JPH08178443A - Regenerator - Google Patents
RegeneratorInfo
- Publication number
- JPH08178443A JPH08178443A JP32310794A JP32310794A JPH08178443A JP H08178443 A JPH08178443 A JP H08178443A JP 32310794 A JP32310794 A JP 32310794A JP 32310794 A JP32310794 A JP 32310794A JP H08178443 A JPH08178443 A JP H08178443A
- Authority
- JP
- Japan
- Prior art keywords
- regenerator
- specific heat
- compound
- additive
- regenerator material
- 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.)
- Pending
Links
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2309/00—Gas cycle refrigeration machines
- F25B2309/003—Gas cycle refrigeration machines characterised by construction or composition of the regenerator
Landscapes
- Hard Magnetic Materials (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、低温で比熱の大きい蓄
冷材が充填された蓄冷器に関するもので、各種の冷凍機
に利用される。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a regenerator filled with a regenerator material having a high specific heat at a low temperature and is used in various refrigerators.
【0002】[0002]
【従来の技術】スターリング式、GM(ギホードマクマ
ホン)式、パルス管式等の各種の蓄冷器を使う冷凍機に
は、冷凍能力の向上という点から蓄冷材が充填された蓄
冷器が必須になる。この蓄冷器は、一方向に流れる圧縮
された作動ガスから熱を奪ってその熱を蓄えると共に、
反対方向に流れる膨張した作動ガスに蓄えた熱を伝達す
るものである。2. Description of the Related Art Refrigerators that use various types of regenerators such as Stirling type, GM (Gihoed McMahon) type, pulse tube type, etc. must have a regenerator filled with a regenerator material in order to improve refrigerating capacity. Become. This regenerator takes heat from the compressed working gas flowing in one direction and stores the heat.
It transfers the heat stored in the expanded working gas flowing in the opposite direction.
【0003】従来、蓄冷器内に充填される蓄冷材として
は、銅や鉛等の合金が多用されている。ところが、銅や
鉛からなる蓄冷材では、格子系の比熱しかもたないた
め、比熱は40K以上では大きいものの、20K以下の
極低温で過度に小さくなる。そのため、前記蓄冷材が充
填された蓄冷器を冷凍機(特に多段式の冷凍機)内で使
用した場合には、圧縮された作動ガスから充分に熱を吸
収することができず、又、膨張した作動ガスに充分に熱
を伝達することができなくなる。その結果、このような
蓄冷材が充填された蓄冷器を使用する冷凍機では、極低
温に到達させることができないという問題点があった。Conventionally, alloys such as copper and lead are often used as the regenerator material filled in the regenerator. However, since the regenerator material made of copper or lead has only the specific heat of the lattice system, the specific heat is large at 40 K or more, but becomes excessively small at an extremely low temperature of 20 K or less. Therefore, when the regenerator filled with the regenerator material is used in a refrigerator (particularly, a multistage refrigerator), heat cannot be sufficiently absorbed from the compressed working gas, and the expansion does not occur. The heat cannot be sufficiently transferred to the working gas. As a result, a refrigerator using a regenerator filled with such a regenerator material has a problem that it cannot reach an extremely low temperature.
【0004】そこで、このような問題点を解決するため
に提案された蓄冷器としては、特開平1−310269
号公報に示されるものが知られている。その代表例とし
て、格子系の比熱だけでなくスピン系の比熱を持つEr
3 Niからなる磁性体の蓄冷材が充填された蓄冷器が開
示されている。これは、20K以下の極低温でその比熱
が銅や鉛からなる蓄冷材よりも大きいため、銅や鉛から
なる蓄冷材よりも20K以下(特に10K未満)の極低
温において蓄冷効率を向上できる。Therefore, as a regenerator proposed in order to solve such a problem, Japanese Patent Laid-Open No. 1-310269 has been proposed.
The one shown in Japanese Patent Publication is known. As a typical example thereof, Er having not only the specific heat of the lattice system but also the specific heat of the spin system
A regenerator filled with a magnetic regenerator material made of 3 Ni is disclosed. This is because at a cryogenic temperature of 20 K or less, the specific heat thereof is larger than that of the regenerator material made of copper or lead, so that the regenerator efficiency can be improved at an extremely low temperature of 20 K or less (particularly less than 10 K) than the regenerator material made of copper or lead.
【0005】[0005]
【発明が解決しようとする課題】ところが、上記したE
r3 Niからなる蓄冷材では、磁気変態点(即ち磁気的
状態間の相転移)が8K付近に存在することから、比熱
が8K未満で大きいものの、8〜30Kでは小さくな
る。このため、8K未満の極低温では蓄冷効率が高くな
るものの、8〜30Kで蓄冷効率が不充分である。従っ
て、上記したEr3Niからなる蓄冷材では、10〜3
0Kの冷凍を発生する冷凍機には適用し難いという問題
点がある。However, the above-mentioned E
In the regenerator material made of r 3 Ni, the magnetic transformation point (that is, the phase transition between magnetic states) exists near 8K, so that the specific heat is large at less than 8K, but becomes small at 8 to 30K. Therefore, although the cold storage efficiency is high at an extremely low temperature of less than 8K, the cold storage efficiency is insufficient at 8 to 30K. Therefore, in the above-mentioned cool storage material composed of Er 3 Ni, 10 to 3
There is a problem that it is difficult to apply to a refrigerator that generates 0K of refrigeration.
【0006】故に、本発明は、8〜30Kで比熱が大き
く、8〜30Kでの蓄冷効率を向上させ得る蓄冷材をも
つ蓄冷器を提供することを、その技術的課題とするもの
である。[0006] Therefore, it is a technical object of the present invention to provide a regenerator having a regenerator material having a large specific heat at 8 to 30K and capable of improving the regenerator efficiency at 8 to 30K.
【0007】[0007]
【課題を解決するための手段】上記技術的課題を解決す
るために本発明において講じた技術的手段は、蓄冷材が
充填されてなる蓄冷器において、蓄冷材を、少なくとも
Ce,Gd,Tb,Dy,Ho,Er,Tm,Pr,N
dの1種又は2種以上である希土類元素35〜95at
%と、少なくともSiを含有する添加物5〜65at%
とから成る磁性体としたことである。In order to solve the above technical problems, the technical means taken in the present invention is a regenerator filled with a regenerator material, wherein the regenerator material is at least Ce, Gd, Tb, Dy, Ho, Er, Tm, Pr, N
rare earth element 35-95 at which is one or more of d
%, And an additive containing at least Si 5 to 65 at%
That is, the magnetic substance is composed of.
【0008】ここで、Ce,Gd,Tb,Dy,Ho,
Er,Tm,Pr,Ndの1種又は2種以上を含有する
希土類元素35〜95at%とSiを含有する添加物5
〜65at%とからなる磁性体を用いた蓄冷材では、図
1及び図2から明らかなように、R、RSi化合物、R
Si2 化合物、R5 Si4 化合物等が混在した組織が生
成する。そして、これらの化合物の磁気変態点が略8〜
30Kとなるものが多く、磁気変態点付近では比熱のピ
ークが存在することから、略8〜30Kで比熱を向上す
ることができる。Here, Ce, Gd, Tb, Dy, Ho,
Additive 5 containing 35 to 95 at% of rare earth element containing one or more of Er, Tm, Pr and Nd and Si
In the regenerator material using the magnetic substance composed of ˜65 at%, as is clear from FIGS. 1 and 2, R, RSi compound, R
A structure in which Si 2 compound, R 5 Si 4 compound, etc. are mixed is generated. And the magnetic transformation point of these compounds is about 8 to
Since many of them have a temperature of 30 K and a peak of the specific heat exists near the magnetic transformation point, the specific heat can be improved at about 8 to 30 K.
【0009】希土類元素の含有量が35at%未満(即
ち添加物の含有量が65at%より多い)であると、図
2に示すEr−Siの状態図の例から明らかなように、
その磁気変態点が略8〜30KとなるEr5 Si3 ,E
r5 Si4 ,ErSi,Er3 Si5 ,ErSi2 等が
混在した組織が全く生成しない(ここで、Er5 S
i3 ,Er3 Si5 ,ErSi2 については、図1によ
り磁気変態点が明らかにされていないが、これらの磁気
変態点も略0〜30Kの範囲内にある。)。さらに、格
子系の比熱しかもたないSi単体の相を生成することか
ら、8〜30Kでの比熱を向上させることができない。
一方、希土類元素の含有量が95at%を越える(即ち
添加物の含有量が5%未満である)と、10K前後での
比熱が低下することが実験的に確認された。When the content of the rare earth element is less than 35 at% (that is, the content of the additive is more than 65 at%), as is clear from the example of the phase diagram of Er-Si shown in FIG.
Its magnetic transformation point becomes substantially 8~30K Er 5 Si 3, E
A structure in which r 5 Si 4 , ErSi, Er 3 Si 5 , ErSi 2 and the like are mixed is not generated at all (here, Er 5 S
The magnetic transformation points of i 3 , Er 3 Si 5 and ErSi 2 are not clarified in FIG. 1, but these magnetic transformation points are also within the range of approximately 0 to 30K. ). Furthermore, since the phase of Si simple substance having only the specific heat of the lattice system is generated, the specific heat at 8 to 30K cannot be improved.
On the other hand, it was experimentally confirmed that when the content of the rare earth element exceeds 95 at% (that is, the content of the additive is less than 5%), the specific heat decreases around 10K.
【0010】又、図2より希土類元素Rの含有量が35
〜40at%(添加物の含有量が60〜65at%)の
ときには、ErSi2 化合物とEr3 Si5 化合物との
混在した組織を生成させることができ、希土類元素Rの
含有量が40〜50at%(添加物の含有量が50〜6
0at%)のときには、Er3 Si5 化合物とErSi
化合物との混在した組織を生成させることができ、希土
類元素Rの含有量が50〜55at%(添加物の含有量
が45〜50at%)のときには、ErSi化合物とE
r5 Si4 化合物との混在した組織を生成させることが
でき、希土類元素の含有量が55at%〜63at%
(添加物の含有量が37〜45at%)のときには、E
r5 Si4 化合物とEr5 Si3 化合物との混在した組
織を生成させることができ、希土類元素が63at%〜
95at%(添加物の含有量が5〜37at%)のとき
にはEr5 Si3 化合物とErとの混在した組織を生成
させることができることから、その混在した組織の比率
に応じて比熱のピークが調節可能となる。Further, from FIG. 2, the content of the rare earth element R is 35.
When the content of the additive is ˜40 at% (the content of the additive is 60-65 at%), a structure in which the ErSi 2 compound and the Er 3 Si 5 compound are mixed can be generated, and the content of the rare earth element R is 40 to 50 at%. (The content of the additive is 50 to 6
0 at%), Er 3 Si 5 compound and ErSi
It is possible to generate a structure mixed with a compound, and when the content of the rare earth element R is 50 to 55 at% (the content of the additive is 45 to 50 at%), the ErSi compound and the E
It is possible to generate a structure in which an r 5 Si 4 compound is mixed, and the content of the rare earth element is 55 at% to 63 at%.
When the content of the additive is 37 to 45 at%, E
It is possible to generate a texture in which an r 5 Si 4 compound and an Er 5 Si 3 compound are mixed, and the rare earth element is 63 at% or more.
When the content is 95 at% (the content of the additive is 5 to 37 at%), a mixed structure of Er 5 Si 3 compound and Er can be generated, so that the peak of specific heat is adjusted according to the ratio of the mixed structure. It will be possible.
【0011】上記技術的手段において、5〜8Kの比熱
を向上させるために、前記添加物内に、B,Al,I
n,Ag,Ge,Ga,Sn,Au,Mg,Zn,P
d,Pt,Re,Cs,Ir,Fe,Mn,Cr,C
d,Hg,Osの内の少なくとも1種の元素を含有させ
ることが望ましい。これらの元素が作る化合物は、磁気
変態点が30K以下であるので、5〜8Kの比熱を一層
向上させることができる。In the above technical means, in order to improve the specific heat of 5 to 8K, B, Al and I are added in the additive.
n, Ag, Ge, Ga, Sn, Au, Mg, Zn, P
d, Pt, Re, Cs, Ir, Fe, Mn, Cr, C
It is desirable to contain at least one element selected from d, Hg and Os. Since the magnetic transformation point of the compound formed by these elements is 30 K or less, the specific heat of 5 to 8 K can be further improved.
【0012】ここで、8〜30Kでの比熱を低下させな
いようにするために、これら元素の含有量を、5at%
以下にすることが望ましい。5at%よりも多くなる
と、8〜30Kでの比熱が低下する恐れがある。Here, in order not to lower the specific heat at 8 to 30 K, the content of these elements is 5 at%.
The following is desirable. If it exceeds 5 at%, the specific heat at 8 to 30 K may decrease.
【0013】[0013]
【作用】上記技術的手段によれば、蓄冷材を、少なくと
もCe,Gd,Tb,Dy,Ho,Er,Tm,Pr,
Ndの1種又は2種以上である希土類元素35〜95a
t%と、少なくともSiを含有する添加物5〜65at
%とから構成したので、磁気変態点が略8〜30Kとな
るR5 Si4 ,RSi,RSi2 等が混在した組織が主
に生成することから、従来のEr3 Niから成る磁気変
態点が略8Kの蓄冷材と比較して、8〜30Kでの比熱
を向上させることができる。According to the above technical means, the regenerator material is at least Ce, Gd, Tb, Dy, Ho, Er, Tm, Pr,
One or more Nd rare earth elements 35-95a
5% to 65 at% of an additive containing t% and at least Si
%, The structure in which R 5 Si 4 , RSi, RSi 2 and the like having a magnetic transformation point of about 8 to 30 K are mainly mixed is generated, so that the conventional magnetic transformation point of Er 3 Ni is The specific heat at 8 to 30K can be improved as compared with the cold storage material at about 8K.
【0014】以上より、8〜30Kでの蓄熱効率を向上
させることができ、上記技術的手段による蓄冷器を8〜
30Kの冷凍を発生する冷凍機に適用可能となる。From the above, the heat storage efficiency at 8 to 30K can be improved, and the regenerator by the above technical means can be used at 8 to 30K.
It can be applied to refrigerators that generate 30K of refrigeration.
【0015】[0015]
〔実施例1〕Erブロック8.56g(50at%)と
Siブロック1.44g(50at%)とをアーク溶解
炉に配置し、アーク溶解炉内を真空吸引した後、アルゴ
ンガスにて置換する。その後、アーク溶解して蓄冷材を
製造し、5×5×7mmに切断する。ここで、図2に示
す状態図から、上記の如く製造した蓄冷材は、ErとS
iが正確に50at%であればErSi(磁気変態点1
0K,比熱ピーク12K)のみしか生成されないが、わ
ずかな配合の誤差により、Er5 Si4 またはEr3 S
i5 とErSiとの混在した組織となる。[Example 1] 8.56 g (50 at%) of Er block and 1.44 g (50 at%) of Si block were placed in an arc melting furnace, and the inside of the arc melting furnace was vacuum-suctioned and then replaced with argon gas. Then, arc melting is performed to manufacture a regenerator material, which is cut into 5 × 5 × 7 mm. Here, from the state diagram shown in FIG. 2, the regenerator materials manufactured as described above are Er and S
If i is exactly 50 at%, ErSi (magnetic transformation point 1
Only 0K, specific heat peak 12K) is produced, but due to a slight composition error, Er 5 Si 4 or Er 3 S
The structure has a mixture of i 5 and ErSi.
【0016】次に、上記の如く製造した蓄冷材の比熱を
Ge温度計を用いて断熱法により略3〜30Kで測定し
た。ここで、断熱法とは、断熱条件下で試料(ここでは
インゴッド)にジュール熱ΔQを加えたときの温度変化
ΔTを測定して、ジュール熱ΔQを温度変化ΔTで割っ
た値を比熱ΔCとする方法である。この比熱測定結果を
図3に示す。Next, the specific heat of the regenerator material manufactured as described above was measured at about 3 to 30 K by the adiabatic method using a Ge thermometer. Here, the adiabatic method is to measure the temperature change ΔT when Joule heat ΔQ is applied to a sample (here, ingot) under adiabatic conditions, and divide the Joule heat ΔQ by the temperature change ΔT to obtain the specific heat ΔC. Is the way to do it. The specific heat measurement result is shown in FIG.
【0017】図3から明らかなように、実施例1の蓄冷
材では、Er3 Niを用いた蓄冷材(従来例1)及びP
bを用いた蓄冷材(従来例2)と比較して、略8〜12
Kでの比熱が大きくなり、12〜30Kで従来例とほぼ
同等の比熱を有していることが分かる。これは、実施例
1の蓄冷材は、大部分がErSi化合物(磁気変態点1
0K)であることから、比熱のピークが略8K〜12K
に存在するためであると考えられる。As is apparent from FIG. 3, in the cold storage material of Example 1, the cold storage material using Er 3 Ni (conventional example 1) and P were used.
Compared with the cold storage material using b (conventional example 2), approximately 8 to 12
It can be seen that the specific heat at K becomes large, and the specific heat at 12 to 30 K is almost the same as the conventional example. Most of the regenerator materials of Example 1 were ErSi compounds (magnetic transformation point 1
0K), the peak of specific heat is about 8K-12K
It is thought to be because it exists in.
【0018】〔実施例2〕Hoブロック8.54g(5
0at%)とSiブロック1.46g(50at%)と
をアーク溶解炉に配置したこと以外は、実施例1と同様
である。この場合、実施例2の蓄冷材は、HoとSiが
正確に50at%であればHoSi(磁気変態点25
K,比熱ピーク21K)のみしか生成されないが、わず
かな配合の誤差により、Ho5 Si4 またはHo3 Si
5 とHoSiとの混在した組織となる。[Embodiment 2] Ho block 8.54 g (5
0 at%) and Si block 1.46 g (50 at%) were placed in an arc melting furnace, and the same as Example 1. In this case, the regenerator material of Example 2 had HoSi (magnetic transformation point 25
K, specific heat peak 21K) is produced, but due to slight composition error, Ho 5 Si 4 or Ho 3 Si
The organization will be a mixture of 5 and HoSi.
【0019】実施例2の蓄冷材の比熱を実施例1と同様
に測定し、その測定結果を図3に示す。The specific heat of the regenerator material of Example 2 was measured in the same manner as in Example 1, and the measurement results are shown in FIG.
【0020】図3から明らかなように、実施例2の蓄冷
材でも、Er3 Niを用いた蓄冷材(従来例1)及びP
bを用いた蓄冷材(従来例2)と比較して、略10〜3
0Kでの比熱が大きくなっている。これは、実施例2の
蓄冷材は、大部分がHoSi化合物(磁気変態点25
K)であることから、比熱ピークが23K付近に存在す
るためと考えられる。As is apparent from FIG. 3, even in the regenerator material of Example 2, the regenerator material using Er 3 Ni (conventional example 1) and P were used.
Compared with the regenerator material using b (conventional example 2), approximately 10 to 3
The specific heat at 0K is large. Most of the regenerator materials of Example 2 were HoSi compounds (magnetic transformation point 25
Since it is K), it is considered that the specific heat peak exists near 23K.
【0021】〔従来例1〕Erブロック8.95g(7
5at%)とNiブロック1.05g(25at%)と
をアーク溶解炉に配置したこと以外は、実施例1と同様
である。ここで、従来例1の蓄冷材は、Er3 Ni(磁
気変態点8K)であり、その比熱を実施例1と同様に測
定し、その測定結果を図3に示す。[Conventional Example 1] Er block 8.95 g (7
5 at%) and Ni block 1.05 g (25 at%) were placed in the arc melting furnace, and the same as Example 1. Here, the regenerator material of Conventional Example 1 was Er 3 Ni (magnetic transformation point 8K), and its specific heat was measured in the same manner as in Example 1, and the measurement result is shown in FIG.
【0022】図4から明らかなように、従来例1の蓄冷
材は、8K以下での比熱は大きいが、8K以上での比熱
は実施例1,2と比較して小さくなっている。これは、
Er3 Niの磁気変態点が8Kに存在し、比熱のピーク
が7K付近に存在するためであると考えられる。As is apparent from FIG. 4, the regenerator material of Conventional Example 1 has a large specific heat at 8 K or less, but the specific heat at 8 K or more is smaller than that of Examples 1 and 2. this is,
It is considered that this is because the magnetic transformation point of Er 3 Ni exists at 8K and the peak of specific heat exists near 7K.
【0023】〔従来例2〕Pb10gを溶解して蓄冷材
を製造したもので、この蓄冷材の比熱を実施例1と同様
に測定し、その測定結果を図3に示す。[Conventional Example 2] A regenerator material was manufactured by melting 10 g of Pb. The specific heat of this regenerator material was measured in the same manner as in Example 1, and the measurement results are shown in FIG.
【0024】図3から明らかなように、従来例2の蓄冷
材は、25K以下での比熱は実施例1,2と比較して小
さくなっている。これは、格子振動に基づく格子系の比
熱が温度降下と共に著しく低下すると共にスピン系の比
熱をもたないためであると考えられる。As is apparent from FIG. 3, the specific heat at 25 K or less is smaller in the regenerator material of Conventional Example 2 than in Examples 1 and 2. It is considered that this is because the specific heat of the lattice system due to the lattice vibration is remarkably lowered with the temperature drop and does not have the specific heat of the spin system.
【0025】尚実施例1,2に係る蓄冷材が充填された
蓄冷器は、30K以下特に8〜30Kの冷凍を発生する
スターリング式,GM式,パルス管式,ゾルベー式,共
鳴管式等の各種の冷凍機に適用できる。又、多段冷凍機
の温度に合わせて、各段に用いることも可能である。The regenerator filled with the regenerator material according to Examples 1 and 2 is of a Stirling type, a GM type, a pulse tube type, a Solvay type, a resonance tube type or the like which produces a refrigeration of 30 K or less, particularly 8 to 30 K. It can be applied to various refrigerators. It is also possible to use each stage according to the temperature of the multistage refrigerator.
【0026】[0026]
【発明の効果】本発明は、以下の如く効果を有する。The present invention has the following effects.
【0027】本発明によれば、蓄冷材を、少なくともC
e,Gd,Tb,Dy,Ho,Er,Tm,Pr,Nd
の1種又は2種以上である希土類元素35〜95at%
と、少なくともSiを含有する添加物5〜65at%と
から構成したので、8〜30Kでの比熱を向上させるこ
とができる。その結果、8〜30Kでの蓄冷効率を向上
させることができ、8〜30Kの冷凍を発生する冷凍機
に適用可能となる。According to the present invention, the regenerator material is at least C
e, Gd, Tb, Dy, Ho, Er, Tm, Pr, Nd
35% to 95 at% of rare earth elements that are one or more of
And at least 5 to 65 at% of an additive containing Si, the specific heat at 8 to 30 K can be improved. As a result, the cold storage efficiency at 8 to 30K can be improved, and the present invention can be applied to a refrigerator that generates refrigeration at 8 to 30K.
【図1】本発明に係る蓄冷材内に存在する合金の磁気変
態点を示すグラフである。FIG. 1 is a graph showing a magnetic transformation point of an alloy existing in a regenerator material according to the present invention.
【図2】Er−Siの状態図である。FIG. 2 is a phase diagram of Er—Si.
【図3】本発明の実施例1,2及び従来例1,2の低温
での比熱特性を示すグラフである。FIG. 3 is a graph showing specific heat characteristics at low temperatures of Examples 1 and 2 of the present invention and Conventional Examples 1 and 2.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 星 野 善 樹 愛知県丹羽郡扶桑町高木473 (72)発明者 水 谷 宇一郎 愛知県名古屋市南区外山2丁目12−6 ─────────────────────────────────────────────────── ─── Continuation of front page (72) Inventor Yoshiki Hoshino 473 Takagi, Fuso-cho, Niwa-gun, Aichi (72) Inventor Uichiro Mizutani 2-12-6 Sotoyama, Minami-ku, Nagoya-shi, Aichi
Claims (3)
て、 前記蓄冷材は、少なくともCe,Gd,Tb,Dy,H
o,Er,Tm,Pr,Ndの1種又は2種以上である
希土類元素35〜95at%と、少なくともSiを含有
する添加物5〜65at%とから成る磁性体であること
を特徴とする蓄冷器。1. A regenerator filled with a regenerator material, wherein the regenerator material is at least Ce, Gd, Tb, Dy, H.
A cold storage characterized by being a magnetic material comprising 35 to 95 at% of a rare earth element which is one or more of o, Er, Tm, Pr and Nd, and 5 to 65 at% of an additive containing at least Si. vessel.
n,Au,Mg,Zn,Pd,Pt,Re,Cs,I
r,Fe,Mn,Cr,Cd,Hg,Osの内の少なく
とも1種の元素を含有していることを特徴とする蓄冷
器。2. The regenerator according to claim 1, wherein the additive is B, Al, In, Ag, Ge, Ga, S.
n, Au, Mg, Zn, Pd, Pt, Re, Cs, I
A regenerator characterized by containing at least one element selected from r, Fe, Mn, Cr, Cd, Hg, and Os.
あることを特徴とする蓄冷器3. The regenerator according to claim 2, wherein the content of the at least one element is 5 at% or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32310794A JPH08178443A (en) | 1994-12-26 | 1994-12-26 | Regenerator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32310794A JPH08178443A (en) | 1994-12-26 | 1994-12-26 | Regenerator |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH08178443A true JPH08178443A (en) | 1996-07-12 |
Family
ID=18151162
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP32310794A Pending JPH08178443A (en) | 1994-12-26 | 1994-12-26 | Regenerator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH08178443A (en) |
-
1994
- 1994-12-26 JP JP32310794A patent/JPH08178443A/en active Pending
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