JPH0531491B2 - - Google Patents

Info

Publication number
JPH0531491B2
JPH0531491B2 JP62200927A JP20092787A JPH0531491B2 JP H0531491 B2 JPH0531491 B2 JP H0531491B2 JP 62200927 A JP62200927 A JP 62200927A JP 20092787 A JP20092787 A JP 20092787A JP H0531491 B2 JPH0531491 B2 JP H0531491B2
Authority
JP
Japan
Prior art keywords
film
superconducting
base material
temperature
superconducting material
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
JP62200927A
Other languages
Japanese (ja)
Other versions
JPS6445014A (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 JP62200927A priority Critical patent/JPS6445014A/en
Publication of JPS6445014A publication Critical patent/JPS6445014A/en
Publication of JPH0531491B2 publication Critical patent/JPH0531491B2/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、厚皮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、基材を500℃から980℃の温度に加
熱しながら、前記基材の表面上に、CuxOy基を含
む複合酸化物超電導物質の皮膜を形成させ、この
ようにして得られた、前記温度に加熱された、前
記基材と前記皮膜とからなる超電導素材を20℃/
min以下の冷却速度で冷却し、かくして、前記皮
膜に所定の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、基材2の表面上に、Y−Ba−Cu−O系等
の酸化物からなる超電導物質の皮膜3を形成させ
る。なお、溶射装置1は、プラズマ溶射以外の、
例えば、ガス溶射等であつてもよい。 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をヒーター9と共に設置し、
基材2をヒーター9によつて、500から980℃の温
度に加熱しながら、真空容器4内を減圧し、 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からなる超
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と電極6との間にプラズマアー
クを発生させる。 このようにして、基材2の表面上に超電導物質
からなる皮膜3が形成された超電導素材8を得た
ら、ヒーター9による加熱温度を徐々に下げ、且
つ、真空容器4内を酸素含有雰囲気に維持して、
超電導材8を20℃/min以下の冷却速度で徐冷す
る。 このように、基材2を加熱しながら超電導物質
の粉末を溶射すると、溶融粉末同士および基材2
と皮膜3との密着性が良くなる。同時に、皮膜中
の残留応力が低減し、皮膜中の微小クラツクの発
生を抑制できる。そして、酸素含有雰囲気下で、
超電導素材8を徐冷すると、超電導素材8の結晶
構造が斜方晶になり、超電導現象が十分に現われ
る。 ここで、基材加熱温度を500〜980℃としたの
は、500℃未満では、皮膜粒子の結合力、密着力
が劣ること、皮膜の割れ発生の危険性が高まるこ
と、および、結晶中の酸素欠損量が過大になり、
所定の結晶構造を得ることが難しくなるためであ
る。また、基材温度が980℃を超えると、基材に
付着した溶融粒子の凝固が遅れ、皮膜形状が劣化
する他、凝固割れ、結晶構造(相分離等)などの
問題が生じる。 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。 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、ヒーター9
によつて基材2を600℃に加熱しながら、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、Y0.3Ba0.7Cu1O3-yからなる超電動
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,ヒーター9による加
熱温度を徐々に下げ、且つ、真空容器4内に空気
を導入し、10℃/minの冷却速度で室温まで徐冷
して、板状超電導材を製造した。 次に、ヒーター9による基材2の加熱温度を
800℃に変えた以外は、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から試験片
(基材厚:2mm、皮膜厚:0.15mm、幅:5mm、長
さ:50mm)を切り出し、これを液体窒素(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
つた。この結果を、基材加熱温度との関係で整理
して第1表に示す。 基材を加熱しない場合(基材温度:室温に相
当)には、液体窒素温度(77K)において、超電
導現象は認められなかつた。皮膜粒子間の結合
性、密着性および皮膜中微小クラツクなどの存在
によるものと考えられる。
[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 amplification, etc., and if these are put into full-scale practical use, they will have great 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. Mu¨ller 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.Additionally, the film formation rate is slow and it takes a long time to form a 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] The present invention provides a method of applying a composite oxide superconducting material containing a Cu x O y group onto the surface of the base material while heating the base material to a temperature of 500°C to 980°C. A superconducting material made of the base material and the film, heated to the temperature described above, was heated at 20°C/20°C.
The film is characterized in that it is cooled at a cooling rate of less than min, thereby imparting predetermined superconducting properties to the film. 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, a film 3 of a superconducting material made of an oxide such as Y--Ba--Cu--O is formed on the surface of a base material 2. Note that the thermal spraying apparatus 1 is capable of other than plasma spraying.
For example, gas spraying or the like may be used. 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 a vacuum container 4, facing a thermal spray nozzle 5, together with a heater 9.
While heating the base material 2 to a temperature of 500 to 980°C with the heater 9, the pressure inside the vacuum vessel 4 is reduced, and a working gas such as argon or helium and a composite containing Cu x O y groups are injected into the thermal spray nozzle 5. Powder (10 to 100 μm) of a superconducting material made of oxide is continuously supplied, and the plasma power supply 7 is activated to generate a plasma arc between the thermal spray nozzle 5 and the electrode 6. After obtaining the superconducting material 8 in which the film 3 made of the superconducting substance is formed on the surface of the base material 2 in this way, the heating temperature by the heater 9 is gradually lowered, and the inside of the vacuum container 4 is made into an oxygen-containing atmosphere. maintain,
The superconducting material 8 is gradually cooled at a cooling rate of 20° C./min or less. In this way, when the superconducting material powder is thermally sprayed while heating the base material 2, the molten powder and the base material 2
The adhesion between the film and the film 3 is improved. At the same time, residual stress in the film is reduced, and the occurrence of microcracks in the film can be suppressed. Then, under an oxygen-containing atmosphere,
When the superconducting material 8 is slowly cooled, the crystal structure of the superconducting material 8 becomes orthorhombic, and the superconducting phenomenon is fully exhibited. Here, the base material heating temperature was set at 500 to 980°C because below 500°C, the bonding force and adhesion of the coating particles will be poor, the risk of cracking of the coating will increase, and the The amount of oxygen deficiency becomes excessive,
This is because it becomes difficult to obtain a predetermined crystal structure. Furthermore, if the substrate temperature exceeds 980° C., the solidification of the molten particles attached to the substrate will be delayed, the film shape will deteriorate, and problems such as solidification cracking and crystal structure (phase separation, etc.) will occur. 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. Next, embodiments of the invention will be described. Vacuum vessel 4 of plasma spraying apparatus 1 shown in FIG.
A plate-shaped base material 2 made of copper is set inside the heater 9.
While heating the base material 2 to 600°C using
is continuously supplied into the thermal spray nozzle 5, and a power of 15 Kw is supplied from the plasma power source 7 between the thermal spray nozzle 5 and the electrode 6 to generate a superelectric material powder consisting of Y 0.3 Ba 0.7 Cu 1 O 3-y. (particle size 10 to 100μm) spray nozzle 5
and 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 made of Manufactured. Next, set the heating temperature of the base material 2 by the heater 9.
Another plate-shaped superconducting material was manufactured under the same conditions as in the above-mentioned example except that the temperature was changed to 800°C. A test piece (base material thickness: 2 mm, film thickness: 0.15 mm, width: 5 mm, length: 50 mm) was cut out from the superconducting material produced in this way, and it was heated in liquid nitrogen (77K).
The critical current density (Jc) was examined using a four-terminal resistance measurement method. In addition, the critical temperature (Tc) was similarly measured using the four-terminal resistance measurement method. The results are summarized in Table 1 in relation to the substrate heating temperature. When the substrate was not heated (substrate temperature: equivalent to room temperature), no superconducting phenomenon was observed at liquid nitrogen temperature (77K). This is thought to be due to the bonding and adhesion between film particles and the presence of microcracks in the film.

【表】 第1表から明らかなように、本発明法によれば
基材加熱によつて皮膜3の結晶構造及び酸素量の
制御が図られるため、(Jc)の値が溶射ままの場
合に比べて著しく大きくなることがわかつた。X
線回折結果から皮膜の結晶構造は斜方晶から成る
ことが確認された。 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:0.15mm、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 and oxygen content of the coating 3 are controlled by heating the base material, so that when the value of (Jc) remains as sprayed, It was found that it was significantly larger. X
The line diffraction results confirmed that the crystal structure of the film was orthorhombic. 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: 0.15 mm, 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。さらに基材を加熱す
ることによつて超電導材の粒子同志が強固にな
り、緻密性が向上する他、皮膜の微小割れを抑制
することができるために、(Jc)の値が大きくな
ると共に、皮膜の強度が高くなるといつたきわめ
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 heating the base material, the particles of the superconducting material become stronger, improving the density, and suppressing microcracks in the film, which increases the value of (Jc) and Increasing the strength of the coating has several very beneficial effects.

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

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、9……ヒーター。
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, 9... Heater.

Claims (1)

【特許請求の範囲】[Claims] 1 基材を500℃から980℃の温度に加熱しなが
ら、前記基材の表面上に、CuxOy基を含む複合酸
化物超電導物質の皮膜を形成させ、このようにし
て得られた、前記温度に加熱された、前記基材と
前記皮膜とからなる超電導素材を20℃/min以下
の冷却速度で冷却し、かくして、前記皮膜に所定
の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. While heating the base material to a temperature of 500 ° C. to 980 ° C., a film of a composite oxide superconducting material containing Cu x O y groups is formed on the surface of the base material, and thus obtained, A superconductor, characterized in that a superconducting material consisting of the base material and the film heated to the temperature is cooled at a cooling rate of 20°C/min or less, thereby imparting predetermined superconducting properties to the film. Method of manufacturing wood.
JP62200927A 1987-08-13 1987-08-13 Manufacture of superconductive material Granted JPS6445014A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62200927A JPS6445014A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62200927A JPS6445014A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Publications (2)

Publication Number Publication Date
JPS6445014A JPS6445014A (en) 1989-02-17
JPH0531491B2 true JPH0531491B2 (en) 1993-05-12

Family

ID=16432596

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62200927A Granted JPS6445014A (en) 1987-08-13 1987-08-13 Manufacture of superconductive material

Country Status (1)

Country Link
JP (1) JPS6445014A (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0753639B2 (en) * 1987-06-11 1995-06-07 住友電気工業株式会社 Method for producing thin film made of oxide superconducting material

Also Published As

Publication number Publication date
JPS6445014A (en) 1989-02-17

Similar Documents

Publication Publication Date Title
Lian et al. The properties of YBCO superconductors prepared by a new approach: the'powder melting process'
JPH0534292B2 (en)
JPH0531491B2 (en)
JPH0534287B2 (en)
JPH0531493B2 (en)
JPH0531492B2 (en)
JPH0534288B2 (en)
JPH0531490B2 (en)
JPH0534290B2 (en)
Kumakura et al. BiSrCaCuO/Ag superconducting composite tapes
JPH0453819B2 (en)
JPH0431021B2 (en)
JPH0559861B2 (en)
JPH0534291B2 (en)
JPH0453818B2 (en)
KR920001675B1 (en) Superconducting Goods
Shibutani et al. Fabrication of silver-sheathed Bi (2: 2: 1: 2) superconducting magnet by means of partial melt and slow cooling process
JPH0453820B2 (en)
Kao et al. A study of Bi-Pb-Sr-Ca-Cu-O/Ag tape prepared by the jelly-roll process
Ashworth et al. Electrical contacts to YBCO using metal spray techniques
Gélinas et al. Texturing of thick films on a metallic substrate
JPH01153521A (en) Method for manufacturing superconducting materials
JPH01257128A (en) Method for manufacturing superconducting materials
JPH02196054A (en) Production of superconducting material
JPH0534289B2 (en)