JPH0745422A - Superconducting magnet device for magnetic levitation type railway - Google Patents

Superconducting magnet device for magnetic levitation type railway

Info

Publication number
JPH0745422A
JPH0745422A JP20374293A JP20374293A JPH0745422A JP H0745422 A JPH0745422 A JP H0745422A JP 20374293 A JP20374293 A JP 20374293A JP 20374293 A JP20374293 A JP 20374293A JP H0745422 A JPH0745422 A JP H0745422A
Authority
JP
Japan
Prior art keywords
superconducting coil
superconducting
switch
magnet device
circuit configuration
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
Application number
JP20374293A
Other languages
Japanese (ja)
Other versions
JP2761452B2 (en
Inventor
Akihiko Kishikawa
昭彦 岸川
Kaoru Nemoto
薫 根本
Eiji Suzuki
栄司 鈴木
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.)
Railway Technical Research Institute
Original Assignee
Railway Technical Research Institute
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 Railway Technical Research Institute filed Critical Railway Technical Research Institute
Priority to JP20374293A priority Critical patent/JP2761452B2/en
Priority to US08/142,911 priority patent/US5432669A/en
Publication of JPH0745422A publication Critical patent/JPH0745422A/en
Application granted granted Critical
Publication of JP2761452B2 publication Critical patent/JP2761452B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Control Of Vehicles With Linear Motors And Vehicles That Are Magnetically Levitated (AREA)

Abstract

PURPOSE:To restrain abnormal rise of a voltage generated when a superconducting coil is out of order during excitation or demagnetizing operation by making a circuit constitution switch element closed only when a superconducting coil is out of order during excitation or demagnetizing operation. CONSTITUTION:Permanent current switches 2a to 2f, protection resistors 3a to 3f installed on the car and diodes 4a to 4f are connected to each of one or more pairs of opposed right and left superconducting coils 1a to 1f and circuit constitution switch elements 5a to 5f are connected thereto to enable shortcircuiting of both ends of a superconducting coil. During excitation or demagnetization, when the superconducting coils 1a to 1f shift to normal conduction with the permanent current switches 2a to 2f opened, abnormal voltage rise generated at both ends of a superconducting coil is restrained by operation of the circuit constitution switches 5a to 5f corresponding to a superconducting coil which shortcircuits both ends of a superconducting coil.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は磁気浮上式鉄道の車両に
搭載される超電導磁石装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a superconducting magnet device mounted on a magnetic levitation railway vehicle.

【0002】[0002]

【従来の技術】図7は従来技術における磁気浮上式鉄道
用超電導磁石装置の回路図である。ここで、1a〜1f
は超電導コイル、2a〜2fは永久電流スイッチ、3a
〜3fは車上配置保護抵抗器、4a〜4fは車上配置ダ
イオード、6a〜6cは電流リード線、7a,7bは励
磁用電源ケーブル、8は励磁用電源、9は地上配置保護
抵抗器、10は地上配置ダイオードである。
2. Description of the Related Art FIG. 7 is a circuit diagram of a conventional magnetically levitated railway superconducting magnet device. Here, 1a to 1f
Is a superconducting coil, 2a to 2f are permanent current switches, and 3a.
˜3f is an on-vehicle protection resistor, 4a to 4f are on-vehicle diodes, 6a to 6c are current lead wires, 7a and 7b are excitation power cables, 8 is an excitation power supply, and 9 is a ground protection resistor. Reference numeral 10 is a ground-based diode.

【0003】励磁用電源8は超電導コイル1a〜1fへ
の励磁または消磁が終了すると切り離されるものであ
る。励磁が終了すると超電導コイル1a〜1fに流れて
いる電流は超電導状態の超電導コイル1a〜1fと永久
電流スイッチ2a〜2fで作られるそれぞれの閉回路を
流れている。そして、この回路に異常が発生したときに
超電導コイル1a〜1fと永久電流スイッチ2a〜2f
を保護する目的で、永久電流スイッチ2a〜2fと並列
に車上配置保護抵抗器3a〜3fが組み込まれている。
車上配置ダイオード4a〜4fと地上配置ダイオード1
0は励磁の際に車上配置保護抵抗器3a〜3fや地上配
置保護抵抗器9に分流電流が流れないようにすることを
目的として配置されている。地上配置保護抵抗器9は励
磁あるいは消磁の際に超電導コイル1a〜1fに異常が
生ずると励磁用電源8の出力部を遮断するが、このとき
電流リード線6aと電流リード線6bとの間に過大電圧
が生じないようにするために配置されている。さらに、
永久電流スイッチ2a〜2fは超電導線で構成されてい
る熱式のスイッチであり、閉状態では超電導状態である
ため抵抗零であり、開状態では熱負荷により常電導転移
させることによって有限の抵抗を持つものである。
The excitation power source 8 is disconnected when the superconducting coils 1a to 1f have been excited or demagnetized. When the excitation is completed, the current flowing through the superconducting coils 1a to 1f flows through the closed circuits formed by the superconducting coils 1a to 1f in the superconducting state and the permanent current switches 2a to 2f. Then, when an abnormality occurs in this circuit, the superconducting coils 1a to 1f and the permanent current switches 2a to 2f.
For protection purposes, on-board protection resistors 3a to 3f are installed in parallel with the permanent current switches 2a to 2f.
On-vehicle diodes 4a-4f and ground diode 1
0 is arranged for the purpose of preventing the shunt current from flowing through the on-vehicle arranged protection resistors 3a to 3f and the ground arranged protection resistor 9 during excitation. The ground protection resistor 9 shuts off the output part of the exciting power source 8 when an abnormality occurs in the superconducting coils 1a to 1f during excitation or demagnetization, but at this time, it is between the current lead wire 6a and the current lead wire 6b. It is arranged to prevent an overvoltage. further,
The permanent current switches 2a to 2f are thermal switches composed of superconducting wires, and have zero resistance in the closed state because they are in the superconducting state. To have.

【0004】磁気浮上式鉄道車両では走行中において、
超電導コイル1a〜1fの一つに異常が生じたとき、そ
れと対向する超電導コイル1f〜1aの電流も速やかに
減衰させることによって電磁力バランスを保持し車両運
動を改善させる必要がある。そのため車上配置保護抵抗
器3a〜3fの抵抗値は、超電導コイル1a〜1fの電
流が永久電流スイッチ2a〜2fから車上配置保護抵抗
器3a〜3fに転流したときに、超電導コイル1a〜1
fに常電導転移を誘発させるに十分な大きさを有するも
のとする必要がある。
When a magnetically levitated railway vehicle is running,
When an abnormality occurs in one of the superconducting coils 1a to 1f, it is necessary to quickly attenuate the current in the superconducting coils 1f to 1a facing it to maintain the electromagnetic force balance and improve the vehicle motion. Therefore, the resistance values of the on-vehicle disposition protective resistors 3a to 3f are such that when the currents of the superconducting coils 1a to 1f are commutated from the permanent current switches 2a to 2f to the on-vehicle disposition protective resistors 3a to 3f. 1
It must be large enough to induce normal conduction transition in f.

【0005】超電導磁石を励磁する場合には、永久電流
スイッチ2a〜2fを開いた状態で通電し、超電導コイ
ル1a〜1fに所定の電流を流した後に永久電流スイッ
チ2a〜2fを閉じる。これにより、超電導コイル1a
〜1fの電流は励磁用電源8を切り離した後において永
久電流モードとなり内部に電流が流れ続け、強力な磁石
を保ち続けるものである。
To excite the superconducting magnet, the permanent current switches 2a to 2f are energized in an open state, a predetermined current is passed through the superconducting coils 1a to 1f, and then the permanent current switches 2a to 2f are closed. Thereby, the superconducting coil 1a
The current of 1f is in the permanent current mode after the excitation power source 8 is disconnected, and the current continues to flow inside to keep the strong magnet.

【0006】超電導磁石を消磁する場合には、永久電流
モードとなっている超電導コイル1a〜1fに対して、
永久電流スイッチ2a〜2fを閉じた状態で励磁用電源
8から通電を開始し、超電導コイル1a〜1fに流れて
いる電流値まで電流をあげた後、永久電流スイッチ2a
〜2fを開き零アンペアまで下げていく。これによって
超電導コイル1a〜1fの強力な磁力が無くなる。
When demagnetizing the superconducting magnet, the superconducting coils 1a to 1f in the permanent current mode are
Energization is started from the excitation power source 8 with the permanent current switches 2a to 2f closed, and the current is increased to the current value flowing in the superconducting coils 1a to 1f.
Open ~ 2f and lower to zero amps. This eliminates the strong magnetic force of superconducting coils 1a-1f.

【0007】[0007]

【発明が解決しようとする課題】従来の技術によれば、
車上配置保護抵抗器は超電導コイルの電流が永久電流ス
イッチから車上配置保護抵抗器に転流したとき、超電導
コイルが常電導転移を生じるだけの値を有し、また、車
上配置ダイオードは励磁中に車上配置保護抵抗器への分
流を阻止する目的で組み込まれている。したがって、励
磁あるいは消磁作業中に1個以上の超電導コイルが異常
を起こして常電導転移した場合には、当該超電導コイル
の両端に異常な電圧上昇が発生し、超電導磁石装置を破
損するという問題点があった。本発明は前記のような問
題点を解決することを目的として、励磁あるいは消磁作
業中に超電導コイルが異常を起こして常電導転移した場
合でも、超電導コイルの両端に発生する異常な電圧上昇
を抑制する超電導磁石装置を提供することにある。
According to the prior art,
The on-board protective resistor has such a value that the superconducting coil causes a normal conduction transition when the current of the superconducting coil is commutated from the permanent current switch to the on-board protective resistor. It is incorporated for the purpose of blocking the shunt current to the onboard protection resistor during excitation. Therefore, when one or more superconducting coils cause an abnormality during the excitation or degaussing operation and transition to normal conduction occurs, an abnormal voltage rise occurs at both ends of the superconducting coils, and the superconducting magnet device is damaged. was there. The present invention aims to solve the above problems, and suppresses an abnormal voltage rise occurring at both ends of the superconducting coil even when the superconducting coil causes an abnormality during the excitation or degaussing operation and changes to the normal conducting state. To provide a superconducting magnet device.

【0008】[0008]

【課題を解決するための手段】本発明における請求項1
の超電導磁石装置は対向する左右一対以上の超電導コイ
ルのそれぞれに永久電流スイッチと車上配置保護抵抗器
とダイオードを接続して、これに超電導コイルの両端を
短絡出来るように回路構成用スイッチ素子を接続してい
る回路である。超電導コイルの電流や電圧に異常が発生
して超電導コイルの電流が永久電流スイッチから車上配
置保護抵抗器に転流した場合に、車上配置保護抵抗器は
超電導コイルが常電導転移を生じるだけの値を有し、さ
らに励磁あるいは消磁の際、永久電流スイッチが開状態
で超電導コイルが常電導転移した場合に、超電導コイル
に対応する回路構成用スイッチ素子が動作して超電導コ
イルの両端を短絡することにより、超電導コイルの両端
に発生する異常な電圧上昇を抑制するものである。本発
明における請求項2の超電導磁石装置は請求項1の超電
導磁石装置に対して、回路構成用スイッチ素子としてス
イッチの電極をあらかじめ不活性ガス中に微小距離をお
いて配置し、電極間に一定値以上の電圧が発生した場合
に、放電による回路構成をする素子を使用するものであ
る。本発明における請求項3の超電導磁石装置は請求項
1の超電導磁石装置に対して、回路構成用スイッチ素子
としてスイッチの電極をあらかじめ空気中に微小距離を
おいて配置し、電極間に一定値以上の電圧が発生した場
合に、放電による回路構成をする素子を使用するもので
ある。
[Means for Solving the Problems] Claim 1 in the present invention
In the superconducting magnet device, the permanent current switch, the on-vehicle protection resistor and the diode are connected to each of the pair of left and right superconducting coils facing each other, and the switch element for circuit configuration is connected to this so that both ends of the superconducting coil can be short-circuited. It is a connected circuit. When an abnormality occurs in the current or voltage of the superconducting coil and the current of the superconducting coil is commutated from the permanent current switch to the on-board protective resistor, the on-vehicle protective resistor only causes the superconducting coil to change to the normal conducting state. When the permanent current switch is open and the superconducting coil undergoes normal conduction transition during excitation or degaussing, the switch element for circuit configuration corresponding to the superconducting coil operates to short-circuit both ends of the superconducting coil. By doing so, it is possible to suppress an abnormal voltage rise occurring at both ends of the superconducting coil. The superconducting magnet device according to a second aspect of the present invention is different from the superconducting magnet device according to the first aspect in that an electrode of a switch as a circuit configuration switch element is arranged in advance in an inert gas at a minute distance, and the electrodes are fixed between the electrodes. When a voltage equal to or higher than the value is generated, an element having a circuit configuration by discharging is used. The superconducting magnet device according to a third aspect of the present invention is different from the superconducting magnet device according to the first aspect in that the electrodes of the switch serving as the switch elements for circuit configuration are previously arranged in the air with a minute distance, and a certain value or more is provided between the electrodes. When a voltage of 1 is generated, an element having a circuit configuration by discharging is used.

【0009】[0009]

【作用】本発明による超電導磁石装置において、回路構
成用スイッチ素子は励磁あるいは消磁作業中に超電導コ
イルに異常が発生したときのみに閉状態になり、励磁あ
るいは消磁作業中に超電導コイルが異常を起こしたとき
に発生する電圧の異常上昇を抑制することができる。
In the superconducting magnet device according to the present invention, the switch element for circuit configuration is closed only when an abnormality occurs in the superconducting coil during the excitation or degaussing work, and the abnormality occurs in the superconducting coil during the excitation or degaussing work. It is possible to suppress an abnormal rise in voltage that occurs when

【0010】[0010]

【実施例】図1は本発明による磁気浮上式鉄道用超電導
磁石装置のうち回路構成用スイッチ素子としてスイッチ
の電極をあらかじめ不活性ガス中に微小距離をおいて配
置し、電極間に一定値以上の電圧が発生したときに放電
により回路を構成するものを使用した実施例の回路図で
ある。図2は図1の超電導磁石装置における超電導コイ
ルの励磁作業中の電流を示す回路図である。図3は図1
の超電導磁石装置における超電導コイルの励磁作業中に
超電導コイルが常電導転移したときの電流を示す回路図
である。図4は図1の超電導磁石装置における超電導コ
イルが励磁され永久電流モードの状態にあるときに一個
の超電導コイルが常電導転移したときの電流を示す回路
図である。図5は本発明による磁気浮上鉄道用超電導磁
石装置のうち、回路構成用スイッチ素子としてスイッチ
の電極あらかじめ空気中に微小距離をおいて配置し、電
極間に一定値以上の電圧が発生したときに放電により回
路を構成するものを使用した実施例の回路図である。図
6は本発明による磁気浮上鉄道用超電導磁石装置のう
ち、回路構成用スイッチ素子として接触器を用いて外部
からの指令により、回路を短絡して構成する場合の実施
例の回路図である。ここで、1a〜1fは超電導コイ
ル、2a〜2fは永久電流スイッチ、3a〜3fは車上
配置保護抵抗器、4a〜4fは車上配置ダイオード、5
a〜5fは回路構成用スイッチ素子、6a〜6cは電流
リード線、7a,7bは励磁用電源ケーブル、8は励磁
用電源、9は地上配置保護抵抗器、10は地上配置ダイ
オードである。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 shows a magnetic levitation type superconducting magnet apparatus for a railway according to the present invention, in which an electrode of a switch as a switch element for circuit configuration is arranged in advance in an inert gas with a minute distance, and a certain value or more is provided between the electrodes. FIG. 6 is a circuit diagram of an embodiment in which a circuit is configured by discharging when a voltage of 1 is generated. FIG. 2 is a circuit diagram showing a current during the excitation work of the superconducting coil in the superconducting magnet device of FIG. FIG. 3 shows FIG.
FIG. 6 is a circuit diagram showing a current when the superconducting coil undergoes normal conduction transition during the operation of exciting the superconducting coil in the superconducting magnet device of FIG. FIG. 4 is a circuit diagram showing a current when one superconducting coil makes a transition to normal conduction when the superconducting coil in the superconducting magnet device of FIG. 1 is excited and in a state of a permanent current mode. FIG. 5 is a view of a superconducting magnet device for a magnetically levitated railway according to the present invention, in which a switch electrode as a circuit configuration switch element is arranged in advance in the air with a minute distance, and when a voltage of a certain value or more is generated between the electrodes. It is a circuit diagram of an example using what constitutes a circuit by discharge. FIG. 6 is a circuit diagram of an embodiment of a magnetic levitation railway superconducting magnet device according to the present invention in which a contactor is used as a circuit configuration switch element to short-circuit a circuit in response to an external command. Here, 1a to 1f are superconducting coils, 2a to 2f are permanent current switches, 3a to 3f are on-vehicle arranged protection resistors, 4a to 4f are on-vehicle arranged diodes, 5
a to 5f are switching elements for circuit configuration, 6a to 6c are current lead wires, 7a and 7b are power cables for excitation, 8 is a power source for excitation, 9 is a protective resistor placed on the ground, and 10 is a diode placed on the ground.

【0011】図1により、本発明による磁気浮上式鉄道
用超電導磁石装置の実施例を説明する。この回路構成用
のスイッチ素子が回路を構成する電圧、すなわち放電開
始電圧の設定条件としては、正常な励磁や消磁作業時に
超電導コイル1a〜1fのそれぞれの両端に発生する電
圧や、永久電流モードとなって超電導コイル1a〜1f
と永久電流スイッチ2a〜2fのそれぞれ一対で構成さ
れる閉回路を流れている状態で、永久電流スイッチ2a
〜2fのいずれかが常電導転移して開状態になったとき
に開状態になった永久電流スイッチ2a〜2fの両端に
発生する電圧を上回る値であり、かつ超電導コイル1a
〜1fや永久電流スイッチ2a〜2fが焼損や溶断する
電圧や超電導磁石装置内部で放電現象がおこる電圧を下
回る必要がある。
An embodiment of a magnetically levitated railway superconducting magnet device according to the present invention will be described with reference to FIG. The voltage at which the switching element for this circuit configuration constitutes the circuit, that is, the discharge start voltage is set to a voltage generated at both ends of each of the superconducting coils 1a to 1f during normal excitation or degaussing work, or a permanent current mode. Superconducting coils 1a-1f
And a persistent current switch 2a to 2f, the persistent current switch 2a
2f is a value higher than the voltage generated across both ends of the persistent current switches 2a to 2f which are in the open state when one of the superconducting coils 2a to 2f is in the open state due to the normal conduction transition, and the superconducting coil 1a.
.About.1f and the persistent current switches 2a to 2f need to be lower than the voltage at which they burn out or melt or the voltage at which the discharge phenomenon occurs inside the superconducting magnet device.

【0012】以下いくつかの図を用いて本発明の機構を
説明する。超電導コイルを励磁する場合、永久電流スイ
ッチ2a〜2fをあらかじめ有限の抵抗状態にして開と
するため、励磁電流のほとんどが図2のように超電導コ
イル1a〜1fを流れる。このとき励磁用電源8は比較
的低い電流上昇率で通電しているため、超電導コイル1
a〜1fのそれぞれの両端に発生する電圧では回路構成
用スイッチ素子5a〜5fは開状態を維持し、超電導コ
イル1a〜1fのそれぞれの両端をつなぐ回路は構成さ
れず超電導磁石装置を正常に励磁することが出来る。
The mechanism of the present invention will be described below with reference to some drawings. When exciting the superconducting coil, since the permanent current switches 2a to 2f are opened in advance in a finite resistance state, most of the exciting current flows through the superconducting coils 1a to 1f as shown in FIG. At this time, since the exciting power source 8 is energized at a relatively low rate of current increase, the superconducting coil 1
With the voltage generated at both ends of each of a to 1f, the circuit configuration switch elements 5a to 5f maintain the open state, the circuit connecting each end of each of the superconducting coils 1a to 1f is not formed, and the superconducting magnet device is normally excited. You can do it.

【0013】次に励磁の際に超電導コイル1a〜1fの
電流や電圧に異常が発生する場合を考える。例えば図3
に示すように、励磁用電源8からの通電電流値が500
Aの時に超電導コイル1aが常電導転移したとすると、
転移直後はそれまで超電導コイル1aに蓄積されていた
エネルギーは永久電流スイッチ2aと車上配置保護抵抗
器3aに分流する回路Iで減衰していき、他の超電導コ
イル1b〜1fに蓄えられていたエネルギーは地上配置
保護抵抗器9と地上配置ダイオード10、および永久電
流スイッチ2aで構成される回路IIで減衰していく。
このとき励磁用電源8は異常を検知してすでに自己遮断
している。永久電流スイッチ2aでは回路Iと回路II
の電流の向きが逆になっているため相殺され、永久電流
スイッチ2aの両端には異常な電圧上昇は発生しない。
Next, consider a case where an abnormality occurs in the current or voltage of the superconducting coils 1a to 1f during excitation. For example, in FIG.
As shown in, the energizing current value from the excitation power source 8 is 500
If the superconducting coil 1a undergoes normal conduction transition at the time of A,
Immediately after the transition, the energy stored in the superconducting coil 1a until then was attenuated by the circuit I shunting to the permanent current switch 2a and the onboard protection resistor 3a, and stored in the other superconducting coils 1b to 1f. Energy is attenuated in the circuit II including the ground protection resistor 9, the ground diode 10, and the permanent current switch 2a.
At this time, the excitation power source 8 has already detected the abnormality and has shut itself off. In the persistent current switch 2a, the circuit I and the circuit II
Since the directions of the currents are reversed, they cancel each other, and no abnormal voltage rise occurs at both ends of the permanent current switch 2a.

【0014】ところが回路Iの超電導コイル1aは常電
導転移しているため、回路IIと比較すると電流の減衰
速度が早い。したがって次第に永久電流スイッチ2aを
流れる電流が増加していき、その両端に発生する電圧も
上昇していくことになる。例えば永久電流スイッチ2a
〜2fの開時抵抗が50Ωで、永久電流スイッチ2aを
流れる電流が増加して10Aになったとすると500V
が両端に発生することになる。ところが回路構成用スイ
ッチ素子5a〜5fの放電開始電圧が例えば350Vで
あるとすると、永久電流スイッチ2aの両端電圧が35
0Vになった時点で回路構成用スイッチ素子5aが放電
を開始することにより永久電流スイッチ2aの両端をつ
なぐため、前記のように永久電流スイッチ2aの両端電
圧が500Vまで上昇することはない。さらにこの回路
構成用のスイッチ素子5a〜5fは超電導コイル1a〜
1fの異常を検知し自動的に回路を構成するので新たに
閉指令のための制御装置を必要としない。
However, since the superconducting coil 1a of the circuit I undergoes normal conduction transition, the current decay speed is faster than that of the circuit II. Therefore, the current flowing through the permanent current switch 2a gradually increases, and the voltage generated across the current also increases. For example, the permanent current switch 2a
If the open resistance of ~ 2f is 50Ω and the current flowing through the permanent current switch 2a increases to 10 A, 500 V
Will occur at both ends. However, if the discharge start voltage of the circuit configuration switch elements 5a to 5f is, for example, 350V, the voltage across the permanent current switch 2a is 35V.
When the voltage reaches 0V, the switching element 5a for circuit configuration starts discharging to connect both ends of the permanent current switch 2a, so that the voltage across the permanent current switch 2a does not rise to 500V as described above. Further, the switch elements 5a to 5f for this circuit configuration are the superconducting coils 1a to
Since the circuit of 1f is detected automatically and the circuit is automatically constructed, a new controller for the closing command is not required.

【0015】前記の内容は、消磁作業中においても同様
である。
The above contents are the same even during the degaussing operation.

【0016】次に磁気浮上式鉄道車両が励磁され永久電
流モードにあり、励磁用電源が切り離されているとき
は、例えば図4に示すように永久電流スイッチ2aが常
電導転移したり、超電導コイル1aが超電導転移するの
と同時に永久電流スイッチ2aも常電導転移したとする
と、超電導コイル1aに永久電流モードとして流されて
いた電流値を500Aとし、車上配置保護抵抗器3aの
抵抗値を0.6Ωとすると、永久電流スイッチ2aの両
端には初期において300Vの電圧が発生することにな
る。ところが回路構成用スイッチ素子5a〜5fの放電
開始電圧の350Vには達していないため回路構成用ス
イッチ素子5aは動作せず、超電導コイル1aの蓄積エ
ネルギーは車上配置保護抵抗器3aで消費させることが
できる。
Next, when the magnetic levitation railway vehicle is excited and in the permanent current mode, and the power source for excitation is disconnected, for example, as shown in FIG. 4, the persistent current switch 2a undergoes normal conduction transition or superconducting coil. Assuming that the permanent current switch 2a also transits to the normal conduction state at the same time that the 1a transitions to the superconducting state, the current value flowing in the superconducting coil 1a in the persistent current mode is set to 500A, and the resistance value of the vehicle-mounted protection resistor 3a is set to 0. When it is set to 0.6Ω, a voltage of 300V is initially generated across the permanent current switch 2a. However, since the circuit configuration switch elements 5a to 5f have not reached the discharge start voltage of 350 V, the circuit configuration switch elements 5a do not operate, and the energy stored in the superconducting coil 1a is consumed by the on-board protection resistor 3a. You can

【0017】図5は、本発明における磁気浮上式鉄道用
超電導磁石装置のうち、回路構成用スイッチ素子として
スイッチの電極をあらかじめ空気中に微小距離をおいて
配置し、電極間に一定値以上の電圧が発生したときに放
電により回路を構成する場合の実施例である。この場合
においても、回路構成用スイッチ素子5a〜5fが回路
を構成する電圧、すなわち放電開始電圧の設定条件とし
ては、正常な励磁や消磁作業時に超電導コイル1a〜1
fの両端に発生する電圧や、永久電流モードとなって超
電導コイル1a〜1fと永久電流スイッチ2a〜2fの
それぞれ一対で構成される閉回路を流れている状態で、
永久電流スイッチ2a〜2fのいずれかが常電導転移し
て開状態になったときに永久電流スイッチ2a〜2fの
両端に発生する電圧を上回る値であり、かつ超電導コイ
ル1a〜1fや永久電流スイッチ2a〜2fが焼損や溶
断する電圧や超電導磁石装置内部で放電現象が起こる電
圧を下回る必要がある。これにより、図5においても図
1と同様の作用をし、スイッチを動作させるための制御
装置を必要としない。
FIG. 5 shows a magnetic levitation railway superconducting magnet device according to the present invention, in which electrodes of a switch serving as a switch element for circuit configuration are arranged in advance in the air at a minute distance, and a predetermined value or more is provided between the electrodes. This is an embodiment in the case of forming a circuit by discharging when a voltage is generated. In this case as well, the setting conditions of the voltage at which the circuit configuration switch elements 5a to 5f configure the circuit, that is, the discharge start voltage, are the superconducting coils 1a to 1 during normal excitation or degaussing work.
In the state where the voltage generated at both ends of f and the permanent current mode flow through the closed circuit composed of a pair of superconducting coils 1a to 1f and permanent current switches 2a to 2f,
The value is higher than the voltage generated at both ends of the persistent current switches 2a to 2f when any of the persistent current switches 2a to 2f is in the open state due to the normal conduction transition, and the superconducting coils 1a to 1f and the persistent current switch. It is necessary that the voltage of 2a to 2f is lower than the voltage at which burnout or fusing occurs or the voltage at which the discharge phenomenon occurs inside the superconducting magnet device. As a result, the same operation as that in FIG. 1 is performed in FIG. 5, and a control device for operating the switch is not required.

【0018】図6は、本発明による磁気浮上式鉄道用超
電導磁石装置のうちで、回路構成用スイッチ素子に接触
器を用いた実施例である。この場合において、作用は図
1と同様であるが、回路構成がスイッチ自身の放電では
なく外部からの指令によるため、異常時に永久電流スイ
ッチ2a〜2fの両端に発生する電圧をコントロールす
ることが可能である。
FIG. 6 shows an embodiment of the magnetic levitation type superconducting magnet device for railway according to the present invention, in which a contactor is used as a switch element for circuit construction. In this case, the operation is similar to that of FIG. 1, but since the circuit configuration is not an electric discharge of the switch itself but an external command, it is possible to control the voltage generated across the permanent current switches 2a to 2f at the time of an abnormality. Is.

【0019】図1,図5,図6に示す地上配置ダイオー
ド10は動作電圧を考慮した回路構成用スイッチ素子5
a〜5fと振り替えることが可能である。
The ground-mounted diode 10 shown in FIGS. 1, 5 and 6 is a switch element 5 for circuit configuration in consideration of operating voltage.
It is possible to transfer to a to 5f.

【発明の効果】本発明による磁気浮上式鉄道用超電導磁
石装置において、超電導コイルの励磁あるいは消磁作業
中に超電導コイルが1個以上常電導転移した場合に、当
該超電導コイルの両端に発生する異常な電圧上昇を抑制
することが可能となり、異常な電圧上昇が発生すること
による超電導磁石装置への影響をなくすことができる。
In the magnetically levitated railway superconducting magnet device according to the present invention, when one or more superconducting coils undergo normal conduction transition during the excitation or degaussing work of the superconducting coil, an abnormal phenomenon occurs at both ends of the superconducting coil. It is possible to suppress the voltage rise, and it is possible to eliminate the influence on the superconducting magnet device due to the abnormal voltage rise.

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

【図1】本発明における磁気浮上式鉄道用超電導磁石装
置の実施例で、スイッチ素子としてスイッチの電極をあ
らかじめ不活性ガス中に微小距離をおいて配置したもの
を使用した回路図である。
FIG. 1 is a circuit diagram of an embodiment of a magnetic levitation type superconducting magnet device for a railway according to the present invention, in which electrodes of a switch are arranged in advance in an inert gas at a minute distance as a switch element.

【図2】図1の超電導磁石装置における超電導コイルの
励磁作業中の電流を示す回路図である。
FIG. 2 is a circuit diagram showing a current during an exciting operation of a superconducting coil in the superconducting magnet device of FIG.

【図3】図1の超電導磁石装置における超電導コイルの
励磁作業中に超電導コイルが常電導転移したときの電流
を示す回路図である。
FIG. 3 is a circuit diagram showing a current when the superconducting coil undergoes normal conduction transition during an operation of exciting the superconducting coil in the superconducting magnet device of FIG.

【図4】図1の超電導磁石装置における超電導コイルが
励磁され永久電流モードの状態にあるときに一個の超電
導コイルが常電導転移したときの電流を示す回路図であ
る。
FIG. 4 is a circuit diagram showing a current when one superconducting coil undergoes normal conduction transition when the superconducting coil in the superconducting magnet device of FIG. 1 is excited and in a state of a permanent current mode.

【図5】本発明における磁気浮上鉄道用超電導磁石装置
の実施例で、回路構成用スイッチ素子としてスイッチの
電極をあらかじめ空気中に微小距離をおいて配置し、電
極間に一定値以上の電圧が発生したときに放電により回
路を構成する場合の回路図である。
FIG. 5 is an embodiment of a magnetic levitation railway superconducting magnet device according to the present invention, in which electrodes of a switch as a circuit configuration switch element are arranged in air at a minute distance in advance, and a voltage of a certain value or more is applied between the electrodes. It is a circuit diagram in the case of forming a circuit by discharge when it occurs.

【図6】本発明における磁気浮上鉄道用超電導磁石装置
の実施例で、回路構成用スイッチ素子として接触器を使
用した場合の回路図である。
FIG. 6 is a circuit diagram in the case where a contactor is used as a switch element for circuit configuration in an embodiment of a magnetic levitation railway superconducting magnet device according to the present invention.

【図7】従来の技術における磁気浮上式鉄道用超電導磁
石装置の回路図である。
FIG. 7 is a circuit diagram of a conventional magnetically levitated railway superconducting magnet device.

【符号の説明】[Explanation of symbols]

1a〜1f 超電導コイル 2a〜2f 永久電流スイッチ 3a〜3f 車上配置保護抵抗器 4a〜4f 車上配置ダイオード 5a〜5f 回路構成用スイッチ素子 6a〜6c 電流リード線 7a,7b 励磁用電源ケーブル 8 励磁用電源 9 地上配置保護抵抗器 10 地上配置ダイオード 1a to 1f Superconducting coil 2a to 2f Permanent current switch 3a to 3f On-board arrangement protection resistor 4a to 4f On-board diode 5a to 5f Circuit configuration switch element 6a to 6c Current lead wire 7a, 7b Excitation power supply cable 8 Excitation Power supply 9 Ground protection resistor 10 Ground diode

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 磁気浮上式鉄道の車両に搭載される超電
導コイルと永久電流スイッチと車上配置保護抵抗器と回
路構成用スイッチ素子とからなる超電導磁石装置におい
て、 対向する左右一対以上の超電導コイルのそれぞれに永久
電流スイッチと車上配置保護抵抗器とダイオードが接続
され、該超電導コイルの両端を短絡出来るように回路構
成用スイッチ素子が接続されている回路からなり、 該超電導コイルの電流や電圧に異常が発生して該超電導
コイルの電流が該永久電流スイッチから該車上配置保護
抵抗器に転流した場合に、該車上配置保護抵抗器は該超
電導コイルが常電導転移を生じるだけの値を有し、 該超電導コイルを励磁あるいは消磁の際、該永久電流ス
イッチが開状態で該超電導コイルが常電導転移した場合
に、該超電導コイルに対応する該回路構成用スイッチ素
子が動作して該超電導コイルの両端を短絡することによ
り、該回路構成用スイッチ素子は該超電導コイルの両端
に発生する異常な電圧上昇を抑制することを特徴とする
磁気浮上式鉄道用超電導磁石装置。
1. A superconducting magnet device comprising a superconducting coil, a permanent current switch, a vehicle-mounted protective resistor, and a circuit-forming switch element, which is mounted on a magnetic levitation railway vehicle. Each of which is connected to a permanent current switch, a vehicle-mounted protective resistor, and a diode, and a circuit configuration switch element connected so that both ends of the superconducting coil can be short-circuited. When an abnormality occurs in the superconducting coil and the current of the superconducting coil is diverted from the permanent current switch to the on-board locating resistor, the on-board locating resistor only causes the superconducting coil to undergo normal conduction transition. Has a value, and when the superconducting coil is excited or degaussed, the superconducting coil is transferred to the normal conducting state with the persistent current switch open The corresponding switch element for circuit configuration operates to short-circuit both ends of the superconducting coil, whereby the switch element for circuit configuration suppresses an abnormal voltage rise occurring at both ends of the superconducting coil. Magnetically levitated railway superconducting magnet device.
【請求項2】 請求項1の超電導磁石装置において、 該回路構成用スイッチ素子としてスイッチの電極をあら
かじめ不活性ガス中に微小距離をおいて配置し、 電極間に一定値以上の電圧が発生した場合に、放電によ
る回路構成をする素子を使用することで超電導コイルの
両端に発生する異常な電圧上昇を抑制することを特徴と
する請求項1記載の磁気浮上式鉄道用超電導磁石装置。
2. The superconducting magnet device according to claim 1, wherein electrodes of a switch serving as the switch element for circuit configuration are previously arranged in an inert gas at a minute distance, and a voltage of a certain value or more is generated between the electrodes. In this case, the magnetic levitation type superconducting magnet device for a railway according to claim 1, wherein an abnormal voltage rise occurring at both ends of the superconducting coil is suppressed by using an element having a circuit configuration by discharge.
【請求項3】 請求項1の超電導磁石装置において、 該回路構成用スイッチ素子としてスイッチの電極をあら
かじめ空気中に微小距離をおいて配置し、 電極間に一定値以上の電圧が発生した場合に、放電によ
る回路構成をする素子を使用することで超電導コイルの
両端に発生する異常な電圧上昇を抑制することを特徴と
する請求項1記載の磁気浮上式鉄道用超電導磁石装置。
3. The superconducting magnet device according to claim 1, wherein the electrodes of the switch serving as the switch element for circuit configuration are previously arranged in the air at a minute distance, and when a voltage of a certain value or more is generated between the electrodes. The magnetic levitation type superconducting magnet device for a railway according to claim 1, wherein an abnormal voltage rise generated at both ends of the superconducting coil is suppressed by using an element having a circuit configuration by discharge.
JP20374293A 1992-11-19 1993-07-27 Magnetically levitated superconducting magnet device for railways Expired - Fee Related JP2761452B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP20374293A JP2761452B2 (en) 1993-07-27 1993-07-27 Magnetically levitated superconducting magnet device for railways
US08/142,911 US5432669A (en) 1992-11-19 1993-10-28 Superconducting magnet apparatus for magnetically levitated train

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20374293A JP2761452B2 (en) 1993-07-27 1993-07-27 Magnetically levitated superconducting magnet device for railways

Publications (2)

Publication Number Publication Date
JPH0745422A true JPH0745422A (en) 1995-02-14
JP2761452B2 JP2761452B2 (en) 1998-06-04

Family

ID=16479103

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20374293A Expired - Fee Related JP2761452B2 (en) 1992-11-19 1993-07-27 Magnetically levitated superconducting magnet device for railways

Country Status (1)

Country Link
JP (1) JP2761452B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002217021A (en) * 2001-01-15 2002-08-02 Central Japan Railway Co Superconducting magnet protective unit
JP2010161398A (en) * 2010-03-03 2010-07-22 Railway Technical Res Inst Superconducting magnet protective unit

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002217021A (en) * 2001-01-15 2002-08-02 Central Japan Railway Co Superconducting magnet protective unit
JP4580561B2 (en) * 2001-01-15 2010-11-17 財団法人鉄道総合技術研究所 Superconducting magnet protector
JP2010161398A (en) * 2010-03-03 2010-07-22 Railway Technical Res Inst Superconducting magnet protective unit

Also Published As

Publication number Publication date
JP2761452B2 (en) 1998-06-04

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