JPH0214868A - Production of superconductor - Google Patents
Production of superconductorInfo
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- JPH0214868A JPH0214868A JP62163254A JP16325487A JPH0214868A JP H0214868 A JPH0214868 A JP H0214868A JP 62163254 A JP62163254 A JP 62163254A JP 16325487 A JP16325487 A JP 16325487A JP H0214868 A JPH0214868 A JP H0214868A
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- 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
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- Compositions Of Oxide Ceramics (AREA)
- Inorganic Compounds Of Heavy Metals (AREA)
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Abstract
Description
【発明の詳細な説明】
A、産業上の利用分野
本発明は、一定の温度で電気抵抗がゼロになる所謂超電
導体に係り、特に液体窒素温度以上で超電導を示す超電
導体に関する。DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a so-called superconductor whose electrical resistance becomes zero at a certain temperature, and particularly to a superconductor which exhibits superconductivity above the temperature of liquid nitrogen.
B0発明の概要
本発明は、粉末を混合して仮焼成し、これを粉砕して得
た加工粉末と、他の粉末とを混合して混合粉を得、この
混合粉を加圧成形した後に酸化性雰囲気中で本焼成して
得た、焼結体であり、液体窒素温度(絶対温度77度)
以上で超電導を示す超電導体の製造方法にある。B0 Summary of the Invention The present invention involves mixing powders, calcining the mixture, pulverizing the processed powder, and mixing other powders to obtain a mixed powder. It is a sintered body obtained by main firing in an oxidizing atmosphere, and the liquid nitrogen temperature (absolute temperature 77 degrees)
The above is a method for manufacturing a superconductor exhibiting superconductivity.
C0従来の技術
西暦1911年カメリング・オンネスにより超電導現象
が発見されていらい、実用化に向けてさまざまな研究開
発が進められている。実用化には、臨界171?L度(
’re)か高ければ高い程、冷却コストが安くて済むた
め、より高温での超電導の可能性をめぐってその超電導
材料の激しい開発競争が展開されている。C0 Conventional Technology Since the discovery of superconductivity by Kamerling Onnes in 1911, various research and development efforts have been underway to put it into practical use. Criticality 171 for practical use? L degree (
The higher the temperature ('re), the lower the cooling cost, so there is intense competition to develop superconducting materials with the potential for superconductivity at higher temperatures.
これまでに明らかにされている超電導材料は、液体ヘリ
ウム温度(Tc約4に、−269℃)で冷却して使用す
るしのがほとんどであり、これはヘリウムガスを液化し
た冷却剤で冷却しなければならない。ヘリウムは希少材
料で高価格であるうえ、臨界温度まで下げるための冷却
コストが非常に高くつくため、超電導材料の普及を遅ら
せる最大の原因となっている。Most of the superconducting materials that have been revealed so far have been cooled to liquid helium temperatures (Tc approximately 4, -269°C); There must be. Helium is a rare and expensive material, and the cost of cooling it down to its critical temperature is extremely high, making it the main reason for delaying the spread of superconducting materials.
ごく最近、超電導材料についての研究開発が世界的にし
進められ、これまでの概念を破る材料が登場しつつある
。Very recently, research and development into superconducting materials has progressed worldwide, and materials that break with conventional concepts are appearing.
これまで知られた超電導材料の最高のTcは、ニオブ3
ゲルマニウム(N bs G e)の22.3Kにとど
まっていたが、La(ランタン)の一部をBa(バリウ
ム)で置換したランタン・ストロンチウム・銅酸化物(
L aS r)y Cuo 4によって、これまでの限
界を超えた37にで超電導現象が始まり、33にで電気
抵抗がゼロになったことが発表され、続いて今年始め同
じ(La−5r−Cuba系で54Kを、また同物質系
で85Kを実現したと発表された。更に続いて、物質名
を1酸化物」としか明らかにされないが、ランタン・ス
トロンチウム・同酸化物系と思われる新物質によってT
c77Kを達成したと発表されるに至った。更に近年、
100Kを超えるバリウム・イッテルビウム・銅酸化物
。The highest Tc of superconducting materials known so far is niobium 3
The temperature was only 22.3K for germanium (N bs Ge), but lanthanum/strontium/copper oxide (in which part of La (lanthanum) is replaced with Ba (barium))
With LaS r)y Cuo 4, it was announced that the superconducting phenomenon began at 37, exceeding the previous limit, and that the electrical resistance became zero at 33, followed by the same (La-5r-Cuba) at the beginning of this year. It was announced that 54K was achieved with a system based on the same material, and 85K with the same material.Furthermore, the name of the material was only disclosed as "monooxide," but a new material believed to be based on lanthanum, strontium, and the same oxide was announced. by T
It was announced that he had achieved c77K. Furthermore, in recent years,
Barium, ytterbium, and copper oxides with temperatures exceeding 100K.
イツトリウム系銅酸化物の超電導材料が発見されたと発
表されるに至っている。It has been announced that a superconducting material made of yttrium-based copper oxide has been discovered.
D0発明が解決しようとする問題点
上記のように液体ヘリウムの温度は、常圧で4.2にで
あり、ヘリウムは希少材料で且つ高価格で、加えて臨界
温度まで下げるための膨張タービンなどを必要とし、冷
却コストが極めて高くつき実用化の一つの障害となって
いた。また、77に以上であれば液体窒素を使用でき、
液体ヘリウムの使用と比較してすべての点において有利
であり、実用化が極めて容易となるため、Tcか77に
以上の超電導材料の開発が望まれているが、その開発は
、上述の通り未だ緒についたばかりであるのが現状であ
る。D0 Problems to be solved by the invention As mentioned above, the temperature of liquid helium is 4.2 at normal pressure. The cooling cost was extremely high, which was an obstacle to practical application. Also, if it is 77 or higher, you can use liquid nitrogen,
It is desired to develop a superconducting material with a Tc of 77 or higher because it is advantageous in all respects compared to the use of liquid helium and is extremely easy to put into practical use. The current situation is that it has just started.
これらの点に鑑み、本発明は、77に以上で超電導状態
となる超電導体の製造方法を提供しようとするものであ
る。In view of these points, the present invention seeks to provide a method for manufacturing a superconductor that becomes superconducting in 77 or more steps.
E9問題点を解決するための手段と作用液体窒素冷却で
超電導体が使用できれば、電力。E9 Means and Functions to Solve Problems If superconductors can be used with liquid nitrogen cooling, power.
運輸、エネルギー変換等の広い分野で利用できる点に着
目し、種々の材料の配合焼成等の実験を重ねた結果、Y
−3r−Cu−0の元素構成にて超電導現象を生じさせ
る斜方晶を含むに、NiF、構造体を持つ焼結体が得ら
れることが判った。Focusing on the fact that it can be used in a wide range of fields such as transportation and energy conversion, as a result of repeated experiments such as blending and firing various materials, Y
It has been found that a sintered body having a NiF structure can be obtained when the elemental composition of -3r-Cu-0 includes orthorhombic crystals that cause a superconducting phenomenon.
しかも、ストロンチウム(Sr)、銅(Cu)の元素に
限らず、これと同様なイオン半径を持つ元素であれば、
同様に超電導現象を生じさせる焼結体が得られることが
判った。Moreover, it is not limited to the elements strontium (Sr) and copper (Cu), but any element with a similar ionic radius,
It was also found that a sintered body capable of producing a superconducting phenomenon could be obtained.
ずなわち、 ■第1成分(A1)であるイツトリウム(Y)。Zunawachi, ■Yttrium (Y), which is the first component (A1).
■イオン半径の近似した元素のSr、Caのうち少なく
とも1つの元素でなる第2成分(A2)。(2) A second component (A2) consisting of at least one element among Sr and Ca, which are elements with similar ionic radii.
■イオン半径の近似した元素の銅(Cu )、亜鉛(Z
n)、ニッケル(N i )、コバルト(Co)、鉄(
Fe)。■ Elements copper (Cu) and zinc (Z) with similar ionic radii
n), nickel (N i ), cobalt (Co), iron (
Fe).
パラジウム(Pd)、銀(A g )、カドミウム(C
d)のうら少なくとら■っの元素でなる第3成分(A2
)。Palladium (Pd), silver (A g ), cadmium (C
d) The third component (A2
).
であって、これらA 1. A t 、 A sに属す
る元素からなる主成分(An)と酸素(0)とによって
超電導現象を生じさせろ斜方晶を含むに2NiF4構造
を持つ焼結体が得られることが判った。These A1. It has been found that a sintered body having a 2NiF4 structure including orthorhombic crystals can be obtained by causing a superconducting phenomenon with the main component (An) consisting of elements belonging to At and As and oxygen (0).
しかし、焼結体の主成分(A n )を形成するA。However, A forms the main component (An) of the sintered body.
A2A2における構成が、
A、を10≦Δ1≦60原子%
Atを20≦At≦50原子%
A3を30≦A3≦65原子%
の範囲であれば、斜方晶を含むKtNtF*構造を持ち
液体窒素による冷却で抵抗ゼロの超電導体が得られるこ
とを見出した。If the composition of A2A2 is within the range of A, 10≦Δ1≦60 atomic%, At, 20≦At≦50 atomic%, and A3, 30≦A3≦65 atomic%, the liquid has a KtNtF* structure including orthorhombic crystals. We have discovered that a superconductor with zero resistance can be obtained by cooling with nitrogen.
すなわち、3成分(A + 、 A t 、 A 2)
のうち2つの成分(例えばA I 、 A ! )に属
する元素を主体とした複数種類の粉末を混合して混合粉
末を作り、この混合粉末を本焼成の温度より低い温度に
て仮焼成し、得られた仮焼成物を粉砕して加工粉末を作
り、この加工粉末と残りの1つの成分(例えばA2)に
属する元素を主体とした粉末とを混合して混合粉を作り
、この混合粉を加圧して成形体を作り、この成形体を酸
化性雰囲気中で且つ950℃〜1200℃の範囲で本焼
結することにより、AI A2 Asからなる主成
分(An)と酸素(0)とからなり且つ斜方晶を含むK
eN i F 4構造を持つ液体窒素による冷却で抵
抗ゼロの超電導体が容易に得られることを見い出した。That is, three components (A + , A t , A 2)
A mixed powder is prepared by mixing multiple types of powder mainly composed of elements belonging to two of the components (for example, A I, A!), and this mixed powder is pre-fired at a temperature lower than the temperature of the main firing, The obtained calcined product is pulverized to make a processed powder, and this processed powder is mixed with a powder mainly composed of elements belonging to the remaining one component (for example, A2) to make a mixed powder. By pressurizing a molded body and sintering this molded body in an oxidizing atmosphere at a temperature of 950°C to 1200°C, the main component (An) consisting of AI A2 As and oxygen (0) are separated. and contains orthorhombic crystals
We have discovered that a superconductor with zero resistance can be easily obtained by cooling with liquid nitrogen having an eN i F 4 structure.
なお、焼結体におけるAI At A3において、
A1が、10原子%未iiJ、60原子%超過A2が、
20原子%未満、50原子%超過A3が、30原子%未
満、65原子%超過の場合には、液体窒素で超電導が生
じる焼結体を得ろことかできなかった。In addition, in AI At A3 in the sintered body,
A1 is less than 10 atom% iiJ, A2 is more than 60 atom%,
Less than 20 atomic % and more than 50 atomic % When A3 is less than 30 atomic % and more than 65 atomic %, it has been impossible to obtain a sintered body in which superconductivity occurs in liquid nitrogen.
また、各成分(A 5. A x 、 A s )に属
する元素を主体とした粉末としては、各元素単体の粉末
、及び化合物(例えば酸化物、炭酸化物、水酸化物)の
粉末が該当するものである。In addition, powders mainly composed of elements belonging to each component (A5. It is something.
F、実施例 以下、本発明を実施例に基づいて説明する。F. Example Hereinafter, the present invention will be explained based on examples.
先ず、出発原料として粒径を10μm以下とした、
第1成分(A2)に有するイツトリウム酸化物(Y 、
03)の粉末をllmol%、第2成分(A2)に有す
るストロンチウム炭酸化物(SrCO5)の粉末を33
mo1%、第3成分(A3)に存する銅酸化物(Cub
)の粉末を56mo1%、
の割合となるように各々秤量する。First, as a starting material, yttrium oxide (Y,
The powder of strontium carbonate (SrCO5) having 1 mol% of the powder of 03) as the second component (A2) was
mo1%, copper oxide (Cub) present in the third component (A3)
) are each weighed to give a ratio of 56 mo1%.
そして、これらの粉末を用いて、混合−仮焼成→粉砕−
混合−本焼成の作業を行うわけであるが、粉末の混合組
合せは次のようにして行った。Then, using these powders, mix - calcining -> pulverize -
The mixing and main firing operations were performed, and the powders were mixed and combined as follows.
次に、製造手段を詳細に説明ずろが、各実施例と乙に同
し手段で行ったので、以下の説明は、実施例−1の場合
を代表にして説明する。Next, since the manufacturing method was explained in detail in each Example and B, the following description will be made using Example 1 as a representative.
先ず、Y、03の粉末と5rCOsの粉末をボールミル
等で十分に混合すると共にエチルアルコールと玉石を入
れ数時間十分に混合し、得られたスラリーを約100℃
の温度で乾燥させる。First, powders of Y and 03 and powders of 5rCOs are thoroughly mixed in a ball mill, etc., and ethyl alcohol and cobblestones are added and mixed thoroughly for several hours, and the resulting slurry is heated to approximately 100°C.
Dry at a temperature of
次に乾燥して得た混合粉末をアルミナ容器に入れ、酸化
性雰囲気中にて後工程の本焼成の温度より低い温度であ
る約900℃の温度で約2時間加熱処理(所謂仮焼成)
する。Next, the mixed powder obtained by drying is placed in an alumina container and heat-treated in an oxidizing atmosphere at a temperature of approximately 900°C, which is lower than the temperature of the main firing in the subsequent process, for approximately 2 hours (so-called pre-calcination).
do.
次に得られた焼成粉は、粉体が反応し合って固くなるの
で、これをライカイキにセットしている乳バチに移し、
アルコールを加えて湿式にて粉砕し微細化した加工粉末
を得ろ。Next, the baked powder obtained becomes hard as the powders react with each other, so transfer it to the milk drum set in the Laikaiki,
Add alcohol and grind in a wet process to obtain a fine processed powder.
そしで得られた加工粉末にCuOの粉末を加えてボール
ミルで十分に混合すると共に水と玉石を入れ数時間十分
に混合し、得られたスラリーを約100℃の温度で乾燥
さ什る。Then, CuO powder is added to the processed powder obtained and thoroughly mixed in a ball mill, water and cobblestones are added, and the mixture is thoroughly mixed for several hours, and the resulting slurry is dried at a temperature of about 100°C.
次に、乾燥して得た混合粉に、バインダーとしてポリビ
ニルアルコールを混合粉末に対し1重量%となるように
ポリビニルアルコール水溶液の形で添加する。そして水
又はアルコールを更に加え十分混練した後、乾燥し、ふ
るいにて150メツシユ以下の顆粒状の造粒粉を得ろ。Next, to the mixed powder obtained by drying, polyvinyl alcohol is added as a binder in the form of an aqueous polyvinyl alcohol solution so that the amount is 1% by weight based on the mixed powder. After further adding water or alcohol and thoroughly kneading, dry and sieve to obtain granulated powder of 150 mesh or less.
次に、この造粒粉を金型に充填した後、700k g
/ c m 2程度の圧力で圧縮成形して外径40m
m 、厚み約6mmの成形体を作る。Next, after filling this granulated powder into a mold, 700 kg
Compression molded at a pressure of about / cm2 to an outer diameter of 40 m.
m, a molded body with a thickness of about 6 mm is made.
次に、この成形体を焼成器に設置し、酸化性雰囲気で且
つ約l050℃(重連の仮焼成温度より高い温度)の温
度で数時間加熱して焼結体(セラミックス)を得る。Next, this molded body is placed in a sintering machine and heated in an oxidizing atmosphere at a temperature of about 1050° C. (a temperature higher than the pre-firing temperature of the multilayer) for several hours to obtain a sintered body (ceramics).
上記の製造方法により得られた焼結体を、i] l1m
m 、厚さ4 m m 、長さ40mmの形状に切り
出して第1図に示すように電極を設けて4端子法により
、焼結体の抵抗を測定した。The sintered body obtained by the above manufacturing method is
The sintered body was cut into a shape with a thickness of 4 mm, a thickness of 4 mm, and a length of 40 mm, and electrodes were provided as shown in FIG. 1 to measure the resistance of the sintered body by a four-terminal method.
即し第1図は、抵抗値を測定するための説明図で、焼結
体Sの艮手力向の両端側に電流を流すための端子a、
a’を設け、その内側に抵抗値を測定するための電圧端
子す、 b′ を設ける、これを液体窒素の低温槽に入
れ、端子a、 a’ に1アンペアの安定化電流を流し
て端子す、 b’間の電圧を電圧計(V)で測定して端
子す、 b′間の電圧降下によって抵抗値を測定する。Therefore, FIG. 1 is an explanatory diagram for measuring the resistance value, and shows terminals a for passing a current to both ends of the sintered body S in the direction of the force applied by the hand;
A' is provided, and a voltage terminal B' is provided inside it for measuring the resistance value.Place this in a liquid nitrogen cryostat, and run a stabilized current of 1 ampere through terminals a and a' to connect the terminals. Measure the voltage between terminals A and B' with a voltmeter (V), and measure the resistance value by the voltage drop between terminals A and B'.
なお、Aは電流計を示す。Note that A indicates an ammeter.
第2図は、その測定結果を示すもので、絶対温度91に
で超電導現象が始まり、約89Kに至って電気抵抗がゼ
ロになることが確認された。FIG. 2 shows the measurement results, and it was confirmed that the superconducting phenomenon started at an absolute temperature of 91 K, and that the electrical resistance became zero at about 89 K.
また、実施例−1と同様な手段によって行った実施例−
2及び実施例−3の焼結体においてら、実施例=1の場
合と同様に絶対温度約91にで超電導現象が始まり、8
9Kに至って電気抵抗がゼロになることが確認された。In addition, an example carried out by the same means as Example 1-
In the sintered bodies of Example 2 and Example 3, the superconducting phenomenon started at an absolute temperature of about 91, similar to the case of Example 1, and
It was confirmed that the electrical resistance became zero at 9K.
なお、Y t O3が5no1%未ii’4,30mo
1%超過、5rCOsが20mo1%未id4,50m
o1%超過、CuOが30mo1%未満、65mo1%
超過、では、超電導を生じる焼結体を得ることができな
かった。In addition, Y t O3 is 5no1% or less ii'4,30mo
Exceeds 1%, 5rCOs is less than 20mo1% id4,50m
Exceeding o1%, CuO less than 30mo1%, 65mo1%
In excess, it was not possible to obtain a sintered body that produced superconductivity.
要は、出発物質換算で第1成分(A1)が5〜30mo
1%、第2成分(A2)が20〜50mo1%、第3成
分(A2)が30〜65mo1%であれば液体窒素で抵
抗ゼロとなる焼結体が得られることが判った。In short, the first component (A1) is 5 to 30 mo in terms of starting material.
1%, the second component (A2) is 20 to 50 mo1%, and the third component (A2) is 30 to 65 mo1%, it has been found that a sintered body with zero resistance can be obtained in liquid nitrogen.
すなわち、焼結体を構成する成分のAn(AIAt
A3) Oにおける、A1 At A3において、
A、がlO〜60原子%、原子炉20〜50原子%、
A 3が30〜65原子%であれば、斜方晶を含むKf
fiNiI?4構造体を持つ超電導体が得られることが
判った。That is, the component An (AIAt) constituting the sintered body
A3) In O, A1 At A3,
A, is lO~60 at%, nuclear reactor 20~50 at%,
If A3 is 30 to 65 at%, Kf containing orthorhombic crystals
fiNiI? It was found that a superconductor having 4 structures can be obtained.
更に、実施例−1の組成条件及び製造条件のらのについ
て、Y2O3粉末と5rCO0粉末との仮焼成のl温度
を900°CにしてCuO粉末を加えての本焼結の温度
を変えて調べた結果、950°C−t200℃の温度に
おいて本焼結すれば所望の超電導体を確実に得ることが
できた。Furthermore, the composition conditions and manufacturing conditions of Example-1 were investigated by changing the temperature of preliminary sintering of Y2O3 powder and 5rCO0 powder to 900 °C and the temperature of main sintering with addition of CuO powder. As a result, the desired superconductor could be reliably obtained by main sintering at a temperature of 950°C-t200°C.
しかし、温度が950℃未満、1200℃超過では所望
の超電導現象を生ずる焼結体を安定して得ることができ
なかった。However, if the temperature is lower than 950°C or higher than 1200°C, a sintered body that produces the desired superconducting phenomenon cannot be stably obtained.
また、本焼成の温度を約1050℃にして、Y2O3扮
末とSrCO3粉末との仮焼成の温度を変えて調べた結
果、約800℃以上で且つ本焼成の温度以下の温度にて
加熱(約10分間以上)して仮焼成しておけば、CuO
粉末を加えての本焼成時において、反応がゆるやかとな
って、割れ、歪の生じない品質の安定した焼結体が得ら
れることが判っ ノじ。In addition, as a result of setting the main firing temperature to about 1050°C and changing the temperature of the preliminary firing of Y2O3 powder and SrCO3 powder, it was found that heating at a temperature of about 800°C or higher and below the main firing temperature (about CuO
It has been found that during main firing after adding powder, the reaction is gradual and a sintered body of stable quality without cracking or distortion can be obtained.
以上のことから、本焼成の温度以下の条件で、まず、2
つの成分群に属する元素を主体とした複数種類の粉末を
混合して仮焼成(熱処理)し、これを粉砕して得た加工
粉末に残りの成分群に属する元素を主体とした粉末を加
えて得た混合粉を用いて本焼成すれば品質の安定した焼
結体すなわち超7[導体が得られることが判った。From the above, first, under the conditions below the main firing temperature,
Mix multiple types of powders mainly composed of elements belonging to one component group, pre-calcined (heat treated), and add powders mainly composed of elements belonging to the remaining component groups to the processed powder obtained by pulverizing the mixture. It has been found that if the obtained mixed powder is used for main firing, a sintered body of stable quality, that is, a super 7 [conductor] can be obtained.
G9発明の効果
以上のような本発明による超電導体は、液体窒素温度(
77K)において完全に超電導状態となる。Effects of the G9 Invention The superconductor according to the present invention as described above has a temperature of liquid nitrogen (
It becomes completely superconducting at 77K).
しかも、An(AI A2 A3) Oの焼結体
における出発物質に、イツトリウム(Y)を主体とした
第1成分(A1)、ストロンチウム(Sr)に代表され
る元素と略同半径のイオン半径を存ずる元素を主体とし
た第2成分(A2)、銅(Cu)に代表される元素と略
同半径のイオン半径を存する元素を主体とした第3成分
(A3)、からなる材料の粉末を用いており、その仮焼
成に際しては、本焼成(950〜1200°C)の温度
より低い温度にて、3つの成分のうちの2つの成分(群
)に該当する複数種類の粉末からなる混合粉末を熱処理
(仮焼成)して得、この加工粉末に残りの成分(群)に
該当する粉末を加えた混合粉を用いて本焼成する乙ので
あるから、割れ、歪がなく、しかも特性の安定した焼成
体、すなわち超電導体を容易に得ることができる。Moreover, the starting material in the sintered body of An(AI A2 A3) O is the first component (A1) mainly composed of yttrium (Y), which has an ionic radius approximately the same as that of the element represented by strontium (Sr). Using powder of a material consisting of a second component (A2) mainly consisting of an element that exists in the present invention, and a third component (A3) mainly consisting of an element whose ionic radius is approximately the same as that of an element represented by copper (Cu). During the preliminary firing, a mixed powder consisting of multiple types of powder corresponding to two of the three components (groups) is mixed at a temperature lower than the temperature of the main firing (950 to 1200°C). The powder is obtained by heat treatment (preliminary firing), and then the powder is mixed with powder corresponding to the remaining components (group) and then the final firing is performed, so there is no cracking or distortion, and the properties are stable. A fired body, that is, a superconductor, can be easily obtained.
現在明らかにされている超電導体は、ヘリウムガスを液
化した冷却剤で冷却しなければなら「、液体ヘリウムの
温度は4.2にで、しかむ希少材料で高(1!1であり
、且つ液化コストも高いため、超電導材料の実用化の壁
となっていた。The currently discovered superconductor requires cooling of helium gas with a liquefied coolant. The high cost of liquefaction has been a barrier to the practical application of superconducting materials.
しかし、液体窒素はどこででも、しかも安く人手でき、
従来の実用化の壁は完全に取り除かれ、特に電力、運輸
等に関連した電気抵抗5及び精密計測素子、その他エネ
ルギー変換などの分野に利用可能となる等極めて優れた
効果を発揮する。However, liquid nitrogen can be used anywhere and cheaply by hand.
The conventional barriers to practical application have been completely removed, and the present invention exhibits extremely excellent effects, such as being able to be used in fields such as electrical resistance 5 and precision measurement elements, particularly related to electric power, transportation, etc., and other fields such as energy conversion.
第1図は本発明の焼結体の抵抗値測定の方法を説明する
ための説明図、第2図は本発明の焼結体の絶対温度(K
)に対4−ろ抵抗値(10−3Ωc m )の特性曲線
図を示す。
a、a′ ・・電流供給用端子、b、b’ ・・・電圧
測定端子、S・・・焼結体。Figure 1 is an explanatory diagram for explaining the method of measuring the resistance value of the sintered body of the present invention, and Figure 2 is the absolute temperature (K) of the sintered body of the present invention.
) is a characteristic curve diagram of the resistance value (10-3 Ωcm) versus 4-Ωcm. a, a'...terminals for current supply, b, b'...voltage measurement terminals, S...sintered body.
Claims (1)
A_2)は、Sr,Caの元素のうち少なくとも1種類
以上の元素を有し、 第3成分(A_3)は、Cu,Zn,Ni,Co.Fe
,Pd,Ag,Cdの元素のうち少なくとも1種類以上
の元素を有し、 前記3つの成分(A_1,A_2,A_3)のうちのい
ずれか2つの成分を選択すると共にこれらの成分に属す
る元素を主体とした複数種類の粉末を混合して混合粉末
を得、該混合粉末を本焼成の温度より低い温度にて仮焼
成し、該仮焼成物を粉砕して加工粉末を得る工程と、 該加工粉末と残りの成分に属する元素を主体とした粉末
とを混合して混合粉を得、該混合粉を加圧して成形体を
得る工程と、 該成形体を酸化性雰囲気中で、且つ950℃〜1200
℃の範囲の温度で本焼成して斜方晶を含むK_2NiF
_4構造体を有する焼結体を形成する工程とからなり、 該焼結体がA_1,A_2,A_3及び酸素(0)の成
分からなり、且つA_1−A_2−A_3における構成
が、A_1を、10≦A_1≦60原子% A_2を、20≦A_2≦50原子% A_3を、30≦A_3≦65原子% であることを特徴とする超電導体の製造方法。[Claims] The first component (A_1) has the element Y, and the second component (A_1) has the element Y.
A_2) contains at least one element among Sr and Ca, and the third component (A_3) contains Cu, Zn, Ni, Co. Fe
, Pd, Ag, and Cd, and select any two of the three components (A_1, A_2, A_3) and select the elements belonging to these components. A step of mixing multiple types of main powder to obtain a mixed powder, pre-calcining the mixed powder at a temperature lower than the main firing temperature, and pulverizing the pre-calcined product to obtain a processed powder; A step of mixing the powder and a powder mainly composed of elements belonging to the remaining components to obtain a mixed powder, and pressurizing the mixed powder to obtain a molded body, and heating the molded body in an oxidizing atmosphere at 950°C ~1200
K_2NiF containing orthorhombic crystals by main firing at a temperature in the range of ℃
a step of forming a sintered body having a _4 structure, the sintered body is composed of components A_1, A_2, A_3 and oxygen (0), and the configuration of A_1-A_2-A_3 is such that A_1 is 10 A method for producing a superconductor, characterized in that ≦A_1≦60 atomic %, A_2 satisfies 20≦A_2≦50 atomic %, and A_3 satisfies 30≦A_3≦65 atomic %.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62163254A JPH0214868A (en) | 1987-06-30 | 1987-06-30 | Production of superconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62163254A JPH0214868A (en) | 1987-06-30 | 1987-06-30 | Production of superconductor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0214868A true JPH0214868A (en) | 1990-01-18 |
Family
ID=15770299
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62163254A Pending JPH0214868A (en) | 1987-06-30 | 1987-06-30 | Production of superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0214868A (en) |
-
1987
- 1987-06-30 JP JP62163254A patent/JPH0214868A/en active Pending
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