JPH0224911A - Ceramic superconductor and manufacture thereof - Google Patents
Ceramic superconductor and manufacture thereofInfo
- Publication number
- JPH0224911A JPH0224911A JP63173348A JP17334888A JPH0224911A JP H0224911 A JPH0224911 A JP H0224911A JP 63173348 A JP63173348 A JP 63173348A JP 17334888 A JP17334888 A JP 17334888A JP H0224911 A JPH0224911 A JP H0224911A
- Authority
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- Japan
- Prior art keywords
- superconductor
- ceramic
- superconducting
- ceramic superconductor
- conductor
- Prior art date
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Classifications
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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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- Superconductors And Manufacturing Methods Therefor (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、セラミック超伝導体の構成および、その製造
方法に関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a structure of a ceramic superconductor and a method of manufacturing the same.
従来の技術
Ba−Y−Cu−0系などのセラミック超伝導体は、高
温まで超伝導現象が現われるため、高価な液体ヘリウム
や冷却器を用いる必要がないことから、各種分野での応
用が検討されている。Conventional technology Ceramic superconductors such as the Ba-Y-Cu-0 system exhibit superconductivity up to high temperatures, so they do not require the use of expensive liquid helium or coolers, and are therefore being considered for application in various fields. has been done.
超伝導体は、超伝導現象を利用した強力磁場形成のため
に大電流を流したさいなどに、なんらかの理由で一部分
の超伝導状態が破れたとき、その部分の温度が部分的に
上昇し、周辺部を加熱し、超伝導状態が波及的に消滅し
ていき、エネルギーが一気に熱となって放出されるクエ
ンチ現象を防止するため、すでに発明者らによって提案
されているような、超伝導は示さないが、電気伝導度が
低く、かつその温度変化が小さい導電体とのコンポジッ
トで使用する必要があった。When a part of a superconductor breaks its superconducting state for some reason, such as when a large current is passed through it to create a strong magnetic field using the superconducting phenomenon, the temperature of that part partially increases. In order to prevent the quench phenomenon, in which the superconducting state heats up the surrounding area, the superconducting state dissipates in a ripple manner, and the energy is released as heat all at once, superconducting, as already proposed by the inventors, is Although not shown, it was necessary to use it in a composite with a conductor that has low electrical conductivity and small temperature changes.
発明が解決しようとする課題
本発明ではクエンチ現象を防止し、かつ臨界電流の大き
いセラミック超伝導体の構成とその製造方法を提供する
ことを目的とする。Problems to be Solved by the Invention It is an object of the present invention to provide a structure of a ceramic superconductor that prevents the quench phenomenon and has a large critical current, and a method for manufacturing the same.
課題を解決するための手段
線状のセラミック超伝導体の断面において超伝導体磁器
層と超伝導を示さない導電体層とが外周面と平行に積層
された構造を有し、かつ超伝導体磁器の結晶粒子が、外
周面と平行に面配向性を何している構成とする。Means for Solving the Problems A linear ceramic superconductor has a structure in which a superconducting ceramic layer and a conductor layer that does not exhibit superconductivity are laminated parallel to the outer peripheral surface in a cross section, and the superconductor The porcelain crystal grains are oriented parallel to the outer circumferential surface.
もしくは、線状のセラミック超伝導体において超伝導体
磁器と超伝導を示さない導電体がおのおの連続し、かつ
混合された構造を存し、かつ超伝導体磁器の結晶粒子が
、外周面と平行に面配向性を有している構成とする。Alternatively, in a linear ceramic superconductor, the superconducting porcelain and the non-superconducting conductor have a continuous and mixed structure, and the crystal grains of the superconducting porcelain are parallel to the outer peripheral surface. The structure has a planar orientation.
また、その製造方法として、あらかじめ板状に成長した
、超伝導体磁器粒子と超伝導を示さない導電体粉末を出
発原料として用い、これにおのおのバインダを加えて混
練した粘土状原料を、超伝導体と超伝導を示さない導電
体が同心円状に積層された柱状に成形する工程とこの成
形体を柱状長さ方向に伸延し、線状に伸延する工程とこ
れを焼成する工程をとる。In addition, as a manufacturing method, superconducting ceramic particles and non-superconducting conductive powder, which have been grown into plate shapes, are used as starting materials, and a binder is added to each of these and kneaded to create a clay-like raw material that has superconducting properties. The process involves forming a columnar shape in which a conductor and a non-superconducting conductor are laminated concentrically, a step of stretching the formed body in the length direction of the columnar shape into a linear shape, and a step of firing it.
もしくは、あらかじめ板状に成長した超伝導体磁器粒子
と超伝導を示さない導電体の混合物を出発原料として用
い、これにバインダを加えて混練した粘土状原料を、柱
状に成形する工程とこの成形体を柱状長さ方向に伸延し
、線状に伸延する工程とこれを焼成する工程をとる。Alternatively, the process of forming a clay-like raw material into a columnar shape by using as a starting material a mixture of superconducting porcelain particles that have grown into plate shapes and a conductor that does not exhibit superconductivity, and adding a binder to this and kneading it into a columnar shape. The process involves stretching the body in the longitudinal direction of the column, stretching it linearly, and firing it.
作用
本発明のセラミック超伝導体は、超伝導体磁器粒子が配
向して焼結しているため、超伝導体磁器粒子どうしの接
着面積が大きくとれ、かつ連続性が向上するため、超伝
導の臨界電流がおおきくなる。また、超伝導を示さない
導電体層との接合面積も大きくなり、クエンチ現象を防
止する効果も大きい。Function In the ceramic superconductor of the present invention, the superconducting ceramic particles are oriented and sintered, so the adhesion area between the superconducting ceramic particles is large and the continuity is improved, so that superconducting Critical current increases. Moreover, the bonding area with the conductor layer that does not exhibit superconductivity becomes large, and the effect of preventing the quench phenomenon is also large.
また、本発明のセラミック超伝導体の製造方法によれば
、あらかじめ板状に成長したセラミック超伝導体磁器粒
子を用い、これを線状に成形する事により、粒子が面配
向する。Further, according to the method for manufacturing a ceramic superconductor of the present invention, ceramic superconductor porcelain particles that have been grown in advance into a plate shape are used and formed into a linear shape, so that the particles are plane-oriented.
実施例
実施例−1
セラミック超伝導体の出発原料としては、化学的に高純
度なりf20a+ SrCO3+ CaCO3+C
ub、 を用いた。 これらの粉末をモル比で、Bf
: Sr: Ca: Cuが、1:1:1:2となり、
全量が150gとなるように秤量した。これらの粉末は
、容ff1600ccのポリエチレン製ボールミル容器
にいれ、直径5mmの安定化ジルコニア製玉石600
g、 高純度アルコール150gとともに17時間混
合した。この粉末は、乾燥後250kg/cm2で成形
し、アルミナ製容器にいれ、管状炉炉心管中に挿入し、
酸素ガスの流速が毎分10cmとなるよう流し、850
’Cまで200°C/hrで昇温し、4時間保持したの
ち室温まで200℃/hrで降温した。この仮焼物は、
冷却後乳鉢で25メツシユパスまで粗砕し、前述のボー
ルミル、玉石を用い、高・純度アルコールとともに6時
間粉砕した。粉砕した粉末は、走査顕微鏡観察で平均厚
さ0.2μm直径2.5μmの形状のそろった板状を呈
していた。Examples Example-1 As starting materials for ceramic superconductors, chemically high purity f20a+ SrCO3+ CaCO3+C
ub, was used. The molar ratio of these powders is Bf
: Sr: Ca: Cu becomes 1:1:1:2,
It was weighed so that the total amount was 150 g. These powders were placed in a polyethylene ball mill container with a capacity of 1600 cc, and 600 stabilized zirconia boulders with a diameter of 5 mm were placed.
g, and 150 g of high-purity alcohol for 17 hours. After drying, this powder was molded at 250 kg/cm2, placed in an alumina container, and inserted into a tubular furnace core tube.
Flow the oxygen gas at a flow rate of 10 cm per minute, and
The temperature was raised to 'C at a rate of 200°C/hr, held for 4 hours, and then lowered to room temperature at a rate of 200°C/hr. This calcined product is
After cooling, it was coarsely crushed in a mortar to 25 mesh passes, and then crushed with high purity alcohol for 6 hours using the aforementioned ball mill and cobblestones. When observed under a scanning microscope, the pulverized powder had a uniform plate shape with an average thickness of 0.2 μm and a diameter of 2.5 μm.
次に、成形体の製造方法を第2図に従ってしめす。この
粉末は乾燥後、粉体重量の15vt%の(50vt%エ
タノール、エチルセルロース樹脂混合物)有機バインダ
と、3vt%のヂブチルフタレート、10wt%のグリ
セリンとともに乳鉢で混練し、直径4mm長さ100m
mの円柱状11(第2図a)と、厚さ1mm幅100m
mのシート状12(第2図b)に成形した。Next, the method for manufacturing the molded body will be shown in accordance with FIG. After drying, this powder was kneaded in a mortar with 15vt% (50vt% ethanol, ethyl cellulose resin mixture) of the powder weight of an organic binder, 3vt% dibutyl phthalate, and 10wt% glycerin, and was mixed with a diameter of 4 mm and a length of 100 m.
m cylindrical shape 11 (Figure 2 a), thickness 1 mm and width 100 m
It was molded into a sheet 12 (FIG. 2b) of m.
超伝導を示さない導電体層の出発原料としては、球状で
平均粒径0. 8μmの銀粒子を用い、粉体重量の32
vt%の(50vt%エタノール、エチルセルロース
樹脂混合物)有機バインダと、8vt%のヂブチルフタ
レート、20wt%のグリセリンとともに乳鉢で混練し
、厚さ1mm幅100mmのシート状13(第2図a)
に成形した。The starting material for a conductor layer that does not exhibit superconductivity is spherical and has an average particle size of 0. Using 8 μm silver particles, the powder weight was 32
Vt% (50vt% ethanol, ethyl cellulose resin mixture) organic binder, 8vt% dibutyl phthalate, and 20wt% glycerin were kneaded in a mortar to form a sheet 13 with a thickness of 1 mm and a width of 100 mm (Fig. 2 a).
It was molded into.
つぎに第2図dに示すように、上述の超伝導体円柱状成
形体11を芯にして、そのまわりに導電体シート13を
1周巻き、そのまわりに、超伝導体シート12を1周巻
いた。以後、導電体シート13、超伝導体シート12を
交互に一周ずつ各4層巻いた。成形体は、直径24mm
長さ100mmの円柱状14となった。Next, as shown in FIG. 2d, the above-mentioned superconductor cylindrical molded body 11 is used as a core, the conductor sheet 13 is wound around it once, and the superconductor sheet 12 is wrapped around it once. rolled. Thereafter, the conductor sheet 13 and the superconductor sheet 12 were alternately wound one round each in four layers. The molded body has a diameter of 24 mm.
It became a columnar shape 14 with a length of 100 mm.
以上の円柱状成形体14は、第2図eに示すように、2
枚の平板15.16にはさみ、平板を左右に動かしなが
ら圧力をかけて線状に伸延した。The above cylindrical molded body 14 is made of 2
It was sandwiched between two flat plates 15 and 16, and stretched linearly by applying pressure while moving the flat plates from side to side.
上述の超伝導体層と導電体層が積層された成形体は、直
径7mmであった。この積層体は、長さ40mmに切断
した。The molded body in which the above-mentioned superconductor layer and conductor layer were laminated had a diameter of 7 mm. This laminate was cut into a length of 40 mm.
上述の積層体は、アルミナ磁器容器中に、100メツシ
ユバスの粗粒アルミナを敷き詰めた上にのせ電気炉に挿
入し、350℃まで20℃/時で昇温し、10時間保持
してバインダーを焼却後冷却した。The above-mentioned laminate was placed in an alumina porcelain container on which 100 mesh baths of coarse-grained alumina was spread, placed in an electric furnace, heated to 350°C at a rate of 20°C/hour, and held for 10 hours to incinerate the binder. It was then cooled down.
試料の焼成は上述のバインダを焼却した試料を容器ごと
管状炉炉心管内に挿入し酸素ガスを毎分5cm/分流し
なから875°Cまで300″C/時で昇温し、2時間
保持後300°C/時で降温した。To sinter the sample, the above-mentioned binder was incinerated and the sample was inserted into the core tube of a tubular furnace together with the container, and while oxygen gas was flowing at 5 cm/min, the temperature was raised to 875°C at a rate of 300"C/hour, and after holding for 2 hours. The temperature was lowered at 300°C/hour.
第1図には、作成したセラミック超伝導体の断面図を示
す。1はセラミック超伝導体焼結体層、2は銀導電体層
である。焼結体の線方向に垂直な破断面は走査型電子顕
微鏡で観察した結果、外周面に平行に超伝導体層磁器粒
子が面配向していた。FIG. 1 shows a cross-sectional view of the produced ceramic superconductor. 1 is a ceramic superconductor sintered body layer, and 2 is a silver conductor layer. When the fracture surface of the sintered body perpendicular to the line direction was observed using a scanning electron microscope, it was found that the superconductor layer ceramic particles were plane-oriented parallel to the outer peripheral surface.
第3図に、断面一部の拡大図模式図を示す。21は超伝
導体磁器粒子22は銅導電体粒子である。FIG. 3 shows an enlarged schematic diagram of a part of the cross section. 21 is a superconductor ceramic particle 22 is a copper conductor particle.
第1表には、作成した試料(No、1)(積層方向に平
行方向)の単位面積あたりの一70Kにおける超伝導の
臨界電流と150K(セラミックは超伝導を示さない温
度)における単位長さあたりの抵抗率を示す。また比較
例として、金属銀の層がはいっていない試料で、成形方
法が実施例と同様のもの(No、2)(面配向性あり)
、粉体プレス(1軸プレス)によって成形したもの(N
o、3)(面配向性なし)の値も示す。Table 1 shows the critical current for superconductivity at 70K and the unit length at 150K (a temperature at which ceramics do not exhibit superconductivity) per unit area of the prepared sample (No. 1) (parallel to the stacking direction). Shows the resistivity of In addition, as a comparative example, a sample without a metallic silver layer and molded using the same method as the example (No. 2) (with plane orientation)
, molded by powder press (uniaxial press) (N
o, 3) (no plane orientation) values are also shown.
第 1 表
本口は本発明の範囲外の比較例
第1表より明かなように、本発明のような構成をとるセ
ラミック超伝導体は、臨界電流が大きくとれ、かつ超伝
導が破れたときの抵抗率も小さい。Table 1: Comparative examples outside the scope of the present invention As is clear from Table 1, the ceramic superconductor having the structure of the present invention has a large critical current, and when superconductivity is broken. The resistivity of is also small.
導電体層を含まない試料は、超伝導が破れたときの抵抗
率が大きく゛なる。セラミック層の配向していない試料
は、臨界電流が小さい。A sample that does not contain a conductor layer has a high resistivity when superconductivity is broken. Samples with unoriented ceramic layers have a small critical current.
実施例−2
セラミック超伝導体の出発原料としては、実施例−1と
同様の物を用いた。超伝導を示さない導電体層の出発原
料としては、実施例−1と同様の物および、板状で平均
厚さ0.15μm1 直径1゜5μmの銀、金、白金
、パラジウム粉末をもちいた。これらの粉末は超伝導を
示さない導電体の体積分率が所定の値となるように混合
した後、実施例−1と同様の方法で混練し、直径20m
m長さ100mmの円柱状に成形した。これは、実施例
−1と同様の方法で伸延し、切断、焼成した。Example 2 The same starting material as in Example 1 was used as the starting material for the ceramic superconductor. As starting materials for the conductor layer that does not exhibit superconductivity, the same materials as in Example 1 and plate-shaped silver, gold, platinum, and palladium powders having an average thickness of 0.15 μm and a diameter of 1°5 μm were used. These powders were mixed so that the volume fraction of the non-superconducting conductor became a predetermined value, and then kneaded in the same manner as in Example-1 to form a powder with a diameter of 20 m.
It was molded into a cylindrical shape with a length of 100 mm. This was stretched, cut, and fired in the same manner as in Example-1.
第2表に、作成した試料の導電体の出発原料組成、形状
、体積分率を、第3表に作成した試料(積層方向に平行
方向)の単位面積あたりの一70Kにおける超伝導の臨
界電流と150K(セラミックは超伝導を示さない温度
)における単位長さあたりの抵抗率を示す。なお、導電
体の体積分率が、30%、65%の試料(番号12.1
4)は、12は導電体が14はセラミックが局在化し連
続せず、本発明の範囲からはずれた比較例である。Table 2 shows the starting material composition, shape, and volume fraction of the conductor of the prepared sample, and Table 3 shows the critical current of superconductivity at 170 K per unit area of the prepared sample (parallel to the stacking direction). and the resistivity per unit length at 150K (a temperature at which ceramics do not exhibit superconductivity). In addition, samples in which the volume fraction of the conductor is 30% and 65% (No. 12.1
4) is a comparative example in which the conductor 12 and the ceramic 14 are localized and not continuous, which is out of the scope of the present invention.
それ以外の試料は、超伝導体、導電体がそれぞれ連続し
ており、かつ混合された状態となった。第4図に試料の
線方向に垂直な破断面一部の拡大模式図をしめす。31
が超伝導体磁器層、32が導電体金属層である。In the other samples, the superconductor and the conductor were both continuous and mixed. Figure 4 shows an enlarged schematic diagram of a portion of the fracture surface perpendicular to the line direction of the sample. 31
is a superconducting ceramic layer, and 32 is a conductive metal layer.
第
表
*印は本発明の範囲外の比較例
第 3 表
木口は本発明の範囲外の比較例
第2表、第3表より明かなように、超伝導体磁器と超伝
導を示さない導電体がおのおの連続し、かつ混合された
構造を有し、かつ超伝導体磁器の結晶粒子が、面配向性
を育している試料は、超伝導の臨界電流が大きく、かつ
超伝導がやぶれたときの抵抗率が小さい。導電体の出発
原料が板状のものは、超伝導体磁器粒子の配向性が向上
し、臨界電流がおおきくなるため、製造方法としてより
好ましい。The asterisks in Table 3 indicate comparative examples outside the scope of the present invention. Kiguchi in Table 3 indicates comparative examples outside the scope of the present invention, as is clear from Tables 2 and 3. Samples in which each body is continuous and have a mixed structure, and the crystal grains of the superconducting porcelain have a planar orientation, have a large critical current for superconductivity, and the superconductivity is broken. When the resistivity is small. A plate-shaped starting material for the conductor is more preferable as a manufacturing method because the orientation of the superconducting ceramic particles is improved and the critical current is increased.
実施例−3
セラミック超伝導体の出発原料としては、化学的に高純
度なT1202+ BaCO2,Ca CCh。Example 3 Chemically high purity T1202+ BaCO2, Ca CCh is used as the starting material for the ceramic superconductor.
Cu O9を用いた。 これらの粉末をモル比Tl:
Ba: Ca: Cuが、2: 2: 2: 3とな
り、全量が150gとなるように拝借した。これらの粉
末は、実施例−1と同様の方法で、混合仮焼粉砕し円柱
状、シート状に成形した。粉砕した粉末は、走査顕微鏡
観察で平均厚さ0.15μm直径1.5μmの形状のそ
ろった板状を呈していた。CuO9 was used. These powders have a molar ratio Tl:
The ratio of Ba: Ca: Cu was 2: 2: 2: 3, and the total amount was 150 g. These powders were mixed, calcined, pulverized, and formed into cylinders and sheets in the same manner as in Example-1. When observed under a scanning microscope, the pulverized powder had a uniform plate shape with an average thickness of 0.15 μm and a diameter of 1.5 μm.
超伝導を示さない導電体層の出発原料としては、板状で
平均厚さ0.2μm平均直径2. 0μmの金粒子を用
い、これも実施例−1と同様の方法でシート状に成形し
た。これらの成形体は、実施例−1と同様の方法で、同
心円状に積層成形した。The starting material for a conductive layer that does not exhibit superconductivity is a plate-like material with an average thickness of 0.2 μm and an average diameter of 2.0 μm. Gold particles of 0 μm were used and formed into a sheet in the same manner as in Example-1. These molded bodies were concentrically laminated and molded in the same manner as in Example-1.
以上の円柱状成形体は、第5図に断面を示すような徐々
に出口をしぼり出口部平行孔41をもった射出器42を
用い、射出方向に積層の同心円が垂直になるように成形
体をいれ、後部より圧力をかけて成形体を出口部平行孔
より射出し、線状に成形した。射出後の超伝導体層43
と導電体層44が積層された成形体は、直径8mmで中
心部に直径1.3mmmの超伝導体層が、その周囲に、
厚さ0.33mmの導電体層と、超伝導体層が各5層ず
つ交互に積層されている。この積層体は、長さ40mm
に切断した。これらの積層体は、実施例−1と同様の方
法で焼成した。The above cylindrical molded body is produced by using an injector 42 with a parallel hole 41 in which the outlet is gradually narrowed as shown in the cross section in FIG. The molded product was injected from the outlet parallel hole by applying pressure from the rear and molded into a linear shape. Superconductor layer 43 after injection
The molded body in which the conductor layer 44 is laminated has a diameter of 8 mm, a superconductor layer with a diameter of 1.3 mm in the center, and a superconductor layer with a diameter of 1.3 mm in the center, and around it,
Five conductor layers and superconductor layers each having a thickness of 0.33 mm are laminated alternately. This laminate has a length of 40mm
It was cut into These laminates were fired in the same manner as in Example-1.
第4表には、作成した試料(No、21)(積層方向に
平行方向)の単位面積あたりの一70Kにおける超伝導
の臨界電流と150K (セラミックは超伝導を示さな
い温度)における単位長さあたりの抵抗率を示す。また
比較例として、金の層がはいっていない試料で、成形方
法が実施例と同様のもの(No、22)(面配向性あり
)、粉体プレス(1軸プレス)によって成形したもの(
No、23)(面配向性なし)の値も示す。Table 4 shows the critical current of superconductivity per unit area of the prepared sample (No. 21) (parallel to the stacking direction) at 70K and the unit length at 150K (a temperature at which ceramics do not exhibit superconductivity). Shows the resistivity of As a comparative example, a sample without a gold layer and molded using the same molding method as in the example (No. 22) (with surface orientation), and a specimen molded by a powder press (uniaxial press) (
The value of No. 23) (no plane orientation) is also shown.
第 4 表
本口は本発明の範囲外の比較例
第4表より明かなように、本発明のような構成をとるセ
ラミック超伝導体は、臨界電流が大きくとれ、かつ超伝
導が破れたときの抵抗率も小さい。Table 4 Comparative Examples Outside the Scope of the Invention As is clear from Table 4, ceramic superconductors having the structure of the present invention have a large critical current and when superconductivity is broken. The resistivity of is also small.
導電体層を含まない試料は、超伝導が破れたときの抵抗
率が大きくなる。セラミック層の配向していない試料は
、臨界電流が小さい。A sample that does not contain a conductor layer has a high resistivity when superconductivity is broken. Samples with unoriented ceramic layers have a small critical current.
また本実施例のような製造方法をとると、線状の成形体
で、セラミックの配向性のよいものが、容易に量産性よ
く製造できる。Furthermore, by using the manufacturing method of this embodiment, a linear molded body with good ceramic orientation can be easily manufactured with good mass production.
実施例−4
セラミック超伝導体の出発原料としては、化学的に高純
度なT12031 BaCO3,CaC0a。Example-4 The starting materials for the ceramic superconductor are chemically highly pure T12031 BaCO3 and CaC0a.
Cu Or を用いた。 これらの粉末をモル比Tl
: Ba: Ca: Cuが、2: 2: 2
: 3となり、全量が150gとなるように秤量した
。これらの粉末は、実施例−1と同様の方法で、混合仮
焼粉砕した。超伝導を示さない導電体層の出発原料とし
ては、板状で平均厚さ0.15μm平均直径1.5μm
のパラジウム粒子を用いた。これらの粉末は、パラジウ
ムの体積%が45%となるよう混合し、実施例−2と同
様の方法で円柱状に成形し実施例−3と同様の方法で、
射出機より射出した。この線状成形体は、実施例−1と
同様の方法で焼成した。CuOr was used. These powders have a molar ratio Tl
: Ba: Ca: Cu is 2: 2: 2
: 3, and the total amount was weighed to be 150 g. These powders were mixed, calcined, and ground in the same manner as in Example-1. The starting material for a conductive layer that does not exhibit superconductivity is a plate with an average thickness of 0.15 μm and an average diameter of 1.5 μm.
palladium particles were used. These powders were mixed so that the volume percent of palladium was 45%, molded into a cylinder in the same manner as in Example-2, and formed in the same manner as in Example-3.
Injected from an injection machine. This linear molded body was fired in the same manner as in Example-1.
第5表には、作成した試料(No、31)(積層方向に
平行方向)の単位面積あたりの−70Kにおける超伝導
の臨界電流と150K(セラミックは超伝導を示さない
温度)における単位長さあたりの抵抗率を示す。また比
較例として、パラジウムの層のはいっていない試料で、
成形方法が実施例と同様のもの(No、32)(面配向
性あり)、パラジウムは混合されているが粉体プレス(
1軸ブレス)によって成形したもの(No、33)(面
配向性なし)の値も示す。Table 5 shows the critical current of superconductivity at -70K per unit area of the prepared sample (No. 31) (parallel to the stacking direction) and the unit length at 150K (a temperature at which ceramics do not exhibit superconductivity). Shows the resistivity of As a comparative example, a sample without a palladium layer was used.
The molding method is the same as in the example (No. 32) (with plane orientation), palladium is mixed but powder press (
The values of the sample (No. 33) (no plane orientation) formed using a uniaxial press are also shown.
第 5 表
X印は本発明の範囲外の比較例
第5表より明かなように、本発明のような構成をとるセ
ラミック超伝導体は、臨界電流が大きくとれ、かつ超伝
導が破れたときの抵抗率も小さい導電体層を含まない試
料は、超伝導が破れたときの抵抗率が大きくなる。セラ
ミック層の配向していない試料は、臨界電流が小さい。Table 5: Comparative examples outside the scope of the present invention As is clear from Table 5, the ceramic superconductor having the structure of the present invention has a large critical current, and when superconductivity is broken. A sample that does not contain a conductor layer with a low resistivity will have a high resistivity when superconductivity is broken. Samples with unoriented ceramic layers have a small critical current.
また本実施例のような製造方法をとると、線状の成形体
で、セラミックの配向性のよいものが、容易に量産性よ
く製造できる。Furthermore, by using the manufacturing method of this embodiment, a linear molded body with good ceramic orientation can be easily manufactured with good mass production.
実施例−4果
セラミック超伝導体の出発原料としては、実施例−1と
同様のものを用い、実施例−1と同様の方法で、混合仮
焼粉砕し、バインダを加えた。超伝導を示さない導電体
層の出発原料としては、板状で平均厚さ0.3μm平均
直径1.5μmの白金粒子を用いこれも実施例−1と同
様に、バインダを加えた。これらは、第6図に示したよ
うな、同心円状に6つの出口部平行孔ノズル51をもつ
射出機にセラミック超伝導体52と導電体53が交互に
配置されるようにいれ射出した。この線状成形体は、実
施例−1と同様の方法で焼成した。Example 4 The same starting materials as in Example 1 were used as the starting materials for the ceramic superconductor, and the materials were mixed, calcined, pulverized, and added with a binder in the same manner as in Example 1. Platinum particles having an average thickness of 0.3 .mu.m and an average diameter of 1.5 .mu.m were used as a starting material for a conductor layer that did not exhibit superconductivity, and a binder was added thereto in the same manner as in Example-1. These were injected into an injection machine having six parallel outlet nozzles 51 arranged concentrically as shown in FIG. 6, with ceramic superconductors 52 and conductors 53 arranged alternately. This linear molded body was fired in the same manner as in Example-1.
第6表には、作成した試料(No、41)(積層方向に
平行方向)の単位面積あたりの一70Kにおける超伝導
の臨界電流と150K(セラミックは超伝導を示さない
温度)における単位長さあたりの抵抗ギを示す。また比
較例として、パラジウムの層のはいっていない試料で、
成形方法が実施例と同様のもの(No、42)(面配向
性あり)粉体プレス(1軸ブレス)によって成形したも
の(No、43)(面配向性なし)の値も示す。Table 6 shows the critical current for superconductivity at 70K and the unit length at 150K (a temperature at which ceramics do not exhibit superconductivity) per unit area of the prepared sample (No. 41) (parallel to the stacking direction). Shows the resistance around the area. As a comparative example, a sample without a palladium layer was used.
The values are also shown for those molded by the same molding method as in Examples (No. 42) (with plane orientation) and those molded by powder press (uniaxial press) (No. 43) (without plane orientation).
第 6 表
末口は本発明の範囲外の比較例
第6表より明らかなように、本発明のような製造方法を
とる、セラミック超伝導体は、臨界電流、もおおきく、
かつ、超伝導が破れたときの抵抗率も小さい。また、本
実施例のように、多重ノズルより射出する工程をとるも
のは、さらにセラミックの配向性が向上し、臨界電流が
大きくなる。The end of Table 6 shows comparative examples outside the scope of the present invention.As is clear from Table 6, the ceramic superconductor produced by the manufacturing method of the present invention has a large critical current.
Moreover, the resistivity when superconductivity is broken is also small. Further, in the case where the injection process is performed through multiple nozzles as in this embodiment, the orientation of the ceramic is further improved and the critical current is increased.
発明の効果
本発明のセラミック超伝導体と、その製造方法によれば
、出発原料に板状の超伝導体磁器粒子を用いるため、超
伝導体磁器層が線外周面に平行に面配向して、超伝導臨
界電流が大きくとれ、かつ超伝導がやぶれても、導電体
層が近傍にあるため、クエンチ現象が防止できる。Effects of the Invention According to the ceramic superconductor and the method for producing the same of the present invention, since plate-shaped superconducting ceramic particles are used as the starting material, the superconducting ceramic layer is plane-oriented parallel to the wire outer peripheral surface. , the superconducting critical current can be large, and even if superconductivity breaks down, the quench phenomenon can be prevented because the conductor layer is nearby.
第1図は本発明の一実施例によるセラミック超伝導体の
構造を示す斜視図、第2図は同セラミック超伝導体の製
造方法を示す図、第3図は、同セラミック超伝導体の断
面拡大図模式図、第4図は、他の実施例におけるセラミ
ック超伝導体の断面拡大図模式図、第5図および第6図
は、他の実施例において用いる射出機の断面図である、
1・・・・セラミック超伝導体焼結体、2・・・・銀導
電体層、゛ 11・・・・セラミック超導電体円柱状成
形体、12・・・・セラミック超伝導体シート状成形体
、13・・・・銀導電体シート状成形体、14・・・・
円柱状成形体、15・・・・16・・・・平行板、21
・・・・超伝導体磁器粒子、22・・・・銀導電体粒子
、31・・・・超伝導体磁器層、32・・・・導電体金
属層、41・・・・出口部平行孔、42・・・・射出機
、43・・・・超伝導体層、44・・・・導電体層、5
1・・・・出口部平行ノズル、52・・・・超伝導体、
53・・・・導電体、代理人の氏名 弁理士 栗野重孝
はか1名第
図
第
図
1セラミック超伝導体沈緒不に
?j及埠電停層
第
図
(d)
第
図
f
734及導電イ取ジートイ大A形停
(e)
第
図
第
図FIG. 1 is a perspective view showing the structure of a ceramic superconductor according to an embodiment of the present invention, FIG. 2 is a diagram showing a method for manufacturing the ceramic superconductor, and FIG. 3 is a cross-sectional view of the ceramic superconductor. FIG. 4 is an enlarged schematic diagram of a ceramic superconductor in another example; FIGS. 5 and 6 are cross-sectional views of an injection machine used in other examples.
1... Ceramic superconductor sintered body, 2... Silver conductor layer, 11... Ceramic superconductor cylindrical molded body, 12... Ceramic superconductor sheet-shaped molded body Body, 13... Silver conductor sheet-like molded body, 14...
Cylindrical molded body, 15...16...Parallel plate, 21
...Superconductor ceramic particles, 22 ... Silver conductor particles, 31 ... Superconductor ceramic layer, 32 ... Conductor metal layer, 41 ... Exit parallel hole , 42... Injection machine, 43... Superconductor layer, 44... Conductor layer, 5
1...Exit parallel nozzle, 52...Superconductor,
53...Electric conductor, name of agent Patent attorney Shigetaka Kurino 1 person Figure 1 Ceramic superconductor Shinofuni? 734 and conductive tram stop (e)
Claims (6)
体磁器層と超伝導を示さない導電体層とが外周面と平行
に積層された構造を有し、かつ超伝導体磁器の結晶粒子
が、外周面と平行に面配向性を有していることを特徴と
するセラミック超伝導体。(1) The cross section of a linear ceramic superconductor has a structure in which a superconducting ceramic layer and a non-superconducting conductive layer are laminated parallel to the outer peripheral surface, and the crystal grains of the superconducting ceramic A ceramic superconductor characterized by having a plane orientation parallel to the outer peripheral surface.
と超伝導を示さない導電体がおのおの連続し、かつ混合
された構造を有し、かつ超伝導体磁器の結晶粒子が、外
周面と平行に面配向性を有していることを特徴とする、
セラミック超伝導体。(2) A linear ceramic superconductor has a structure in which the superconducting porcelain and the non-superconducting conductor are continuous and mixed, and the crystal grains of the superconducting porcelain are connected to the outer peripheral surface. characterized by having parallel plane orientation,
Ceramic superconductor.
もしくはTl−Ba−Ca−Cu−O系の酸化物を主成
分とし、導電体が金、銀、白金、パラジウムからなる群
のすくなくともひとつを主成分とする金属からなること
を特徴とする特許請求の範囲第1項または第2項記載の
セラミック超伝導体。(3) The superconductor porcelain has a Bi-Sr-Ca-Cu-O or Tl-Ba-Ca-Cu-O oxide as its main component, and the conductor is made of gold, silver, platinum, or palladium. The ceramic superconductor according to claim 1 or 2, characterized in that the ceramic superconductor is made of a metal whose main component is at least one of the following.
超伝導を示さない導電体粉末を出発原料として用い、こ
れにおのおのバインダを加えて混練した粘土状原料を、
超伝導体と超伝導を示さない導電体が同心円状に積層さ
れた柱状に成形する工程と、この成形体を柱状長さ方向
に伸延して線状に伸延する工程と、これを焼成する工程
とを含むことを特徴とするセラミック超伝導体の製造方
法。(4) Using superconducting porcelain particles and non-superconducting conductive powder, which have been grown into plate shapes, as starting materials, binders are added to each of these and kneaded to create a clay-like raw material.
A process of forming a column in which a superconductor and a non-superconducting conductor are laminated concentrically, a process of stretching this formed body in the length direction of the column to form a linear shape, and a process of firing this. A method for producing a ceramic superconductor, comprising:
伝導を示さない導電体の混合物を出発原料として用い、
これにバインダを加えて混練した粘土状原料を柱状に成
形する工程と、この成形体を柱状長さ方向に伸延して線
状に伸延する工程と、これを焼成する工程とを含むこと
を特徴とするセラミック超伝導体の製造方法。(5) Using a mixture of superconducting ceramic particles that have been grown in the form of a plate in advance and a conductor that does not exhibit superconductivity as a starting material,
The method includes the steps of forming the clay-like raw material mixed with a binder into a columnar shape, stretching the formed body in the longitudinal direction of the columnar shape into a linear shape, and firing the same. A method for producing a ceramic superconductor.
銀、白金、パラジウムからなる群より選ばれた少なくと
も一種類の金属の、板状の形状を有する粉末を用いるこ
とを特徴とする特許請求の範囲第4項または第5項に記
載のセラミック超伝導体の製造方法。(6) As starting materials for conductors that do not exhibit superconductivity, gold,
The ceramic superconductor according to claim 4 or 5, characterized in that a plate-shaped powder of at least one metal selected from the group consisting of silver, platinum, and palladium is used. How the body is manufactured.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63173348A JPH0224911A (en) | 1988-07-12 | 1988-07-12 | Ceramic superconductor and manufacture thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63173348A JPH0224911A (en) | 1988-07-12 | 1988-07-12 | Ceramic superconductor and manufacture thereof |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0224911A true JPH0224911A (en) | 1990-01-26 |
Family
ID=15958749
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63173348A Pending JPH0224911A (en) | 1988-07-12 | 1988-07-12 | Ceramic superconductor and manufacture thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0224911A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02186508A (en) * | 1988-07-27 | 1990-07-20 | Furukawa Electric Co Ltd:The | Oxide superconductive lead and manufacture thereof |
-
1988
- 1988-07-12 JP JP63173348A patent/JPH0224911A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02186508A (en) * | 1988-07-27 | 1990-07-20 | Furukawa Electric Co Ltd:The | Oxide superconductive lead and manufacture thereof |
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