JPS6286703A - Protecting method for superconductive magnet - Google Patents

Protecting method for superconductive magnet

Info

Publication number
JPS6286703A
JPS6286703A JP22845385A JP22845385A JPS6286703A JP S6286703 A JPS6286703 A JP S6286703A JP 22845385 A JP22845385 A JP 22845385A JP 22845385 A JP22845385 A JP 22845385A JP S6286703 A JPS6286703 A JP S6286703A
Authority
JP
Japan
Prior art keywords
magnet
pcs
resistance
current switch
permanent current
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
JP22845385A
Other languages
Japanese (ja)
Inventor
Kohei Furukawa
晃平 古川
Nobuhiro Shibuta
渋田 信広
Toshio Namikata
南方 寿夫
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.)
Sumitomo Electric Industries Ltd
Original Assignee
Sumitomo Electric Industries 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 Sumitomo Electric Industries Ltd filed Critical Sumitomo Electric Industries Ltd
Priority to JP22845385A priority Critical patent/JPS6286703A/en
Publication of JPS6286703A publication Critical patent/JPS6286703A/en
Pending legal-status Critical Current

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

Abstract

PURPOSE:To reduce current running in a protective circuit when a magnet is being excited and to reduce the Joule loss by a method wherein a protective circuit, in which a low resistor and a permanent current switch are series-connected, is parallel- connected to a magnet coil, the permanent current switch is maintained in a normal conductive state when a magnet is excited, and the permanent current switch is maintained in a superconductive state after said excitation is finished. CONSTITUTION:The current loss generating in a protective circuit is indicated by the quantity of heat W1=V<2>/(R+r) when the resistance value of a permanent current switch (PCS) 4 is set at (r). Accordingly, if the PCS 4 is maintained in the normal conductive state and allows the resistance (r) in that state when a magnet is excited, the resistance of the protective circuit is brought to (R+r), which is larger than before, and the value of W1 is reduced. Also, in the mode of permanent current, a magnet coil and the PCS 2 can be protected by the desired protective resistor 3 by having the PCS 4 in the superconductive state of r=0 in the same manner as the PCS 2 of a magnet. The permanent current switch usually has the structure wherein an electric heater is wound on a superconductive wire, electric resistance is generated on the superconductive wire or its resistance in brought to zero by turning ON or OFF the heater. This well known switch can be the PCS 4.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、保護抵抗を有する超電導マグネットを励磁
する際の電流ロス及びマグネット冷却用寒剤(一般には
液体ヘリウム)の蒸発ロスを低減し得る超電導マグネッ
トの保護方法に関する。
Detailed Description of the Invention [Field of Industrial Application] The present invention is directed to a superconducting magnet that can reduce current loss when exciting a superconducting magnet having a protective resistance and evaporation loss of a cryogen for cooling the magnet (generally liquid helium). Regarding how to protect magnets.

〔従来の技術〕[Conventional technology]

超電導マグネットでは、クエンチ(超電導がら常電導へ
の転移)時のコイル保護及び永久電流スイッチの保護を
目的として、マグネットコイルと並列に低抵抗を接続す
ることが考えられている。
In superconducting magnets, it has been considered to connect a low resistance in parallel with the magnet coil for the purpose of protecting the coil during quench (transition from superconducting to normal conducting) and protecting the persistent current switch.

第3図ζこそのコイル励磁時の等価回路を示す。図の符
号1はマグネットコイル、2は永久電流スイッチ(以下
ではp、 c、 s、と云う)、3は保護抵抗である。
Figure 3 shows the equivalent circuit when the coil is excited. In the figure, numeral 1 is a magnet coil, 2 is a persistent current switch (hereinafter referred to as p, c, s), and 3 is a protective resistor.

この回路は、コイル及びp、c、s部でクエンチが起き
て異常電圧が発生した場合、低抵抗値の保護抵抗3番こ
電流を分流し、コイルに蓄積されたエネルギーを保護抵
抗3に消費させるようにしたものである。
In this circuit, when a quench occurs in the coil and parts P, C, and S and an abnormal voltage occurs, the current is shunted to the protective resistor 3 with a low resistance value, and the energy accumulated in the coil is consumed by the protective resistor 3. It was designed to let you do so.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところが、この等価回路において、コイル1のインダク
タンスをL、そのコイルに流れる電流を電流ロスが発生
し、また、その熱により寒剤の蒸光量も増加する。
However, in this equivalent circuit, when the inductance of the coil 1 is L, a current loss occurs in the current flowing through the coil, and the amount of evaporation of the cryogen increases due to the heat.

〔問題点を解決するための手段〕[Means for solving problems]

この発明は、上述の問題を無くすため、マグネットの保
護回路を第1図に示す構成、即ち、低抵抗3に第2のP
、C,S4を直列につないだ構成とし、この第2 p、
 c、 s 4をON、OFF動作させることで、保護
回路を励磁時に高抵抗、永久電流モード時に低抵抗に保
つようにしている。
In order to eliminate the above-mentioned problem, this invention has the structure of the magnet protection circuit shown in FIG.
, C, and S4 are connected in series, and this second p,
By turning c and s 4 ON and OFF, the protection circuit is kept at high resistance during excitation and low resistance during persistent current mode.

即ち、第1図に示す励磁時の等価回路において、従って
、励磁時に、第2 p、 c、s 4を常電導状態に保
って抵抗rをそのま\機能させれば、保護回路の抵抗が
R十rと従来より大きくなってWlの値が低減される。
That is, in the equivalent circuit during excitation shown in Fig. 1, if the second p, c, s 4 are kept in a normally conductive state and the resistor r is allowed to function as is during excitation, the resistance of the protection circuit becomes The value of Wl is reduced by R0r, which is larger than the conventional value.

また、永久電流モード時には、第2 p、c、 s4を
マクネットのp、c、a2と同様に超電導状態にしてr
 = Qにすることにより、第1図の等価回路が第2図
の等価回路に変わって、所期の保護抵抗3によるマグネ
ットコイルとP、C,S)、の保護が行われる。
In addition, in persistent current mode, the second p, c, s4 are set to superconducting state like p, c, a2 of McNet, and r
=Q, the equivalent circuit in FIG. 1 changes to the equivalent circuit in FIG. 2, and the magnet coil and P, C, S) are protected by the intended protection resistor 3.

なお、永久電流スイッチは、一般に、超電導線に電気ヒ
ータを巻き付けた構造であり、ヒータのON 、OFF
によって超電導線に抵抗を生じさせ、又はその抵抗を0
にするようにしであるが、本発明で使用する第2 p、
 c、 s4は、この周知のスイッチでよい。
A persistent current switch generally has a structure in which an electric heater is wrapped around a superconducting wire, and the heater is turned on and off.
to create resistance in the superconducting wire or reduce the resistance to 0.
However, the second p used in the present invention,
c and s4 may be these well-known switches.

〔効果〕〔effect〕

以上述べたように、この発明の方法によれば、保護抵抗
に直列につないだ第2 p、 c、 sの抵抗によって
マグネットの励磁時に保護回路に流れる電流が低減され
るため、ジュール損が小さくなり、また、そのために、
寒剤の蒸発量も少なくなる。
As described above, according to the method of the present invention, the current flowing through the protection circuit when the magnet is excited is reduced by the second P, C, and S resistors connected in series with the protection resistor, so the Joule loss is reduced. To become, and for that purpose,
The amount of evaporation of the refrigerant is also reduced.

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

第1図は、この発明の方法による超電導マグネットの励
磁時の等価回路、第2図はそのマグネットの永久電流モ
ード時の等価回路、第3図は保護抵抗をつけた従来の超
電導マグネットの励磁時の等価回路である。 1・・・マグネットコイル、2・・・永久電流スイッチ
(P、C,S)、3・・・保護抵抗、4・・・第2永久
電流スイッチ(p、c、s) 特許出願人  住友電気工業株式会社 同 代理人   鎌   1)  文   二第1図
Figure 1 shows an equivalent circuit when a superconducting magnet is excited by the method of the present invention, Figure 2 shows an equivalent circuit when the magnet is in persistent current mode, and Figure 3 shows an equivalent circuit when a conventional superconducting magnet with a protective resistor is excited. This is the equivalent circuit of 1... Magnet coil, 2... Persistent current switch (P, C, S), 3... Protective resistor, 4... Second persistent current switch (P, C, S) Patent applicant Sumitomo Electric Industrial Co., Ltd. Agent Kama 1) Letter 2 Figure 1

Claims (1)

【特許請求の範囲】[Claims]  永久電流スイッチを具備した超電導マグネットにおい
て、マグネットコイルに低抵抗体と第2の永久電流スイ
ッチとを直列につないだ保護回路を並列接続し、上記第
2永久電流スイッチを、マグネットの励磁時に常電導状
態、励磁終了後に超電導状態に保つようにした超電導マ
グネットの保護方法。
In a superconducting magnet equipped with a persistent current switch, a protection circuit in which a low resistance element and a second persistent current switch are connected in series is connected to the magnet coil in parallel, and the second persistent current switch is normally conductive when the magnet is energized. A method of protecting superconducting magnets that maintains them in a superconducting state after excitation.
JP22845385A 1985-10-12 1985-10-12 Protecting method for superconductive magnet Pending JPS6286703A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22845385A JPS6286703A (en) 1985-10-12 1985-10-12 Protecting method for superconductive magnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22845385A JPS6286703A (en) 1985-10-12 1985-10-12 Protecting method for superconductive magnet

Publications (1)

Publication Number Publication Date
JPS6286703A true JPS6286703A (en) 1987-04-21

Family

ID=16876728

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22845385A Pending JPS6286703A (en) 1985-10-12 1985-10-12 Protecting method for superconductive magnet

Country Status (1)

Country Link
JP (1) JPS6286703A (en)

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