電導材料は、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。 これまでに開発された超電導材料の代表的なも
のとして、Nb−Ti合金があり、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材料
が開発され、現在Nb3Sn(Tc:18K)とV3Ga
(Tc: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。 このように長年に亘つて高Tc超電導材料を得
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材料においては、Tc23Kが
大きな壁になつている。Tcが23K以下の超電導
材料の冷却には、高価な液体Heが必要であり、
このことが超電導材料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Muller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、酸化物系超電導材料の開発競争
に拍車がかかつた。1986年にはTc40K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系超電導材料が開
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
す超電導材料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材料の発見は、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、実際の応用化に当つては、線材化、皮膜化な
どの加工技術の開発が伴わなければならない。 〔発明が解決しようとする問題点〕 超電導物質を皮膜化するには、超電導物質を溶
射法や蒸着法によつて基材上に付与させることが
考えられるが、これらの方法によれば、安定して
形成できる皮膜の厚さはたかだか1μm程度であ
り、給電容量が制限されること、加えて皮膜形成
速度が小さく、所定の膜形成に多大の時間を要す
る等の問題が残されている。 この発明の目的は、厚被膜を安定に形成させ、
加えて大きな成膜速度で超電導物質からなる皮膜
を基材上に形成させることができる、超電導材の
製造方法を提供することにある。 〔問題点を解決するための手段〕 この発明は、基材の表面上に、溶射法によつて
CuxOy基を含む複合酸化物超電導物質の皮膜を形
成させ、次いで、このようにして得られた前記基
材と前記皮膜とからなる超電導素材を、酸素含有
雰囲気中において500℃から980℃の温度に加熱
し、次いで、20℃/min以下の速度で冷却し、か
くして、前記皮膜の結晶構造および酸素量を制御
することによつて、前記皮膜に超電導特性を付与
することに特徴を有するものである。 次に、この発明の、超電導材の製造方法の一実
施態様を図面を参照しながら説明する。 第1図は、この発明の、超電導材の製造方法の
一実施態様を示す断面図である。 第1図に示すようなプラズマ溶射装置1を使用
して、銅製基材2の表面上に、Y−Ba−Cu−O
系等のCuxOy基を含む複合酸化物超電導物質の皮
膜3を形成する。溶射装置1は、熱源としてプラ
ズマを用いるもの以外であつても良い。 プラズマ溶射装置1は、真空容器4と、真空容
器4内に設けられた溶射ノズル5と、溶射ノズル
5内に設けられたタングステン電極6と、溶射ノ
ズル5と電極6との間に接続されたプラズマ電源
7とからなつている。 真空容器4内に、溶射ノズル5と対向して板状
または棒状の基材2を設置し、真空容器4内のガ
スを吸引しながら、溶射ノズル5内にアルゴン、
ヘリウム等の作動ガスおよびCuxOy基を含む複合
酸化物超電導物質の粉末(10から100μm)をそれ
ぞれ連続的に供給し、そして、プラズマ電源7を
作動させて、溶射ノズル5から電極6に向けてプ
ラズマジエツトを発生させる。 このようにして、基材2と皮膜3とからなる超
電導素材8を得たら、次に、超電導素材8を酸素
含有雰囲気中において500から980℃の温度に加熱
し、この後、必要に応じて、超電導素材8を所定
時間、前記温度範囲に保持した後、超電導素材8
を20℃/min以下の速度で冷却する。 ここで、熱処理温度を500〜980℃としたのは、
500℃未満では、均質な斜方晶を得ることが難し
く、且つ、酸素欠損量が大きく、十分な超電導特
性を得ることが困難であり、一方、熱処理温度が
980℃を超えると、基材と皮膜とが反応し、皮膜
中に基材物質が侵入し、超電導特性を示さなくな
るためである。 また、冷却速度を20℃/min以下としたのは、
20℃/minを超える冷却速度においては、皮膜に
割れが生じる危険性が高まること、皮膜と基材が
ハクリし易いこと、および結晶中の酸素欠損量が
大きくなるためである。 このように、超電導素材8に熱処理を施こすの
は、次の理由による。 超電導素材8の溶融粒子が、溶射によつて基材
2の表面に付着すると、溶融粒子は直ちに冷却さ
れる。従つて、基材2の表面上に形成される皮膜
3の大部分の結晶構造は、高温度で安定な正方晶
に近い斜方晶となる。また、皮膜3の含有酸素量
も減少する。この結果、皮膜3に超電導現象が十
分に現われない。そこで、皮膜3を上述した温度
に加熱すると、もともと斜方晶になり易すい性質
を有する皮膜3の結晶構造が正方晶に近い斜方晶
から斜方晶に容易に変わる。これによつて、皮膜
3には完全に超電導現象が現われる。 次に、この発明の実施例について説明する。 第1図に示すプラズマ溶射装置1の真空容器4
内に、銅製の板状基材2をセツトし、プラズマガ
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5内に連続的に供給し、プラズマ電源7
から溶射ノズル5と電極6との間に15Kwの電力
を供給し、Y0.3−Ba0.7−Cu1−O3-yからなる超電
導物質の粉末(粒径10から100μm)を溶射ノズル
5内に供給し、そして、真空容器4内の気圧を
80mbarに減圧して、基材2の表面上に150μmの
膜厚を有する、超電導物質からなる皮膜3を形成
した。 次いで、このようにして得た、基材2と皮膜3
とからなる超電導素材8を真空容器4から取り出
し、超電導素材8を500℃の温度に加熱し、大気
中において、20℃/minの速度で室温まで冷却し
て、板状の超電導材を製造した。 次に、超電導素材8の加熱温度を800℃とした
以外は、上述した実施例と同一条件に従つて別の
板状超電導材を製造した。 このようにして製造した超電導材の試験片(基
材厚:2mm、皮膜厚:150μm、幅:5mm、長さ:
50mm)を液体窒素(77K)中に浸漬し、四端子抵
抗測定法によつて、臨界電流密度(Jc)について
調べた。また、臨界温度(Tc)の測定も同様に
四端子抵抗測定法により行なつた。この結果を、
超電導素材8に熱処理を施こさない場合、即ち、
溶射ままの場合と合わせて第1表に示す。なお、
溶射ままの場合、皮膜は超電導現象を示さなかつ
た。
[Industrial Field of Application] The present invention relates to a method for manufacturing a superconducting material. [Conventional technology and its problems] Superconducting materials have already been 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. Nb-Ti alloy is a typical superconducting material developed so far, and is currently widely used as a wire for generating magnetic fields up to 9T. Nb−
Tc of Ti alloy (critical temperature at which superconducting state exists)
is 9K. In addition, compound superconducting materials have been developed as materials with Tc much higher than Nb-Ti alloys, and currently Nb 3 Sn (Tc: 18K) and V 3 Ga
(Tc: 15K) has been made into wire and put into practical use. Furthermore, a Tc of 23K has been obtained with Nb 3 Ge. Although efforts have been made to obtain high Tc superconducting materials for many years, Tc23K has become a major barrier to conventional alloy-based and compound-based superconducting materials. Expensive liquid He is required to cool superconducting materials with Tc below 23K.
This hinders the widespread application of superconducting materials. In 1986, Mr. Muller of IBM Zurich and others proposed Ba-La-
Since the announcement that signs of superconductivity were observed in Cu-O-based oxides, the race to develop oxide-based superconducting materials has accelerated. In 1986, Tc was 40K, but in early 1987, a Y-Ba-Cu-O based superconducting material was developed that exceeded the liquid nitrogen temperature of 77K, and Tc reached approximately 93K. Furthermore, vigorous development has continued since then, and there have been reports of the development of superconducting materials that exhibit superconductivity at room temperature, 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, but for actual application, it is necessary to develop processing techniques such as wire rods and coatings. must be accompanied by [Problems to be solved by the invention] In order to form a film with a superconducting material, it is possible to apply the superconducting material onto a base material by a thermal spraying method or a vapor deposition method. The thickness of the film that can be formed using this method is approximately 1 μm at most, which limits the power supply capacity, and in addition, the film formation rate is slow and it takes a long time to form the desired film. The purpose of this invention is to form a thick film stably,
In addition, it is an object of the present invention to provide a method for producing a superconducting material that can form a film made of a superconducting material on a base material at a high film formation rate. [Means for Solving the Problems] This invention provides a method of spraying onto the surface of a base material by a thermal spraying method.
A film of a composite oxide superconducting material containing a Cu x O y group is formed, and then the superconducting material consisting of the base material and the film thus obtained is heated at 500°C to 980°C in an oxygen-containing atmosphere. The method is characterized in that superconducting properties are imparted to the film by heating the film to a temperature of It is something. Next, one embodiment of the method for manufacturing a superconducting material according to the present invention will be described with reference to the drawings. FIG. 1 is a sectional view showing one embodiment of the method for manufacturing a superconducting material according to the present invention. Using a plasma spraying apparatus 1 as shown in FIG. 1, Y-Ba-Cu-O
A film 3 of a composite oxide superconducting material containing a Cu x O y group such as a Cu x O y group is formed. The thermal spraying device 1 may be other than one that uses plasma as a heat source. The plasma spraying apparatus 1 includes a vacuum vessel 4, a thermal spray nozzle 5 provided in the vacuum vessel 4, a tungsten electrode 6 provided in the thermal spray nozzle 5, and connected between the thermal spray nozzle 5 and the electrode 6. It consists of a plasma power supply 7. A plate-shaped or rod-shaped base material 2 is placed in the vacuum container 4 facing the thermal spray nozzle 5, and while the gas in the vacuum container 4 is sucked, argon,
A working gas such as helium and a powder (10 to 100 μm) of a composite oxide superconducting material containing Cu x O y groups are each continuously supplied, and the plasma power supply 7 is activated to flow from the spray nozzle 5 to the electrode 6. Generates a plasma jet towards the enemy. After obtaining the superconducting material 8 consisting of the base material 2 and the film 3 in this way, the superconducting material 8 is heated to a temperature of 500 to 980°C in an oxygen-containing atmosphere, and then, if necessary, , after holding the superconducting material 8 in the temperature range for a predetermined time, the superconducting material 8
Cool at a rate of 20℃/min or less. Here, the heat treatment temperature was set at 500 to 980℃ because
At temperatures below 500℃, it is difficult to obtain homogeneous orthorhombic crystals, and the amount of oxygen vacancies is large, making it difficult to obtain sufficient superconducting properties.
This is because if the temperature exceeds 980°C, the base material and the film will react, the base material will penetrate into the film, and the superconducting property will no longer be exhibited. In addition, the cooling rate was set to 20℃/min or less because
This is because at a cooling rate exceeding 20°C/min, the risk of cracking in the film increases, the film and the base material tend to peel off, and the amount of oxygen vacancies in the crystal increases. The reason why the superconducting material 8 is heat-treated in this way is as follows. When the molten particles of the superconducting material 8 adhere to the surface of the base material 2 by thermal spraying, the molten particles are immediately cooled. Therefore, the crystal structure of most of the film 3 formed on the surface of the base material 2 is orthorhombic, which is stable at high temperatures and is close to tetragonal. Moreover, the amount of oxygen contained in the film 3 also decreases. As a result, the superconducting phenomenon does not sufficiently appear in the film 3. Therefore, when the film 3 is heated to the above-mentioned temperature, the crystal structure of the film 3, which originally has a tendency to form an orthorhombic crystal, easily changes from an orthorhombic crystal close to a tetragonal crystal to an orthorhombic crystal. As a result, the superconducting phenomenon completely appears in the film 3. Next, embodiments of the invention will be described. Vacuum vessel 4 of plasma spraying apparatus 1 shown in FIG.
A copper plate-shaped substrate 2 is set inside the spray nozzle 5, and a mixed gas of argon gas and helium gas (Ar: 20/min, He: 40/min) is continuously supplied as plasma gas into the thermal spray nozzle 5. and plasma power supply 7
A power of 15 Kw is supplied between the thermal spray nozzle 5 and the electrode 6 from Then, the atmospheric pressure inside the vacuum container 4 is
The pressure was reduced to 80 mbar, and a film 3 made of a superconducting material having a film thickness of 150 μm was formed on the surface of the base material 2. Next, the base material 2 and the film 3 obtained in this way
The superconducting material 8 consisting of . Next, another plate-shaped superconducting material was manufactured under the same conditions as in the above example except that the heating temperature of the superconducting material 8 was 800°C. Test piece of superconducting material manufactured in this way (base material thickness: 2 mm, film thickness: 150 μm, width: 5 mm, length:
50mm) was immersed in liquid nitrogen (77K), and the critical current density (Jc) was investigated using a four-terminal resistance measurement method. In addition, the critical temperature (Tc) was similarly measured using the four-terminal resistance measurement method. This result,
When the superconducting material 8 is not subjected to heat treatment, that is,
The results are shown in Table 1 together with the as-sprayed case. In addition,
When as-sprayed, the coating did not exhibit superconducting phenomena.

【表】 第1表から明らかなように、本発明法によれ
ば、熱処理によつて、皮膜3の結晶構造が正方晶
に近い斜方晶から均質な斜方晶に変るために、超
電導現象が明確に認められる。 次に、皮膜3の強度について調べた。これは、
第2図に示すように、超電導材の試験片(基準
厚:2mm、皮膜厚:150μm、幅:5mm、長さ50
mm)を三点曲げ試験に供し、皮膜3の割れ発生時
の試験片の曲げ角度によつて評価した。この結果
を、溶射ままの場合と合わせて第2表に示す。
[Table] As is clear from Table 1, according to the method of the present invention, the crystal structure of the film 3 changes from an orthorhombic crystal close to a tetragonal crystal to a homogeneous orthorhombic crystal due to the heat treatment, so that the superconducting phenomenon occurs. is clearly recognized. Next, the strength of the film 3 was examined. this is,
As shown in Figure 2, a test piece of superconducting material (standard thickness: 2 mm, film thickness: 150 μm, width: 5 mm, length 50
mm) was subjected to a three-point bending test, and evaluated based on the bending angle of the test piece when cracking occurred in the coating 3. The results are shown in Table 2 together with the as-sprayed case.

〔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、皮膜
を溶射法によつて形成することによつて、皮膜の
膜厚を厚くすることができ、しかも、皮膜を短時
間で形成することができる。さらに、皮膜を熱処
理することによつて、超電導材の粒子同士が強固
になり、同時に、結晶構造および結晶中酸素量を
適正化できるため、皮膜に超電導特性を付与する
ことができるといつたきわめて有用な効果がもた
らされる。
As explained above, according to the present invention, by forming the coating by thermal spraying, the thickness of the coating can be increased, and moreover, the coating can be formed in a short time. Furthermore, by heat-treating the film, the particles of the superconducting material become stronger, and at the same time, the crystal structure and the amount of oxygen in the crystals can be optimized, making it possible to impart superconducting properties to the film. Useful effects are produced.

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

第1図は、この発明の方法によつて、基材の表
面上に超電導物質からなる皮膜を形成している状
態様を示す断面図、第2図は、三点曲げ試験法を
示す正面図である。 図面において、1……プラズマアーク溶射装
置、2……基材、3……皮膜、4……真空容器、
5……溶射ノズル、6……電極、7……プラズマ
電源、8……超電導素材。
Figure 1 is a cross-sectional view showing how a film made of superconducting material is formed on the surface of a base material by the method of the present invention, and Figure 2 is a front view showing the three-point bending test method. It is. In the drawings, 1... plasma arc thermal spraying device, 2... base material, 3... film, 4... vacuum vessel,
5...Thermal spray nozzle, 6...Electrode, 7...Plasma power source, 8...Superconducting material.

Claims (1)

【特許請求の範囲】[Claims] 1 基材の表面上に、溶射法によつてCuxOy基を
含む複合酸化物超電導物質の皮膜を形成させ、次
いで、このようにして得られた、前記基材と前記
皮膜とからなる超電導素材を、酸素含有雰囲気中
において500℃から980℃の温度に加熱し、次い
で、20℃/min以下の速度で冷却し、かくして、
前記皮膜の結晶構造および酸素量を制御すること
によつて、前記皮膜に超電導特性を付与すること
を特徴とする、超電導材の製造方法。
1. A film of a composite oxide superconducting material containing a Cu x O y group is formed on the surface of a base material by a thermal spraying method, and then a film consisting of the base material and the film obtained in this way is formed. The superconducting material is heated to a temperature of 500°C to 980°C in an oxygen-containing atmosphere and then cooled at a rate of no more than 20°C/min, thus
A method for producing a superconducting material, characterized in that superconducting properties are imparted to the film by controlling the crystal structure and oxygen content of the film.
JP62200926A 1987-08-13 1987-08-13 Manufacture of superconductive material Granted JPS6445013A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62200926A JPS6445013A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62200926A JPS6445013A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Publications (2)

Publication Number Publication Date
JPS6445013A JPS6445013A (en) 1989-02-17
JPH0531490B2 true JPH0531490B2 (en) 1993-05-12

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP62200926A Granted JPS6445013A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Country Status (1)

Country Link
JP (1) JPS6445013A (en)

Also Published As

Publication number Publication date
JPS6445013A (en) 1989-02-17

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