JPH013099A - Method for manufacturing superconducting materials - Google Patents
Method for manufacturing superconducting materialsInfo
- Publication number
- JPH013099A JPH013099A JP62-155599A JP15559987A JPH013099A JP H013099 A JPH013099 A JP H013099A JP 15559987 A JP15559987 A JP 15559987A JP H013099 A JPH013099 A JP H013099A
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- materials
- heat treatment
- amorphous
- heat source
- 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
Links
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は超電導材料の製造方法に関する。[Detailed description of the invention] (Industrial application field) The present invention relates to a method for manufacturing superconducting materials.
本発明の方法により製造された超電導材料は磁気浮上列
車、医療診断用断層ffl影装置(核磁気共鳴CT、π
中間子照射治療袋j4)、核融合炉、電力貯蔵、電気回
転機(モータ、発電機)などの超電導磁石材料およびジ
ョセフソン素子用の超電導基盤材料として用いられる。The superconducting material produced by the method of the present invention can be used in magnetic levitation trains, medical diagnostic tomography ffl imaging devices (nuclear magnetic resonance CT, π
It is used as a superconducting magnet material for meson irradiation therapy bags (j4), nuclear fusion reactors, power storage, electric rotating machines (motors, generators), and superconducting base materials for Josephson elements.
(従来の技術)
超電導物質としては、金属元素、こわら金属の合金や金
属間化合物、有機材料、セラミックス等が考えられ、最
近ではLa−5r−Cu系酸化物、 Y−Ba−Cc+
J5酸化物等のセラミックス系の、液体窒素の沸点 (
77K)より高い温度域でも超電導特性を示すいわゆる
高温超電導物質に関する基礎研究が進展している。(Prior art) Examples of superconducting materials include metal elements, alloys of stiff metals, intermetallic compounds, organic materials, and ceramics.Recently, La-5r-Cu oxides, Y-Ba-Cc+
Boiling point of liquid nitrogen for ceramics such as J5 oxide (
Basic research is progressing on so-called high-temperature superconducting materials that exhibit superconducting properties even at temperatures higher than 77K.
一方、これら物質の実用化の面でも研究が進んでおり、
電磁石などに用いられる超電導線材、帯材あるいは板材
が試作されている。金属間化合物、セラミックス系の超
電導材料は極めて硬く脆いため、超電導材料そのものを
線材化することは困難である。したがって、工業的には
超電導物質組成に相当する割合で配合された粉末素材を
用いて、これを管状体内等に充填して線材化した陵、加
熱処理を施して超電導物質を生成させる手段が用いられ
ることが多い。On the other hand, research is progressing on the practical application of these materials.
Superconducting wires, strips, and plates used in electromagnets and other devices are being prototyped. Superconducting materials such as intermetallic compounds and ceramics are extremely hard and brittle, so it is difficult to turn the superconducting materials themselves into wires. Therefore, industrially, it is necessary to use a powder material mixed in a proportion corresponding to the composition of a superconducting material, fill it into a tubular body, etc. to form a wire rod, and then heat-treat it to generate a superconducting material. often.
(発明が解決しようとする問題点)
しかし、粉粒体材料を用いて超電導物質を生成させるに
は次のような問題がある。(Problems to be Solved by the Invention) However, there are the following problems in producing a superconducting substance using a powder material.
管状体内等に粉末素材を充填し、加熱処理を施して超電
導物質を生成させる従来の技術いおいては、超電導物質
の反応場所は粉末素材どうしの接触部のみに限定される
ため、超電導物質を生成するには長時間の加熱処理が必
要であり、また未反応物質が残留しやすい問題かある。In the conventional technology of filling a powder material into a tubular body or the like and subjecting it to heat treatment to generate a superconducting material, the reaction site of the superconducting material is limited to the contact area between the powder materials. It requires a long heat treatment to produce it, and there is also the problem that unreacted substances tend to remain.
また粉末素材を均一に攪拌混合することは、材料の比重
、粒度分布の違い等が原因となって技術的に非常に困難
であり、この素材の不均一性から製造された線材として
超電導性が劣ったり、さらには超電導を示さなくなる問
題点が生じる。In addition, it is technically extremely difficult to uniformly stir and mix powder materials due to differences in specific gravity and particle size distribution of the materials, and due to the non-uniformity of this material, the wire material manufactured has poor superconductivity. The problem arises that the superconductivity is poor or even that the superconductivity is not exhibited.
そこで、本発明は優れた超電導特性を示す線材、板材そ
の他の超電導材料の製造方法を提供しようとするもので
ある。Therefore, the present invention seeks to provide a method for manufacturing wires, plates, and other superconducting materials exhibiting excellent superconducting properties.
(問題点を解決するための手段)
本発明は高エネルギー密度熱源を用い混合粉粒体材料に
溶融凝固処理を施し、その均一性を高めるとともに完全
に反応を進め、優れた特性を持つ超電導材料の製造方法
を提供するものである。(Means for Solving the Problems) The present invention uses a high energy density heat source to melt and solidify a mixed powder material to improve its uniformity and completely proceed with the reaction, thereby producing a superconducting material with excellent properties. The present invention provides a method for manufacturing.
本発明に係る超電導材料の製造方法は、セラミックス系
超電導物質組成に配合した粉粒体材料を高エネルギー密
度熱源を用いて溶融凝固処理によりアモルファス化し、
ついで、アモルファス化した材料を結晶生成熱処理する
。The method for producing a superconducting material according to the present invention includes amorphousizing a granular material blended with a ceramic superconducting material composition by melting and solidifying it using a high energy density heat source.
Next, the amorphous material is subjected to crystal formation heat treatment.
粉粒体材料としては、生成される超電導材料の成分に応
じた材料が選ばれる。たとえば、超7「導材料がY −
11a −Cu系酸化物である場合には、 Y2O3゜
11aCO3,CuOの粉末混合物が用いられる。粉粒
体材料はC02および不純物を除去するために予め仮焼
しておくことが好ましい。As the powder material, a material is selected depending on the components of the superconducting material to be produced. For example, if the conductive material is Y −
In the case of a 11a-Cu-based oxide, a powder mixture of Y2O3°11aCO3, CuO is used. The powder material is preferably calcined in advance to remove CO2 and impurities.
ここで高密度エネルギー熱源とは、電子ビーム、レーザ
ービームおよびプラズマ熱源を意味する。粉粒体材料に
高密度エネルギー熱源を通用するには、粉粒体材料を管
状体内に充填、もしくは板上などに散布して高密度エネ
ルギー流を照射する。Here, high-density energy heat sources mean electron beams, laser beams, and plasma heat sources. In order to apply a high-density energy heat source to a granular material, the granular material is filled in a tubular body or spread on a plate and irradiated with a high-density energy flow.
ここで用いる管状体の材料としては超電導組成に混合さ
れた粉末素材の溶融温度以上の融点をもつ材料を選択し
、高密度エネルギ熱源の照射で管状体が溶融せず、内部
の粉末素材か溶融するようにする。As the material for the tubular body used here, a material with a melting point higher than the melting temperature of the powder material mixed in the superconducting composition is selected, so that the tubular body does not melt when irradiated with a high-density energy heat source, and the powder material inside melts. I'll do what I do.
材料をアモルファス化するには、たとえば1200℃に
加熱し、2℃/sec程度の冷却速度で急冷する。また
、結晶生成熱処理は、たとえば950℃に加熱し、1〜
数時間保持し、徐冷する。この混合粉粒体材料のアモル
ファス化は、素材すべてがアモルファス化される必要は
ない。To make the material amorphous, it is heated to, for example, 1200° C. and then rapidly cooled at a cooling rate of about 2° C./sec. In addition, the crystal formation heat treatment is performed by heating to, for example, 950°C, and
Hold for several hours and slowly cool. It is not necessary for all of the raw material to be amorphous when this mixed powder and granular material is made amorphous.
超電導性を示す結晶を生成させるための熱処理において
、熱源は特に限定されず、たとえば話導加熱炉、あるい
は燃焼ガス炉であってもよい。また、結晶生成熱処理は
連続的なオンラインの加熱処理装置を設けることによっ
ても可能であるし、高エネルギー密度熱源による溶融凝
固処理後、別途用意された加熱処理装置によるバッチ処
理によっても可能である。In the heat treatment for producing crystals exhibiting superconductivity, the heat source is not particularly limited, and may be, for example, a conduction heating furnace or a combustion gas furnace. Further, the crystal formation heat treatment can be performed by providing a continuous online heat treatment device, or by performing batch processing using a separately prepared heat treatment device after melting and solidifying treatment using a high energy density heat source.
結晶生成熱処理にさきがけ必要に応じて当線材を冷間、
温間もしくは熱間加工することも可能である。Preceding crystallization heat treatment, the wire material is subjected to cold treatment as necessary.
Warm or hot working is also possible.
(作用)
本発明によれば混合粉粒体材料を一旦溶融した後、凝固
するようにしているので、ある程度の不均一性を持った
混合粉粒体材料であっても材料の均一・性は飛躍的に高
まる。さらに高密度エネルギ熱源の特徴である急速な凝
固過程を利用して粉粒体材料をアモルファス化すれば、
凝固時の局所的な偏析もさけることか可能となり、素材
の均一性はさらに向上する。また、−旦溶融凝固された
連続体となった素材においては、超電導物質の生成熱処
理時の反応面積は粉粒体材料を用いた場合のそれと比較
してはるかに大きく短時間で反応が素材全域にわたって
完全にすすむ。また、アモルファス化された部分は、準
安定相であることから熱処理によって安定相である超電
導物質がさらに短時間で形成される。したがって、高密
度エネルギ熱源を用いた本発明によれば、従来法で得ら
れた超電導材料に比較してはるかに優れた特性の超電導
材料がはるかに短時間で得られる。さらに、管状体内に
充填、もしくは板上などに散布された混合粉粒体材料を
高エネルギー密度熱源を用いて連続的に溶融凝固処理を
施せば、連続したアモルファス層が形成される結果、長
尺にわたって均一に優れた超電導特性を示す超電導線材
や均質な超電導特性を持つ超電導基盤等の製造が可能と
なる。(Function) According to the present invention, the mixed powder and granular material is once melted and then solidified, so even if the mixed powder and granular material has some degree of non-uniformity, the uniformity and properties of the material are maintained. It increases dramatically. Furthermore, if the powder material is made amorphous by utilizing the rapid solidification process that is a characteristic of high-density energy heat sources,
It is also possible to avoid local segregation during solidification, further improving the uniformity of the material. In addition, for materials that have been melted and solidified to form a continuum, the reaction area during heat treatment to produce superconducting substances is much larger than that when using powdered materials, and the reaction can occur over the entire material area in a short time. Completely complete. Further, since the amorphous portion is a metastable phase, a superconducting material that is a stable phase can be formed in a shorter time by heat treatment. Therefore, according to the present invention using a high-density energy heat source, a superconducting material with far superior properties can be obtained in a much shorter time than superconducting materials obtained by conventional methods. Furthermore, if the mixed powder material filled in a tubular body or spread on a plate is continuously melted and solidified using a high energy density heat source, a continuous amorphous layer is formed, resulting in the formation of a long It becomes possible to manufacture superconducting wires that exhibit uniformly excellent superconducting properties over the entire area and superconducting substrates that have uniform superconducting properties.
(実施例1)
原子数比でY:Ba:Cu = 1 : 2 : 3比
に配合したY2O3,BaCO3,(:uOの混合粉末
を外径25mm、肉厚5mi+、のステンレス製円柱形
容器のなかに充填し、両端を溶接して封をした後、冷間
線引きによって外径を縮小加工し、外径3m01の線材
とした。そのうち一部は本発明による高エネルギー密度
熱源による溶融凝固処理をjyts L/、アモルファ
ス化した後管状炉で結晶生成熱処理を施した。一方、比
較材として他の一部を用いて、従来から行われている管
状炉による噴なる熱処理を施した線材を用意した。(Example 1) A mixed powder of Y2O3, BaCO3, (:uO) blended in an atomic ratio of Y:Ba:Cu = 1:2:3 was placed in a stainless steel cylindrical container with an outer diameter of 25 mm and a wall thickness of 5 mm. After filling the inside of the wire and welding and sealing both ends, the outer diameter was reduced by cold drawing to obtain a wire rod with an outer diameter of 3 m01.A part of the wire rod was melted and solidified using a high energy density heat source according to the present invention. jyts L/, which was made amorphous and then subjected to crystal formation heat treatment in a tube furnace.On the other hand, as a comparative material, a wire rod that had been subjected to the conventional jet heat treatment in a tube furnace was prepared using some other materials. .
高エネルギー密度熱源として電子ビームを用い、第1表
に示すような条件を用いて、線材を電子ビーム流に連続
的に供給することによ)てステンレス容器内の超電導素
材を均質なアモルファス状とした。また、管状炉による
熱処理条件は、本発明および従来法とも加熱温度は95
0℃とし、種々の保持時間における線材の超電導特性を
調べた。結果を第2表に示す。Using an electron beam as a high-energy density heat source and using the conditions shown in Table 1, the superconducting material in the stainless steel container was transformed into a homogeneous amorphous state by continuously feeding wire into the electron beam stream. did. In addition, the heat treatment conditions using the tube furnace are as follows: The heating temperature is 95% for both the present invention and the conventional method.
The superconducting properties of the wire were investigated at 0°C for various holding times. The results are shown in Table 2.
第1表
第2表
第2表から明らかなように、本発明によるサンプルは短
い熱処理時間においても液体窒素温度(77K)で完全
な超電導特性を示し、高エネルギー密度熱源による溶融
凝固処理の効果が明らかにみられる。一方、従来の方法
では、長時間の熱処理によっても優れた超電導特性が得
られない。As is clear from Table 1 and Table 2, the sample according to the present invention exhibits perfect superconducting properties at liquid nitrogen temperature (77K) even during short heat treatment times, and the effect of melting and solidification treatment using a high energy density heat source is It's clearly visible. On the other hand, with conventional methods, excellent superconducting properties cannot be obtained even by long-term heat treatment.
このように、高エネルギー密度熱源による溶融凝固処理
により、素材の均質化と超電導物質の生成速度が従来法
に比較して飛躍的に高まり、短時間の加熱で優れた特性
を持つ超電導線材が製造できる。In this way, the melting and solidification process using a high-energy density heat source dramatically increases the homogenization of the material and the production rate of superconducting materials compared to conventional methods, making it possible to produce superconducting wire with excellent properties in a short heating time. can.
(実71!i例2)
肉厚3+nm 、幅10mm、長さ20mmの銅板上に
実施例1と同一混合粉末を厚さ100 umで均一に散
布した。この粉末層に第3表に示す条件のレーザービー
ムを照射し、溶融凝固処理を施した。(Example 71!i Example 2) The same mixed powder as in Example 1 was uniformly sprinkled to a thickness of 100 um on a copper plate with a wall thickness of 3+ nm, a width of 10 mm, and a length of 20 mm. This powder layer was irradiated with a laser beam under the conditions shown in Table 3 to undergo melting and solidification treatment.
第3表
銅板上の混合粉末層はレーザービームによる急速加熱急
速冷却過程においていったん溶融した後、アモルファス
化される。その後、管状炉で950℃において1時間の
結晶生成熱処理を施した。レーザービームによる溶融凝
固層は超電導の臨界温度90に、臨界?5流密度382
0 A/cm2の優れた超電導特性を示した。The mixed powder layer on the copper plate in Table 3 is once melted in the rapid heating and rapid cooling process by a laser beam, and then becomes amorphous. Thereafter, crystal formation heat treatment was performed at 950° C. for 1 hour in a tube furnace. The melted and solidified layer produced by the laser beam reaches the critical temperature of superconductivity of 90 degrees, which is critical? 5 flow density 382
It exhibited excellent superconducting properties of 0 A/cm2.
(発明の効果)
本発明によれば、高エネルギー密度熱源による溶融凝固
処理により素材が均質化し、臨界温度および臨界電流密
度の向上を図ることができる。また、超電導物質の生成
速度が従来法に比較して飛躍的に高まり、短時間の加熱
で超電導材料が製造できる。これより、優れた特性を示
す超電導材料を廉価に提供することができる。(Effects of the Invention) According to the present invention, the material is homogenized by melting and solidifying treatment using a high energy density heat source, and the critical temperature and critical current density can be improved. Additionally, the production rate of superconducting materials is dramatically increased compared to conventional methods, and superconducting materials can be produced with short heating times. As a result, a superconducting material exhibiting excellent properties can be provided at a low cost.
Claims (1)
を高エネルギー密度熱源を用いて溶融凝固処理により少
なくとも一部をアモルファス化し、ついでアモルファス
を含む材料を結晶生成熱処理することを特徴とする超電
導材料の製造方法。Production of a superconducting material characterized by making at least a part of a powder material blended into a ceramic superconducting material composition amorphous by melting and solidifying using a high energy density heat source, and then subjecting the amorphous-containing material to crystallization heat treatment. Method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62155599A JPS643099A (en) | 1987-06-24 | 1987-06-24 | Production of superconducting material |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62155599A JPS643099A (en) | 1987-06-24 | 1987-06-24 | Production of superconducting material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH013099A true JPH013099A (en) | 1989-01-06 |
| JPS643099A JPS643099A (en) | 1989-01-06 |
Family
ID=15609546
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62155599A Pending JPS643099A (en) | 1987-06-24 | 1987-06-24 | Production of superconducting material |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS643099A (en) |
-
1987
- 1987-06-24 JP JP62155599A patent/JPS643099A/en active Pending
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Shi et al. | Crystallization of metal-oxide glasses in Bi-Sr-Ca-Cu-O systems | |
| DE1159903B (en) | Device for melting the purest silicon and other pure semiconductor materials | |
| JPH0512320B2 (en) | ||
| JPH013099A (en) | Method for manufacturing superconducting materials | |
| JPH07115924B2 (en) | Method for manufacturing oxide superconductor | |
| JPS60165338A (en) | Compound super-conductor and its preparation | |
| JP2550253B2 (en) | Method for producing oxide high temperature superconductor | |
| JP2590103B2 (en) | Method for manufacturing compound superconducting wire | |
| JP3569743B2 (en) | Skutterudite single crystal and method for producing the same | |
| JPH01226735A (en) | Method for manufacturing superconducting materials | |
| JPS6229017A (en) | Manufacture of superconductor compound by electron beam irradiation | |
| JPH01252567A (en) | Method for manufacturing ceramic-based oxide superconducting material moldings | |
| JPH0453050B2 (en) | ||
| JP2655797B2 (en) | Method for forming oriented thick film of bismuth-based superconducting ceramics | |
| JPH0354103A (en) | Production of oxide superconductor | |
| JPS63241828A (en) | Manufacture of superconducting wire | |
| Concalves et al. | Preparation of superconductors of the BiSrCaCuO system by glass crystallization | |
| JPH01130419A (en) | Superconductive ceramic wire material and its production | |
| JPH01246719A (en) | Manufacture of oxide superconductor | |
| JPH02186511A (en) | Manufacture of superconductor | |
| JPS6386208A (en) | Manufacture of compound superconductor | |
| JPS63294625A (en) | Manufacture of ceramic superconductive wire material | |
| RADIATIVE et al. | Birmingham, B15 2TT, UK | |
| JPH02213011A (en) | Method for manufacturing conductive materials | |
| JPH0717380B2 (en) | Method for producing superconducting fibrous crystal |