JPH0817620A - Current lead of superconducting equipment - Google Patents

Current lead of superconducting equipment

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Publication number
JPH0817620A
JPH0817620A JP15252394A JP15252394A JPH0817620A JP H0817620 A JPH0817620 A JP H0817620A JP 15252394 A JP15252394 A JP 15252394A JP 15252394 A JP15252394 A JP 15252394A JP H0817620 A JPH0817620 A JP H0817620A
Authority
JP
Japan
Prior art keywords
current lead
cooling gas
particles
current
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.)
Pending
Application number
JP15252394A
Other languages
Japanese (ja)
Inventor
Kazuto Shimada
一人 島田
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP15252394A priority Critical patent/JPH0817620A/en
Publication of JPH0817620A publication Critical patent/JPH0817620A/en
Pending legal-status Critical Current

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  • Containers, Films, And Cooling For Superconductive Devices (AREA)

Abstract

(57)【要約】 【目的】 超電導機器の電流リードに冷却ガスを導いて
電流リードを冷却する装置において、冷却効率の高い、
熱的に安定した超電導機器の電流リードを提供する。 【構成】 電流リードの冷却ガス流路(12)に粒子(1
4)を充填し、例えば、この粒子(14)を流動化して流
動層として電流リードを冷却するよう構成する。
(57) [Abstract] [Purpose] High cooling efficiency in the device that cools the current lead by guiding the cooling gas to the current lead of the superconducting equipment.
To provide a thermally stable current lead for a superconducting device. [Constitution] Particles (1
4) is filled and, for example, the particles (14) are fluidized to form a fluidized bed to cool the current leads.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、超電導機器の電流リー
ドに関する。
FIELD OF THE INVENTION The present invention relates to current leads for superconducting equipment.

【0002】[0002]

【従来の技術】現在、超電導材料は合金超電導材料が一
般的である。超電導材料の超電導状態を保つため、超電
導材料から構成される超電導機器をクライオスタット内
に納めヘリウム温度に維持する必要がある。このため、
常温側の端子とヘリウム温度の超電導機器を結ぶ電流リ
ードが必要となる。電流リードには外部からの入熱の
他、電流リード自体の発熱などがあり、これらの熱を除
するために通常熱交換型のものが用いられている。熱交
換型の電流リードは、常電導金属、または、超電導金属
から構成され、その表面積をできるだけ大きく取り、電
流リードの下部におかれたヘリウム溜から蒸発してくる
ヘリウムガスと熱交換を行い冷却を行う。図4に、超電
導機器の一例として超電導マグネットと電流リードの一
構成例を示す。超電導マグネット1を励磁する電流は、
常温の電源2から常温の導体3を経てクライオスタット
4内の極低温の超電導マグネット1に流れる。クライオ
スタット4上部の常温の電流端子6から超電導マグネッ
ト1側の極低温の電流端子7までを電流リード5と呼
ぶ。図5に電流リード5の構成例を示す。電流リード5
は、ヘリウム溜9からヘリウムガスからなる冷却ガス10
を取り込み、冷却ガス10と電流リード通電部8の間で熱
交換を行なう構成である。電流リードの設計は、通電電
流、電流リードの外形寸法、クライオスタットの熱損失
等を考慮して行う。例えば、常電導金属から構成する電
流リードの設計において、常温部からの熱侵入を減らす
ために電流リードの断面積を小さくすると、電流リード
自体の電気抵抗が大きくなりジュール発熱が増える。逆
に電流リードの断面積を大きくすると、熱伝導による外
部からの入熱が増える。従って、外部からの入熱量、電
流リードの発熱量、冷却ガスの冷却効果等のバランスを
考慮した熱設計が必要であり、電流リードにフィンを設
け冷却効果の高い構造にするなど各種の工夫がなされて
いる。
2. Description of the Related Art Currently, alloy superconducting materials are generally used as superconducting materials. In order to maintain the superconducting state of the superconducting material, it is necessary to put the superconducting device made of the superconducting material in the cryostat and maintain the helium temperature. For this reason,
A current lead connecting the terminal on the room temperature side and the superconducting device at the helium temperature is required. In addition to heat input from the outside, the current lead also generates heat from the current lead itself, and a heat exchange type is usually used to remove this heat. The heat exchange type current lead is composed of normal conducting metal or superconducting metal, takes the surface area as large as possible, and exchanges heat with the helium gas evaporated from the helium reservoir placed under the current lead to cool it. I do. FIG. 4 shows a configuration example of a superconducting magnet and a current lead as an example of a superconducting device. The current that excites the superconducting magnet 1 is
It flows from a room temperature power source 2 to a cryogenic superconducting magnet 1 in a cryostat 4 via a room temperature conductor 3. The current terminal 6 at the room temperature above the cryostat 4 to the cryogenic current terminal 7 on the side of the superconducting magnet 1 is called a current lead 5. FIG. 5 shows a configuration example of the current lead 5. Current lead 5
Is a cooling gas 10 consisting of helium gas from the helium reservoir 9
Is taken in and heat is exchanged between the cooling gas 10 and the current lead energization section 8. When designing the current leads, consider the energizing current, the outer dimensions of the current leads, the heat loss of the cryostat, etc. For example, in the design of a current lead made of a normal-conducting metal, if the cross-sectional area of the current lead is reduced in order to reduce heat intrusion from the room temperature portion, the electric resistance of the current lead itself increases and Joule heat generation increases. On the contrary, if the cross-sectional area of the current lead is increased, heat input from the outside due to heat conduction increases. Therefore, it is necessary to design the heat considering the balance of the heat input from the outside, the heat generation of the current leads, the cooling effect of the cooling gas, etc. Has been done.

【0003】[0003]

【発明が解決しようとする課題】ところで、近年超電導
機器は大型化してきており、必要とする電流リードも大
電流化の傾向にある。それに伴い外部からの熱侵入、お
よび、電流リードのジュール発熱も大きくなる。また、
交流用の超電導機器に用いる電流リードは、電流リード
を超電導金属で構成すると、交流損失による発熱が大き
くなり熱的に不安定となる。そこで本発明の目的は、冷
却効率の高い、熱的に安定した超電導機器の電流リード
を提供することにある。
By the way, in recent years, the size of superconducting devices has been increasing, and the current lead required has a tendency to increase in current. Along with this, heat intrusion from the outside and Joule heat generation of the current leads also increase. Also,
In the current lead used in the superconducting device for alternating current, if the current lead is made of a superconducting metal, heat generation due to AC loss becomes large and it becomes thermally unstable. Therefore, an object of the present invention is to provide a thermally stable current lead of a superconducting device with high cooling efficiency.

【0004】[0004]

【課題を解決するための手段】本発明による超電導機器
の電流リードは、上記目的を達成するために、電流リー
ドの冷却ガス流路に粒子を充填したことを特徴とするも
のである。
In order to achieve the above object, the current lead of the superconducting device according to the present invention is characterized in that the cooling gas passage of the current lead is filled with particles.

【0005】[0005]

【作用】本発明によれば、電流リードの冷却ガス流路に
粒子を充填することにより冷却ガスの流れが乱れるこ
と、また、粒子と電流リード間の接触熱伝導が加わるこ
とにより、電流リードと冷却ガス間の熱交換が促進され
電流リードは熱的に安定したものとすることができる。
According to the present invention, the flow of the cooling gas is disturbed by filling the cooling gas flow path of the current lead with particles, and the contact heat conduction between the particles and the current lead is added, whereby The heat exchange between the cooling gases is promoted and the current leads can be made thermally stable.

【0006】[0006]

【実施例】以下、本発明の超電導機器の電流リードの一
実施例を、図1、図2、および、図3を参照して説明す
る。図1、図2、および図3において図5と同じ部分に
は同一の符号をつけてその説明は省略する。図1、およ
び、図2で図5と異なる点は冷却ガス流路12に分散板13
を設け、冷却ガス流路12の中に粒子14を充填したことで
ある。図1は電流リード通電部8の外周に冷却ガス流路
12を設けた構成例であり、図2は電流リードの通電部8
内部に冷却ガス流路12を設けた構成例である。図3は粒
子を充填したときの電流リード通電部8と冷却ガス10、
および、粒子14間の伝熱機構を表した図である。従来の
ように粒子14を充填しない場合、電流リードの冷却は、
冷却ガス10と電流リード通電部8との間の熱伝達のみで
ある。しかし、粒子14を充填することにより冷却ガス10
の流れが乱れること、および電流リード通電部8と粒子
14間の接触熱伝導が加わることにより電流リードの冷却
効果が促進される。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the current lead of a superconducting device of the present invention will be described below with reference to FIGS. 1, 2 and 3. 1, 2, and 3, the same parts as those in FIG. 5 are designated by the same reference numerals, and the description thereof will be omitted. 1 and 2 is different from FIG. 5 in that the cooling gas passage 12 has a dispersion plate 13
And the particles 14 are filled in the cooling gas channel 12. FIG. 1 shows a cooling gas flow path on the outer periphery of the current lead conducting portion 8.
FIG. 2 shows a configuration example in which 12 is provided, and FIG.
This is an example of a configuration in which a cooling gas channel 12 is provided inside. FIG. 3 shows the current lead conducting part 8 and the cooling gas 10 when the particles are filled,
3 is a diagram showing a heat transfer mechanism between particles 14. FIG. If the particles 14 are not filled as in the conventional case, the cooling of the current lead is
There is only heat transfer between the cooling gas 10 and the current lead energization portion 8. However, by filling the particles 14 with the cooling gas 10
The flow of electricity is disturbed, and the current lead conducting part 8 and particles
The cooling effect of the current leads is promoted by the addition of contact heat conduction between them.

【0007】例えば、充填粒子としてプラスチックやア
ルミナ粒子などの比重の小さい微少な粒子を用い、流路
断面積、分散板の圧損、粒子の充填量、および、冷却ガ
ス流量を勘案することで、充填粒子と冷却ガスによる流
動層を形成する。この時、流動化粒子により電流リード
近傍の温度境界層が乱されることにより、飛躍的に電流
リードの冷却効果を向上させることが期待できる。
For example, minute particles having a small specific gravity such as plastic or alumina particles are used as the packing particles, and the packing is performed by considering the flow path cross-sectional area, the pressure loss of the dispersion plate, the packing amount of the particles, and the cooling gas flow rate. A fluidized bed is formed by the particles and the cooling gas. At this time, the fluidized particles disturb the temperature boundary layer in the vicinity of the current leads, which can be expected to dramatically improve the cooling effect of the current leads.

【0008】さらに、図2のように冷却ガス流路を二重
化し、それぞれの流路の圧損を分散板13で調査すること
により冷却ガス流量を適切な割合に配分することが期待
できる。
Further, as shown in FIG. 2, it is expected that the cooling gas flow paths will be duplicated and the pressure loss of each flow path will be investigated by the dispersion plate 13 to distribute the cooling gas flow rate to an appropriate ratio.

【0009】[0009]

【発明の効果】本発明によれば、電流リードの冷却ガス
流路に粒子を充填することにより冷却ガスの流れの乱
れ、および、粒子と電流リード間の接触熱伝導により伝
熱効果が促進され、電流リードは熱的に安定したもので
ある。
According to the present invention, the cooling gas flow path of the current lead is filled with particles to disturb the flow of the cooling gas, and the heat transfer effect is promoted by the contact heat conduction between the particles and the current lead. , The current leads are thermally stable.

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

【図1】本発明の超電導機器の電流リードの一実施例を
示す構成図
FIG. 1 is a configuration diagram showing an embodiment of a current lead of a superconducting device of the present invention.

【図2】本発明の超電導機器の電流リードの一実施例を
示す構成図
FIG. 2 is a configuration diagram showing an embodiment of a current lead of a superconducting device of the present invention.

【図3】本発明の超電導機器の電流リードの伝熱機構を
示す図
FIG. 3 is a diagram showing a heat transfer mechanism of a current lead of the superconducting device of the present invention.

【図4】従来の超電導機器の一実施例を示す構成図FIG. 4 is a configuration diagram showing an example of a conventional superconducting device.

【図5】従来の超電導機器の電流リードの一実施例を示
す構成図
FIG. 5 is a configuration diagram showing an example of a current lead of a conventional superconducting device.

【符号の説明】[Explanation of symbols]

1…超電導コイル、2…電源、3…常温導体、4…クラ
イオスタット、5…電流リード、6…常温電流端子、7
…極低温電流端子、8…電流リード通電部、9…ヘリウ
ム溜、10…冷却ガス、11…液体ヘリウム、12…冷却ガス
流路、13…分散板、14…粒子、15…接触熱伝導。
1 ... Superconducting coil, 2 ... Power supply, 3 ... Room temperature conductor, 4 ... Cryostat, 5 ... Current lead, 6 ... Room temperature current terminal, 7
... cryogenic current terminal, 8 ... current lead conducting part, 9 ... helium reservoir, 10 ... cooling gas, 11 ... liquid helium, 12 ... cooling gas passage, 13 ... dispersion plate, 14 ... particles, 15 ... contact heat conduction.

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 超電導機器の電流リードに冷却ガスを導
き前記電流リードを冷却する装置において、前記冷却ガ
ス流路に粒子を充填したことを特徴とする超電導機器の
電流リード。
1. A current lead for a superconducting device in which a cooling gas is introduced into a current lead for the superconducting device to cool the current lead, wherein the cooling gas passage is filled with particles.
【請求項2】 電流リードの一端をクライオスタット内
の上部空間に挿入してクライオスタット内の冷却ガスを
電流リードに導き前記電流リードを冷却する装置におい
て、前記冷却ガス流路端に分散板を設けるとともに、前
記冷却ガス流路に粒子を充填したことを特徴とする超電
導機器の電流リード。
2. An apparatus for inserting one end of a current lead into an upper space in a cryostat to guide cooling gas in the cryostat to the current lead and cooling the current lead, and providing a dispersion plate at an end of the cooling gas flow path. A current lead for a superconducting device, characterized in that the cooling gas channel is filled with particles.
【請求項3】 電流リード外周に冷却ガス流路を設け、
該冷却ガス流路に粒子を充填したことを特徴とする請求
項1または請求項2記載の超電導機器の電流リード。
3. A cooling gas passage is provided on the outer periphery of the current lead,
The current lead of the superconducting device according to claim 1 or 2, wherein the cooling gas channel is filled with particles.
【請求項4】 電流リード内部に冷却ガス流路を設け、
該冷却ガス流路に粒子を充填したことを特徴とする請求
項1または請求項2記載の超電導機器の電流リード。
4. A cooling gas passage is provided inside the current lead,
The current lead of the superconducting device according to claim 1 or 2, wherein the cooling gas channel is filled with particles.
【請求項5】 粒子を冷却ガスにより流動化し流動層と
して電流リードを冷却することを特徴とする請求項3ま
たは請求項4記載の超電導機器の電流リード。
5. The current lead of a superconducting device according to claim 3, wherein the particles are fluidized by a cooling gas to cool the current lead as a fluidized bed.
JP15252394A 1994-07-05 1994-07-05 Current lead of superconducting equipment Pending JPH0817620A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15252394A JPH0817620A (en) 1994-07-05 1994-07-05 Current lead of superconducting equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15252394A JPH0817620A (en) 1994-07-05 1994-07-05 Current lead of superconducting equipment

Publications (1)

Publication Number Publication Date
JPH0817620A true JPH0817620A (en) 1996-01-19

Family

ID=15542304

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15252394A Pending JPH0817620A (en) 1994-07-05 1994-07-05 Current lead of superconducting equipment

Country Status (1)

Country Link
JP (1) JPH0817620A (en)

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