JPH01201062A - Production of ceramic superconducting material - Google Patents

Production of ceramic superconducting material

Info

Publication number
JPH01201062A
JPH01201062A JP63252166A JP25216688A JPH01201062A JP H01201062 A JPH01201062 A JP H01201062A JP 63252166 A JP63252166 A JP 63252166A JP 25216688 A JP25216688 A JP 25216688A JP H01201062 A JPH01201062 A JP H01201062A
Authority
JP
Japan
Prior art keywords
superconducting material
sintering
powder
superconducting
oxide
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.)
Pending
Application number
JP63252166A
Other languages
Japanese (ja)
Inventor
Takayuki Inuzuka
孝之 犬塚
Toshinori Ando
安藤 敏範
Kiyoshi Sawano
清志 澤野
Hiroshi Tanemoto
種本 啓
Hiroshi Kubo
紘 久保
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.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
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 Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP63252166A priority Critical patent/JPH01201062A/en
Publication of JPH01201062A publication Critical patent/JPH01201062A/en
Pending legal-status Critical Current

Links

Classifications

    • Y—GENERAL 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
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Landscapes

  • Superconductors And Manufacturing Methods Therefor (AREA)
  • Compositions Of Oxide Ceramics (AREA)
  • Inorganic Compounds Of Heavy Metals (AREA)

Abstract

PURPOSE:To densify a superconducting material and to improve a critical current density in producing the superconducting material by subjecting a raw material of oxide-based superconducting substance blended in a superconducting substance composition to kneading-calcining-grinding-molding and sintering, by specifying the grinding and sintering methods. CONSTITUTION:Each oxide powder blended in a superconducting composition is repeatedly calcined and ground until a single phase of superconducting mate rial is obtained and the powder is finally ground in an anhydrous organic disper sion medium by a ball mill or jet mill to give fine powder having <=1mu average particle diameter. The fine powder is molded, sintered at 900-970 deg.C for 2-100hr and the average crystal particle diameter of the sintered material is made <=3mu. In this method, when the average crystal particle diameter of the sintered material is >=3mu, uniform denseness is not sufficient and high critical current density JC can not be attained. The sintering condition should be made to select a lower temperature side than the above-mentioned range if the particle size of the fine powder before the sintering is small and uniform. But if the sintering temperature is <900 deg.C, sintering is insufficient and JC is extremely lowered.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は酸化物系高温超電導材料等を製造する方法に関
するもので、この発明によって臨界電流密度が大きい超
電導材料の製造が容易となる。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a method for producing an oxide-based high-temperature superconducting material, etc. The present invention facilitates producing a superconducting material having a high critical current density.

[従来の技術] 最近、Y、Ba2C:u30.−、 (Xは酸素欠損度
)の組成に代表される各種の酸化物系セラミックスが超
電導臨界温度(Tc)か液体窒素温度を越すところのい
わゆる高温超電導物質として発見され、その実用化への
研究・開発が各方面で推進されている。そしてこれを磁
気浮上列車、核磁気共鳴断層撮影装置、超電導推進船等
への応用を図る場合には、単位断面積あたりの回通電流
量の大きい導体(例えば線材、テープ)すなわち臨界電
流密度(Jc)の大きい超電導材料か必須のものとして
製造技術確立が要請される。
[Prior Art] Recently, Y, Ba2C:u30. - Various oxide-based ceramics, represented by the composition of (X is the degree of oxygen vacancy), have been discovered as so-called high-temperature superconducting materials that exceed the superconducting critical temperature (Tc) or liquid nitrogen temperature, and research is underway to put them into practical use.・Development is being promoted in all areas. When applying this to magnetically levitated trains, nuclear magnetic resonance tomography devices, superconducting propulsion ships, etc., conductors (e.g. wires, tapes) with a large amount of circulating current per unit cross-sectional area, i.e. critical current density (Jc ), it is necessary to establish manufacturing technology for superconducting materials with large values.

しかしながら、これら酸化物系セラミックスの超電導特
性に関して、Tcについては90に以上の高温領域とな
し得ることが基礎物質すなわち該種セラミックスの粉体
等において確認されているものの大きなJcの達成は困
難性大とされており、実用化の研究開発の実績の蓄積が
ないこともあり、Jc改善のための有効かつ具体的な提
案等はほとんど報告されていない。
However, regarding the superconducting properties of these oxide-based ceramics, although it has been confirmed that Tc can be achieved in the high temperature range of 90 or higher in the basic material, ie, the powder of such ceramics, it is extremely difficult to achieve a large Jc. Partly because there is no accumulation of research and development results for practical application, very few effective and specific proposals for improving Jc have been reported.

[発明が解決しようとする課題] Y1Ba2Cu3O7−Xやこれと類似の形態の酸化物
等のセラミックス系超電導材料の製造は、 La2O3
゜Y2O3,SrCO3,BaC0,、、CuOなとの
原料粉末を超電導物質組成となる所定の割合で配合し、
これを仮焼して炭酸等の目的外の成分の揮発除去を図り
、ついで粉砕していったん中間材料としてのセラミック
ス系超電導物質の粉体とし、この粉体を加圧成形して所
望の材料の形状としたあと熱処理(仕上げ焼結)すると
いう方法によって行うことが一般的である。
[Problems to be Solved by the Invention] Production of ceramic superconducting materials such as Y1Ba2Cu3O7-X and oxides with similar forms is as follows: La2O3
゜Blending raw material powders such as Y2O3, SrCO3, BaC0, CuO, etc. in a predetermined ratio to form a superconducting material composition,
This is calcined to volatilize and remove unintended components such as carbonic acid, and then pulverized to produce ceramic superconducting material powder as an intermediate material, and this powder is pressure-molded to form the desired material. This is generally done by heat treatment (finish sintering) after shaping.

ところで、セラミツスス系超電導物質の粉体は、粒度が
小さく、かつ分散性が高いほど緻密かつ成分的に均一な
焼結体すなわち超電導材料が得られる。超電導材料が緻
密であれば粒界の影響が小さくなるため臨界温度Tc、
臨界電流密度Jcおよび臨界磁場しは高くなる。これに
より、電気機器の高性能かつ小型化を図ることができる
。また微細かつ複雑な加工が可能となり電子デバイスに
応用することが可能となる。したがって、超電導材料の
緻密化が電気機器および電子デバイスの性能向上にもた
らす効果は極めて大きい。
Incidentally, the smaller the particle size and the higher the dispersibility of the powder of the ceramitsu-based superconducting material, the more dense and compositionally uniform a sintered body, ie, the superconducting material, can be obtained. If the superconducting material is dense, the influence of grain boundaries will be reduced, so the critical temperature Tc,
The critical current density Jc and the critical magnetic field become higher. Thereby, it is possible to achieve high performance and miniaturization of electrical equipment. Furthermore, it becomes possible to perform fine and complicated processing, making it possible to apply it to electronic devices. Therefore, the densification of superconducting materials has an extremely large effect on improving the performance of electrical equipment and electronic devices.

しかるに上記従来の製造方法において得られるセラミッ
クス系超電導物質粉は、La2O3,Y2O3゜5rC
O,、、BaCO3,CuO等の形態の複数種の成分原
料をポットミル等で機械的に粉砕・分散しているだけで
あるので粒度は数JJmから数101Jmにわたり分布
する。このような粉体を加圧成形したものは、複数種の
組成の、かつ粗粒細粒が入り混った状態を呈するので、
部分的(セミマクロ的)な成分の不均一はさけかたく、
その上、CuO(融点: 1026℃)のような低融点
物質とY2O3(融点: 2410℃)のような高融点
物質の混合物であるため上記のようなセミマクロ的な成
分の不均一がある場合には仕上げ焼結による成分の均一
拡散の達成は極めて難かしい。すなわち、従来法では均
質で緻密な焼結体から形成される超電導材料(バルク)
がなかなか得られない。これが臨界温度Tc、臨界電流
密度Jcおよび臨界磁場■。の向上に対して製造技術面
での大きな障害となっている。すなわち、別の角度から
言うならば、極めて微細なセラミックス系超電導物質の
粉体が工業的に製造入手できれば、セラミックス系超電
導材料の実用特性(例えばTC,Jc)の向上・安定に
供するところ甚大ということになり、その実現か要請さ
れていた。
However, the ceramic superconducting material powder obtained by the above conventional manufacturing method is La2O3,Y2O3゜5rC
Since a plurality of types of component raw materials in the form of O, . Pressure molded powders of this type have multiple compositions and are a mixture of coarse and fine particles.
Partial (semi-macro) non-uniformity of components is difficult to avoid,
Furthermore, since it is a mixture of a low melting point substance such as CuO (melting point: 1026°C) and a high melting point substance such as Y2O3 (melting point: 2410°C), it can be It is extremely difficult to achieve uniform diffusion of components through final sintering. In other words, in conventional methods, superconducting materials (bulk) are formed from homogeneous and dense sintered bodies.
is difficult to obtain. This is the critical temperature Tc, critical current density Jc, and critical magnetic field ■. This poses a major obstacle in terms of manufacturing technology to the improvement of manufacturing technology. In other words, from another perspective, if extremely fine powder of ceramic superconducting materials could be manufactured and obtained industrially, it would greatly contribute to improving and stabilizing the practical properties (e.g. TC, Jc) of ceramic superconducting materials. Therefore, there was a request to make this happen.

[課題を解決するための手段] 本発明は超電導物質組成に配合した酸化物系超電導物質
の原料から混練−仮焼一粉砕一成形一焼結の工程により
超電導材料を製造する方法において、粉砕および焼結を
適切な方法で行うことによって均一緻密な焼結体とする
もので、その要旨は仮焼−粉砕工程の最終粉砕で無水有
機分散媒中でホールミル処理し、或いはまた窒素気流中
にのせてジットミル処理し、平均粒径1ミクロン以下の
Mi電導物質の微粉とし、かつ、成形後の焼結を900
℃〜970℃で2〜100時間の処理として焼結体の平
均結晶粒径3ミクロン以下の超電導材料とすることであ
る。上記の「成形」とは、超電導物質粉を加圧成形して
直接に所望の最終的形状とするもののほか、これに限ら
ず、加圧成形後に別の塑性加工等を付与して所望の形状
とするものを含む。
[Means for Solving the Problems] The present invention provides a method for producing a superconducting material from raw materials of an oxide-based superconducting material blended into a superconducting material composition through the steps of kneading, calcination, pulverization, shaping, and sintering. A uniform and dense sintered body is obtained by performing sintering in an appropriate manner, and the gist is that in the final pulverization of the calcination and pulverization process, the sintered body is treated with a whole mill in an anhydrous organic dispersion medium, or placed in a nitrogen stream. The powder is made into a fine powder of Mi conductive material with an average particle size of 1 micron or less, and the sintering after molding is
The process is carried out for 2 to 100 hours at a temperature of .degree. C. to 970.degree. C. to produce a superconducting material having an average crystal grain size of 3 microns or less. The above-mentioned "molding" refers to not only pressure-molding the superconducting material powder to directly form the desired final shape, but also applying another plastic processing etc. after pressure-forming to form the desired shape. Including those who are.

また、本発明を一層有効ならしめるため、成形後の焼結
を実質的に純酸素雰囲気下で行うことが好適である。
Further, in order to make the present invention even more effective, it is preferable to perform sintering after molding in a substantially pure oxygen atmosphere.

ここで最終粉砕時に用いる無水有機分散媒としては1価
アルコール(例えばエタノール)、1価ケトン(例えば
アセトン)その他各種のものが適用可能である。この選
択は各製造場の諸条件(例えば、ボールミルの強度、処
理時間)と分散媒物質の特性(例えば沸点)その他を勘
案して決定すればよい。
As the anhydrous organic dispersion medium used in the final pulverization, monohydric alcohols (for example, ethanol), monovalent ketones (for example, acetone), and other various types can be used. This selection may be made by taking into consideration the various conditions of each manufacturing plant (for example, the strength of the ball mill, processing time), the characteristics of the dispersion medium (for example, the boiling point), and other factors.

なお、焼結の条件(温度、時間)は焼結前(−最終粉砕
後)の微粉の粒度に応じて、具体的には粒径か小さくか
つ均一であれば低温側もしくは短時間側の条件が選択で
きる。
The sintering conditions (temperature, time) depend on the particle size of the fine powder before sintering (-after final pulverization).Specifically, if the particle size is small and uniform, the conditions are on the lower temperature side or the shorter time side. can be selected.

[作用] 酸化物系超電導材料の臨界温度Tc、臨界電流密度Jc
、臨界磁場■。などの超電導特性に密接に関連するもの
として、焼結体(超電導材料バルク)の結晶粒の均一性
、緻密度がある。これらに支配的な影響を与えるのか、
原料となる超電導物質粉体の平均粒径と粒度分布である
。平均粒径が細かく粒度分布幅の狭いもの程焼結体の結
晶粒の均一性、緻密度を向上させることができる。
[Function] Critical temperature Tc, critical current density Jc of oxide-based superconducting material
, critical magnetic field■. The uniformity and density of the crystal grains of the sintered body (the bulk of the superconducting material) are closely related to the superconducting properties. Does it have a dominant influence on these?
This is the average particle size and particle size distribution of the superconducting material powder used as the raw material. The finer the average grain size and the narrower the grain size distribution width, the more uniformity and density of the crystal grains of the sintered body can be improved.

この発明では、超電導物質の微細粉化の方策として、超
′1「導組成となるように配合した各酸化物粉体を超電
導物質の単相になるまで仮焼−粉砕を繰り返し、そして
最終粉砕を無水有機分散媒中で湿式ボールミル、あるい
はジェットミルにより粉砕して平均粒径1ミクロン以下
の超電導物質の微粉とする。従来法に対して末法によっ
て得られる平均粒径は1ミクロン以下、粒度分布として
は最大粒径5ミクロン以下の良好な徴砕粉が得られる。
In this invention, as a measure to finely powder a superconducting material, each oxide powder blended to have a superconducting composition is repeatedly calcined and pulverized until it becomes a single phase of superconducting material, and then finally pulverized. is pulverized in an anhydrous organic dispersion medium using a wet ball mill or a jet mill to obtain a fine powder of superconducting material with an average particle size of 1 micron or less.In contrast to the conventional method, the powder method obtains an average particle size of 1 micron or less, with a particle size distribution. As a result, good pulverized powder with a maximum particle size of 5 microns or less can be obtained.

第1図に従来法による粉砕粉と、末法のうち湿式ホール
ミルによる粉砕粉の粒度分布のヒストグラムを示す。従
来法のものには数lOミクロン程度の未粉砕粉も残り、
平均粒径約3ミクロンと大きいものになっている。
FIG. 1 shows a histogram of the particle size distribution of the pulverized powder obtained by the conventional method and the pulverized powder obtained by the wet whole mill among the powder methods. Conventional methods leave unpulverized powder on the order of several 1O microns,
It has a large average particle size of about 3 microns.

具体的なボールミル処理条件として、ボールの材質とし
て高純度Al2O3またはzr02を使用し直径はI 
Ommφ〜lromゆである。無水有機分散媒としては
アセトン、メタノール、エタノールなどが好適なものと
して使用できる。比重が大きいZrO□ボールで粒径が
小さいものを用いる程微細粉化には効果がある。無水有
機分散媒としては、粉砕後の乾燥の際にはアセトンが有
利であるか、長時間の運転を行うような場合は、アセト
ンは沸点が低いので気化して内圧が急増する危険も考え
られ、エタノール、メタノールの使用が望ましい。また
水の使用はこの超電導物質は吸水し分解するので使用で
きない。
As specific ball milling conditions, high purity Al2O3 or ZR02 is used as the ball material, and the diameter is I.
Boil to Ommφ~lrom. Acetone, methanol, ethanol, etc. can be suitably used as the anhydrous organic dispersion medium. The use of ZrO□ balls with a larger specific gravity and a smaller particle size is more effective in making the particles finer. As an anhydrous organic dispersion medium, acetone is advantageous for drying after pulverization, or when operating for a long time, acetone has a low boiling point, so there is a risk of vaporization and a sudden increase in internal pressure. It is preferable to use , ethanol, or methanol. Also, water cannot be used because this superconducting material absorbs water and decomposes.

次にジェットミルにより粉砕する方法について説明する
。ジェットミルはAl2O3などで内部をライニングし
たものが粉体衝突時の摩耗による粉体の汚染が少ないの
で好ましい。また粉体を搬送する気体は圧縮空気でも良
いが水分を含まない乾燥空気あるいは窒素の方が望まし
い。ジェットミルの粉砕条件はその装置にもよるが、1
μm以下にするような条件を選定すればよく、従来の一
般的な粉砕条件でよい。
Next, a method of pulverizing using a jet mill will be explained. It is preferable to use a jet mill whose inside is lined with Al2O3 or the like because there is less contamination of the powder due to wear when the powder collides with the mill. The gas for transporting the powder may be compressed air, but dry air containing no moisture or nitrogen is preferable. The grinding conditions of a jet mill depend on the equipment, but 1
It is sufficient to select conditions that will reduce the particle size to .mu.m or less, and conventional general pulverization conditions may be used.

成形は基本的には従来の一般的な手段によればよい。な
かでもCIP (冷間等方圧縮加工)は成形体の緻密度
向上に対して効果がある。
Basically, the molding may be carried out by conventional and common means. Among these, CIP (cold isostatic pressing) is effective in improving the compactness of the molded product.

焼結条件の選択目的は焼結体の結晶粒を均一、緻密に制
御することである。具体的には平均結晶粒径3ミクロン
以下(かつ最大結晶粒径5ミクロン以下)、好ましくは
平均結晶粒径2ミクロン以下(かつ最大結晶粒径5ミク
ロン以下)を達成目標とする。平均結晶粒径が3ミクロ
ンより大きいときは、均一緻密性が充分とならず、高い
Jcは達成できない。この目標達成のためには、平均粒
径1ミクロン以下(かつ最大粒径5ミクロン以下)の粉
体を900℃〜970℃で2〜100時間の焼結をする
ことが適当である。焼結のより詳細な条件としては、焼
結前の微粉の粒度に応じてその粒径か小さくかつ均一で
あれば上記の範囲のうちより低温側を選択しなければな
らない。高温側による過度(長時間)の焼結は、結晶粒
の異常粒成長をもたらし粒子の異方性が大きいことから
、粒界に応力が集中しクラックか生成してJcの著しい
低下が起こるからである。
The purpose of selecting the sintering conditions is to uniformly and precisely control the crystal grains of the sintered body. Specifically, the goal is to achieve an average crystal grain size of 3 microns or less (and a maximum crystal grain size of 5 microns or less), preferably an average crystal grain size of 2 microns or less (and a maximum crystal grain size of 5 microns or less). When the average crystal grain size is larger than 3 microns, uniform density is not sufficient and a high Jc cannot be achieved. In order to achieve this goal, it is appropriate to sinter powder having an average particle size of 1 micron or less (and a maximum particle size of 5 microns or less) at 900°C to 970°C for 2 to 100 hours. As for more detailed sintering conditions, depending on the particle size of the fine powder before sintering, if the particle size is small and uniform, the lower temperature side of the above range must be selected. Excessive (long-term) sintering at high temperatures causes abnormal grain growth and large anisotropy of grains, which causes stress to concentrate at grain boundaries and generate cracks, resulting in a significant decrease in Jc. It is.

また低温側の焼結では、焼結時間を長時間にできること
から焼結体の緻密化、結晶粒どうしの結合力の強化も可
能となる。しかし900℃未満では焼結が不充分となり
、Jcはまた著しく低下する。
Furthermore, in low-temperature sintering, since the sintering time can be extended, it is possible to make the sintered body denser and strengthen the bonding force between crystal grains. However, below 900°C, sintering becomes insufficient and Jc also decreases significantly.

焼結は実質的に純酸素雰囲気下で行うべきである。PO
2は焼結後冷却の際に超電導相の形成に影響を及ぼし、
Po2増大雰囲気が有利である。酸素分圧としてfat
…以上が望ましい。
Sintering should be performed under a substantially pure oxygen atmosphere. P.O.
2 affects the formation of superconducting phase during cooling after sintering,
A Po2 enriched atmosphere is advantageous. fat as oxygen partial pressure
...The above is desirable.

[実施例コ 実施例l Y2O3,BaCO3,CuO粉末を原子数比でY:B
a:Cu =1=2・3の割合となるように配合してポ
ットミルに人わてエタノール中で1δhr混練した。こ
れを真空乾燥し950℃x8hの仮焼とボールミルによ
る粉砕混合を2回繰り返し、超電導物質(組成:YBa
2Cu307−x)単相にした。そして、最終粉砕とし
てZrO,ボール10mmφを使用しエタノール中で2
4hrのボールミル粉砕を行い、とり出して真空乾燥し
た。得られた粉体は平均粒径0.8ミクロン、最大粒径
4ミクロンであった。これを20mmφ厚さ2ffII
11のベレットにCIP 7t/cm2の成形を行い、
純酸素雰囲気中で各種条件により焼結を行った。これを
四端子法により臨界温度Tcと臨界電流密度Jcを測定
した。臨界温度Tcは全て90 Kを超えていた。第−
表にJcの測定結果を示す。比較のため、従来法により
得られた平均粒径3ミクロン、最大粒径30ミクロンの
粉体を使用し、同様な焼結を行ったものの結果を同表中
に合わせて示す。その結果、本発明による平均粒径1ミ
クロン以下の超電導粉体を用い900℃〜970℃で適
切な時間焼結したものは焼結体の平均結晶粒径か3ミク
ロン以下となり良好なJcを示した。特に、平均結晶粒
径が2ミクロ以下の焼結体のJcは大きい。焼結時の雰
囲気を02富化とすると著効のあることも同しく第1表
から明らかである。また、第1表金体から、900〜9
70℃で2〜100時間の焼結が好適であることが認め
られる。
[Example 1 Y2O3, BaCO3, CuO powder in atomic ratio Y:B
The mixture was mixed in a ratio of a:Cu = 1 = 2.3, and kneaded in ethanol for 1δhr in a pot mill. This was dried in vacuum, calcined at 950°C for 8 hours, and pulverized and mixed using a ball mill twice.
2Cu307-x) Single phase. Then, for the final grinding, a ZrO ball with a diameter of 10 mm was used, and the powder was ground in ethanol for 2 hours.
Ball milling was performed for 4 hours, and the product was taken out and dried under vacuum. The obtained powder had an average particle size of 0.8 microns and a maximum particle size of 4 microns. This is 20mmφ thickness 2ffII
11 pellets were molded with CIP 7t/cm2,
Sintering was performed under various conditions in a pure oxygen atmosphere. The critical temperature Tc and critical current density Jc were measured using the four-terminal method. The critical temperature Tc was all above 90K. No.-
The table shows the measurement results of Jc. For comparison, the same sintering was performed using powder with an average particle size of 3 microns and a maximum particle size of 30 microns obtained by the conventional method, and the results are also shown in the same table. As a result, when the superconducting powder according to the present invention with an average grain size of 1 micron or less was sintered at 900°C to 970°C for an appropriate time, the average crystal grain size of the sintered body was 3 μm or less, showing good Jc. Ta. In particular, the Jc of a sintered body with an average crystal grain size of 2 microns or less is large. It is also clear from Table 1 that an O2-enriched atmosphere during sintering has a significant effect. Also, from the first surface metal body, 900 to 9
Sintering at 70°C for 2 to 100 hours is found to be suitable.

実施例2 Y2O3,口act3. CuO粉末を原子数比でY:
Ba:Cu =1:2:3の割合となるように、配合し
てポットミルに入れてエタノール中で16hr混線した
。こわを真空乾燥し、925℃X 8hrの仮焼とボー
ルミルによる乾式粉砕を2回繰り返し超電導物質単相(
YBa2Cu307−X)の粉末を得た。この時点でこ
の粉末の粒度分布は第2図に示すようであり、粒度の中
間値は1.6μmであった。この粉末をジェットミルを
用いて乾式粉砕を行なった。粉砕後の粒度分布は第3図
に示すごとく、中間値は0.9μmであり51以上の粒
子は検出できなかった。これを20mmφ厚さ2 mm
のベレットにCIP 2t/cm2の条件で成形し、純
酸素気流中で各種条件で焼結した。この焼成体の臨界温
度Tcと臨界電流密度Jcを四端子法により測定した。
Example 2 Y2O3, mouth act3. CuO powder in atomic ratio Y:
The mixture was mixed in a ratio of Ba:Cu = 1:2:3, placed in a pot mill, and mixed in ethanol for 16 hours. The solids were vacuum dried, calcined at 925°C for 8 hours, and dry ground in a ball mill twice to produce a single phase superconducting material (
A powder of YBa2Cu307-X) was obtained. At this point, the particle size distribution of this powder was as shown in FIG. 2, with the median particle size being 1.6 μm. This powder was dry-pulverized using a jet mill. As shown in FIG. 3, the particle size distribution after pulverization had a median value of 0.9 μm, and no particles larger than 51 could be detected. This is 20mmφ and 2mm thick.
It was molded into a pellet under conditions of CIP 2t/cm2 and sintered under various conditions in a pure oxygen stream. The critical temperature Tc and critical current density Jc of this fired body were measured by a four-terminal method.

臨界温度Tcは全て90にを越えていた。第4図にJC
の測定結果と焼成温度の関係を示す。焼成時間は8時間
であり、Jc最大値は100OA/cm2を越えている
。従来法でのJcの値は実施例工にも示しであるが、最
大250A/Cl112であり、末法によりJCが向上
したことが明らかである。
The critical temperature Tc was all over 90. JC in Figure 4
The relationship between the measurement results and firing temperature is shown. The firing time was 8 hours, and the maximum Jc value exceeded 100 OA/cm2. The value of Jc in the conventional method, as shown in the example work, was a maximum of 250 A/Cl112, and it is clear that the JC was improved by the final method.

[発明の効果] 本発明によれば均質で結晶粒径の細い緻密なセラミック
系超電導物質の焼結体が得られ、その結果として臨界電
流密度の高い超電導材料を製造することが可能となった
。
[Effects of the Invention] According to the present invention, a sintered body of a dense ceramic superconducting material that is homogeneous and has a small crystal grain size can be obtained, and as a result, it has become possible to manufacture a superconducting material with a high critical current density. .

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

第1図は本発明によるセラミックス超電導材料と通常の
乾式ホールミルで粉砕したセラミック超電導材料の粒度
分布を示す図、第2図は通常の乾式ボールミル2回粉砕
したセラミック、8電導材料の粒度分布を示す図、第3
図は第2図に示した超電導材料の粉末をジェットミルで
粉砕した後の粒度分布を示す図、および第4図はジェッ
トミルで粉砕した超電導材料の粉末を各種温度で焼成し
た超電導体の臨界電流密度Jcと相対密度の関係を示し
た図である。
Fig. 1 shows the particle size distribution of the ceramic superconducting material according to the present invention and the ceramic superconducting material ground with a normal dry ball mill, and Fig. 2 shows the particle size distribution of the ceramic superconducting material ground twice with a normal dry ball mill. Figure, 3rd
The figure shows the particle size distribution after the superconducting material powder shown in Fig. 2 is pulverized with a jet mill, and Fig. 4 shows the criticality of superconductors obtained by firing the superconducting material powder pulverized with a jet mill at various temperatures. It is a figure showing the relationship between current density Jc and relative density.

Claims (3)

【特許請求の範囲】[Claims] 1.超電導物質組成となるように配合した酸化物系超電
導物質の原料を混練し、ついで仮焼−粉砕を1回以上行
って超電導物質の粉体とし、この粉体を成形−焼結して
超電導材料を製造する方法において、仮焼−粉砕工程の
最終粉砕で無水有機分散媒中でボールミル処理して、平
均粒径1ミクロン以下の超電導物質の微粉とし、該微粉
を成形し、900℃〜970℃で2〜100時間の焼結
を行い、焼結体の平均結晶粒径3ミクロン以下の超電導
材料とすることを特徴とする酸化物系超電導材料の製造
方法。
1. Raw materials for an oxide-based superconducting material blended to have a superconducting material composition are kneaded, then calcined and pulverized one or more times to obtain a superconducting material powder, and this powder is molded and sintered to form a superconducting material. In the method for producing a superconducting material, the final pulverization of the calcination-pulverization step is performed by ball milling in an anhydrous organic dispersion medium to obtain a fine powder of a superconducting material with an average particle size of 1 micron or less, and the fine powder is shaped and heated to a temperature of 900°C to 970°C. 1. A method for producing an oxide-based superconducting material, characterized in that sintering is performed for 2 to 100 hours to obtain a sintered body of a superconducting material having an average crystal grain size of 3 microns or less.
2.超電導物質組成となるように配合した酸化物系超電
導物質の原料を混練し、ついで仮焼−粉砕を1回以上行
って超電導物質の粉体とし、この粉体を成形−焼結して
超電導材料を製造する方法において、仮焼−粉砕工程の
最終粉砕で窒素気流中に前記超電導物質の粉体をのせて
ジェットミル処理して、平均粒径1ミクロン以下の超電
導物質の微粉とし、該微粉を成形し、900℃〜970
℃で2〜100時間の焼結を行い、焼結体の平均結晶粒
径3ミクロン以下の超電導材料とすることを特徴とする
酸化物系超電導材料の製造方法。
2. Raw materials for an oxide-based superconducting material blended to have a superconducting material composition are kneaded, then calcined and pulverized one or more times to obtain a superconducting material powder, and this powder is molded and sintered to form a superconducting material. In the method for manufacturing, in the final pulverization of the calcination-pulverization step, the powder of the superconducting material is placed in a nitrogen stream and subjected to jet mill treatment to obtain a fine powder of the superconducting material with an average particle size of 1 micron or less, and the fine powder is Molding, 900℃~970℃
A method for producing an oxide-based superconducting material, which comprises sintering at a temperature of 2 to 100 hours to obtain a sintered body of a superconducting material having an average crystal grain size of 3 microns or less.
3.成形後の焼結を実質的に純酸素雰囲気下で行うこと
を特徴とする請求項1または2記載の酸化物系超電導材
料の製造方法。
3. 3. The method for producing an oxide-based superconducting material according to claim 1, wherein the sintering after shaping is performed in a substantially pure oxygen atmosphere.
JP63252166A 1987-10-07 1988-10-07 Production of ceramic superconducting material Pending JPH01201062A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63252166A JPH01201062A (en) 1987-10-07 1988-10-07 Production of ceramic superconducting material

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP62-251465 1987-10-07
JP25146587 1987-10-07
JP63252166A JPH01201062A (en) 1987-10-07 1988-10-07 Production of ceramic superconducting material

Publications (1)

Publication Number Publication Date
JPH01201062A true JPH01201062A (en) 1989-08-14

Family

ID=26540208

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63252166A Pending JPH01201062A (en) 1987-10-07 1988-10-07 Production of ceramic superconducting material

Country Status (1)

Country Link
JP (1) JPH01201062A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007070157A (en) * 2005-09-06 2007-03-22 Kengo Ebina Method for forming superconductive ceramic thin film

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007070157A (en) * 2005-09-06 2007-03-22 Kengo Ebina Method for forming superconductive ceramic thin film

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