JP2856946B2 - Superconducting magnet - Google Patents
Superconducting magnetInfo
- Publication number
- JP2856946B2 JP2856946B2 JP12989691A JP12989691A JP2856946B2 JP 2856946 B2 JP2856946 B2 JP 2856946B2 JP 12989691 A JP12989691 A JP 12989691A JP 12989691 A JP12989691 A JP 12989691A JP 2856946 B2 JP2856946 B2 JP 2856946B2
- Authority
- JP
- Japan
- Prior art keywords
- shield plate
- heat shield
- heat
- inner tank
- superconducting
- 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 - Fee Related
Links
Landscapes
- Control Of Vehicles With Linear Motors And Vehicles That Are Magnetically Levitated (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
Description
【0001】[発明の目的][Object of the Invention]
【0002】[0002]
【産業上の利用分野】本発明は超電導磁気浮上車などに
使われる超電導磁石に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a superconducting magnet used for a superconducting magnetic levitation vehicle or the like.
【0003】[0003]
【従来の技術】磁気浮上式鉄道に用いる超電導磁石につ
いて図8〜図10を参照して説明する。2. Description of the Related Art A superconducting magnet used in a magnetic levitation railway will be described with reference to FIGS.
【0004】超電導磁気浮上車に使用する超電導磁石は
車体下の台車に取付けられ、地上コイルと対向してい
る。A superconducting magnet used in a superconducting magnetic levitation vehicle is mounted on a bogie below the vehicle body and faces a ground coil.
【0005】この超電導磁石は超電導コイル1を液体ヘ
リウム等の媒体で冷却し収納する内槽2と、この内槽2
を収納する真空容器である外槽3と、前記内槽2と外槽
3との間に設置された熱シールド板4等から構成され、
地上コイル5に対向して推力、浮上力ならびに案内力を
発生させている。The superconducting magnet comprises an inner tank 2 for cooling and storing the superconducting coil 1 with a medium such as liquid helium,
An outer tank 3 which is a vacuum container for storing the water, a heat shield plate 4 and the like provided between the inner tank 2 and the outer tank 3, and the like.
A thrust, a levitation force and a guide force are generated facing the ground coil 5.
【0006】超電導線を巻回した超電導コイル1は液体
ヘリウム等の冷媒が通る穴が明いている金具6により内
槽2に固定される。内槽2は溶接気密性ならびに磁力に
対する強度から通常ステンレス鋼が使われている。The superconducting coil 1 wound with a superconducting wire is fixed to the inner tank 2 by a metal fitting 6 having a clear hole through which a coolant such as liquid helium passes. The inner tank 2 is usually made of stainless steel from the viewpoint of welding airtightness and strength against magnetic force.
【0007】熱シールド板4は内槽2に入る輻射入熱を
低減させるため内槽2を囲う形で形成され、更にシール
ド板の冷却器として、その表面に液体窒素等の冷媒を流
す配管7を取付け、その熱伝導によりシールド板を液体
窒素温度領域に保たせている。[0007] The heat shield plate 4 is formed so as to surround the inner tank 2 in order to reduce radiant heat entering the inner tank 2, and as a cooler for the shield plate, a pipe 7 through which a coolant such as liquid nitrogen flows on the surface thereof. And the heat conduction keeps the shield plate in the liquid nitrogen temperature range.
【0008】熱シールド板4は、全体を均一温度に保つ
ため良熱伝導材であり、かつ外槽3と共に地上コイル5
からの交流磁界を遮蔽する必要があることから導電率の
高い材料すなわちアルミニウムや鋼の板が使用されてい
る。The heat shield plate 4 is a good heat conductive material for keeping the whole at a uniform temperature.
Since it is necessary to shield an AC magnetic field from the material, a material having high conductivity, that is, a plate made of aluminum or steel is used.
【0009】ところで、超電導磁気浮上車においては、
超電導コイル1と地上コイル5との電磁作用により推
力、浮上力ならびに案内力を得ているので、効率良く浮
上し走行するためには前記コイル間隔ができるだけ小さ
い方がよい。このため地上コイル5との対向側にある熱
シールド板4aは可能な限り薄く、かつ内槽2aと外槽
3aとの間隔もできるだけ小さくする必要がある。By the way, in a superconducting magnetic levitation vehicle,
Since the thrust, the levitation force and the guide force are obtained by the electromagnetic action of the superconducting coil 1 and the ground coil 5, the distance between the coils is preferably as small as possible in order to levitate and travel efficiently. Therefore, the heat shield plate 4a on the side facing the ground coil 5 must be as thin as possible, and the interval between the inner tank 2a and the outer tank 3a must be as small as possible.
【0010】[0010]
【発明が解決しようとする課題】このように熱シールド
板4は、車両が走行中に地上コイル5から受ける電磁的
な外乱により超電導コイル1と一体となった内槽2が振
動し、それを支持する荷重支持材8を介してその振動を
受ける。この時、超電導コイル1の磁界中で熱シールド
板4が超電導コイルと相対変位するため磁界変動を受
け、渦電流が熱シールド板4に発生する。As described above, the heat shield plate 4 causes the inner tank 2 integrated with the superconducting coil 1 to vibrate due to the electromagnetic disturbance received from the ground coil 5 while the vehicle is traveling, and the heat is transmitted to the heat shield plate 4. The vibration is received via the supporting load member 8. At this time, the heat shield plate 4 is displaced relative to the superconducting coil in the magnetic field of the superconducting coil 1 and receives a magnetic field fluctuation, and an eddy current is generated in the heat shield plate 4.
【0011】ところで、地上コイル5と対向する側の熱
シールド板4aは前述のように内槽2aとの間隔を可能
な限り小さく取っているため超電導コイル1の磁界の強
い所に晒されて流れる渦電流は多くなり、その渦電流が
作る磁界により熱シールド板4aと対向する内槽2aに
も2次的な渦電流が強く誘起される。このため、熱シー
ルド板4aと内槽2aに渦電流による発熱が過大に生
じ、超電導磁石全体の熱負荷が大きく増大する傾向があ
る。By the way, the heat shield plate 4a on the side facing the ground coil 5 is exposed to the place where the magnetic field of the superconducting coil 1 is strong because the space between the heat shield plate 4a and the inner tank 2a is made as small as possible. The eddy current increases, and a secondary eddy current is strongly induced in the inner tank 2a facing the heat shield plate 4a by the magnetic field generated by the eddy current. For this reason, excessive heat is generated in the heat shield plate 4a and the inner tank 2a due to the eddy current, and the heat load on the entire superconducting magnet tends to increase significantly.
【0012】これを防止するため、熱シールド板4の振
動を押さえる補強材9を設けて熱シールド板4の剛性を
高める工夫をしているが、地上コイル5と対向する側の
熱シールド板4aは前述の寸法制約のため、補強材9を
取付けることができず、その効果が十分には得られてい
ない。In order to prevent this, a reinforcing member 9 for suppressing the vibration of the heat shield plate 4 is provided to increase the rigidity of the heat shield plate 4, but the heat shield plate 4a on the side facing the ground coil 5 is designed. Due to the dimensional restrictions described above, the reinforcing member 9 cannot be attached, and the effect is not sufficiently obtained.
【0013】そこで、本発明はこのような超電導磁石が
走行中に発生する渦電流による熱負荷の増大を低減でき
るようにすることを目的としたものである。SUMMARY OF THE INVENTION It is an object of the present invention to reduce an increase in thermal load due to an eddy current generated during running of such a superconducting magnet.
【0014】[発明の構成][Configuration of the Invention]
【0015】[0015]
【課題を解決するための手段】本発明はこの問題を解消
するため前記熱シールド板を剛性の高いハニカム構造の
板により構成し、かつそのハニカム構造内に冷媒を流せ
るようにしたものとする。According to the present invention, in order to solve this problem, the heat shield plate is made of a plate having a high rigidity honeycomb structure, and a refrigerant can flow through the honeycomb structure.
【0016】[0016]
【作用】熱シールド板をハニカム構造とすることにより
そのスペースが小さくても十分に剛性が高く、熱シール
ド板の振動特に膜振動を抑制でき、超電導コイルとの相
対変位を低減する。When the heat shield plate has a honeycomb structure, the rigidity is sufficiently high even if the space is small, vibration of the heat shield plate, particularly film vibration, can be suppressed, and relative displacement with the superconducting coil can be reduced.
【0017】さらに、ハニカム構造内に冷媒を流すこと
により熱シールド板の渦電流による発熱を直接冷却で
き、内槽への入熱増を低減する。Further, by flowing the refrigerant through the honeycomb structure, the heat generated by the eddy current of the heat shield plate can be directly cooled, and the increase in heat input to the inner tank is reduced.
【0018】[0018]
【実施例】図1〜図4に示す実施例に基づいて本発明を
説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described with reference to the embodiments shown in FIGS.
【0019】超電導磁石の熱シールド板4を剛性の高い
ハニカム構造の板を用い、このハニカム構造内に冷媒を
流せる構造とする。As the heat shield plate 4 of the superconducting magnet, a plate having a honeycomb structure having high rigidity is used, and a structure in which a refrigerant can flow through the honeycomb structure is used.
【0020】ハニカム構造としては、一般的な六角形状
のハニカムコア4bとし、その製作時に必要となる気抜
け穴4cを冷媒の通路として利用する。As the honeycomb structure, a general hexagonal honeycomb core 4b is used, and a vent hole 4c required for manufacturing the honeycomb core 4b is used as a refrigerant passage.
【0021】または、図3、図4に示すように、ハニカ
ムコア4bを波板形状のものとし、その空間4dを冷媒
の通路として利用する。Alternatively, as shown in FIGS. 3 and 4, the honeycomb core 4b has a corrugated plate shape, and its space 4d is used as a refrigerant passage.
【0022】上でのべたように熱シールド板4をハニカ
ム構造とすることにより、地上コイル5と対向する側の
ような寸法制約のある部分でも剛性を高くでき、かつ補
強材9の取付けの場合と比べて熱シールド板全体の剛性
を高くできる。As described above, by forming the heat shield plate 4 into a honeycomb structure, the rigidity can be increased even in a portion having dimensional restrictions such as the side facing the ground coil 5 and the reinforcing member 9 is attached. The rigidity of the entire heat shield plate can be made higher than that of the heat shield plate.
【0023】このようにシールド板を構成したので、熱
シールド板の振動、特に膜振動を抑制でき、超電導コイ
ル1との相対変位を低減できる。さらに、ハニカム構造
内に液体窒素等の冷媒を流すことにより発熱する熱シー
ルド板4を直接冷却できるため、熱シールド板4の渦電
流による温度上昇が押さえられ内槽2への輻射熱及び荷
重支持材8を介しての伝導熱が低減できる。Since the shield plate is configured as described above, vibration of the heat shield plate, particularly, film vibration can be suppressed, and relative displacement with respect to the superconducting coil 1 can be reduced. Furthermore, since the heat shield plate 4 that generates heat by flowing a coolant such as liquid nitrogen into the honeycomb structure can be directly cooled, the temperature rise due to the eddy current of the heat shield plate 4 is suppressed, and the radiant heat to the inner tank 2 and the load supporting material are reduced. 8 can reduce the heat of conduction.
【0024】熱シールド板のハニカム構造による高剛性
により、熱シールド板4と超電導導コイル1との相対変
位を低減でき、熱シールド板4および内槽2に流れる渦
電流が減り、発熱を低減できる。さらに、ハニカム構造
内に液体窒素等の冷媒を流すことにより内槽2への入熱
量を押さえることができ、走行中の超電導磁石全体の熱
負荷の増大を大幅に低減できる。Due to the high rigidity of the heat shield plate due to the honeycomb structure, the relative displacement between the heat shield plate 4 and the superconducting coil 1 can be reduced, the eddy current flowing through the heat shield plate 4 and the inner tank 2 can be reduced, and the heat generation can be reduced. . Furthermore, by flowing a coolant such as liquid nitrogen into the honeycomb structure, the amount of heat input to the inner tank 2 can be suppressed, and the increase in the heat load of the entire superconducting magnet during traveling can be significantly reduced.
【0025】ハニカム構造の熱シールド板を少なくとも
地上コイル5と対向する側のような寸法制約のある部分
にだけ設置し、他の寸法制約の厳しくない面は図9の補
強材9を取付ける構成としても同様のに効果が得られ
る。A heat shield plate having a honeycomb structure is provided only at a portion having a dimensional restriction such as at least a side facing the ground coil 5, and the other surface where the dimensional restriction is not strict is provided with a reinforcing member 9 shown in FIG. 9. The same effect can be obtained.
【0026】図5〜図7に示す本発明の他の実施例を説
明する。Another embodiment of the present invention shown in FIGS. 5 to 7 will be described.
【0027】図5の例は、熱シールド板4に強化プラス
チックもしくはステンレス鋼等からなるハニカム板10
をリべット等で断続的に取付け、熱シールド板4の剛性
を高くし前記相対変位を低減して、同様の効果を得るも
のである。さらに、リベット等の断続的固定ピッチを適
切に選ぶことにより熱シールド板4とハニカム板10の
振動が打消し合い、振動の振幅が押さえられ前記相対変
位を大幅に低減でき、より一層の効果を持たすことがで
きる。FIG. 5 shows an example in which the heat shield plate 4 has a honeycomb plate 10 made of reinforced plastic or stainless steel.
Are intermittently attached with a rivet or the like to increase the rigidity of the heat shield plate 4 and reduce the relative displacement to obtain the same effect. Further, by appropriately selecting the intermittent fixed pitch of the rivet or the like, the vibrations of the heat shield plate 4 and the honeycomb plate 10 cancel each other, the amplitude of the vibration is suppressed, and the relative displacement can be greatly reduced. You can have.
【0028】さらに図6に示すように、ハニカム構造も
しくはハニカム板取付けの剛性を高められた熱シールド
板4と内槽2との間にFRP等の熱伝動率の低くかつ高
強度の振れ止め部材11を取付けることにより、荷重支
持材8で決まる熱シールド板全体としての曲げ振動を抑
制し前記相対変位を大幅に低減でき、より一層の効果が
ある。Further, as shown in FIG. 6, a high-strength anti-vibration member such as FRP having a low heat transfer coefficient is provided between the inner tank 2 and the heat shield plate 4 having the honeycomb structure or the rigidity for mounting the honeycomb plate. By mounting 11, the bending vibration of the heat shield plate as a whole determined by the load supporting member 8 can be suppressed, and the relative displacement can be greatly reduced.
【0029】なお、振れ止め部材11の取付け位置とし
ては、図7に示すようレーストラック形状の超電導磁石
の場合、曲部コーナー部の荷重支持材8から離れた位置
に配する方が更により効果が得られる。In the case of a race track-shaped superconducting magnet as shown in FIG. 7, it is more effective to dispose the steady rest member 11 at a position away from the load supporting member 8 at the corner of the curved portion. Is obtained.
【0030】[0030]
【発明の効果】本発明によれば、超電導磁石の熱シール
ド板のスペースを大きくとることなく剛性を高めること
ができ、そのため熱シールド板の振動、特に膜振動を抑
制して超電導コイルとの相対変位を低減することがで
き、熱シールド板および内槽に流れる渦電流が減り、発
熱を低減できる。さらに、ハニカム構造内に液体窒素等
の冷媒を流すことにより発熱する熱シールド板を直接冷
却できるため温度上昇が押さえられ、内槽への輻射熱お
よび荷重支持材を介しての伝導熱が低減でき、走行中の
超電導磁石全体の熱負荷の増大を大幅に低減できる。According to the present invention, the rigidity can be increased without increasing the space for the heat shield plate of the superconducting magnet. Displacement can be reduced, eddy current flowing through the heat shield plate and the inner tank is reduced, and heat generation can be reduced. Furthermore, since the heat shield plate that generates heat by flowing a coolant such as liquid nitrogen into the honeycomb structure can be directly cooled, the temperature rise is suppressed, and radiant heat to the inner tank and conduction heat through the load supporting material can be reduced. The increase in the thermal load on the entire superconducting magnet during traveling can be greatly reduced.
【図1】本発明による超電導磁石の部分断面図である。FIG. 1 is a partial sectional view of a superconducting magnet according to the present invention.
【図2】本発明によるシールド板の斜視図である。FIG. 2 is a perspective view of a shield plate according to the present invention.
【図3】本発明による他のシールド板の斜視図である。FIG. 3 is a perspective view of another shield plate according to the present invention.
【図4】本発明による更に他のシールド板の斜視図であ
る。FIG. 4 is a perspective view of still another shield plate according to the present invention.
【図5】本発明の他の実施例の部分断面図である。FIG. 5 is a partial cross-sectional view of another embodiment of the present invention.
【図6】本発明の更に他の実施例の部分断面図である。FIG. 6 is a partial sectional view of still another embodiment of the present invention.
【図7】図6の側面図である。FIG. 7 is a side view of FIG. 6;
【図8】従来の超電導磁石の断面斜視図である。FIG. 8 is a sectional perspective view of a conventional superconducting magnet.
【図9】図8の部分断面図である。FIG. 9 is a partial sectional view of FIG.
【図10】図9のX 〜X 線矢視図である。FIG. 10 is a view taken along line X-X of FIG. 9;
1 超電導コイル 2,2a 内槽 3,3a 外槽 4,4a 熱シールド板 4b ハニカムコア 4d 冷媒通路 5 地上コイル 10 ハニカム板 Reference Signs List 1 superconducting coil 2, 2a inner tank 3, 3a outer tank 4, 4a heat shield plate 4b honeycomb core 4d refrigerant passage 5 ground coil 10 honeycomb plate
Claims (1)
槽を収納する真空容器である外槽と、内槽を覆って内外
槽の間に設けた冷却器付熱シールド板等からなる超電導
磁石において、冷媒の通路穴を設けたハニカム構造の板
で前記熱シールド板を構成したことを特徴とする超電導
磁石。1. A superconducting device comprising an inner tank for storing a superconducting coil, an outer tank as a vacuum container for storing the inner tank, and a heat shield plate with a cooler provided between the inner and outer tanks to cover the inner tank. A superconducting magnet, wherein the heat shield plate is formed of a plate having a honeycomb structure provided with a passage hole for a refrigerant.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12989691A JP2856946B2 (en) | 1991-05-31 | 1991-05-31 | Superconducting magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12989691A JP2856946B2 (en) | 1991-05-31 | 1991-05-31 | Superconducting magnet |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04354307A JPH04354307A (en) | 1992-12-08 |
| JP2856946B2 true JP2856946B2 (en) | 1999-02-10 |
Family
ID=15021051
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12989691A Expired - Fee Related JP2856946B2 (en) | 1991-05-31 | 1991-05-31 | Superconducting magnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2856946B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2584518Y2 (en) * | 1992-06-09 | 1998-11-05 | 三菱電機株式会社 | Superconducting coil device |
| DE69618342T2 (en) * | 1996-05-01 | 2002-08-29 | General Electric Co., Schenectady | Support structure for a superconducting winding |
| CN103624491A (en) * | 2013-11-22 | 2014-03-12 | 四川大学 | Forming process of magnetic refrigeration material |
-
1991
- 1991-05-31 JP JP12989691A patent/JP2856946B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04354307A (en) | 1992-12-08 |
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