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JPH0428985B2 - - Google Patents
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JPH0428985B2 - - Google Patents

Info

Publication number
JPH0428985B2
JPH0428985B2 JP57067272A JP6727282A JPH0428985B2 JP H0428985 B2 JPH0428985 B2 JP H0428985B2 JP 57067272 A JP57067272 A JP 57067272A JP 6727282 A JP6727282 A JP 6727282A JP H0428985 B2 JPH0428985 B2 JP H0428985B2
Authority
JP
Japan
Prior art keywords
magnetic
cylinder
magnetic field
liquid helium
opening
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
Application number
JP57067272A
Other languages
Japanese (ja)
Other versions
JPS58184469A (en
Inventor
Hisanao Ogata
Yoshinori Shiraku
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP6727282A priority Critical patent/JPS58184469A/en
Publication of JPS58184469A publication Critical patent/JPS58184469A/en
Publication of JPH0428985B2 publication Critical patent/JPH0428985B2/ja
Granted legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F25REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
    • F25BREFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
    • F25B2321/00Details of machines, plants or systems, using electric or magnetic effects
    • F25B2321/002Details of machines, plants or systems, using electric or magnetic effects by using magneto-caloric effects
    • F25B2321/0021Details of machines, plants or systems, using electric or magnetic effects by using magneto-caloric effects with a static fixed magnet

Description

【発明の詳細な説明】 本発明は磁性体の断熱消磁によつて冷凍を発生
する磁気冷凍機に係り、特に超流動ヘリウムの発
生に好適な回転型磁気冷凍機に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic refrigerator that generates refrigeration by adiabatic demagnetization of a magnetic material, and particularly to a rotary magnetic refrigerator suitable for generating superfluid helium.

従来の磁気冷凍機としては往復動型および回転
型のものが知られている。往復動型のものは、磁
性体を高磁界中に往復運動によつて出し入れする
ものであるが、モータ駆動の場合、回転運動を直
線運動に変換する機構を要し、かつストロークが
大きくなるため駆動部分が複雑かつ大形になる。
また、回転型のものは、回転体中に作動流体を流
すため気密の確保に問題があり、流体循環の手段
を要するなど、きわめて複雑な構成であつた。
Reciprocating type and rotary type types are known as conventional magnetic refrigerators. The reciprocating type moves the magnetic material in and out of a high magnetic field by reciprocating motion, but motor drive requires a mechanism to convert rotational motion into linear motion and requires a large stroke. The driving part becomes complicated and large.
In addition, the rotary type has a problem in ensuring airtightness because the working fluid flows through the rotating body, and requires means for fluid circulation, and has an extremely complicated structure.

本発明の目的は、このような問題点を解決した
単純な構造の回転型磁気冷凍機を提供することに
ある。
An object of the present invention is to provide a rotary magnetic refrigerator with a simple structure that solves these problems.

本発明の回転型磁気冷凍機は、外表面が一部露
出した複数個の磁性体を断熱性の円柱体の周面に
埋め込み、この円柱体の外周側に極めて小さい間
隙を保つて設けられた静止円筒の一部に少なくと
も高温の液体ヘリウム浴につながる開口と、低温
の超流動ヘリウム浴につながる開口を有し、前記
の液体ヘリウム浴につながる開口周辺に高磁界を
発生する電磁石を配置し、円柱体の周面に埋め込
まれた磁性体の露出した外表面が前記各ヘリウム
と各開口部において直接に接触し、かつ該磁性体
が高磁界部と超流動ヘリウム浴につながる開口部
を交互に通過するよう円柱体を回転させることを
特徴とする。
In the rotary magnetic refrigerator of the present invention, a plurality of magnetic bodies whose outer surfaces are partially exposed are embedded in the circumferential surface of an insulating cylindrical body, and an extremely small gap is maintained on the outer periphery of the cylindrical body. A part of the stationary cylinder has at least an opening connected to a high-temperature liquid helium bath and an opening connected to a low-temperature superfluid helium bath, and an electromagnet that generates a high magnetic field is arranged around the opening connected to the liquid helium bath, The exposed outer surface of the magnetic material embedded in the circumferential surface of the cylindrical body is in direct contact with the helium at each opening, and the magnetic material alternates between the openings connected to the high magnetic field part and the superfluid helium bath. The feature is that the cylindrical body is rotated so that it passes through.

すなわち外表面が一部露出した磁性体を断熱性
の円柱体の周面に埋め込み、この磁性体部分が高
磁界部と寒冷取り出し部(低磁界部)とを交互に
通過するように円柱体を回転させ、円柱体の周囲
は極めて小さい間隙を保つた円筒で囲まれてい
る。
In other words, a magnetic material whose outer surface is partially exposed is embedded in the circumferential surface of a heat-insulating cylindrical body, and the cylindrical body is constructed such that the magnetic material portion alternately passes through a high magnetic field section and a cold extraction section (low magnetic field section). The cylindrical body is rotated and surrounded by a cylinder with an extremely small gap.

超流動ヘリウム対応の冷凍機を例にとれば、高
温部(高磁界部)は4.2Kの液体ヘリウム浴に開
口することになり、低温部(低磁界部)は2K以
下の超流動ヘリウム浴に開口することになる。
Taking a superfluid helium compatible refrigerator as an example, the high temperature section (high magnetic field section) opens into a 4.2K liquid helium bath, and the low temperature section (low magnetic field section) opens into a superfluid helium bath below 2K. It will be opened.

尚、低温液体ヘリウム側において、磁性体は低
磁場中にあるため液体ヘリウムよりも低温にあ
る。この液体ヘリウムが超流動ヘリウムの場合
は、カピツツア熱伝達(固体同士の接触熱伝達の
ようなもの。超流動ヘリウムは液体ヘリウムの一
態様だが通常の液体とは異なり、伝熱に関しては
固体と同じ。)が生じ、液体ヘリウムを冷却する。
液体ヘリウムが超流動ヘリウムでない場合は、磁
性体表面近傍の自然対流により液体ヘリウムを冷
却する(これは、冷えた容器に熱い水を入れると
自然対流で水が冷えてしまう場合と同じ。)。本発
明においては、回転速度は非常にゆつくりとして
いるのでこれら冷却において“回転している場
合”は、実質的に“静止している場合”と同様で
ある。
Note that on the low-temperature liquid helium side, the magnetic material is in a low magnetic field, so it is at a lower temperature than the liquid helium. If this liquid helium is superfluid helium, Kapitatsu heat transfer (like contact heat transfer between solids). Superfluid helium is a form of liquid helium, but it is different from normal liquids and has the same heat transfer as solids. ) occurs and cools the liquid helium.
If the liquid helium is not superfluid helium, it is cooled by natural convection near the surface of a magnetic material (this is the same as when hot water is poured into a cold container and the water is cooled by natural convection). In the present invention, since the rotational speed is very slow, the "rotating case" in cooling is substantially the same as the "stationary case".

以下、本発明の一実施例を第1図及び第2図に
より説明する。2個の磁性体1a及び1bが円柱
体2中に、表面を露出させた状態で埋め込まれて
いる。磁性体1a,1bとしては、Gd3Ga5O12
(ガドリウム・ガリウム・ガーネツト)やGd2
(SO438H2Oと銅網を積層したものなどを使い、
円柱2としてはアルミナ、結晶化ガラス、繊維強
化樹脂など磁性体1と同程度の膨張係数をもちか
つ熱伝導率の低いものを使う。磁性体1a及び1
bの表面は円柱2と同一外径とする。円筒3の内
径は円柱2の外径より20〜40μm大きい。円筒3
の材料は熱伝導率の低いものがよい。円筒3に設
けた開口4aと4bは軸対称の位置に設けてあ
り、周囲の液体ヘリウム5と連通している。鞍形
に巻かれた2ケの超電導コイル6aと6bは2極
マグネツトを構成し、一方向磁界7を発生する。
いつぽう、円筒3の開口4a,4bから90°ずれ
た位置に開口8a,8bを設け、断熱壁からなる
寒冷発生室9a,9bと連結されている。
An embodiment of the present invention will be described below with reference to FIGS. 1 and 2. Two magnetic bodies 1a and 1b are embedded in a cylindrical body 2 with their surfaces exposed. As the magnetic materials 1a and 1b, Gd 3 Ga 5 O 12
(gadolium gallium garnet) or Gd 2
(SO 4 ) 3 8H 2 O and copper mesh are used.
The cylinder 2 is made of a material such as alumina, crystallized glass, or fiber-reinforced resin that has a coefficient of expansion comparable to that of the magnetic material 1 and has a low thermal conductivity. Magnetic materials 1a and 1
The surface of b has the same outer diameter as the cylinder 2. The inner diameter of the cylinder 3 is 20 to 40 μm larger than the outer diameter of the cylinder 2. cylinder 3
The material should have low thermal conductivity. Openings 4a and 4b provided in the cylinder 3 are provided at axially symmetrical positions and communicate with the surrounding liquid helium 5. Two superconducting coils 6a and 6b wound in a saddle shape constitute a two-pole magnet and generate a unidirectional magnetic field 7.
On the other hand, openings 8a and 8b are provided at positions shifted by 90 degrees from the openings 4a and 4b of the cylinder 3, and are connected to cold generation chambers 9a and 9b consisting of heat insulating walls.

第2図は、回転軸10を中心に、A−O−B断
面を示してある。ただし、いずれも磁性体がその
断面内にある時を想定している。
FIG. 2 shows an A-O-B cross section centered on the rotating shaft 10. However, both assume that the magnetic material is within the cross section.

第1図の状態で磁性体1a,1bは磁化され発
熱し、液体ヘリウム5の沸騰によつて冷却され
る。次いで、円柱2は90°回転し、磁性体は点線
で示した位置11にくる。磁界が小さくなるため
に磁性体中で吸熱がおこり、寒冷発生室9a,9
b内の液体ヘリウム12の温度が下がる。寒冷発
生室9aと9bは配管等で連結してある。このよ
うなサイクルを繰り返すことにより、液体ヘリウ
ム12を2.2K以下の超流動ヘリウムにすること
ができる。寒冷発生室9a,9bの周囲は、低熱
伝導率の壁または真空断熱壁で形成され、液体ヘ
リウム5と液体ヘリウム12との熱的隔離は、円
筒3と円柱2の間隙を微小にすることによつて実
現されている。
In the state shown in FIG. 1, the magnetic bodies 1a and 1b are magnetized and generate heat, and are cooled by boiling of the liquid helium 5. The cylinder 2 is then rotated 90°, and the magnetic body is at position 11, indicated by the dotted line. As the magnetic field becomes smaller, heat absorption occurs in the magnetic material, and the cold generation chambers 9a, 9
The temperature of liquid helium 12 in b decreases. The cold generation chambers 9a and 9b are connected by piping or the like. By repeating such a cycle, the liquid helium 12 can be made into superfluid helium of 2.2K or less. The periphery of the cold generation chambers 9a and 9b is formed by a wall with low thermal conductivity or a vacuum insulation wall, and thermal isolation between the liquid helium 5 and the liquid helium 12 is achieved by making the gap between the cylinder 3 and the cylinder 2 minute. It has been realized.

第3図は本発明の別の実施例で、磁界発生部に
ポールピースを使つたものである。すなわち、第
1図における超電導コイル6aと6bのかわりに
ポールピース13a,13bおよび超電導コイル
14a,14bを設けたもので、磁界の方向はポ
ールピースの先端を結ぶような向きになる。
FIG. 3 shows another embodiment of the present invention, in which a pole piece is used as the magnetic field generating section. That is, pole pieces 13a and 13b and superconducting coils 14a and 14b are provided in place of superconducting coils 6a and 6b in FIG. 1, and the direction of the magnetic field is oriented to connect the tips of the pole pieces.

第4図は、ポールピースを使つた別の実施例を
示す。高磁界発生部と寒冷発生部を同一断面に示
してある。ここで、ポールピース15は超電導コ
イル16と組み合わされ、磁性体に対して回転軸
と平行な磁界を加えることができる。
FIG. 4 shows another embodiment using pole pieces. The high magnetic field generation part and the cold generation part are shown in the same cross section. Here, the pole piece 15 is combined with the superconducting coil 16, and can apply a magnetic field parallel to the rotation axis to the magnetic body.

以上述べた如く、本発明は流体が作業物質に直
接触れているので、作業物質と流体との直接的な
熱接触が図れ、接触熱抵抗はない。しかも本発明
では、磁性体自体を回転移動させて流体に接触さ
せており、流体を回転体に流す構造ではないか
ら、簡単な装置構成で寒冷発生が可能となるとい
う効果がある。また、円筒体と円柱体の間は回転
させるべく間隙を有するが、この間隙は極めて小
さくしてあるので、回転体が流体に直接接触する
ことに起因する熱のリークを防ぐことができる。
As described above, in the present invention, since the fluid is in direct contact with the working substance, direct thermal contact between the working substance and the fluid can be achieved, and there is no contact thermal resistance. Moreover, in the present invention, since the magnetic body itself is rotated and brought into contact with the fluid, and the structure is not such that the fluid flows through the rotating body, there is an effect that cooling can be generated with a simple device configuration. Further, although there is a gap between the cylindrical bodies for rotation, this gap is made extremely small, so that heat leakage due to direct contact of the rotating body with the fluid can be prevented.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明の一実施例を示す横断面図、第
2図は第1図のA−O−B線の縦断面図、第3図
は本発明の別の実施例を示す横断面図、第4図は
本発明の他の実施例を示す縦断面図である。 1a,1b……磁性体、2……円柱、3……円
筒、6a,6b,14a,14b,16……超電
導コイル、9a,9b……寒冷発生部。
FIG. 1 is a cross-sectional view showing one embodiment of the present invention, FIG. 2 is a vertical cross-sectional view taken along line A-O-B in FIG. 1, and FIG. 3 is a cross-sectional view showing another embodiment of the present invention. 4 are longitudinal sectional views showing other embodiments of the present invention. 1a, 1b...Magnetic material, 2...Cylinder, 3...Cylinder, 6a, 6b, 14a, 14b, 16...Superconducting coil, 9a, 9b...Cold generation part.

Claims (1)

【特許請求の範囲】[Claims] 1 外表面が一部露出した複数個の磁性体を断熱
性の円柱体の周面に埋め込み、この円柱体の外周
側に極めて小さい間隙を保つて設けられた静止円
筒の一部に少なくとも高温の液体ヘリウム浴につ
ながる開口と、低温の超流動ヘリウム浴につなが
る開口を有し、前記液体ヘリウム浴につながる開
口周辺に高磁界を発生する電磁石を配置し、前記
円柱体の周面に埋め込まれた磁性体の露出した外
表面が前記ヘリウムと各開口部において直接に接
触し、かつ該磁性体が高磁界部と超流動ヘリウム
浴につながる開口部を交互に通過するよう円柱体
を回転させることを特徴とする回転型磁気冷凍
機。
1. A plurality of magnetic bodies whose outer surfaces are partially exposed are embedded in the circumferential surface of a heat-insulating cylinder, and at least a part of a stationary cylinder provided with an extremely small gap on the outer circumference of the cylinder is heated to a high temperature. It has an opening connected to a liquid helium bath and an opening connected to a low-temperature superfluid helium bath, and an electromagnet that generates a high magnetic field is arranged around the opening connected to the liquid helium bath, and is embedded in the circumferential surface of the cylindrical body. The cylindrical body is rotated so that the exposed outer surface of the magnetic body is in direct contact with the helium at each opening, and the magnetic body passes alternately through the high magnetic field section and the opening leading to the superfluid helium bath. A rotating magnetic refrigerator with special features.
JP6727282A 1982-04-23 1982-04-23 Rotary type magnetic refrigerator Granted JPS58184469A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6727282A JPS58184469A (en) 1982-04-23 1982-04-23 Rotary type magnetic refrigerator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6727282A JPS58184469A (en) 1982-04-23 1982-04-23 Rotary type magnetic refrigerator

Publications (2)

Publication Number Publication Date
JPS58184469A JPS58184469A (en) 1983-10-27
JPH0428985B2 true JPH0428985B2 (en) 1992-05-15

Family

ID=13340153

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6727282A Granted JPS58184469A (en) 1982-04-23 1982-04-23 Rotary type magnetic refrigerator

Country Status (1)

Country Link
JP (1) JPS58184469A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006112709A (en) * 2004-10-14 2006-04-27 Ebara Corp Magnetic refrigerating device
FR2904098B1 (en) * 2006-07-24 2008-09-19 Cooltech Applic Soc Par Action MAGNETOCALORIC THERMAL GENERATOR

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3108444A (en) * 1962-07-19 1963-10-29 Martin Marietta Corp Magneto-caloric cryogenic refrigerator
US4107935A (en) * 1977-03-10 1978-08-22 The United States Of America As Represented By The United States Department Of Energy High temperature refrigerator
FR2517415A1 (en) * 1981-11-27 1983-06-03 Commissariat Energie Atomique METHOD FOR REFRIGERATING OR HEAT PUMPING AND DEVICE FOR CARRYING OUT SAID METHOD

Also Published As

Publication number Publication date
JPS58184469A (en) 1983-10-27

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