JP2905862B2 - Method for producing superconducting whisker composite - Google Patents
Method for producing superconducting whisker compositeInfo
- Publication number
- JP2905862B2 JP2905862B2 JP5016724A JP1672493A JP2905862B2 JP 2905862 B2 JP2905862 B2 JP 2905862B2 JP 5016724 A JP5016724 A JP 5016724A JP 1672493 A JP1672493 A JP 1672493A JP 2905862 B2 JP2905862 B2 JP 2905862B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- whisker
- composite
- powder crystal
- sintered body
- 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
Links
- 239000002131 composite material Substances 0.000 title claims description 55
- 238000004519 manufacturing process Methods 0.000 title claims description 10
- 239000013078 crystal Substances 0.000 claims description 56
- 239000000843 powder Substances 0.000 claims description 54
- 238000002156 mixing Methods 0.000 claims description 13
- 229910004247 CaCu Inorganic materials 0.000 claims description 10
- 238000000465 moulding Methods 0.000 claims description 8
- 229910052797 bismuth Inorganic materials 0.000 claims description 6
- 229910052760 oxygen Inorganic materials 0.000 claims description 6
- 229910052802 copper Inorganic materials 0.000 claims description 5
- 238000005245 sintering Methods 0.000 claims description 5
- 229910052712 strontium Inorganic materials 0.000 claims description 5
- 229910052791 calcium Inorganic materials 0.000 claims description 4
- 239000002245 particle Substances 0.000 claims description 4
- 230000005291 magnetic effect Effects 0.000 description 14
- 239000000463 material Substances 0.000 description 12
- 238000010304 firing Methods 0.000 description 11
- 238000003825 pressing Methods 0.000 description 9
- 239000011575 calcium Substances 0.000 description 7
- 238000001816 cooling Methods 0.000 description 6
- 239000010949 copper Substances 0.000 description 6
- 238000000034 method Methods 0.000 description 6
- 239000000203 mixture Substances 0.000 description 6
- 239000002994 raw material Substances 0.000 description 6
- 239000002887 superconductor Substances 0.000 description 5
- 238000002441 X-ray diffraction Methods 0.000 description 4
- 238000010438 heat treatment Methods 0.000 description 4
- 238000005452 bending Methods 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- VTYYLEPIZMXCLO-UHFFFAOYSA-L Calcium carbonate Chemical compound [Ca+2].[O-]C([O-])=O VTYYLEPIZMXCLO-UHFFFAOYSA-L 0.000 description 2
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 2
- 150000001875 compounds Chemical class 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 238000011161 development Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005485 electric heating Methods 0.000 description 2
- 230000004907 flux Effects 0.000 description 2
- 239000007789 gas Substances 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 239000000155 melt Substances 0.000 description 2
- 238000013001 point bending Methods 0.000 description 2
- 238000000634 powder X-ray diffraction Methods 0.000 description 2
- 238000003860 storage Methods 0.000 description 2
- 238000012360 testing method Methods 0.000 description 2
- 229910015902 Bi 2 O 3 Inorganic materials 0.000 description 1
- BVKZGUZCCUSVTD-UHFFFAOYSA-L Carbonate Chemical compound [O-]C([O-])=O BVKZGUZCCUSVTD-UHFFFAOYSA-L 0.000 description 1
- QPLDLSVMHZLSFG-UHFFFAOYSA-N Copper oxide Chemical compound [Cu]=O QPLDLSVMHZLSFG-UHFFFAOYSA-N 0.000 description 1
- 229910001275 Niobium-titanium Inorganic materials 0.000 description 1
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 229910000416 bismuth oxide Inorganic materials 0.000 description 1
- 229910000019 calcium carbonate Inorganic materials 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 230000006378 damage Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 230000005292 diamagnetic effect Effects 0.000 description 1
- TYIXMATWDRGMPF-UHFFFAOYSA-N dibismuth;oxygen(2-) Chemical compound [O-2].[O-2].[O-2].[Bi+3].[Bi+3] TYIXMATWDRGMPF-UHFFFAOYSA-N 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- BDAGIHXWWSANSR-NJFSPNSNSA-N hydroxyformaldehyde Chemical compound O[14CH]=O BDAGIHXWWSANSR-NJFSPNSNSA-N 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- RJSRQTFBFAJJIL-UHFFFAOYSA-N niobium titanium Chemical compound [Ti].[Nb] RJSRQTFBFAJJIL-UHFFFAOYSA-N 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 238000010791 quenching Methods 0.000 description 1
- 230000000171 quenching effect Effects 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 238000012827 research and development Methods 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 238000003980 solgel method Methods 0.000 description 1
- 239000007858 starting material Substances 0.000 description 1
- 229910000018 strontium carbonate Inorganic materials 0.000 description 1
- 238000010189 synthetic method Methods 0.000 description 1
Landscapes
- Compositions Of Oxide Ceramics (AREA)
- Inorganic Compounds Of Heavy Metals (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、超電導ウィスカー複合
体の製造方法に関する。The present invention relates to a method for producing a superconducting whisker composite.
【0002】[0002]
【従来の技術とその問題点】近年の酸化物超電導体に関
しては、基礎および応用の両分野において目ざましい発
展が認められる。基礎分野においては、新組成超電導体
の発見、新しい合成法の開発、超電導発現機構の解明な
どについての進展がある。また、応用分野においても、
電気材料から医療分野での応用までとその研究範囲は広
がっており、様々な分野において酸化物超電導材料の開
発、機能性向上などへの期待が高まりつつある。2. Description of the Related Art In recent years, remarkable development has been recognized in oxide superconductors in both basic and applied fields. In the basic fields, progress has been made in discovering new composition superconductors, developing new synthetic methods, and elucidating the mechanism of superconductivity. Also, in application fields,
The range of research from electrical materials to applications in the medical field is expanding, and expectations for the development and functional improvement of oxide superconducting materials are increasing in various fields.
【0003】現在、超電導材料として広く利用されてい
るものは、ニオブ・チタン合金などの非酸化物超電導材
料である。しかしながら、これら非酸化物超電導材料の
臨界温度は低いので、冷却のためには液体ヘリウムを用
いなければならず、冷却コストが高くなる。At present, non-oxide superconducting materials such as niobium-titanium alloy are widely used as superconducting materials. However, since the critical temperature of these non-oxide superconducting materials is low, liquid helium must be used for cooling, which increases the cooling cost.
【0004】一方酸化物超電導材料には、液体窒素以上
の臨界温度を有するものがあり、これを用いば、冷却コ
ストは低減される。そのため、酸化物超電導材料を利用
する電力貯蔵、電力輸送、強磁場発生などについての研
究開発が活発になされている。これらの用途において
は、超電導体物質を線材化する必要がある。その方法と
して、酸化物超電導体の仮焼粉末を銀シースに詰めて再
熱処理する方法、ゾル−ゲル法、酸化物超電導体の融液
からの線引き法などがある。しかしながら、これらの方
法により得られた線材は、多結晶体であるため、結晶粒
界による超電導特性および機械的強度の低下、加工性の
悪さなどの欠点を有しており、広く実用化されるには至
っていない。On the other hand, some oxide superconducting materials have a critical temperature equal to or higher than that of liquid nitrogen, and if used, the cooling cost can be reduced. Therefore, research and development on power storage, power transport, generation of a strong magnetic field, and the like using an oxide superconducting material have been actively conducted. In these applications, it is necessary to convert the superconductor material into a wire. Examples of the method include a method in which calcined powder of an oxide superconductor is packed in a silver sheath and reheat-treated, a sol-gel method, and a method of drawing an oxide superconductor from a melt. However, since the wires obtained by these methods are polycrystalline, they have drawbacks such as a decrease in superconducting properties and mechanical strength due to crystal grain boundaries, poor workability, and are widely put to practical use. Has not been reached.
【0005】[0005]
【発明が解決しようとする課題】本発明は、超電導特性
および機械的強度に優れた酸化物超電導材料を提供する
ことを主な目的とする。SUMMARY OF THE INVENTION An object of the present invention is to provide an oxide superconducting material having excellent superconducting properties and mechanical strength.
【0006】本発明者は、上記の様な技術の現状に鑑み
て種々研究を重ねた結果、一定の大きさのBi2Sr2
CaCu2O8構造を有する超電導ウィスカーとBi2
Sr2CaCu2O8構造を有する超電導粉末結晶とを
混合し、加圧成形した後、焼結する場合には、上記の粉
末結晶のみから得られる焼結体よりも超電導特性および
機械的強度に優れた酸化物超電導複合材料が得られるこ
とを見出した。The present inventor has conducted various studies in view of the state of the art as described above, and as a result, has found that Bi 2 Sr 2 having a certain size is obtained.
Superconducting whisker having CaCu 2 O 8 structure and Bi 2
When mixed with a superconducting powder crystal having an Sr 2 CaCu 2 O 8 structure, pressed and then sintered, the superconducting properties and mechanical strength are higher than those of a sintered body obtained from the above powder crystal alone. It has been found that an excellent oxide superconducting composite material can be obtained.
【0007】即ち、本発明は、下記の超電導ウィスカー
と超電導粉末結晶との焼結体からなる超電導ウィスカー
複合体の製造方法を提供するものである:1.Bi、S
r、Ca、CuおよびOからなり、Bi2Sr2CaC
u2O8構造を有し、粒径1〜50μmである超電導粉
末結晶と、Bi、Sr、Ca、CuおよびOからなり、
Bi2Sr2CaCu2O8構造を有し、長さ1〜10
mm、幅10〜150μm、厚さ1〜10μmである超
電導ウィスカーとを、〔粉末結晶〕:〔ウィスカー〕=
1.00:0.01〜0.50の重量比で混合し、加圧
成形した後、820〜875℃で焼結することを特徴と
する超電導ウィスカー複合体の製造方法。That is, the present invention provides a method for producing a superconducting whisker composite comprising a sintered body of the following superconducting whiskers and superconducting powder crystals: Bi, S
consisting of r, Ca, Cu and O, Bi 2 Sr 2 CaC
a superconducting powder crystal having a u 2 O 8 structure and a particle size of 1 to 50 μm, and Bi, Sr, Ca, Cu and O;
It has a Bi 2 Sr 2 CaCu 2 O 8 structure and a length of 1 to 10
mm, a width of 10 to 150 μm, and a thickness of 1 to 10 μm with a superconducting whisker: [powder crystal]: [whisker] =
1.00: A method for producing a superconducting whisker composite, comprising mixing at a weight ratio of 0.01 to 0.50, forming the mixture under pressure, and sintering at 820 to 875 ° C.
【0008】本発明の超電導ウィスカー複合体の製造に
際し使用する超電導粉末結晶は、原子組成比が、Bi=
1.00として、Sr=1.00、Ca=0.50、C
u=1.00となるように原料物質を混合した後、焼成
し、粉砕して得られる。この際の焼成条件は、通常温度
820〜860℃程度、時間20〜100時間程度で、
より具体的な一例として、820℃で60時間程度、さ
らに860℃で20時間程度である。粉末の粒径は、通
常1〜50μm程度であり、より好ましくは1〜10μ
m程度である。The superconducting powder crystal used for producing the superconducting whisker composite of the present invention has an atomic composition ratio of Bi =
1.00, Sr = 1.00, Ca = 0.50, C
After mixing the raw materials so that u = 1.00, the mixture is calcined and pulverized. The firing conditions at this time are usually about 820 to 860 ° C. for about 20 to 100 hours.
As a more specific example, the heat treatment is performed at 820 ° C. for about 60 hours, and further at 860 ° C. for about 20 hours. The particle size of the powder is usually about 1 to 50 μm, more preferably 1 to 10 μm.
m.
【0009】また、本発明の超電導ウィスカー複合体の
製造に際して使用する超電導ウィスカーは、本発明者ら
により特開平2−252621号の開示されている様
に、原料物質の融液を急冷することにより得られ、原子
組成比がBi=1.00として、Sr=1.00、Ca
=1.00、Cu=2.00、Al=0.50〜1.0
0であるガラス板を酸素気流中、例えば865℃で80
時間熱処理することにより、得られる。超電導ウィスカ
ーの寸法は、通常長さ1〜10mm程度、幅10〜15
0μm程度、厚さ1〜10μm程度であり、より好まし
くは長さ5mm程度、幅100μm程度、厚さ5μm程
度である。The superconducting whiskers used in the production of the superconducting whisker composite of the present invention are prepared by quenching the melt of the raw material as disclosed in Japanese Patent Application Laid-Open No. 2-252621. Assuming that the atomic composition ratio is Bi = 1.00, Sr = 1.00, Ca
= 1.00, Cu = 2.00, Al = 0.50-1.0
The glass plate which is 0 in an oxygen stream, for example,
It is obtained by heat treatment for a time. The dimensions of the superconducting whisker are usually about 1 to 10 mm in length and 10 to 15 in width.
The thickness is about 0 μm and the thickness is about 1 to 10 μm, more preferably about 5 mm in length, about 100 μm in width, and about 5 μm in thickness.
【0010】上記の粉末結晶およびウィスカーのいずれ
の場合にも、原料物質としては、焼成により酸化物を形
成し得るものであれば、特に限定されず、金属単体、酸
化物、各種化合物(炭酸塩など)が使用できる。原料物
質としては、上記の原子を2種以上併せて含む化合物を
使用してもよい。上記の焼成工程に際しては、電気加熱
炉、ガス加熱炉などの公知の任意の装置を採用し得る。[0010] In any of the above-mentioned powder crystals and whiskers, the raw material is not particularly limited as long as it can form an oxide by firing, and may be a simple metal, an oxide, various compounds (carbonate). Etc.) can be used. As the raw material, a compound containing two or more of the above atoms may be used. In the firing step, any known apparatus such as an electric heating furnace or a gas heating furnace may be used.
【0011】次いで、上記の方法で得られた超電導粉末
結晶と超電導ウィスカーとを〔粉末結晶〕:〔ウィスカ
ー〕=1.00:y(0.01≦y≦0.50)の重量
比で十分に混合し、加圧成形した後、820〜875℃
程度で15〜30時間程度(例えば、860℃で20時
間)焼成する。成形時の圧力は、特に限定されないが、
通常10〜1000kg/cm2 程度であり、より好ま
しくは100〜500kg/cm2 程度である。この際
の焼成手段としても、特に限定されず、電気加熱炉、ガ
ス加熱炉などの公知の任意の装置を採用し得る。Next, the superconducting powder crystal and the superconducting whisker obtained by the above method are sufficiently mixed at a weight ratio of [powder crystal]: [whisker] = 1.00: y (0.01 ≦ y ≦ 0.50). 820 to 875 ° C.
Firing is performed for about 15 to 30 hours (for example, at 860 ° C. for 20 hours). The pressure during molding is not particularly limited,
Usually, it is about 10 to 1000 kg / cm 2 , more preferably about 100 to 500 kg / cm 2 . The firing means at this time is not particularly limited, and any known apparatus such as an electric heating furnace or a gas heating furnace can be adopted.
【0012】本発明において、超電導粉末結晶1重量部
に対する超電導ウィスカーの配合量が0.01部未満と
なる焼結体では、複合体内で超電導特性(臨界電流密
度、磁気シールド特性)および機械的強度において、ウ
ィスカーを混合した効果がほとんど認められない。これ
に対し、前者に対する後者の配合量が0.50部を上回
る場合には、860℃以上の高温で焼成しても、焼結が
十分に行なわれないので、複合体の機械的強度は、粉末
結晶焼結体よりも低くなる。In the present invention, in a sintered body in which the amount of superconducting whiskers is less than 0.01 part per 1 part by weight of superconducting powder crystal, superconducting properties (critical current density, magnetic shielding properties) and mechanical strength are within the composite. , The effect of mixing whiskers is hardly recognized. On the other hand, when the amount of the latter is more than 0.50 parts with respect to the former, even if firing at a high temperature of 860 ° C. or more, the sintering is not sufficiently performed, so that the mechanical strength of the composite is: It becomes lower than the powder crystal sintered body.
【0013】本発明において得られた超電導ウィスカー
複合体(粉末結晶:ウィスカーの重量混合比=1.0
0:0.05)の1例(これは、後記の実施例1におけ
るNo.1であり、その製造方法などについては、実施
例1を参照)の粉末X線回折パターンを図1に示す。超
電導ウィスカー複合体および超電導粉末結晶焼結体の全
ての製造例で同様のX線回折パターンが観察された。こ
れらの回折パターンは、Bi2 Sr2 CaCu2 O8 構
造に特有のものである。The superconducting whisker composite (powder crystal: whisker weight mixing ratio = 1.0) obtained in the present invention.
FIG. 1 shows a powder X-ray diffraction pattern of one example (0: 0.05) (this is No. 1 in Example 1 described later, and the production method and the like refer to Example 1). Similar X-ray diffraction patterns were observed in all the production examples of the superconducting whisker composite and the superconducting powder crystal sintered body. These diffraction patterns are unique to the Bi 2 Sr 2 CaCu 2 O 8 structure.
【0014】本発明実施例1で得られた超電導ウィスカ
ー複合体および超電導粉末結晶焼結体の臨界温度(Tc
zero)は70〜75Kであった(後記表1参照)。The critical temperature (Tc) of the superconducting whisker composite and the superconducting powder crystal sintered body obtained in Example 1 of the present invention.
zero ) was 70 to 75K (see Table 1 below).
【0015】直流四端子法で測定した超電導ウィスカー
複合体(粉末結晶:ウィスカーの重量混合比=1.0
0:0.05)の一例(後記の実施例1におけるNo.
1である)の電気抵抗と絶対温度との関係を図2に示
す。電気抵抗がゼロになる温度は、72Kであった。Superconducting whisker composite (weight ratio of powder crystal: whisker = 1.0
0: 0.05) (No. 1 in Example 1 described later).
2 is shown in FIG. 2. The temperature at which the electrical resistance became zero was 72K.
【0016】より焼結性を増すために、上記の加圧成形
体を875℃で長時間(例えば、10時間)焼成した
後、さらに860℃で20時間焼成し、炉冷して得られ
た超電導ウィスカー複合体の臨界温度は、同様の加圧成
形体を875℃で短時間(例えば、3時間)焼成した
後、860℃で20時間焼成して得られた複合体の臨界
温度よりも、低くなった。875℃で長時間焼成して得
られた複合体の臨界温度を875℃で短時間焼成して得
られた複合体の臨界温度まで高めるためには、焼成後8
00℃以上の高温から複合体を急冷することが必要とな
る。また、超電導ウィスカー複合体の作製時に、875
℃以上の高温で焼成すると超電導ウィスカー或いは超電
導粉末結晶の表面が一部融解し、結晶構造が壊れてしま
うため、複合体の超電導特性の劣化(例えば、臨界温度
の低下)が生じる。従って、加圧成形体の焼成温度は、
820〜875℃の範囲とする。In order to further improve the sinterability, the above-mentioned pressed body was fired at 875 ° C. for a long time (for example, 10 hours), and further fired at 860 ° C. for 20 hours, followed by furnace cooling. The critical temperature of the superconducting whisker composite is higher than the critical temperature of the composite obtained by baking the same pressed molded body at 875 ° C. for a short time (for example, 3 hours) and then baking at 860 ° C. for 20 hours. Got lower. In order to raise the critical temperature of the composite obtained by firing at 875 ° C. for a long time to the critical temperature of the composite obtained by firing at 875 ° C. for a short time, the temperature after firing is 8
It is necessary to rapidly cool the composite from a high temperature of 00 ° C. or higher. In addition, when the superconducting whisker composite is manufactured, 875
If baked at a high temperature of not less than ° C., the surface of the superconducting whisker or the superconducting powder crystal is partially melted and the crystal structure is broken, so that the superconducting properties of the composite are deteriorated (for example, the critical temperature is lowered). Therefore, the firing temperature of the pressed body is
The range is 820 to 875 ° C.
【0017】図3は、粉末結晶:ウィスカーの重量混合
比が1.00:0.05である本発明実施例1のNo.
1による超電導ウィスカー複合体(a)および実施例1
のNo.2による超電導粉末結晶焼結体(b)の、それ
らの製造過程における加圧成形段階での加圧平面のX線
回折パターンを比較して示す。本発明による超電導ウィ
スカー複合体(a)では、(00n)面によるピークの
強度が他のピークに比べ大きくなってる。このことは、
超電導ウィスカー複合体内で、超電導ウィスカーのab
面が加圧平面に対し平行に配向している事実を示してい
る。このab面の配向は、加圧成形の際に起こると考え
られる。これに対し、超電導粉末結晶焼結体(b)の場
合には、(a)の場合の様なab面の配向による特徴的
な大きなピークは、認められない。FIG. 3 shows No. 1 of Example 1 of the present invention in which the weight mixing ratio of powder crystal: whisker was 1.00: 0.05.
1 and superconducting whisker composite (a) according to Example 1
No. 2 shows an X-ray diffraction pattern of a pressing plane of a superconducting powder crystal sintered body (b) according to No. 2 in a pressing step in a production process thereof. In the superconducting whisker composite (a) according to the present invention, the peak intensity due to the (00n) plane is larger than the other peaks. This means
Ab of superconducting whisker in superconducting whisker complex
This shows the fact that the plane is oriented parallel to the pressing plane. It is considered that the orientation of the ab plane occurs during pressure molding. On the other hand, in the case of the superconducting powder crystal sintered body (b), a characteristic large peak due to the orientation of the ab plane as in the case of (a) is not recognized.
【0018】粉末結晶:ウィスカーの重量混合比が1.
00:0.05である本発明実施例1のNo.6による
超電導ウィスカー複合体(a)および実施例1のNo.
2による超電導粉末結晶焼結体(b)の加圧成形時の加
圧平面に対して、0.01Gの磁場を垂直に掛けた時の
磁化率の温度依存性を図4に示す。この場合、超電導ウ
ィスカー複合体(a)中のウィスカーへは、上で述べた
様に、超電導ウィスカーのab面が加圧平面に対し平行
に配向しているので、このab面に垂直に磁場が掛けら
れている。70K以下の温度で、同一重量、同一形状で
の反磁性磁化率は、超電導ウィスカー複合体(曲線A)
の方が、超電導粉末結晶焼結体(曲線B)よりも大きく
なった。この結果から、本発明による超電導ウィスカー
複合体は、1G以下程度の低磁場における磁気シールド
効果において、超電導粉末結晶焼結体よりも優れている
ことが明らかである。これは、上記の様に、超電導ウィ
スカー複合体内のウィスカーのab面が加圧平面に対し
て平行に配向しているためである。即ち、超電導粉末結
晶焼結体では、結晶粒界を通って磁束が焼結体内部に侵
入してしまうのに対し、超電導ウィスカー複合体では、
超電導ウィスカーのab面が磁場に対して垂直に配向し
ているため、ウィスカーが磁束の複合体内部への侵入を
妨げている。The powder crystal: whisker weight mixing ratio is 1.
No. 00 of Example 1 of the present invention, that is, No. 00: 0.05. 6 and the superconducting whisker composite (a) according to No. 6 of Example 1.
FIG. 4 shows the temperature dependency of the magnetic susceptibility when a magnetic field of 0.01 G is applied perpendicularly to the pressing plane at the time of pressing the superconducting powder crystal sintered body (b) according to No. 2. In this case, as described above, the whisker in the superconducting whisker composite (a) has a magnetic field perpendicular to the ab plane because the ab plane of the superconducting whisker is oriented parallel to the pressing plane. It is hung. The diamagnetic susceptibility at the same weight and the same shape at a temperature of 70 K or less is determined by the superconducting whisker composite (curve A).
Was larger than the superconducting powder crystal sintered body (curve B). From this result, it is clear that the superconducting whisker composite according to the present invention is superior to the superconducting powder crystal sintered body in the magnetic shielding effect in a low magnetic field of about 1 G or less. This is because the ab plane of the whisker in the superconducting whisker complex is oriented parallel to the pressing plane as described above. That is, in the superconducting powder crystal sintered body, the magnetic flux penetrates into the sintered body through the crystal grain boundary, whereas in the superconducting whisker composite,
Since the ab plane of the superconducting whisker is oriented perpendicular to the magnetic field, the whisker prevents the magnetic flux from entering the inside of the composite.
【0019】通電法により測定した臨界電流密度Jc
は、超電導粉末結晶焼結体で33.8A/cm2 (測定
温度65.8K)、粉末結晶:ウィスカーの重量混合比
が1.00:0.05である本発明の超電導ウィスカー
複合体で252A/cm2 (測定温度71.1K)とな
り、ウィスカー複合体の方が測定温度とTc との温度差
が小さいにもかかわらず、Jc値は1桁近く大きくなっ
た。Critical current density Jc measured by energization method
Is 33.8 A / cm 2 (measuring temperature 65.8 K) for a superconducting powder crystal sintered body, and 252 A for a superconducting whisker composite of the present invention having a powder crystal: whisker weight mixing ratio of 1.00: 0.05. / Cm 2 (measurement temperature 71.1K), and the Jc value of the whisker composite was increased by almost one digit, even though the temperature difference between the measurement temperature and Tc was smaller.
【0020】本発明による超電導ウィスカー複合体と超
電導粉末結晶焼結体との機械的強度を比較評価するため
に、長さ25mm×厚さ4.0〜4.6mm×幅3.0
〜6.5mmで、#800のラップ板により表面を研磨
した試験片を使用し、スパンを20mmとして三点曲げ
強度を測定した。この結果から、超電導ウィスカー複合
体と超電導粉末結晶焼結体の間では、曲げ強度には大き
な差が無いことが分かった(粉末結晶:ウィスカーの重
量混合比が1.00:0.05である実施例1のNo.
1の超電導ウィスカー複合体の平均値=6.73MP
a;超電導粉末結晶のみからなる実施例1のNo.2の
焼結体の平均値=8.52MPa)。In order to compare and evaluate the mechanical strength between the superconducting whisker composite according to the present invention and the sintered superconducting powder crystal, the length is 25 mm × thickness 4.0 to 4.6 mm × width 3.0.
Using a test piece whose surface was polished with a # 800 lap plate at a distance of 6.5 mm, the three-point bending strength was measured with a span of 20 mm. From this result, it was found that there was no significant difference in bending strength between the superconducting whisker composite and the superconducting powder crystal sintered body (the weight mixing ratio of powder crystal: whisker was 1.00: 0.05. No. 1 of the first embodiment.
Average value of superconducting whisker composite of No. 1 = 6.73MP
a: No. 1 of Example 1 consisting of only superconducting powder crystals Average value of the sintered body of No. 2 = 8.52 MPa).
【0021】なお、曲げ強度は、以下の式から算出し
た。The bending strength was calculated from the following equation.
【0022】曲げ強度=(3×荷重×スパン)/(2×
幅×(厚さ)2 ) 但し、スパンは三点曲げ測定時の引っ張り面側の二支点
間の距離である。Bending strength = (3 × load × span) / (2 ×
Width x (thickness) 2 ) However, the span is the distance between two fulcrums on the tensile surface side during three-point bending measurement.
【0023】しかしながら、超電導ウィスカー複合体と
粉末結晶焼結体の荷重−変異曲線(第5図)から破壊の
様子を比較すると、粉末結晶焼結体(b)は、最大荷重
後、応力が瞬時に減少してしまう不安定破壊を示したの
に対し、超電導ウィスカー複合体(a)は、応力が徐々
に減少していく準安定破壊を示した。この結果は、焼結
体にひびが入った場合に、超電導粉末結晶焼結体では、
そのひびが瞬時に焼結体全体に進展して、焼結体が一気
に破断してしまうのに対し、超電導ウィスカー複合体で
は、ひびの進展が粉末結晶焼結体に比して緩やかで、瞬
時の破壊が起きないことを示している。因みに、両焼結
体試験片の破断面を電子顕微鏡(SEM)で観察する
と、超電導粉末結晶焼結体では、主に荷重線に沿って数
本の太いひびが入っていたのに対し、超電導ウィスカー
複合体では、細いひびがウィスカーを避けるようにその
縁を迂回している箇所が観察された。以上の結果から、
超電導ウィスカー複合体に過大な荷重が掛けられて、ひ
びが入った場合には、複合体内のウィスカーが、ひびの
進展を遅らせて、瞬時の破断を妨げていることが判明し
た。However, comparing the state of fracture with the load-mutation curve (FIG. 5) of the superconducting whisker composite and the powder crystal sintered body, the powder crystal sintered body (b) shows that the stress is instantaneous after the maximum load. In contrast, the superconducting whisker composite (a) showed metastable fracture in which the stress gradually decreased. This result shows that when the sintered body is cracked,
While the cracks spread instantaneously throughout the sintered body and break at once, the superconducting whisker composite cracks more slowly than the powder crystal sintered body, No destruction will occur. By the way, when the fracture surface of both sintered body test pieces was observed with an electron microscope (SEM), in the superconducting powder crystal sintered body, several thick cracks were mainly formed along the load line. In the whisker complex, thin cracks were observed circumventing the rim to avoid the whiskers. From the above results,
When an excessive load was applied to the superconducting whisker composite and the composite was cracked, it was found that the whiskers in the composite delayed the crack growth and prevented instantaneous fracture.
【0024】超電導ウィスカー複合体の超電導特性およ
び機械的強度は、作製時の焼結条件および粉末結晶とウ
ィスカーとの混合比に影響される。超電導特性の向上の
ためには、ウィスカーの混合比を増加すればよいが、ウ
ィスカーの混合比が0.5以上になると、焼結性は悪く
なり、機械的強度が低下する。一方、機械的強度の向上
のためには、高温(例えば875℃以上)で、長時間焼
成することが好ましいが、高温で長時間焼成した焼結体
では、上記の様に、ウィスカーおよび分目津結晶の表面
が溶融してしまい、超電導特性が低下してしまう。以上
の互いに相反する事象を考慮しつつ、超電導特性および
機械的強度の両方を調和させるためには、超電導ウィス
カー複合体の原料における粉末結晶:ウィスカーの重量
混合比を1.00:0.05とし、且つ加圧成形体の焼
成温度を860℃とした場合に得られた焼結体が、高温
超電導材料として最も優れている。The superconducting properties and mechanical strength of the superconducting whisker composite are affected by the sintering conditions during production and the mixing ratio between the powder crystal and the whiskers. In order to improve the superconductivity, the mixing ratio of the whiskers may be increased. However, when the mixing ratio of the whiskers is 0.5 or more, the sinterability deteriorates and the mechanical strength decreases. On the other hand, in order to improve the mechanical strength, it is preferable to fire at a high temperature (for example, 875 ° C. or more) for a long time, but in the case of a sintered body fired at a high temperature for a long time, the whisker and the The surface of the tsu crystal is melted, and the superconductivity is reduced. In order to harmonize both the superconducting properties and the mechanical strength while considering the above conflicting events, the weight ratio of powder crystal: whisker in the raw material of the superconducting whisker composite is set to 1.00: 0.05. Further, the sintered body obtained when the firing temperature of the press-formed body is 860 ° C. is the most excellent as a high-temperature superconducting material.
【0025】[0025]
【発明の効果】本発明によれば、Bi、Sr、Ca、C
uおよびOからなり、Bi2 Sr2 CaCu2 O8 構造
を有する超電導粉末結晶と、同じくBi、Sr、Ca、
CuおよびOからなり、Bi2 Sr2 CaCu2 O8 構
造を有する超電導ウィスカーとを混合し、加圧成形した
後、820〜875℃で焼結することにより、超電導ウ
ィスカー複合体を得ることができる。According to the present invention, Bi, Sr, Ca, C
and a superconducting powder crystal having a structure of Bi 2 Sr 2 CaCu 2 O 8 , and Bi, Sr, Ca,
Made of Cu and O, were mixed and the superconducting whiskers having a Bi 2 Sr 2 CaCu 2 O 8 structure, after pressure molding, by sintering at eight hundred and twenty to eight hundred and seventy-five ° C., can be obtained superconducting whisker composites .
【0026】この様にして得られた本発明の超電導ウィ
スカー複合体は、その内部に超電導ウィスカー間の接合
が存在し、成形時の加圧平面に対してウィスカーのab
面が平行に配向するため、超電導粉末結晶のみからなる
焼結体に比して、超電導特性に優れている。また、超電
導ウィスカーが、複合体に生じたひびの進展を遅らせる
ため、機械的強度においても、超電導粉末結晶焼結体よ
りも優れている。The superconducting whisker composite of the present invention thus obtained has a junction between the superconducting whiskers inside, and the whisker ab
Since the planes are oriented in parallel, the superconductivity is superior to that of a sintered body composed of only superconducting powder crystals. Further, since the superconducting whisker delays the growth of cracks generated in the composite, the superconducting whisker is also superior in mechanical strength to the superconducting powder crystal sintered body.
【0027】従って、本発明による超電導ウィスカー複
合体は、焼成前の加圧成形段階で必要な形状に加圧成形
し、得られた成形体を焼結することにより、電力輸送
用、電力貯蔵用および磁場発生マグネット用の線材、磁
気シールド材などの高温超電導材料としての利用が期待
される。Therefore, the superconducting whisker composite according to the present invention is subjected to pressure molding to a required shape in a pressure molding step before firing, and the obtained molded body is sintered to be used for power transport and power storage. It is also expected to be used as a high-temperature superconducting material such as a wire for a magnetic field generating magnet and a magnetic shielding material.
【0028】[0028]
【実施例】以下に実施例を示し、本発明の特徴とすると
ころをより一層明確にする。 実施例1 Bi=1.00として、Sr=1.00、Ca=0.5
0、Cu=1.00となる様に下記の出発原料を十分に
混合した後、アルミナルツボに入れ、電気炉中820℃
で20時間仮焼した後、さらに成形後860℃で20時
間仮焼した。次いで得られた焼成体を十分に粉砕して、
Bi2 Sr2 CaCu2 O8 なる構造を有する超電導粉
末結晶(平均粒径約10μm)を得た。EXAMPLES Examples are shown below to further clarify the features of the present invention. Example 1 Bi = 1.00, Sr = 1.00, Ca = 0.5
0, and after sufficiently mixing the following starting materials so that Cu = 1.00, the mixture was placed in an alumina crucible and placed in an electric furnace at 820 ° C.
And then calcined at 860 ° C. for 20 hours after molding. Next, the obtained fired body is sufficiently pulverized,
A superconducting powder crystal (average particle size: about 10 μm) having a structure of Bi 2 Sr 2 CaCu 2 O 8 was obtained.
【0029】次いで、この超電導粉末結晶1.00gと
Bi2 Sr2 CaCu2 O8 なる構造を有する超電導ウ
ィスカー(平均長5mm、平均幅100μm、平均厚さ
5μm)0.05gとを十分に混合し、100kg/c
m2 で加圧成形した後、アルミナ皿にのせ、電気炉中8
60℃で20時間焼成し、約50℃/分の冷却速度で炉
冷した。得られた超電導ウィスカー複合体No.1は、
直径16mm、厚さ1.5mmの円板であった。Then, 1.00 g of the superconducting powder crystal and 0.05 g of superconducting whiskers (average length 5 mm, average width 100 μm, average thickness 5 μm) having a structure of Bi 2 Sr 2 CaCu 2 O 8 were sufficiently mixed. , 100kg / c
After pressing under m 2 , place on an alumina plate and place in an electric furnace for 8 minutes.
It was baked at 60 ° C. for 20 hours and cooled in a furnace at a cooling rate of about 50 ° C./min. The obtained superconducting whisker composite No. 1 is
It was a disk having a diameter of 16 mm and a thickness of 1.5 mm.
【0030】また、上記の超電導粉末結晶と超電導ウィ
スカーとを表1に示す所定の割合で混合した後加圧成形
するか、或いは上記の超電導粉末結晶を単独で加圧成形
するした後、表1に示す条件下に焼成して、焼結体N
o.2〜13を得た。Further, the superconducting powder crystal and the superconducting whisker are mixed at a predetermined ratio shown in Table 1 and then press-molded, or the above-mentioned superconducting powder crystal is press-molded alone, and then, as shown in Table 1. And sintered under the conditions shown in
o. 2-13 were obtained.
【0031】表1に得られた各焼結体の臨界温度を示
す。Table 1 shows the critical temperature of each of the obtained sintered bodies.
【0032】[0032]
【表1】 なお、本実施例において用いた超電導ウィスカーおよび
超電導粉末結晶の製造原料は、下記に示すものであっ
た。 −Bi源…酸化ビスマス(Bi2 O3 ) −Sr源…炭酸ストロンチウム(SrCO3 ) −Ca源…炭酸カルシウム(CaCO3 ) −Cu源…酸化銅(CuO) また、図6に超電導ウィスカー複合体No.6(a)お
よび超電導粉末結晶焼結体No.2(b)のSEM写真
を示す。本発明による超電導ウィスカー複合体が、超電
導ウィスカーが粉末結晶に完全に埋め込まれているとい
う特異な構造を有していることが明らかである。[Table 1] The raw materials for producing superconducting whiskers and superconducting powder crystals used in this example were as follows. -Bi source ... bismuth oxide (Bi 2 O 3) -Sr source ... strontium carbonate (SrCO 3) -Ca source ... calcium carbonate (CaCO 3) -Cu source ... copper oxide (CuO) Further, the superconducting whisker composites 6 No. 6 (a) and superconducting powder crystal sintered body no. The SEM photograph of 2 (b) is shown. It is clear that the superconducting whisker composite according to the invention has a unique structure in which the superconducting whiskers are completely embedded in the powder crystals.
【図面の簡単な説明】[Brief description of the drawings]
【図1】実施例1で得られた超電導ウィスカー複合体N
o.1の粉末X線回折パターンである。FIG. 1 shows a superconducting whisker composite N obtained in Example 1.
o. 1 is an X-ray powder diffraction pattern of Example 1.
【図2】実施例1で得られた超電導ウィスカー複合体N
o.1の電気抵抗の温度依存性を示すグラフである。FIG. 2 shows a superconducting whisker composite N obtained in Example 1.
o. 3 is a graph showing the temperature dependence of the electrical resistance of No. 1.
【図3】実施例1で得られた超電導ウィスカー複合体N
o.1の加圧平面のX線回折パターン(a)と超電導粉
末結晶焼結体No.2の加圧成形時の加圧平面のX線回
折パターン(b)である。FIG. 3 shows a superconducting whisker composite N obtained in Example 1.
o. X-ray diffraction pattern (a) of the pressing plane of No. 1 and superconducting powder crystal sintered body No. 2 is an X-ray diffraction pattern (b) of a pressurized plane at the time of press-molding No. 2;
【図4】実施例1で得られた超電導ウィスカー複合体N
o.6(曲線A)と超電導粉末結晶焼結体No.2(曲
線B)のゼロ磁場冷却後の0.01Gにおける磁化率の
温度依存性を示すグラフである。FIG. 4 shows a superconducting whisker composite N obtained in Example 1.
o. 6 (curve A) and superconducting powder crystal sintered body no. 2 is a graph showing the temperature dependence of the magnetic susceptibility at 0.01 G after the zero magnetic field cooling of Curve 2 (curve B).
【図5】実施例1で得られた超電導ウィスカー複合体N
o.6(a)と超電導粉末結晶焼結体No.2(b)の
荷重−変位曲線である。FIG. 5 shows a superconducting whisker composite N obtained in Example 1.
o. 6 (a) and superconducting powder crystal sintered body no. 2B is a load-displacement curve of FIG.
【図6】実施例1で得られた超電導ウィスカー複合体N
o.6(a)と超電導粉末結晶焼結体No.2(b)の
破断面を撮影したものである。FIG. 6 shows a superconducting whisker composite N obtained in Example 1.
o. 6 (a) and superconducting powder crystal sintered body no. 2 (b) is a photograph of the fracture surface.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 山下 博志 兵庫県川西市笹部字土井ノ内18−8 (72)発明者 木下 実 大阪府池田市緑丘1−2−17−106 (56)参考文献 特開 昭63−285159(JP,A) 特開 平3−150225(JP,A) 特開 平2−252621(JP,A) ──────────────────────────────────────────────────続 き Continued on the front page (72) Inventor Hiroshi Yamashita 18-8 Doinouchi, Sasabe, Kawanishi-shi, Hyogo (72) Inventor Minoru Kinoshita 1-2-17-106 Midorioka, Ikeda-shi, Osaka (56) References JP-A-63-285159 (JP, A) JP-A-3-150225 (JP, A) JP-A-2-252621 (JP, A)
Claims (1)
り、Bi2Sr2CaCu2O8構造を有し、粒径1〜
50μmである超電導粉末結晶と、Bi、Sr、Ca、
CuおよびOからなり、Bi2Sr2CaCu2O8構
造を有し、長さ1〜10mm、幅10〜150μm、厚
さ1〜10μmである超電導ウィスカーとを、〔粉末結
晶〕:〔ウィスカー〕=1.00:0.01〜0.50
の重量比で混合し、加圧成形した後、820〜875℃
で焼結することを特徴とする超電導ウィスカー複合体の
製造方法。The present invention comprises Bi, Sr, Ca, Cu and O, has a Bi 2 Sr 2 CaCu 2 O 8 structure, and has a particle size of 1 to 2.
50 μm superconducting powder crystal, Bi, Sr, Ca,
A superconducting whisker made of Cu and O, having a Bi 2 Sr 2 CaCu 2 O 8 structure, a length of 1 to 10 mm, a width of 10 to 150 μm, and a thickness of 1 to 10 μm is referred to as [powder crystal]: [whisker] = 1.00: 0.01-0.50
After mixing at a weight ratio and press-molding, 820-875 ° C.
A method for producing a superconducting whisker composite, characterized by sintering.
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|---|---|---|---|
| JP5016724A JP2905862B2 (en) | 1993-01-05 | 1993-01-05 | Method for producing superconducting whisker composite |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5016724A JP2905862B2 (en) | 1993-01-05 | 1993-01-05 | Method for producing superconducting whisker composite |
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| Publication Number | Publication Date |
|---|---|
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| JP2905862B2 true JP2905862B2 (en) | 1999-06-14 |
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|---|---|---|---|---|
| JPH0816022B2 (en) * | 1987-05-19 | 1996-02-21 | 松下電器産業株式会社 | Method for manufacturing oxide superconductor |
| US5096879A (en) * | 1989-08-28 | 1992-03-17 | General Electric Company | Synthesis of bi-ca-sr-cu-o superconductive material |
-
1993
- 1993-01-05 JP JP5016724A patent/JP2905862B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH06256059A (en) | 1994-09-13 |
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