JPH0825249B2 - Bismuth superconducting-precious metal laminate - Google Patents
Bismuth superconducting-precious metal laminateInfo
- Publication number
- JPH0825249B2 JPH0825249B2 JP2195551A JP19555190A JPH0825249B2 JP H0825249 B2 JPH0825249 B2 JP H0825249B2 JP 2195551 A JP2195551 A JP 2195551A JP 19555190 A JP19555190 A JP 19555190A JP H0825249 B2 JPH0825249 B2 JP H0825249B2
- Authority
- JP
- Japan
- Prior art keywords
- based superconducting
- thickness
- noble metal
- laminate
- superconducting layer
- 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
- 229910052797 bismuth Inorganic materials 0.000 title claims description 16
- JCXGWMGPZLAOME-UHFFFAOYSA-N bismuth atom Chemical compound [Bi] JCXGWMGPZLAOME-UHFFFAOYSA-N 0.000 title claims description 16
- 239000010970 precious metal Substances 0.000 title description 5
- 229910000510 noble metal Inorganic materials 0.000 claims description 39
- 239000000758 substrate Substances 0.000 claims description 31
- 230000007423 decrease Effects 0.000 claims description 4
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 18
- 239000002887 superconductor Substances 0.000 description 17
- 239000000843 powder Substances 0.000 description 10
- 239000007788 liquid Substances 0.000 description 9
- 229910052757 nitrogen Inorganic materials 0.000 description 9
- KFZMGEQAYNKOFK-UHFFFAOYSA-N Isopropanol Chemical compound CC(C)O KFZMGEQAYNKOFK-UHFFFAOYSA-N 0.000 description 6
- 238000010304 firing Methods 0.000 description 6
- 239000000203 mixture Substances 0.000 description 6
- 229910052751 metal Inorganic materials 0.000 description 5
- 239000002184 metal Substances 0.000 description 5
- 238000001816 cooling Methods 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 239000011812 mixed powder Substances 0.000 description 4
- 230000035939 shock Effects 0.000 description 4
- 239000012298 atmosphere Substances 0.000 description 3
- KDLHZDBZIXYQEI-UHFFFAOYSA-N palladium Substances [Pd] KDLHZDBZIXYQEI-UHFFFAOYSA-N 0.000 description 3
- 239000002002 slurry Substances 0.000 description 3
- 229910004247 CaCu Inorganic materials 0.000 description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 2
- 239000011575 calcium Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 230000000052 comparative effect Effects 0.000 description 2
- 239000010949 copper Substances 0.000 description 2
- 238000005336 cracking Methods 0.000 description 2
- 239000013078 crystal Substances 0.000 description 2
- 239000011888 foil Substances 0.000 description 2
- -1 for example Substances 0.000 description 2
- 229910052737 gold Inorganic materials 0.000 description 2
- 238000002595 magnetic resonance imaging Methods 0.000 description 2
- 239000001301 oxygen Substances 0.000 description 2
- 229910052760 oxygen Inorganic materials 0.000 description 2
- 229910052763 palladium Inorganic materials 0.000 description 2
- 239000011802 pulverized particle Substances 0.000 description 2
- 238000010791 quenching Methods 0.000 description 2
- 230000000171 quenching effect Effects 0.000 description 2
- 239000002994 raw material Substances 0.000 description 2
- 229910052709 silver Inorganic materials 0.000 description 2
- 229910015902 Bi 2 O 3 Inorganic materials 0.000 description 1
- 229910015901 Bi-Sr-Ca-Cu-O Inorganic materials 0.000 description 1
- OYPRJOBELJOOCE-UHFFFAOYSA-N Calcium Chemical compound [Ca] OYPRJOBELJOOCE-UHFFFAOYSA-N 0.000 description 1
- 241000219122 Cucurbita Species 0.000 description 1
- 235000009852 Cucurbita pepo Nutrition 0.000 description 1
- MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 description 1
- 238000002441 X-ray diffraction Methods 0.000 description 1
- 150000004703 alkoxides Chemical class 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910052787 antimony Inorganic materials 0.000 description 1
- WATWJIUSRGPENY-UHFFFAOYSA-N antimony atom Chemical compound [Sb] WATWJIUSRGPENY-UHFFFAOYSA-N 0.000 description 1
- 238000001354 calcination Methods 0.000 description 1
- 229910052791 calcium Inorganic materials 0.000 description 1
- 150000004649 carbonic acid derivatives Chemical class 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 229910001882 dioxygen Inorganic materials 0.000 description 1
- 238000007606 doctor blade method Methods 0.000 description 1
- 238000001035 drying Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 150000004679 hydroxides Chemical class 0.000 description 1
- 238000007654 immersion Methods 0.000 description 1
- 229910001026 inconel Inorganic materials 0.000 description 1
- 239000013067 intermediate product Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910044991 metal oxide Inorganic materials 0.000 description 1
- 150000002823 nitrates Chemical class 0.000 description 1
- 239000012299 nitrogen atmosphere Substances 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229910052697 platinum Inorganic materials 0.000 description 1
- 238000012827 research and development Methods 0.000 description 1
- 238000005245 sintering Methods 0.000 description 1
- 239000007921 spray Substances 0.000 description 1
- 238000005507 spraying Methods 0.000 description 1
- 229910052712 strontium Inorganic materials 0.000 description 1
- CIOAGBVUUVVLOB-UHFFFAOYSA-N strontium atom Chemical compound [Sr] CIOAGBVUUVVLOB-UHFFFAOYSA-N 0.000 description 1
- 238000007751 thermal spraying Methods 0.000 description 1
- 238000003325 tomography Methods 0.000 description 1
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
- Laminated Bodies (AREA)
- Compositions Of Oxide Ceramics (AREA)
- Inorganic Compounds Of Heavy Metals (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、貴金属基体上にビスマス系超電導層が形成
されてなるビスマス系超電導−貴金属積層体に関する。TECHNICAL FIELD The present invention relates to a bismuth-based superconducting-noble metal laminate in which a bismuth-based superconducting layer is formed on a noble metal substrate.
近年、酸化物超電導体は高い臨界温度(Tc)を示すこ
とで注目を集め、電力分野、核磁気共鳴コンピュータ断
層診断装置(MRI:Magnetic Resonance Imaging)、磁気
シールド等の各分野での用途が期待されている。酸化物
超電導体の中でもBi−Sr−Ca−Cu−O酸化物等のビスマ
ス系(以下、単にBi系とする。)超電導体は、特にTcが
より高くそれを利用する研究開発が盛んである。In recent years, oxide superconductors have attracted attention due to their high critical temperature (Tc), and are expected to be used in various fields such as electric power, magnetic resonance computerized tomography (MRI: Magnetic Resonance Imaging), and magnetic shielding. Has been done. Among oxide superconductors, bismuth-based (hereinafter simply referred to as Bi-based) superconductors such as Bi-Sr-Ca-Cu-O oxides have a particularly high Tc, and research and development using them are actively conducted. .
従来から、金属やセラミックス等の基板上に酸化物超
電導体層を形成して酸化物超電導体を構造体に利用する
ことが提案されている。金属基板上にBi系超電導体層を
形成する方法も各種提案され、例えば特開昭64−82597
号公報や特開平1−252533号公報では、Ag、Au、Pt等貴
金属を基板としてその上にBi系超電導体層を積層するこ
とが提案されている。Conventionally, it has been proposed to use an oxide superconductor for a structure by forming an oxide superconductor layer on a substrate such as metal or ceramics. Various methods for forming a Bi-based superconductor layer on a metal substrate have been proposed, for example, Japanese Patent Laid-Open No. 64-82597.
In Japanese Patent Laid-Open No. 1-252533 and Japanese Patent Laid-Open No. 1-252533, it is proposed that a noble metal such as Ag, Au, or Pt is used as a substrate and a Bi-based superconductor layer is laminated thereon.
しかし、Bi系超電導体とは化学的に安定とされ塑性変
形性を有する貴金属はBi系超電導層との密着性もよく良
好に積層体が形成されるが、室温から900℃の熱膨張係
数は、貴金属が20〜22×10-6/℃であり、Bi系超電導体
が13〜14×10-6/℃であるため、超電導特性を発現させ
る液体窒素温度への急冷が繰り返されるような冷却速度
の大きいサイクル状態に適用する場合には、両者の熱膨
張差により積層界面に大きな内部応力が残留する。However, noble metals that are chemically stable and have plastic deformability with the Bi-based superconductor have good adhesion to the Bi-based superconducting layer and form a good laminate, but the coefficient of thermal expansion from room temperature to 900 ° C is , The noble metal is 20-22 × 10 -6 / ° C, and the Bi-based superconductor is 13-14 × 10 -6 / ° C, so that the rapid cooling to the liquid nitrogen temperature that develops superconducting properties is repeated. When applied to a cycle state with a high speed, a large internal stress remains at the laminated interface due to the difference in thermal expansion between the two.
そのため、積層体にクラックが生じる等の耐熱衝撃性
が劣る等の問題があり、従来、その対処としてBi系超電
導層の厚さを薄くして発生応力を軽減することも行われ
ているが、Bi系超電導層を薄くすると磁気シールド能が
劣る等の新たな問題が生じることになる。Therefore, there is a problem such as inferior thermal shock resistance such as cracking in the laminated body, and conventionally, as a countermeasure, it is also possible to reduce the generated stress by reducing the thickness of the Bi-based superconducting layer, If the Bi-based superconducting layer is thinned, new problems such as poor magnetic shielding ability will occur.
発明者等は、貴金属基板上にBi系超電導体が積層形成
されたBi系超電導−貴金属積層体において発生する内部
応力が、特に該積層体の端部で局部的に顕著であること
を知見し、本発明を完成した。即ち、本発明は、貴金属
基板とBi系超電導層との熱膨張差による上記欠点を、超
電導層を薄くすることなく解消し耐熱衝撃性に優れ、超
電導特性が優れ高磁気シールド能を有するBi系超電導−
貴金属積層体を提供する。The inventors have found that the internal stress generated in a Bi-based superconducting-noble metal laminate in which a Bi-based superconductor is laminated on a noble metal substrate is locally significant especially at the end of the laminate. The present invention has been completed. That is, the present invention eliminates the above-mentioned drawbacks due to the difference in thermal expansion between the noble metal substrate and the Bi-based superconducting layer, eliminates the superconducting layer without making it thin, and has excellent thermal shock resistance. Superconductivity
A precious metal laminate is provided.
本発明によれば、厚さ300μm〜2mmの貴金属基体上に
厚さ100μm〜5mmのビスマス系超電導層が形成されてな
るビスマス系超電導−貴金属積層体において、該ビスマ
ス系超電導層の肉厚が、該積層体端部における該積層体
長さの1%〜5%の領域で、該積層体端部方向に減少し
てなることを特徴とるビスマス系超電導−貴金属積層体
が提供される。According to the present invention, in a bismuth-based superconducting-noble metal laminate in which a bismuth-based superconducting layer having a thickness of 100 μm to 5 mm is formed on a noble metal substrate having a thickness of 300 μm to 2 mm, the thickness of the bismuth-based superconducting layer is There is provided a bismuth-based superconducting-noble metal laminate characterized by being reduced in the end portion of the laminate in the region of 1% to 5% of the length of the laminate.
以下、本発明をさらに詳細に説明する。 Hereinafter, the present invention will be described in more detail.
本発明のビスマス系超電導−貴金属積層体の基体は、
いわゆる貴金属であるAg、Au、Pt、Pd(パラジウム)及
びこれらの合金が用いられ、工業的にはAgが好適であ
る。The substrate of the bismuth-based superconducting-noble metal laminate of the present invention is
So-called noble metals Ag, Au, Pt, Pd (palladium) and their alloys are used, and Ag is industrially preferable.
本発明におけるBi系超電導体としては、組成が限定さ
れるものでなく、例えば低Tc相のBi2Sr2CaCu2Ox、高Tc
相のBi2Sr2Ca2Cu3Oxに代表される組成、鉛(Pb)、アン
チモン(Sb)等を含有する組成、定比組成からずれた組
成、主要元素を他の元素で一部または全部置換した組成
等のいずれのBi系超電導体であってもよい。The composition of the Bi-based superconductor in the present invention is not limited, and examples include low Tc phase Bi 2 Sr 2 CaCu 2 O x and high Tc.
Composition represented by Bi 2 Sr 2 Ca 2 Cu 3 O x , composition containing lead (Pb), antimony (Sb), etc., composition deviating from stoichiometric composition, main elements partially with other elements Alternatively, it may be any Bi-based superconductor having a composition in which all are replaced.
本発明の積層体は、球体の如く端部を有さない形状体
を除き、端部を有する形状体であれば全てに適用でき、
特に形状は限定されない。一般的には、円筒状、平板状
のものが挙げられる。The laminated body of the present invention can be applied to any shape body having an end portion, except a shape body having no end portion such as a sphere,
The shape is not particularly limited. Generally, a cylindrical shape and a flat plate shape are mentioned.
円筒状体としては、横断面形状が円形だけに限定され
ず、楕円形、多角形、瓢箪形のもの、複数個の円筒体が
結合された形状等各種の横断面形状を有するものが含ま
れ、また、長手方向の形態も特に限定されず、直円筒
状、コニカル状等各種形態を採ることができる。更にま
た、貫通状でも、有底のいずれでもよく、底は平底、丸
底等特に限定されない。The cylindrical body is not limited to a circular cross-sectional shape, but includes ones having various cross-sectional shapes such as an elliptical shape, a polygonal shape, a gourd shape, and a shape in which a plurality of cylindrical bodies are combined. Also, the form in the longitudinal direction is not particularly limited, and various forms such as a right cylindrical shape and a conical shape can be adopted. Furthermore, it may be penetrating or bottomed, and the bottom is not particularly limited, such as a flat bottom or a round bottom.
また、平板状体としては、正方形に限定されず、長方
形、多角形、円、楕円、雲形等あらゆる形状にも適用さ
れる。Further, the plate-like body is not limited to a square, but may be any shape such as a rectangle, a polygon, a circle, an ellipse, and a cloud.
本発明において、貴金属基体上に形成するBi系超電導
層は、Bi系超電導体原料粉末、例えばビスマス、カルシ
ウム、ストロンチウム及び銅の金属酸化物,炭酸塩,水
酸化物,金属アルコキシド及び硝酸塩の粉末を焼成によ
り酸化物超電導体を構成するように配合した混合粉末、
その混合粉末を800〜950℃で仮焼したBi系超電導結晶相
からなる粉末、混合粉末を400〜800℃で仮焼し焼成によ
り超電導特性を発現するようにした仮焼中間生成物粉
末、混合粉末のフリット粉末またはこれらの混合粉末等
を用い、スプレー塗布法、パウダー塗布法、ドクターブ
レード法、溶射法等の公知のいずれの成形法によっても
よい。In the present invention, the Bi-based superconducting layer formed on the noble metal substrate is a Bi-based superconductor raw material powder, for example, powders of bismuth, calcium, strontium and copper metal oxides, carbonates, hydroxides, metal alkoxides and nitrates. A mixed powder compounded to form an oxide superconductor by firing,
A powder consisting of a Bi-based superconducting crystal phase obtained by calcining the mixed powder at 800 to 950 ° C, a calcined intermediate product powder that is calcined at 400 to 800 ° C so as to exhibit superconducting properties by firing, and mixed. Any known forming method such as a spray coating method, a powder coating method, a doctor blade method, or a thermal spraying method may be used using a powder frit powder or a mixed powder thereof.
本発明の積層体端部とは、例えば、貫通円筒状体の上
下部や平板状体の全周辺部等をいう。The laminated body end portion of the present invention refers to, for example, the upper and lower portions of the through cylindrical body or the entire peripheral portion of the flat body.
従来の超電導積層体は、第4図に示したように、例え
ばAg基体2上にBi系超電導層3が積層された積層体1に
おいて、基体2の端部4及びBi系超電導層の端部5は積
層体全域と同様に形成されていた。As shown in FIG. 4, the conventional superconducting layered body has, for example, a layered body 1 in which a Bi type superconducting layer 3 is layered on an Ag substrate 2, and the end 4 of the base 2 and the end of the Bi type superconducting layer No. 5 was formed similarly to the whole laminated body.
一方、本発明は、上記端部から所定距離に位置する領
域のBi系超電導層肉厚を他の領域より薄く形成し、Bi系
超電導体と貴金属基体との熱膨張係数の差により生ずる
局部的内部応力を緩和する。この場合、Bi系超電導層の
肉厚の減少形態は、各種の方式を適用することができる
が、例えば、第1図または第2図に示したように、Bi系
超電導層3の端部5がAg基体2の端部4方向に直線的
に、または凹形状に傾斜して、積層体端部からの所定領
域に位置する部分のBi系超電導層を該端部方向に減少さ
せるように形成して積層体の他の領域の肉厚より薄くす
るのが好ましい。On the other hand, the present invention, the thickness of the Bi-based superconducting layer in the region located a predetermined distance from the end is formed thinner than other regions, the local expansion caused by the difference in thermal expansion coefficient between the Bi-based superconductor and the noble metal substrate. Relieves internal stress. In this case, various methods can be applied to reduce the thickness of the Bi-based superconducting layer. For example, as shown in FIG. 1 or FIG. Is formed so as to be linearly or concavely inclined in the direction of the end 4 of the Ag substrate 2 so as to reduce the Bi-based superconducting layer in a portion located in a predetermined region from the end of the laminated body in the direction of the end. Then, it is preferable to make the thickness thinner than the other regions of the laminate.
また、本発明の積層体において、上記Bi系超電導層の
肉厚を端部の領域で減少させると同時に、貴金属基体の
肉厚も同一の端部の領域で減少させてもよい。例えば、
第3図に示したように、Bi系超電導層3の端部5を第1
図と同様に直線的に傾斜させると共に、Ag基体2の端部
4をやや曲率を持たせて肉厚を減少させることができ
る。Further, in the laminated body of the present invention, the thickness of the Bi-based superconducting layer may be reduced in the end regions, and at the same time, the thickness of the noble metal substrate may be reduced in the same end regions. For example,
As shown in FIG. 3, the end 5 of the Bi-based superconducting layer 3 is first
Similar to the figure, the wall thickness can be reduced by linearly inclining the end 4 of the Ag substrate 2 and giving it a slight curvature.
更にまた、Bi系超電導層を積層体の端部方向に層厚を
減少するときに端部が貴金属基体部分のみとなる場合
は、その部分に局部的応力が発生するようになり、好ま
しくない。従って、そのような状態を回避するか、或い
は、貴金属基体のみとなる部分の基体の肉厚を端部方向
に減少するようにするのが好ましい。Furthermore, when the thickness of the Bi-based superconducting layer is reduced toward the end of the laminated body, if the end is only the noble metal base portion, local stress will be generated in that portion, which is not preferable. Therefore, it is preferable to avoid such a state, or to reduce the thickness of the base body in the portion that is only the noble metal base body in the end direction.
本発明において、上記のように、積層体の端部の所定
領域で、他の領域よりBi系超電導層または/及び貴金属
基体の肉厚が減少することになる。従って、本発明で
は、貴金属基体の肉厚に対するBi系超電導層の肉厚の比
は、積層体全域において一定となるか、または端部方向
に減少するようになる。貴金属基体とBi系超電導層との
肉厚比が一定の場合は、下記するように約0.05〜17の範
囲で、使用目的等で適宜選択することができる。また、
減少させる場合においても、原則的には上記範囲内とす
るのが好ましい。In the present invention, as described above, the thickness of the Bi-based superconducting layer and / or the noble metal substrate is reduced in the predetermined region at the end of the laminated body as compared with other regions. Therefore, in the present invention, the ratio of the thickness of the Bi-based superconducting layer to the thickness of the noble metal substrate is constant over the entire laminate or decreases in the end direction. When the thickness ratio between the noble metal substrate and the Bi-based superconducting layer is constant, it can be appropriately selected according to the purpose of use, etc. within the range of about 0.05 to 17 as described below. Also,
Even in the case of decreasing the amount, it is preferable in principle to set it within the above range.
Bi系超電導層の肉厚を減少させる端部から所定距離に
位置する領域は、各端部から、例えば、円筒状等の長軸
を有する形状体にあっては該長軸方向の長さの1%〜5
%、好ましくは2%〜5%の長さ、また、平板状体にあ
っては対向辺間の距離の約1%〜5%、好ましくは2%
〜5%の長さを有する位置とするのが好ましい。1%よ
り狭い位置の領域だけでは、端部の応力軽減が不十分と
なり好ましくなく、また5%を超えた位置の領域では、
Bi系超電導層と貴金属基体との界面に発生する内部応力
がほぼ一定となり局部的応力による影響がない。The region located at a predetermined distance from the end portion that reduces the thickness of the Bi-based superconducting layer is, from each end portion, for example, in the case of a shape body having a long axis such as a cylindrical shape, the length in the long axis direction 1% to 5
%, Preferably 2% to 5%, and about 1% to 5%, preferably 2% of the distance between opposing sides in the case of a flat plate.
It is preferable that the position has a length of ˜5%. If the area is narrower than 1%, stress reduction at the end is insufficient, which is not preferable, and if the area exceeds 5%,
The internal stress generated at the interface between the Bi-based superconducting layer and the noble metal substrate is almost constant and is not affected by the local stress.
本発明の積層体において、貴金属基体は端部の所定領
域を除き300μm〜2mmの範囲の厚さが好ましい。300μ
m未満では基体としての強度が不十分であり、2mmを超
えた場合はコスト的に実用的でない。Bi系超電導層の厚
さは、端部の所定領域を除き100μm〜5mmの範囲の厚さ
が好ましい。100μm未満では超電導特性の発現が不十
分となるおそれがあり、特に磁気シールド材としては不
適当である。5mmを超える場合はBi系超電導層の剥離や
クラックの発生のおそれがあり、また、焼結が均一に進
行せず十分な超電導特性が得られないこともあり、好ま
しくない。In the laminated body of the present invention, the noble metal substrate preferably has a thickness in the range of 300 μm to 2 mm except for a predetermined region at the end. 300μ
If it is less than m, the strength of the substrate is insufficient, and if it exceeds 2 mm, it is not practical in terms of cost. The thickness of the Bi-based superconducting layer is preferably in the range of 100 μm to 5 mm except for the predetermined region at the end. If it is less than 100 μm, the superconducting properties may be insufficiently expressed, and it is particularly unsuitable as a magnetic shield material. If it exceeds 5 mm, peeling or cracking of the Bi-based superconducting layer may occur, and sintering may not proceed uniformly, and sufficient superconducting properties may not be obtained, which is not preferable.
本発明においては、上記のように貴金属金属基体上に
Bi系超電導体原料による層を形成し、乾燥及び焼成し
て、金属基体及びBi系超電導層とが一体化された酸化物
超電導積層体を得ることができる。また、超電導層にAg
またはAg2Oを、好ましくは0.5〜10重量%添加して焼成
することにより、より均質な超電導層を得ることができ
る。In the present invention, as described above, on the noble metal substrate
It is possible to obtain an oxide superconducting laminate in which the metal base and the Bi-based superconducting layer are integrated by forming a layer of the Bi-based superconducting raw material, drying and firing. In addition, Ag is added to the superconducting layer.
Alternatively, a more uniform superconducting layer can be obtained by adding Ag 2 O, preferably in an amount of 0.5 to 10% by weight, and baking it.
本発明における焼成は、酸素または空気中の酸素含有
ガス雰囲気中で行う。焼成温度は、一般に860〜920℃が
好ましい。The firing in the present invention is performed in an atmosphere of oxygen or an oxygen-containing gas in air. Generally, the firing temperature is preferably 860 to 920 ° C.
また、本発明において、貴金属基体とBi系超電導層と
の間に中間層を形成してもよい。その場合、好ましくは
Bi系超電導体を構成する複合酸化物に基板に用いる貴金
属を含有させた貴金属−Bi系超電導複合酸化物を中間層
として形成するのがよく、貴金属の含有量を基体からBi
系超電導層へと逓減するようにすればより好ましい。こ
の中間層の厚さは20μm〜1mmの範囲が好ましく、Bi系
超電導層と共に積層体端部の領域で同様に、肉厚を減少
させるのが好ましい。Further, in the present invention, an intermediate layer may be formed between the noble metal substrate and the Bi-based superconducting layer. In that case, preferably
It is preferable to form a noble metal-Bi-based superconducting complex oxide containing a noble metal used for the substrate in the complex oxide constituting the Bi-based superconductor as the intermediate layer.
It is more preferable to gradually reduce to the system superconducting layer. The thickness of this intermediate layer is preferably in the range of 20 μm to 1 mm, and it is also preferable to reduce the thickness in the region of the end of the laminate together with the Bi-based superconducting layer.
本発明のBi系超電導−貴金属積層体は、貴金属基体上
にBi系超電導層を形成し一体化し、且つその積層体端部
の所定領域においてBi系超電導層の層厚を減少させるこ
とにより、従来、該端部において局部的に発生し超電導
体にクラックを生じさせた不都合を防止することができ
る。Bi-based superconducting-precious metal laminate of the present invention, by forming and integrating a Bi-based superconducting layer on the precious metal substrate, and by reducing the layer thickness of the Bi-based superconducting layer in a predetermined region of the end of the laminate, conventional. It is possible to prevent the inconvenience of locally occurring cracks in the superconductor at the ends.
このため本発明のBi系超電導−貴金属積層体は、超電
導特性を発現させる液体窒素中への浸漬、取り出し等急
冷サイクルで繰り返して使用しても剥離やクラックが生
じることがない。Therefore, the Bi-based superconducting-noble metal laminate of the present invention does not cause peeling or cracks even when it is repeatedly used in a rapid cooling cycle such as immersion in liquid nitrogen that exhibits superconducting properties and removal.
以下、本発明を実施例により、さらに詳しく説明す
る。但し、本発明は、下記実施例に限定されるものでな
い。Hereinafter, the present invention will be described in more detail with reference to examples. However, the present invention is not limited to the following examples.
実施例1〜3及び比較例1〜2 Bi2O3,SrCO3,CaCO3及びCuOの粉末を1:2:1:2のモル比
で調合し、乾式ミルにより10時間混合した。混合粉末を
800℃で10時間大気中で仮焼し、仮焼粉末をイソプロピ
ルアルコール中ZrO2玉石で20時間粉砕した。得られた粉
砕粒子の平均粒径は3μmで、X線回折から主たる結晶
相がBi2Sr2CaCu2Oy相であることが確認された。得られ
た粉砕粒子とイソプロピルアルコールとを所定の粘度に
なるように混合してスラリーを作成した。Examples 1 to 3 and Comparative Examples 1 to 2 Bi 2 O 3 , SrCO 3 , CaCO 3 and CuO powders were mixed at a molar ratio of 1: 2: 1: 2 and mixed for 10 hours by a dry mill. Mixed powder
The powder was calcined in the air at 800 ° C. for 10 hours, and the calcined powder was crushed with ZrO 2 boulders in isopropyl alcohol for 20 hours. The average particle size of the obtained pulverized particles was 3 μm, and it was confirmed by X-ray diffraction that the main crystal phase was Bi 2 Sr 2 CaCu 2 O y phase. The obtained pulverized particles and isopropyl alcohol were mixed so as to have a predetermined viscosity to prepare a slurry.
Ag製の厚さ500μmで、直径100mm、高さ450mmの円筒
基体の外側表面に上記スラリーを用いてスプレー塗布
し、円筒端部から20mmの範囲でスラリー厚さが端部方向
に減少するように塗布した。塗布後、酸素ガス雰囲気
下、890℃で1時間焼成した。Spray the above slurry onto the outer surface of a cylindrical substrate made of Ag and having a thickness of 500 μm and a diameter of 100 mm and a height of 450 mm, so that the slurry thickness decreases in the end direction in the range of 20 mm from the end of the cylinder. Applied. After coating, baking was performed at 890 ° C. for 1 hour in an oxygen gas atmosphere.
焼成後、850℃まで0.5℃/分の速度で降温し、850℃
で15時間保持した。その後窒素雰囲気中、400℃で10時
間熱処理した。得られたBi系超電導層の端部以外の厚さ
は300μmであった。また、円筒端部は、それぞれ第1
図〜第4図のいずれかの形態で、Bi系超電導層厚が減少
する端部からの領域は、第1表に示した。After firing, lower the temperature to 850 ° C at a rate of 0.5 ° C / min to 850 ° C.
Hold for 15 hours. Then, it heat-processed at 400 degreeC in nitrogen atmosphere for 10 hours. The thickness of the obtained Bi-based superconducting layer other than the end portion was 300 μm. Also, the cylindrical ends are respectively the first
The region from the end where the thickness of the Bi-based superconducting layer is reduced in any one of FIGS. 4 to 4 is shown in Table 1.
上記のようにして得られた円筒Bi系超電導−貴金属積
層体の磁気シールド能を、第5図に概要説明図を示した
磁気シールド能測定装置を用いて測定した。第5図にお
いて、液体窒素容器1内に液体窒素を満たし、得られた
積層体1を液体窒素中に浸漬して積層体が液体窒素温度
に達した後に、容器11の外側に配設した電磁石12で外部
磁場を印加して、円筒積層体内に配置したガウスメータ
13でバックグラウンドより増加し始める最大外部磁場ガ
ウス(G)を磁気シールド能として測定した。その後、
円筒積層体1を室内大気中に瞬時に取り出し、室温にな
るまで放置した後、再び液体窒素中に浸漬急冷する冷却
サイクルを繰り返し、磁気シールド能を測定した。The magnetic shield ability of the cylindrical Bi-based superconducting-noble metal laminate obtained as described above was measured by using the magnetic shield ability measuring apparatus whose schematic explanatory view is shown in FIG. In FIG. 5, the liquid nitrogen container 1 is filled with liquid nitrogen, and the obtained laminated body 1 is immersed in liquid nitrogen to reach the liquid nitrogen temperature. An external magnetic field is applied at 12, and the Gauss meter is placed inside the cylindrical laminated body.
At 13, the maximum external magnetic field Gauss (G), which starts to increase from the background, was measured as the magnetic shielding ability. afterwards,
The cylindrical laminate 1 was instantaneously taken out into the room atmosphere, allowed to stand at room temperature, then immersed in liquid nitrogen and rapidly cooled again, and the cooling cycle was repeated to measure the magnetic shielding ability.
この結果の冷熱サイクルによる磁気シールド能の変化
を第1表に示した。Table 1 shows the changes in the magnetic shielding ability as a result of the cooling / heating cycle.
実施例4 厚さ1.5mmで、300×300(mm)のインコネル製平板基
体上に、厚さ500μmのAg箔をガラスを用いて焼付け
た。そのAg箔上に、実施例1と同様にして端部以外は30
0μmの厚さにBi系超電導層を形成し、各辺端から6mmの
位置から端部方向にBi系超電導層を第1図の形態で減少
させた。 Example 4 An Ag foil having a thickness of 500 μm was baked using glass on a flat plate substrate made of Inconel having a thickness of 1.5 mm and a size of 300 × 300 (mm). On the Ag foil, in the same manner as in Example 1, except for the edges, 30
A Bi-based superconducting layer was formed in a thickness of 0 μm, and the Bi-based superconducting layer was reduced in the form of FIG.
得られた平板上Bi系超電導−貴金属積層体の液体窒素
中での磁気シールド能を測定した結果、30Gであった。
また、実施例1と同様の急冷サイクルを50回繰り返した
後の磁気シールド能は、30Gで変化が認められなかっ
た。The magnetic shielding ability of the obtained flat Bi-based superconducting-noble metal laminate in liquid nitrogen was 30 G.
Further, the magnetic shield ability after repeating the same quenching cycle as in Example 1 50 times was 30 G and no change was observed.
上記実施例及び比較例より、明らかなように端部から
所定の領域において、Bi系超電導層の層厚を減少させた
本発明のBi系超電導−貴金属積層体は、急冷サイクル後
においても超電導特性が劣化することなく、高磁気シー
ルドを示す。更にまた、Bi系超電導層の層厚を減少させ
ると共に貴金属基体厚さを減少させた実施例3における
積層体は、より一層の耐熱衝撃性に富むことが分かる。From the above Examples and Comparative Examples, it is clear that the predetermined region from the end portion has a Bi-based superconducting layer of the present invention in which the layer thickness of the Bi-based superconducting layer is reduced. Shows a high magnetic shield without deterioration. Furthermore, it can be seen that the laminated body in Example 3 in which the layer thickness of the Bi-based superconducting layer is reduced and the thickness of the noble metal substrate is reduced is further excellent in thermal shock resistance.
本発明のBi系超電導−貴金属積層体は、十分な超電導
特性を有すると共に、耐熱衝撃性にも優れ急冷サイクル
で繰り返し使用しても、磁気シールド能が低下すること
なく、磁気シールド用として有用である。The Bi-based superconducting-precious metal laminate of the present invention has sufficient superconducting properties, is also excellent in thermal shock resistance, and is repeatedly used in the quenching cycle, but the magnetic shielding ability does not decrease, and it is useful as a magnetic shield. is there.
第1図は本発明の一実施例のBi系超電導−貴金属積層体
の端部、第2図は本発明の他の実施例のBi系超電導−貴
金属積層体の端部、第3図は本発明の他の実施例のBi系
超電導−貴金属積層体の端部をそれぞれ示す断面説明図
である。第4図は従来の超電導−金属積層体の一例を示
す断面説明図である。第5図は本発明の一実施例で用い
る磁気シールド能測定装置の概要説明図である。 1……Bi系超電導−貴金属積層体 2……Ag基体、3……Bi系超電導層 4……Ag基体端部、5……Bi系超電導層端部 11……液体窒素容器、12……電磁石 13……ガウスメータFIG. 1 is an end portion of a Bi-based superconducting-noble metal laminate according to one embodiment of the present invention, FIG. 2 is an end portion of a Bi-based superconducting-noble metal laminate according to another embodiment of the present invention, and FIG. It is sectional explanatory drawing which shows each edge part of the Bi type | system | group superconducting-noble metal laminated body of the other Example of this invention. FIG. 4 is a sectional explanatory view showing an example of a conventional superconducting-metal laminate. FIG. 5 is a schematic explanatory view of a magnetic shield capacity measuring device used in one embodiment of the present invention. 1 …… Bi-based superconducting-noble metal laminate 2 …… Ag substrate, 3 …… Bi-based superconducting layer 4 …… Ag substrate end, 5 …… Bi-based superconducting layer end 11 …… Liquid nitrogen container, 12 …… Electromagnet 13 ... Gauss meter
Claims (2)
0μm〜5mmのビスマス系超電導層が形成されてなるビス
マス系超電導−貴金属積層体において、該ビスマス系超
電導層の肉厚が、該積層体端部における該積層体長さの
1%〜5%の領域で、該積層体端部方向に減少してなる
ことを特徴とするビスマス系超電導−貴金属積層体。1. A noble metal substrate having a thickness of 300 μm to 2 mm and a thickness of 10
In a bismuth-based superconducting-noble metal laminate in which a bismuth-based superconducting layer having a thickness of 0 μm to 5 mm is formed, the thickness of the bismuth-based superconducting layer is 1% to 5% of the length of the laminate at the end of the laminate. And a bismuth-based superconducting-noble metal laminate, which is reduced in the end direction of the laminate.
導層の肉厚の比が該積層体全域において一定、または端
部方向に減少してなる請求項(1)記載のビスマス系超
電導−貴金属積層体。2. A bismuth-based superconducting-noble metal laminate according to claim 1, wherein the ratio of the thickness of the bismuth-based superconducting layer to the thickness of the noble metal substrate is constant over the entire laminate or decreases toward the edges. body.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2195551A JPH0825249B2 (en) | 1990-07-24 | 1990-07-24 | Bismuth superconducting-precious metal laminate |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2195551A JPH0825249B2 (en) | 1990-07-24 | 1990-07-24 | Bismuth superconducting-precious metal laminate |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0480026A JPH0480026A (en) | 1992-03-13 |
| JPH0825249B2 true JPH0825249B2 (en) | 1996-03-13 |
Family
ID=16342988
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2195551A Expired - Lifetime JPH0825249B2 (en) | 1990-07-24 | 1990-07-24 | Bismuth superconducting-precious metal laminate |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0825249B2 (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5367927B1 (en) * | 2012-04-16 | 2013-12-11 | 古河電気工業株式会社 | Superconducting film-forming substrate, superconducting wire, and method of manufacturing superconducting wire |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0694198B2 (en) * | 1986-01-24 | 1994-11-24 | 日本発条株式会社 | Composite material consisting of graphite and metal |
| JP2649242B2 (en) * | 1988-03-31 | 1997-09-03 | 三井金属鉱業株式会社 | Superconducting ceramic laminate and its manufacturing method |
-
1990
- 1990-07-24 JP JP2195551A patent/JPH0825249B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0480026A (en) | 1992-03-13 |
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