JPH0428210A - Cryogenic temperature device for superconducting coil - Google Patents
Cryogenic temperature device for superconducting coilInfo
- Publication number
- JPH0428210A JPH0428210A JP13303490A JP13303490A JPH0428210A JP H0428210 A JPH0428210 A JP H0428210A JP 13303490 A JP13303490 A JP 13303490A JP 13303490 A JP13303490 A JP 13303490A JP H0428210 A JPH0428210 A JP H0428210A
- Authority
- JP
- Japan
- Prior art keywords
- liquid nitrogen
- pipe
- thermal shielding
- shielding plate
- heat shield
- 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.)
- Granted
Links
Landscapes
- Containers, Films, And Cooling For Superconductive Devices (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は、超電導マグネットにおける液体窒素熱シー
ルド板の冷却方式に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a method for cooling a liquid nitrogen heat shield plate in a superconducting magnet.
[従来の技術]
これまで製作されてきた極低温装置を用いた超電導マグ
ネットの一例を第5図に示す。第5図は文献(電気学会
・リニアドライブ研究会資料(1988−4−26)2
7ページ)に掲載された磁気浮上式鉄道用の超電導マグ
ネットであり、熱シールド板に取り付けられた冷却配管
にポンプあるいは液体窒素槽内の加圧により液体窒素を
強制供給する場合の従来例である。図において、 (2
)が超電導コイルを収めたヘリウム容器である内槽、(
3)は熱シールド板、 (7)は超電導コイルを永久電
流にするための永久電流スイッチ、 (8)は内槽(2
)を断熱的に支持するための荷重支持材、 〈6)はこ
れら内槽(2)、熱シールド板(3)、永久電流スイッ
チ(7)、荷重支持材(8)の各構成物を収納した真空
容器すなわち外槽である。 (4)は図示されていない
液体窒素槽から導かれた液体窒素供給配管である。[Prior Art] FIG. 5 shows an example of a superconducting magnet using a cryogenic device that has been manufactured so far. Figure 5 shows the literature (Institute of Electrical Engineers of Japan/Linear Drive Study Group Materials (1988-4-26) 2
This is a superconducting magnet for magnetic levitation railways published on page 7), and is a conventional example in which liquid nitrogen is forcibly supplied to cooling piping attached to a heat shield plate using a pump or pressurization in a liquid nitrogen tank. . In the figure, (2
) is the inner tank, which is a helium container containing the superconducting coil, (
3) is a heat shield plate, (7) is a persistent current switch to make the superconducting coil persistent current, (8) is an inner tank (2)
) for adiabatic support; <6) houses the components of the inner tank (2), heat shield plate (3), persistent current switch (7), and load support material (8). It is a vacuum container, that is, an outer tank. (4) is a liquid nitrogen supply pipe led from a liquid nitrogen tank (not shown).
次に従来マグネットの動作について熱ンールド関連を主
眼として説明する。内槽く2)には超電導コイルが納め
られており、これと供に超電導コイルを超電導状態に維
持すべく液体ヘリウムが封入されている。この超電導コ
イルは図示されていない電源により電流を供給され、永
久電流スイッチ(7)を利用することにより永久電流モ
ー ドで励磁運転される。超電導コイルを永久電流モー
ドで運転するには超電導状態を維持しなければならない
。そのためには内槽(2)への外部からの熱侵入を極力
減らす必要があるため多くの対策が施されている。それ
か、例えば断熱荷重支持材(8)の採用であり、熱シー
ルド板く3)の設置である。Next, the operation of conventional magnets will be explained with a focus on heat rolling. A superconducting coil is housed in the inner tank 2), and liquid helium is also sealed therein to maintain the superconducting coil in a superconducting state. This superconducting coil is supplied with current by a power source (not shown), and is excited in persistent current mode by using a persistent current switch (7). To operate a superconducting coil in persistent current mode, a superconducting state must be maintained. For this purpose, it is necessary to reduce heat intrusion into the inner tank (2) from the outside as much as possible, and therefore, many measures are taken. Alternatively, for example, the use of heat insulating load supports (8) and the installation of heat shield plates 3) are possible.
断熱荷重支持材(8)は外槽(6)から内槽(2)への
熱伝導による熱侵入を低減するための対策であり、熱シ
ールド板(3)は同じく熱ふく射による熱侵入を低減す
るための対策である。この熱シルト板(3)は通常液体
窒素温度(1気圧下で77.3にルベルに冷却されるが
、この従来例では冷却配管(4)に液体窒素を通ずるこ
とにより液体窒素温度に維持する方法を採用している。The heat insulating load support material (8) is a measure to reduce heat intrusion due to heat conduction from the outer tank (6) to the inner tank (2), and the heat shield plate (3) similarly reduces heat intrusion due to heat radiation. This is a measure to ensure that This thermal silt plate (3) is normally cooled to liquid nitrogen temperature (77.3 lb. under 1 atm), but in this conventional example, it is maintained at the liquid nitrogen temperature by passing liquid nitrogen through the cooling pipe (4). method is adopted.
つまり、この冷却配管(4)は図示されていない液体窒
素槽から導かれており、本装置では窒素貯めに取り例け
られ、だ液体窒素ポンプにより冷却配管(4)内に液体
窒素を強制循環させ、熱シールド板(3)を液体窒素温
度に維持するようにしている。もちろん熱シールド板(
3)にも外槽(6)からの大きな熱ふく射が存在するが
、その分を液体ヘリウムより安価な液体窒素により賄う
というのがこの種の超電導マグネットを設計する際の基
本的思想といえる。In other words, this cooling pipe (4) is led from a liquid nitrogen tank (not shown), which is used as a nitrogen reservoir in this device, and liquid nitrogen is forcedly circulated inside the cooling pipe (4) by a liquid nitrogen pump. The heat shield plate (3) is maintained at the liquid nitrogen temperature. Of course, the heat shield plate (
3) also has a large amount of heat radiation from the outer tank (6), but the basic idea when designing this type of superconducting magnet is to compensate for this with liquid nitrogen, which is cheaper than liquid helium.
[発明が解決しようとする課題]
従来の超伝導コイル用極低温装置は、上述のように構成
され動作しているため以下の問題点がある。先ず液体窒
素用の強制循環装置が必要となるが、これは決して安価
なものではない。また駆動部を持つことから保守も必要
となる。加えて循環装置が異常を来した場合には液体窒
素貯槽内の内圧を」1昇させ液体窒素な自圧供給するの
が通例であるが、そのためバルブ等の装置が別途必要と
なる。[Problems to be Solved by the Invention] Conventional cryogenic devices for superconducting coils are configured and operated as described above, and therefore have the following problems. First, a forced circulation system for liquid nitrogen is required, which is by no means inexpensive. Also, since it has a drive unit, maintenance is required. In addition, if the circulation system malfunctions, it is customary to increase the internal pressure in the liquid nitrogen storage tank by 1 to supply liquid nitrogen at its own pressure, but this requires a separate device such as a valve.
二の発明は上記のような問題点を解消するためになされ
たもので、液体窒素供給のための強制循環装置を必要と
しない送液系を得ることを目的としている。The second invention was made to solve the above-mentioned problems, and aims to provide a liquid feeding system that does not require a forced circulation device for supplying liquid nitrogen.
[課題を解決するための手段]
二の発明に係る超伝導コイ/し用極低温装置は、超伝導
コイノペ この超伝導コイルを収納するヘリウム容器、
このヘリウム容器への外部からの熱侵入を低減するため
の熱シールド板、およびこの熱シールド板を冷却するた
め重力を駆動力とし液体窒素を供給するよう液体窒素貯
槽から導かれかつ熱的に」二層熱シールド板と接続設置
された15m+n以上の内径を有する冷却配管を真空容
器内に備えるものである。[Means for Solving the Problems] The cryogenic device for superconducting coils according to the second invention includes: a superconducting coil; a helium container for storing the superconducting coil;
A heat shield plate is provided to reduce heat intrusion into the helium container from the outside, and a liquid nitrogen is supplied from a liquid nitrogen storage tank using gravity as a driving force to cool the heat shield plate. A vacuum vessel is provided with a cooling pipe having an inner diameter of 15 m+n or more and connected to a two-layer heat shield plate.
[作用]
このように構成された超伝導コイル用極低温装置では、
重力をその駆動力とするため液体窒素槽を熱シールド板
の最高点より高い位置に設置し、冷却配管をふく射熱侵
入により蒸発した窒素ガスが浮力により確実に除去でき
るような大きさ(内径)で構成したので、液体窒素用の
強制循環装置カ必要ではなくかつベー/<−口・ンクに
よる液体窒素不在の現象も引き起こさず極めてシンプル
な装置でありながら熱シールド板を確実に液体窒素温度
レベルに保持できる。[Function] In the cryogenic device for superconducting coils configured in this way,
In order to use gravity as the driving force, the liquid nitrogen tank is installed at a position higher than the highest point of the heat shield plate, and the cooling piping is sized (inner diameter) to ensure that nitrogen gas evaporated due to radiant heat can be removed by buoyancy. Because of this structure, there is no need for a forced circulation device for liquid nitrogen, and the phenomenon of absence of liquid nitrogen due to vaporization does not occur.Although it is an extremely simple device, it can reliably bring the heat shield plate to the liquid nitrogen temperature level. Can be retained.
[実施例]
以下、この発明の一実施例を図について説明する。第1
図において、 (1)は超電導コイル、 (2)はヘリ
ウム容器すなわち内槽、 (3)は熱シルト板、 く4
)は冷却配管、 (5)は液体窒素槽、 (6)は真空
容器すなわち外槽である。第5図の従来例で示されてい
る永久電流スイッチく7)および荷重支持材(8)は簡
略のため図示していない。[Example] Hereinafter, an example of the present invention will be described with reference to the drawings. 1st
In the figure, (1) is a superconducting coil, (2) is a helium container or inner tank, (3) is a thermal silt plate, and (4) is a helium container or inner tank.
) is the cooling pipe, (5) is the liquid nitrogen tank, and (6) is the vacuum container, that is, the outer tank. The persistent current switch 7) and load support member (8) shown in the conventional example of FIG. 5 are not shown for the sake of simplicity.
このように構成された実施例の超電導マグネットとじて
の基本的動作は従来例と同様である。たたし実施例では
、熱シールド板(3)を液体窒素温度に維持するため冷
却配管(4)に液体窒素を供給する駆動力が重力となっ
ている。この場合の問題点は、熱シールド板(3)への
熱負荷に応じて冷却配管(4)内の液体窒素が蒸発する
ためガス成分を巧く液体窒素槽く5)に回収することで
ある。つまり液成分とガス成分とを冷却配管内で巧く向
流的に交換させる必要がある。鉛直的な管内において気
液成分の向流交換を行なおうとした場合、時として蒸発
したガスにより液の落下が妨げられるペーパーロックと
称する現象が現われる。The basic operation of the superconducting magnet of the embodiment configured as described above is the same as that of the conventional example. In this embodiment, the driving force for supplying liquid nitrogen to the cooling pipe (4) is gravity in order to maintain the heat shield plate (3) at the liquid nitrogen temperature. The problem in this case is that the liquid nitrogen in the cooling pipe (4) evaporates depending on the heat load on the heat shield plate (3), so it is necessary to skillfully recover the gas component into the liquid nitrogen tank 5). . In other words, it is necessary to skillfully exchange the liquid component and the gas component in a countercurrent manner within the cooling pipe. When attempting to perform countercurrent exchange of gas-liquid components in a vertical pipe, a phenomenon called paper lock sometimes occurs in which evaporated gas prevents the liquid from falling.
この現象は厳密には管径、熱負荷、流体の粘性、管内壁
面の状態等に影響されため出現・不出現を概に記述する
ことはできないが、管径が小さい場合には非常に生じや
すくなる。従って、冷却配管(4)は太い程良いことに
なる。しかしながら冷却配管く4)を太くすればする程
、外槽(6)内のデッドスペースが増えるため超電導マ
グネツ)・ (外槽)そのものが大きくなり経済的にも
スペス的にも問題となることから、おのずと限度がある
。本発明はこの管径について、どの位に設定すれば良い
かを提供するものである。第2図は長す800 rn
nlのステンレス管を液体窒素槽(5)に垂直にぶらさ
げ、管に熱負荷を印加した場合の最下端部温度を測定し
たものである。この図において、特性曲線A、 B、
C,Dはそれぞれ内径18、14、10.6mmの
場合である。これらの特性曲線より内径が18mmであ
れば全く問題ないことがわかる。つまり特性曲線Aの場
合である。Strictly speaking, this phenomenon is affected by the pipe diameter, heat load, fluid viscosity, condition of the pipe inner wall surface, etc., so it is not possible to describe its appearance or non-appearance generally, but it is very likely to occur when the pipe diameter is small. Become. Therefore, the thicker the cooling pipe (4), the better. However, the thicker the cooling pipe 4), the more dead space inside the outer tank (6), which increases the size of the superconducting magnet (outer tank) itself, which becomes a problem both economically and in terms of space. , there is a limit naturally. The present invention provides information on how much the pipe diameter should be set. Figure 2 is 800 rn long
The temperature at the lowest end was measured when a NL stainless steel tube was hung vertically in a liquid nitrogen tank (5) and a heat load was applied to the tube. In this figure, characteristic curves A, B,
C and D are cases where the inner diameter is 18, 14, and 10.6 mm, respectively. From these characteristic curves, it can be seen that there is no problem at all if the inner diameter is 18 mm. That is, this is the case of characteristic curve A.
また、特性曲線Bの内径14 m mの場合も温度−ヒ
昇は数に程度であり大きな問題があるとは言えないこと
から、概ね15mm以上の管内径を有していればペーパ
ーロックを起こすことなく重力により液体窒素を送液す
ることが可能といえ、熱シルト板(3)を十分冷却でき
るといえる。従って、15mm以上の内径を有する管を
用いることにより重力を駆動力とした液体窒素送液系お
よび熱シールド板が構成できる。In addition, even in the case of characteristic curve B with an inner diameter of 14 mm, the temperature rise is only a few and it cannot be said that there is a major problem, so if the pipe has an inner diameter of 15 mm or more, paper lock will occur. It can be said that it is possible to send liquid nitrogen by gravity without any friction, and it can be said that the thermal silt plate (3) can be sufficiently cooled. Therefore, by using a tube having an inner diameter of 15 mm or more, a liquid nitrogen liquid feeding system and a heat shield plate using gravity as a driving force can be constructed.
なお、第1図の実施例に関して、熱シールド板(3)へ
冷却配管く4)を取り付ける場合の具体的な形状構成例
を第3図および第4図に示しておく。要は、蒸発ガスが
管内に留まってしまうような平坦な部分あるいは中途の
貯めの部分を避けるよう構成されていれば良い。Regarding the embodiment shown in FIG. 1, specific examples of the shape and configuration when attaching the cooling pipe 4) to the heat shield plate (3) are shown in FIGS. 3 and 4. In short, it is sufficient that the structure is such as to avoid flat parts or midway storage parts where evaporated gas may remain in the pipe.
このように、重力による落下を利用した熱シルト用配管
において十分に液体窒素が行き渡り確実に熱シールド板
の冷却が行なえるように、冷却配管を15〜20 m
m程度の管径で構成したので、ペーパーロックを引き起
こすことなく、しかも装置の著しい大型化を産むことも
なく熱シールド系を構成できる。In this way, in order to ensure that liquid nitrogen is sufficiently distributed in the thermal silt piping that uses gravity to cool the heat shield plate, the cooling piping is installed at a distance of 15 to 20 m.
Since it is constructed with a tube diameter of approximately 1.5 m, a heat shield system can be constructed without causing paper lock and without significantly increasing the size of the device.
[発明の効果]
以上のように、この発明によれば、超伝導コイル、この
超伝導コイルを収納するヘリウム容器、このヘリウム容
器への外部からの熱侵入を低減するための熱シールド板
、およびこの熱シールド板を冷却するため重力を駆動力
とし液体窒素を供給するよう液体窒素貯槽から導かれか
つ熱的に上記熱シールド板と接続設置された15mm以
上の内径を有する冷却配管を真空容器内に備えるので、
液体窒素用の強制循環装置が必要ではなく、かつペーパ
ーロックによる液体窒素不在の現象も引き起こさず、極
めてシンプルな装置でありながら熱シールド板を確実に
液体窒素温度レベルに保持できる効果がある。[Effects of the Invention] As described above, according to the present invention, there are provided a superconducting coil, a helium container housing the superconducting coil, a heat shield plate for reducing heat intrusion into the helium container from the outside, and In order to cool this heat shield plate, a cooling pipe with an inner diameter of 15 mm or more is guided from a liquid nitrogen storage tank and thermally connected to the heat shield plate to supply liquid nitrogen using gravity as a driving force. In preparation for
A forced circulation device for liquid nitrogen is not required, and the phenomenon of absence of liquid nitrogen due to paper lock does not occur, and although it is an extremely simple device, it has the effect of reliably maintaining the heat shield plate at the liquid nitrogen temperature level.
第1図はこの発明の一実施例による超伝導コイル用極低
温装置を模式的に示す構成図、第2図は下端部を閉鎖し
た垂直管の熱負荷に応じた温度特性を示す特性図、第3
0,94図はそれぞれこの発明の一実施例による冷却配
管の設置例を示す斜視図、第5図は従来の超電導コイル
用極低温装置を示す斜視図である。
(1)は超電導コイル、
(2)は内槽、
(3)は熱シールド板、
(4)は冷却配管、
く5)は液体窒素槽、
(6)は外槽。
なお、図中同一符号は同一または相当部分な示ず。
代 理 人 大 岩 増 雄第1図
1聞 Q M
二]ノ);ンIフ1く;ノシ≧:4 本舎ヶ第2図
然贋荷童(W)
第d凶
労ζ1’t″Lrr、′J日′\
第4図
例狛オ寛木槽へ
レ−
第5図FIG. 1 is a configuration diagram schematically showing a cryogenic device for superconducting coils according to an embodiment of the present invention, and FIG. 2 is a characteristic diagram showing temperature characteristics according to heat load of a vertical tube with its lower end closed. Third
FIGS. 0 and 94 are perspective views showing examples of installation of cooling piping according to an embodiment of the present invention, and FIG. 5 is a perspective view showing a conventional cryogenic device for superconducting coils. (1) is a superconducting coil, (2) is an inner tank, (3) is a heat shield plate, (4) is a cooling pipe, 5) is a liquid nitrogen tank, and (6) is an outer tank. Note that the same reference numerals in the figures do not indicate the same or corresponding parts. Agent Dai Iwa Masuo 1st Figure 1 Q M 2] ノ); んI ふ 1 く; ノシ ≧: 4 Honshaga 2 Unsurprisingly Fake Packer (W) th d Bad Labor ζ 1't'' Lrr, 'J日'\ Fig. 4 Example Komao Hiroki Tank Here Fig. 5
Claims (1)
容器、このヘリウム容器への外部からの熱侵入を低減す
るための熱シールド板、およびこの熱シールド板を冷却
するため重力を駆動力とし液体窒素を供給するよう液体
窒素貯槽から導かれかつ熱的に上記熱シールド板と接続
設置された15mm以上の内径を有する冷却配管を真空
容器内に備える超伝導コイル用極低温装置。A superconducting coil, a helium container that houses the superconducting coil, a heat shield plate to reduce heat intrusion into the helium container from the outside, and liquid nitrogen using gravity as the driving force to cool the heat shield plate. A cryogenic device for superconducting coils, comprising a cooling pipe having an inner diameter of 15 mm or more, which is led from a liquid nitrogen storage tank for supply and is thermally connected to the heat shield plate, in a vacuum container.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2133034A JP2701517B2 (en) | 1990-05-23 | 1990-05-23 | Cryogenic equipment for superconducting coils |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2133034A JP2701517B2 (en) | 1990-05-23 | 1990-05-23 | Cryogenic equipment for superconducting coils |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0428210A true JPH0428210A (en) | 1992-01-30 |
| JP2701517B2 JP2701517B2 (en) | 1998-01-21 |
Family
ID=15095265
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2133034A Expired - Lifetime JP2701517B2 (en) | 1990-05-23 | 1990-05-23 | Cryogenic equipment for superconducting coils |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2701517B2 (en) |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6367706A (en) * | 1986-09-09 | 1988-03-26 | Mitsubishi Electric Corp | Cryostat |
-
1990
- 1990-05-23 JP JP2133034A patent/JP2701517B2/en not_active Expired - Lifetime
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6367706A (en) * | 1986-09-09 | 1988-03-26 | Mitsubishi Electric Corp | Cryostat |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2701517B2 (en) | 1998-01-21 |
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