JPH0534288B2 - - Google Patents

Info

Publication number
JPH0534288B2
JPH0534288B2 JP62229121A JP22912187A JPH0534288B2 JP H0534288 B2 JPH0534288 B2 JP H0534288B2 JP 62229121 A JP62229121 A JP 62229121A JP 22912187 A JP22912187 A JP 22912187A JP H0534288 B2 JPH0534288 B2 JP H0534288B2
Authority
JP
Japan
Prior art keywords
film
superconducting
base material
superconducting material
oxygen
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
JP62229121A
Other languages
Japanese (ja)
Other versions
JPS6472422A (en
Inventor
Kyoji Tachikawa
Shigechika Kosuge
Makoto Kabasawa
Minoru Matsuda
Yukio Shinho
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 JP62229121A priority Critical patent/JPS6472422A/en
Publication of JPS6472422A publication Critical patent/JPS6472422A/en
Publication of JPH0534288B2 publication Critical patent/JPH0534288B2/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】 〔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.

〔従来の技術およびその問題点〕[Conventional technology 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、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)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。
A typical superconducting material developed so far is Nb-Ti alloy, which 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-based 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.

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、Tc23K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He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、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。
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 as a material to break down this Tc wall.
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 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 superconducting phenomena at room temperature, although there are currently safety issues. The discovery of a high-temperature superconducting material that can be used at liquid nitrogen temperatures has raised expectations for the aforementioned application fields, but actual application requires the development of processing techniques such as wire rods and coatings. must be accompanied by

従来、上述した皮膜化に関しては、基材表面上
にスパツタリング法または電子ビーム蒸着法によ
つて酸化物超電導物質からなる皮膜を形成する方
法が試みられている。
Conventionally, with regard to the above-mentioned film formation, attempts have been made to form a film made of an oxide superconducting material on the surface of a base material by sputtering or electron beam evaporation.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかし、上述した従来法においては、安定して
形成できる皮膜の厚さは、たかだか1μm程度であ
るので給電容量が制限され、しかも、皮膜形成速
度が遅いために所定厚の膜形成に長時間を要す
る。
However, in the conventional method described above, the thickness of the film that can be stably formed is about 1 μm at most, which limits the power supply capacity, and the film formation speed is slow, so it takes a long time to form a film of a predetermined thickness. It takes.

この発明の目的は、厚皮膜を安定して且つ短時
間で形成でき、さらに、酸化物超電導物質の酸素
量を容易に制御することができる、超電導材の製
造方法を提供することにある。
An object of the present invention is to provide a method for producing a superconducting material, which allows a thick film to be formed stably and in a short period of time, and which also allows easy control of the amount of oxygen in an oxide superconducting material.

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

この発明は、基材の表面に向けて溶射法によつ
て、CuxOy基を含む複合酸化物超電導物質からな
る粉末を吹き付けて、前記表面に前記物質からな
る皮膜を形成し、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、700から980℃に所定
時間加熱し、徐冷後、同雰囲気中において、400
から600℃に所定時間加熱し、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特徴
を有するものである。
This invention sprays a powder made of a composite oxide superconducting material containing a Cu x O y group onto the surface of a base material by thermal spraying to form a film made of the material on the surface, and then: A superconducting material consisting of the base material and the film obtained in this way,
Heated at 700 to 980℃ for a specified time in an oxygen-containing atmosphere, cooled slowly, and heated to 400℃ in the same atmosphere.
The film is characterized in that it is heated to 600° C. for a predetermined period of time, thereby controlling the crystal structure and oxygen content of the film.

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。
Next, one embodiment of the method for manufacturing a superconducting material according to the present invention will be described with reference to the drawings.

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。
FIG. 1 is a sectional view showing one embodiment of the method for manufacturing a superconducting material according to the present invention.

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。なお、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。
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. Note that the thermal spraying apparatus 1 may be other than one that uses plasma as a heat source.

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。
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.

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内を減
圧しながら、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、前記粉
末をその体積の40〜100%溶融させて、基材2の
表面上に溶射する。
A plate-shaped or rod-shaped base material 2 is installed in a vacuum vessel 4 facing a thermal spray nozzle 5, and while the pressure inside the vacuum vessel 4 is reduced, a working gas such as argon or helium and Cu x O are injected into the thermal spray nozzle 5. Powder (10 to 100 μm) of a composite oxide superconducting material containing a y group is continuously supplied, and the plasma power source 7 is activated to generate a plasma jet from the spray nozzle 5 toward the electrode 6. In this way, the powder is melted to 40-100% of its volume and sprayed onto the surface of the substrate 2.

上述した溶射装置1によつて、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、700から980
℃の温度に所定時間加熱し、この後、20℃/min
以下の速度で400から600℃の温度まで冷却し、ま
たは、一旦室温まで冷却し、この後、400から600
℃の温度に再加熱し、この温度域に所定時間保持
後、室温まで徐冷する。
The base material 2 and the coating 3 are coated by the thermal spraying device 1 described above.
After obtaining the superconducting material 8 consisting of
℃ for a specified period of time, then 20℃/min.
Cool to a temperature of 400 to 600℃ at the following rate, or cool to room temperature once, then cool to a temperature of 400 to 600℃.
The sample is reheated to a temperature of 0.degree. C., maintained in this temperature range for a predetermined period of time, and then slowly cooled to room temperature.

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。
The reason why the superconducting material 8 is heat-treated in this way is as follows.

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、高温で安定な正方晶と
なる。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を上述した温度範囲、
即ち、700から980℃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(第
2図参照)。
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 tetragonal, which is stable at high temperatures. As a result, the superconducting phenomenon does not sufficiently appear in the film 3. Therefore, the temperature range of the film 3 mentioned above,
That is, when heated from 700 to 980° C., the crystal structure of the film 3, which originally tends to be orthorhombic, easily changes from tetragonal to orthorhombic. As a result, a superconducting phenomenon completely appears in the film 3 (see FIG. 2).

次に、超電導素材8を400から600℃の温度に所
定時間保持するのは、上述した前段の加熱によつ
て欠損した皮膜3中の酸素量を補なつて、超電導
現象を現出させるためである。第2図から明らか
なように、400から600℃の温度域において酸素吸
収量が特に多い。従つて、この温度域において、
加熱時間を調整すれば、皮膜中の酸素量を容易に
制御する。
Next, the reason why the superconducting material 8 is held at a temperature of 400 to 600°C for a predetermined period of time is to compensate for the amount of oxygen in the film 3 that has been lost due to the heating in the previous stage, and to make the superconducting phenomenon appear. be. As is clear from Figure 2, the amount of oxygen absorbed is particularly large in the temperature range of 400 to 600°C. Therefore, in this temperature range,
By adjusting the heating time, the amount of oxygen in the film can be easily controlled.

なお、冷却速度を20℃/min以下としたのは、
20℃/minを超えると皮膜に割れが生じる危険性
が高まること、皮膜が剥離しやすくなること、お
よび、皮膜中の酸素欠損量が大きくなるからであ
る。
In addition, the cooling rate was set to 20℃/min or less because
This is because if it exceeds 20°C/min, the risk of cracking in the film increases, the film becomes easier to peel off, and the amount of oxygen vacancies in the film increases.

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-x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。
Vacuum vessel 4 of plasma spraying apparatus 1 shown in FIG.
A copper plate-shaped base material 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.

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
して、大気中で900℃の温度に1時間保持し、こ
の後、20℃/minの速度で500℃の温度まで冷却
し、この温度に2時間保持し、次いで、室温まで
徐冷して、板状超電導材を製造した。
Next, the base material 2 and the film 3 obtained in this way
The superconducting material 8 consisting of The mixture was held and then slowly cooled to room temperature to produce a plate-shaped superconducting material.

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
測定も同様な測定法により行なつた。さらに、X
線回折によつて皮膜の結晶構造についても調べ
た。この結果、皮膜の結晶構造は斜方晶となつて
いて、Jcは80A/cm2,Tcは90Kであつた。
A test piece from the superconducting material produced in this way (base material thickness 2 mm, coating 0.15 mm, width 5 mm, length 50 mm)
This was cut out and immersed in liquid nitrogen (77K), and the critical current density (Jc) was examined by four-terminal resistance measurement method. The critical temperature (Tc) was also measured using a similar method. Furthermore, X
The crystal structure of the film was also investigated by line diffraction. As a result, the crystal structure of the film was orthorhombic, with Jc of 80A/cm 2 and Tc of 90K.

なお、マイスナー効果について調べたところ、
77Kでその効果が確認された。
Furthermore, when we investigated the Meissner effect, we found that
The effect was confirmed at 77K.

次に、皮膜の強度について調べた。これは、上
述した試験片と同一寸法の試験片を第3図に示す
三点曲げ試験に供し、皮膜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、試験片
を4.4度まで曲げても皮膜に割れは生じなかつた。
Next, the strength of the film was investigated. This was evaluated by subjecting a test piece having the same dimensions as the above-mentioned test piece to the three-point bending test shown in FIG. 3, and determining the bending angle of the test piece when cracking occurred in the film. As a result, no cracks occurred in the film even when the test piece was bent up to 4.4 degrees.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、超電導物質からなる厚皮
膜を基材上に安定して且つ短時間に形成でき、さ
らに、皮膜中の酸素量を容易に制御することがで
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, a thick film made of a superconducting substance can be stably formed on a substrate in a short time, and furthermore, the amount of oxygen in the film can be easily controlled, which is an extremely useful effect. brought about.

【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上に超
電導皮膜を形成している状態を示す断面図、第2
図は、温度と吸収酸素量および結晶構造との関係
を示すグラフ、第3図は、三点曲げ試験を示す正
面図である。 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。
FIG. 1 is a sectional view showing the state in which a superconducting film is formed on a base material by the method of the present invention, and FIG.
The figure is a graph showing the relationship between temperature, absorbed oxygen amount, and crystal structure, and FIG. 3 is a front view showing a three-point bending test. 1... Plasma arc thermal spraying device, 2... Base material,
3... Film, 4... Vacuum container, 5... Thermal spray nozzle, 6... Electrode, 7... Plasma power source, 8... Superconducting material.

Claims (1)

【特許請求の範囲】[Claims] 1 基材の表面に向けて溶射法によつて、CuxOy
基を含む複合酸化物超電導物質からなる粉末を吹
き付けて、前記表面に前記物質からなる皮膜を形
成し、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材を、酸素含有雰囲
気中において、700から980℃に所定時間加熱し、
徐冷後、同雰囲気中において、400から600℃に所
定時間加熱し、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を特徴とする、超電導
材の製造方法。
1 Cu x O y is applied onto the surface of the base material by thermal spraying.
A powder made of a composite oxide superconducting substance containing groups is sprayed to form a film made of the substance on the surface, and then the superconducting material made of the base material and the film thus obtained is exposed to oxygen. Heating at 700 to 980℃ for a specified period of time in a containing atmosphere,
1. A method for producing a superconducting material, which comprises heating the film at 400 to 600° C. for a predetermined time in the same atmosphere after slow cooling, thereby controlling the crystal structure and oxygen content of the film.
JP62229121A 1987-09-12 1987-09-12 Manufacture of superconducting wire Granted JPS6472422A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62229121A JPS6472422A (en) 1987-09-12 1987-09-12 Manufacture of superconducting wire

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62229121A JPS6472422A (en) 1987-09-12 1987-09-12 Manufacture of superconducting wire

Publications (2)

Publication Number Publication Date
JPS6472422A JPS6472422A (en) 1989-03-17
JPH0534288B2 true JPH0534288B2 (en) 1993-05-21

Family

ID=16887074

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62229121A Granted JPS6472422A (en) 1987-09-12 1987-09-12 Manufacture of superconducting wire

Country Status (1)

Country Link
JP (1) JPS6472422A (en)

Also Published As

Publication number Publication date
JPS6472422A (en) 1989-03-17

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)
JPH0534288B2 (en)
Tiefel et al. Fabrication and properties of high‐T c superconducting wires
JPH0534287B2 (en)
JPH0531491B2 (en)
JPH0531490B2 (en)
JPH0531492B2 (en)
JPH01100022A (en) Method for producing superconducting thin films
Kumakura et al. BiSrCaCuO/Ag superconducting composite tapes
Tiefel et al. Fabrication of thin‐film superconductors by bulk processing
JPH0534290B2 (en)
JPH0431021B2 (en)
JPH0453819B2 (en)
JPH01153521A (en) Method for manufacturing superconducting materials
JPH0559861B2 (en)
JPH0453818B2 (en)
Ashworth et al. Electrical contacts to YBCO using metal spray techniques
JPH0534291B2 (en)
JPH0453820B2 (en)
JPH03109204A (en) Production of superconducting thin film
KR920001675B1 (en) Superconducting Goods
Gélinas et al. Texturing of thick films on a metallic substrate
JPH0534289B2 (en)
EP0386283A1 (en) Superconducting article