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JP7246712B2 - Functional composite material - Google Patents
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JP7246712B2 - Functional composite material - Google Patents

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JP7246712B2
JP7246712B2 JP2019087578A JP2019087578A JP7246712B2 JP 7246712 B2 JP7246712 B2 JP 7246712B2 JP 2019087578 A JP2019087578 A JP 2019087578A JP 2019087578 A JP2019087578 A JP 2019087578A JP 7246712 B2 JP7246712 B2 JP 7246712B2
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superconducting
composite material
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JP2020183555A (en
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健二 松田
直人 中村
克彦 西村
昇原 李
大樹 土屋
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University of Toyama NUC
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    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02BCLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO BUILDINGS, e.g. HOUSING, HOUSE APPLIANCES OR RELATED END-USER APPLICATIONS
    • Y02B30/00Energy efficient heating, ventilation or air conditioning [HVAC]
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

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Description

本発明は、磁気冷凍性能と超伝導性能を有する機能複合材に関する。 TECHNICAL FIELD The present invention relates to a functional composite material having magnetic refrigeration performance and superconductivity performance.

超伝導材料は、超伝導転移温度まで冷却すると、電気抵抗がゼロとなる現象を示す。
このような超伝導の現象を応用した強力な電磁石,低損失送電,低損失電子デバイス等、各種分野での検討が進められている。
A superconducting material exhibits a phenomenon in which the electrical resistance becomes zero when cooled to the superconducting transition temperature.
Investigations are being made in various fields such as powerful electromagnets, low-loss power transmission, and low-loss electronic devices that apply such superconductivity phenomena.

超伝導材料には、液体ヘリウム温度(-269℃)で超伝導状態になる低温超伝導材料と液体窒素(-196℃)で超伝導状態になる高温超伝導材料とがある。
超伝導材料を使用する分野では、何らかの原因により導体の一部が超伝導状態から通常伝導状態に転移すると、大きな局部発熱により周囲の導体も急速に超伝導現象を消失してしまうという現象が起こる。
この現象をクエンチと言い、極低温の寒剤が沸騰して爆発的に放出されたり、発熱により超伝導体が破損したりする恐れがある。
Superconducting materials include low-temperature superconducting materials that become superconducting at liquid helium temperature (-269°C) and high-temperature superconducting materials that become superconducting at liquid nitrogen (-196°C).
In fields where superconducting materials are used, when a portion of a conductor transitions from a superconducting state to a normal conducting state for some reason, a large amount of local heat is generated, causing the surrounding conductors to rapidly lose their superconducting properties. .
This phenomenon is called quenching, and there is a risk that cryogen at extremely low temperatures will boil and be released explosively, or the superconductor will be damaged by heat generation.

超伝導転移温度まで冷却する方法としては現在、ジュール・トムソン効果を利用した冷媒の圧縮,膨張による方法が使用されているが、エネルギー損失が大きく冷却効果が低いという技術的課題がある。
近年、新たな冷凍技術として磁性体のエントロピーと温度の磁場依存性から生じる磁気熱量効果を用いた磁気冷凍技術が検討されている。
しかし、この磁気熱量効果と超伝導特性は相反的な関係があるといわれ、これまでに充分に検討された例は見当たらない。
また、磁気熱量効果を示す材料は一般に熱伝導率が低いことも課題である。
As a method of cooling to the superconducting transition temperature, a method of compressing and expanding a refrigerant using the Joule-Thomson effect is currently used, but it has the technical problem of large energy loss and low cooling effect.
In recent years, as a new refrigeration technology, magnetic refrigeration technology using the magnetocaloric effect caused by the magnetic field dependence of the entropy and temperature of magnetic materials has been studied.
However, the magnetocaloric effect and the superconducting properties are said to have a contradictory relationship, and no examples have been found that have been sufficiently investigated so far.
Another problem is that materials exhibiting the magnetocaloric effect generally have low thermal conductivity.

例えば非特許文献1には、磁気熱量材料の冷凍性能を向上させるために、母相に熱伝導性の高いタンタルを用いた焼結材料が記載されているが、焼結であるために内部欠陥が発生しやすく、超伝導性能も有していない。
なお、本出願人は先に超伝導性能を有する複合材料を提案している(特許文献1)が、この際には磁気熱量効果については検討されていなかった。
For example, Non-Patent Document 1 describes a sintered material using tantalum with high thermal conductivity in the matrix in order to improve the refrigeration performance of the magnetocaloric material, but internal defects due to sintering is likely to occur, and does not have superconducting properties.
Although the present applicant previously proposed a composite material having superconductivity (Patent Document 1), the magnetocaloric effect was not considered at this time.

特許第5483078号公報Japanese Patent No. 5483078

Microstructure, magnetic properties and thermal conductivity of LaFe11.2Si1.8/Ta magnetocaloric composite Qiming Wu, Naikun Sun, Xiangjie Wang, Lingwei Li J. Magn. Mang. Mater. Vol. 476 (2019) No.15Microstructure, magnetic properties and thermal conductivity of LaFe11.2Si1.8/Ta magnetocaloric composite Qiming Wu, Naikun Sun, Xiangjie Wang, Lingwei Li J. Magn. Mang. Mater. Vol. 476 (2019) No.15

本発明は、磁気熱量効果を用いて冷却可能な超伝導材料であって、クエンチ発生の防止にも効果的な機能複合材の提供を目的とする。 An object of the present invention is to provide a functional composite material that is a superconducting material that can be cooled using the magnetocaloric effect and that is also effective in preventing quenching.

本発明に係る機能複合材は、磁気熱量効果を示す粒子と、超伝導効果を示す粒子とが金属基材に分散されていることを特徴とする。 A functional composite material according to the present invention is characterized in that particles exhibiting a magnetocaloric effect and particles exhibiting a superconducting effect are dispersed in a metal substrate.

ここで、磁気熱量効果を示す粒子とは、一定温度で磁場を加えると磁気モーメントが磁場方向に揃いエントロピーが減少し、逆に断熱状態で磁場を減少させると温度が減少する磁気熱量効果を示す粒子をいい、この性質を利用した冷凍技術を磁気冷凍と表現する。
磁気熱量効果が大きいほど冷却効果が大きい。
本発明は、磁気熱量効果を示す粒子として現在知られているもののみならず、今後提案されるものも用いることができると推定される。
現在大きな磁気熱量効果を示すことが知られている物質としては、Gd化合物系又はLa-Fe-Si系化合物が代表例である。具体例としては、Gd,GdSiGe,GdSi1.8Ge1.8Sn0.4,La(Fe0.88Si0.1213等が挙げられる。
Here, a particle exhibiting magnetocaloric effect means that when a magnetic field is applied at a constant temperature, the magnetic moment aligns in the direction of the magnetic field, and the entropy decreases. It refers to particles, and the refrigeration technology that uses this property is called magnetic refrigeration.
The greater the magnetocaloric effect, the greater the cooling effect.
It is presumed that the present invention can use not only presently known particles exhibiting magnetocaloric effects, but also those proposed in the future.
Gd compounds and La--Fe--Si compounds are typical examples of substances currently known to exhibit a large magnetocaloric effect. Specific examples include Gd, Gd5Si2Ge2 , Gd5Si1.8Ge1.8Sn0.4 , La ( Fe0.88Si0.12 ) 13 , and the like .

超伝導効果を示す粒子には、超伝導転移温度まで冷却すると超伝導現象が出現する物質であれば、現在報告されているものに限定されないが、例えば前記超伝導特性を有する粒子は、金属間化合物の例としてMgB,NbGe,NbSn,NbTi等、銅酸化物の例としてY-Ba-Cu-O系,La-Sr-Cu-O系,Hg-Ba-Ca-Cu-O系等が挙げられる。 Particles exhibiting a superconducting effect are not limited to those currently reported as long as they are substances that exhibit a superconducting phenomenon when cooled to the superconducting transition temperature. Examples of compounds include MgB 2 , Nb 3 Ge, Nb 3 Sn, NbTi, etc. Examples of copper oxides include Y—Ba—Cu—O system, La—Sr—Cu—O system, Hg—Ba—Ca—Cu— O type etc. are mentioned.

本発明において特徴的なのは、上記磁気熱量効果を示す粒子と超伝導効果を示す粒子とをマグネシウム又はアルミニウム等の金属基材(マトリックス)中に分散させることで、それぞれの機能が発揮されるように機能の複合化を図った点にある。
ここでマグネシウムには、その合金が含まれ、アルミニウムにもその合金が含まれる。
このような軽金属を基材として使用することで軽量化が可能になる。
A characteristic feature of the present invention is that the particles exhibiting the magnetocaloric effect and the particles exhibiting the superconducting effect are dispersed in a metal substrate (matrix) such as magnesium or aluminum so that their functions are exhibited. The point is that the functions have been combined.
Here, magnesium includes its alloys, and aluminum also includes its alloys.
By using such a light metal as a base material, it becomes possible to reduce the weight.

本発明に係る機能複合材の製造方法は、磁気熱量効果を示す粒子と超伝導効果を示す粒子との混合物に、溶融又は半溶融状態の金属を加圧浸透させることを特徴とする。
ここで、磁気熱量効果を示す粒子と超伝導効果を示す粒子を混合し、それをプリフォーム体に加圧成形した混合物を用いてもよい。
A method for producing a functional composite material according to the present invention is characterized by infiltrating molten or semi-molten metal into a mixture of particles exhibiting a magnetocaloric effect and particles exhibiting a superconducting effect under pressure.
Here, a mixture obtained by mixing particles exhibiting a magnetocaloric effect and particles exhibiting a superconducting effect and molding the mixture into a preform may be used.

本発明は、磁気熱量特性と超伝導特性とを複合化したことにより、磁気冷凍により超伝導転移温度以下に冷却することができるとともに基材に金属を用いたことにより、この金属基材の熱伝導性によりクエンチ発生を防止する効果が期待される。 By combining the magnetocaloric properties and the superconducting properties of the present invention, it is possible to cool the metal base material to below the superconducting transition temperature by magnetic refrigeration. The conductivity is expected to prevent the occurrence of quenching.

機能複合体の成型例を示す。An example of forming a functional complex is shown. 複合体の断面写真を示す。A cross-sectional photograph of the composite is shown. 外部磁場0-5Tでの磁気エントロピー変化を示す。Magnetic entropy change at external magnetic field 0-5T is shown. Relative cooling power(RCP)と比RCPの値を示す。Relative cooling power (RCP) and ratio RCP values are shown. 比重とRCPの分布図を示す。The distribution map of specific gravity and RCP is shown. 複合材の電気抵抗測定結果を示す。4 shows the electrical resistance measurement results of the composite material. 複合材の熱伝導測定結果を示す。Figure 2 shows thermal conductivity measurement results for composite materials. 熱伝導の比較表を示す。A comparison table of heat conduction is shown.

本発明に係る機能複合体を試作し、他の材料と比較評価したので以下、説明する。 A functional composite according to the present invention was prototyped and compared with other materials for evaluation, which will be described below.

磁気熱量効果を示す粒子としては、アーク溶解法によりGdSi1.8Ge1.8Sn0.4化合物を作製し用いた。
なお、鋳造法にて製作したり、市販されているものを用いたりしてもよい。
本実施例は、上記アーク溶解法にて作製したGdSi1.8Ge1.8Sn0.4を乳鉢にて粉砕し、粒径で10~200μmの粉末にした。
As particles exhibiting a magnetocaloric effect, a Gd 5 Si 1.8 Ge 1.8 Sn 0.4 compound was prepared by an arc melting method and used.
In addition, you may manufacture by the casting method, or you may use what is marketed.
In this example, the Gd 5 Si 1.8 Ge 1.8 Sn 0.4 produced by the arc melting method was pulverized in a mortar to obtain a powder having a particle size of 10 to 200 μm.

超伝導効果を示す粒子としては、平均粒径約50μmのMgB粉末(株式会社高純度化学研究所製)を用いた。
粒子は平均粒径で20~100μmのものが好ましい。
As particles exhibiting a superconducting effect, MgB2 powder (manufactured by Kojundo Chemical Laboratory Co., Ltd.) having an average particle size of about 50 μm was used.
The particles preferably have an average particle diameter of 20 to 100 μm.

金属基材には、純度99.99%のマグネシウムを用いた。 Magnesium with a purity of 99.99% was used for the metal substrate.

<プリフォーム体の作製>
底部が取り外しできる円筒状の金型を使用し、内壁を包むように薬包紙を敷き、磁気熱量効果を示す粒子(以下、磁気熱量粒子)と超伝導効果を示す粒子(以下、超伝導粒子)とを所定の割合に混合し、上記金型内に少量ずつ入れ、押し棒で軽く加圧する工程を繰り返しながら約100gの圧粉プリフォーム体を作製した。
<Production of preform body>
A cylindrical mold with a detachable bottom is used, and the inner wall is covered with wrapping paper, and particles exhibiting a magnetocaloric effect (hereinafter referred to as magnetocaloric particles) and particles exhibiting a superconducting effect (hereinafter referred to as superconducting particles) are placed. The mixture was mixed in a predetermined ratio, put into the mold little by little, and pressed lightly with a push rod while repeating the process to produce a powder preform of about 100 g.

<三次元溶湯浸透法による複合体の作製>
図1に示すように、金型1内にプリフォーム体Pを入れ、その上にこのプリフォーム体Pの外径よりも少し小さい外径のグラファイト製の蓋体2を載せる。
その上に、金型の段差部に絞り3を支持させた。
この絞り3は、中央部に孔を有している。
この絞り3の上に基材となるマグネシウムを配置した。
周囲からマグネシウムの燃焼を防ぐために、COとSFの混合ガスを吹きかけながら金型1を約700℃まで昇温した。
マグネシウムが溶解したのを確認し、その上から黒鉛のパンチ4を載せて加圧することでプリフォーム体Pにマグネシウムの溶湯を加圧浸透させた。
なお、金型1の底部は冷却可能になっているものが好ましい。
<Preparation of composite by three-dimensional molten metal penetration method>
As shown in FIG. 1, a preform body P is placed in a mold 1, and a lid body 2 made of graphite having an outer diameter slightly smaller than the outer diameter of the preform body P is placed thereon.
On top of that, the diaphragm 3 was supported on the stepped portion of the mold.
This diaphragm 3 has a hole in its central portion.
Magnesium as a base material was arranged on the diaphragm 3 .
The temperature of the mold 1 was raised to about 700° C. while blowing a mixed gas of CO 2 and SF 6 to prevent burning of magnesium from the surroundings.
After confirming that the magnesium had melted, a graphite punch 4 was placed on the preform body P and pressurized to permeate the preform body P with the molten magnesium.
In addition, it is preferable that the bottom of the mold 1 can be cooled.

機能複合材(以下、複合材)としては、体積率でGdGe1.8Si1.8Sn0.4:MgB:Mg=40:40:20の複合体Aと、GdGe1.8Si1.8Sn0.4:MgB:Mg=25:50:25の複合体Bとを作製した。
その断面写真を図2に示す。
鋳巣などの内部欠陥は認められず、SE像より各粒子が均一に分散していることが確認できた。
図3に、外部磁場を0Tから5Tでに励磁した際の磁気エントロピー変化を示す。
図中、△は複合体A,□は複合体Bを示し、◇としてGdGe1.8Si1.8Sn0.4の値を参考に示した。
上記、磁気エントロピー変化に基づいて冷却1サイクルにて、どの程度の熱量を汲み出すことができるかを示す指標として、RCP(Relative cooling power)とその値を試料の比重で除した比RCPの値を図4の表に示す。
なお、表中、複合体A,B及びGdSi1.8Ge1.8のSn0.4の値以外は、他の文献にて報告されている値を参考に表示した。
図5に比重と磁気熱量効果の散布図を示す。
この図4,5から本発明に係る複合材は、磁気熱量粒子の体積率が小さいにも関わらず、比RCPの値RCP/ρはGdSiGeやLa(Fe0.88Si0.1213レベルの値を示した。
図6に電気抵抗測定結果を示し、図7に熱伝導の測定結果を示す。
また、他の材料との熱伝導度との比較表を図8に示す。
これらを比較すると、本発明に係る複合体は基材として金属を用いたことで、熱伝導度が2~20倍に改善されている。
磁気熱量効果により磁気冷凍ができ、低温で熱伝導度が高いことは超伝導材料におけるクエンチ現象の防止が期待される。
また、複合材AとBとを図6のグラフにて比較すると、磁気熱量粒子と超伝導粒子との体積比率が1:1の複合材Aよりも1:2の複合材Bの方が、優れた超伝導特性を示したことも明らかになった。
このことは体積比率で、磁気熱量粒子よりも超伝導粒子の方が大きいのが好ましいと推定される。
As a functional composite material (hereinafter referred to as a composite material), a composite A having a volume ratio of Gd 5 Ge 1.8 Si 1.8 Sn 0.4 :MgB 2 :Mg=40:40:20 and Gd 5 Ge 1 .8 Si 1.8 Sn 0.4 :MgB 2 :Mg=25:50:25 Composite B was prepared.
A photograph of the cross section is shown in FIG.
No internal defects such as blowholes were observed, and it was confirmed from the SE image that each particle was uniformly dispersed.
FIG. 3 shows the change in magnetic entropy when the external magnetic field is excited from 0T to 5T.
In the figure, Δ indicates composite A, □ indicates composite B, and ◇ indicates the value of Gd 5 Ge 1.8 Si 1.8 Sn 0.4 for reference.
As an index indicating how much heat can be pumped out in one cooling cycle based on the magnetic entropy change, RCP (Relative Cooling Power) and a ratio RCP value obtained by dividing the value by the specific gravity of the sample. are shown in the table of FIG.
In the table, the values reported in other literatures are referred to, except for the value of Sn 0.4 of composites A and B and Gd 5 Si 1.8 Ge 1.8.
FIG. 5 shows a scatter diagram of specific gravity and magnetocaloric effect.
4 and 5, the composite material according to the present invention has a ratio RCP value RCP/ρ of Gd 5 Si 2 Ge 2 or La (Fe 0.88 Si 0 .12 ) showed a value of 13 levels.
FIG. 6 shows the electrical resistance measurement results, and FIG. 7 shows the heat conduction measurement results.
Also, FIG. 8 shows a comparison table of thermal conductivity with other materials.
Comparing these, the composite according to the present invention has improved thermal conductivity by 2 to 20 times due to the use of metal as the base material.
Magnetic refrigeration is possible by the magnetocaloric effect, and high thermal conductivity at low temperatures is expected to prevent quenching in superconducting materials.
Also, when comparing the composite materials A and B in the graph of FIG. It was also revealed that they exhibited excellent superconducting properties.
This presumes that the superconducting particles are preferably larger than the magnetocaloric particles by volume.

1 金型
2 蓋体
3 絞り
4 パンチ
P プリフォーム体
1 mold 2 lid 3 diaphragm 4 punch P preform body

Claims (5)

磁気熱量効果を示す粒子と、超伝導効果を示す粒子とが金属基材に分散されていることを特徴とする機能複合材。 A functional composite material comprising particles exhibiting a magnetocaloric effect and particles exhibiting a superconducting effect dispersed in a metal substrate. 前記金属基材は、マグネシウム又はアルミニウムであることを特徴とする請求項1記載の機能複合材。 2. The functional composite material according to claim 1, wherein said metal substrate is magnesium or aluminum. 前記磁気熱量効果を示す粒子は、Gd化合物系又はLa-Fe-Si系化合物であることを特徴とする請求項1又は2記載の機能複合材。 3. The functional composite material according to claim 1, wherein the particles exhibiting the magnetocaloric effect are Gd compounds or La--Fe--Si compounds. 前記超伝導効果を示す粒子は、金属間化合物又は銅酸化物であることを特徴とする請求項1~3のいずれかに記載の機能複合材。 The functional composite material according to any one of claims 1 to 3, wherein the particles exhibiting superconductivity are intermetallic compounds or copper oxides. 磁気熱量効果を示す粒子と超伝導効果を示す粒子との混合物に、溶融又は半溶融状態の金属を加圧浸透させることを特徴とする機能複合材の製造方法。 1. A method for producing a functional composite material, characterized in that a molten or semi-molten metal is impregnated under pressure into a mixture of particles exhibiting a magnetocaloric effect and particles exhibiting a superconducting effect.
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CN1389536A (en) 2002-07-15 2003-01-08 南京大学 Composite room temperature magnetic refrigerating material and its prepn.
JP2005536630A (en) 2002-07-01 2005-12-02 南京大学 Molding and manufacturing method of room temperature magnetic cooling material combined with high thermal conductive material
JP2008200711A (en) 2007-02-20 2008-09-04 Toyama Univ Method for producing light metal composite material and light metal composite material obtained by this method
JP2011113951A (en) 2009-11-30 2011-06-09 Toyama Univ Magnesium based composite material
JP2014122406A (en) 2012-12-21 2014-07-03 Nihon Ceratec Co Ltd Metal-ceramic composite material, and method for manufacturing the same

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005536630A (en) 2002-07-01 2005-12-02 南京大学 Molding and manufacturing method of room temperature magnetic cooling material combined with high thermal conductive material
CN1389536A (en) 2002-07-15 2003-01-08 南京大学 Composite room temperature magnetic refrigerating material and its prepn.
JP2008200711A (en) 2007-02-20 2008-09-04 Toyama Univ Method for producing light metal composite material and light metal composite material obtained by this method
JP2011113951A (en) 2009-11-30 2011-06-09 Toyama Univ Magnesium based composite material
JP2014122406A (en) 2012-12-21 2014-07-03 Nihon Ceratec Co Ltd Metal-ceramic composite material, and method for manufacturing the same

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