JPH0261593A - Self-actuation type electromagnet for control rod holding mechanism - Google Patents

Self-actuation type electromagnet for control rod holding mechanism

Info

Publication number
JPH0261593A
JPH0261593A JP63212114A JP21211488A JPH0261593A JP H0261593 A JPH0261593 A JP H0261593A JP 63212114 A JP63212114 A JP 63212114A JP 21211488 A JP21211488 A JP 21211488A JP H0261593 A JPH0261593 A JP H0261593A
Authority
JP
Japan
Prior art keywords
iron core
attraction
temperature
coil
magnetic flux
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
JP63212114A
Other languages
Japanese (ja)
Other versions
JPH0559400B2 (en
Inventor
Makoto Saito
誠 斎藤
Minoru Gunji
軍司 稔
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.)
Power Reactor and Nuclear Fuel Development Corp
Original Assignee
Power Reactor and Nuclear Fuel Development 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 Power Reactor and Nuclear Fuel Development Corp filed Critical Power Reactor and Nuclear Fuel Development Corp
Priority to JP63212114A priority Critical patent/JPH0261593A/en
Publication of JPH0261593A publication Critical patent/JPH0261593A/en
Publication of JPH0559400B2 publication Critical patent/JPH0559400B2/ja
Granted legal-status Critical Current

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Classifications

    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E30/00Energy generation of nuclear origin
    • Y02E30/30Nuclear fission reactors

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  • Electromagnets (AREA)

Abstract

PURPOSE:To surely cut off control rods at the time of temperature abnormal increase by incorporating heat sensitive magnetic materials among a coil and all the attraction faces. CONSTITUTION:A first iron core is rotation symmetry, structure in which a center leg part 20a and a peripheral cylindrical part 20b are connected in the upper part thereof is made and a coil is wound on the center leg part 20a. The lower end faces of the leg part 20a and the cylindrical part 20b are attraction faces respectively and a second circular plate-like iron core 22 which becomes are an armature is attracted. Further, respective heat sensitive magnetic materials 26a, 26b are provided between a coil attaching part and an attraction face of the iron core 20. In the case where temperature does not reach Curie temperature, magnetic flux which generates in the coil 24 almost passes in a magnetic circuit because the magnetic materials 26a, 26b are ferromagnetic substances and sufficient attraction works on an attraction face X, Y to hold control rods. Further, when circumstance temperature exceeds a Curie point, the magnetic materials 26a, 26b lose magnetization and the magnetic flux density of the attraction faces X, Y is remarkably lowered. As the result, the attraction decreases to cur off the iron core, which drops to stop a reactor.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、異常発生時に原子炉を緊急停止させるため制
御棒を炉心へ自動的に挿入する自己作動型電磁石に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a self-actuating electromagnet that automatically inserts a control rod into a reactor core in order to emergency stop a nuclear reactor when an abnormality occurs.

更に詳しく述べると本発明は、一方の鉄芯の全ての吸着
面とコイル取付は部との間にそれぞれ感温磁性材を設け
ることによって、キュリー点以上での残留磁束が特定の
吸着部に集中することを防ぎ、キュリー点以上での吸着
力の変化を大きくして動作の信頼性を向上した制御棒保
持機構用の自己作動型電磁石に関するものである。
To be more specific, the present invention provides temperature-sensitive magnetic materials between all the attraction surfaces of one iron core and the coil mounting portion, so that the residual magnetic flux above the Curie point is concentrated on a specific attraction portion. This invention relates to a self-actuating electromagnet for a control rod holding mechanism, which prevents this from occurring and increases the change in attraction force above the Curie point, thereby improving operational reliability.

[従来の技術] 一般に高速炉等では炉停止の信頼性を高めるため異常時
に制御棒を炉心に挿入する機構を備えている。この機構
の信頼性を高めるために、外部からの操作や信号に依存
せずに原子炉を安全に停止することができるように自己
作動型電磁石を用い、それで制御棒を保持する構成が提
案されている。
[Prior Art] In general, fast reactors and the like are equipped with a mechanism for inserting control rods into the reactor core in the event of an abnormality in order to increase the reliability of reactor shutdown. In order to increase the reliability of this mechanism, a configuration has been proposed that uses self-actuating electromagnets to hold the control rods so that the reactor can be safely stopped without relying on external operations or signals. ing.

従来の自己作動型電磁石としては、第7図に示すように
、第1の鉄芯10と第2の鉄芯12とを組み合わせ、そ
れにコイル14を組み込み、鉄芯の一部に感温磁性材1
6を配置した構成がある0両鉄芯10,12は回転対称
体で、コイル14は第1の鉄芯lOの中央脚部に巻装さ
れている。感温磁性材16は、カップ状をなす第2の鉄
芯12の外側円筒部に組み込まれている。
As shown in FIG. 7, a conventional self-actuating electromagnet combines a first iron core 10 and a second iron core 12, incorporates a coil 14 therein, and incorporates a temperature-sensitive magnetic material into a part of the iron core. 1
The two iron cores 10 and 12 are rotationally symmetric bodies, and the coil 14 is wound around the central leg of the first iron core IO. The temperature-sensitive magnetic material 16 is incorporated into the outer cylindrical portion of the cup-shaped second iron core 12 .

このような自己作動型電磁石は炉心近傍の高温冷却材中
に設置される。炉心に何らかの異常が生じ周囲温度が上
昇して感温磁性材16のキュリー点を超えると、感温磁
性材16は磁性を失いその部分で磁気回路が遮断される
。従って磁気回路全体の磁気抵抗が増大するため、吸着
面X、Yを通過する磁束密度が低下する。そのため吸着
力が低下し、制御棒の自重によって第2の鉄芯12は第
1の鉄芯10から切り離され落下する。これがこの自己
作動型電磁石の動作原理である。
Such self-actuated electromagnets are installed in the high temperature coolant near the reactor core. When some abnormality occurs in the core and the ambient temperature rises to exceed the Curie point of the temperature-sensitive magnetic material 16, the temperature-sensitive magnetic material 16 loses its magnetism and the magnetic circuit is interrupted at that portion. Therefore, since the magnetic resistance of the entire magnetic circuit increases, the magnetic flux density passing through the attraction surfaces X and Y decreases. Therefore, the suction force decreases, and the second iron core 12 is separated from the first iron core 10 and falls due to the control rod's own weight. This is the operating principle of this self-actuated electromagnet.

[発明が解決しようとする課題] しかしながら磁気回路は電気回路と異なり、空間にはあ
る程度の透磁率が存在するため、鉄芯の一部が磁気的に
遮断されても空間を通る磁束が残留する。これによる残
留吸着力がこの電磁石では大きな問題となる。制御棒を
確実に切り離すためには遮断後の吸着力は制御棒の自重
に対して十分に小さいことが必要なためである。
[Problem to be solved by the invention] However, unlike an electric circuit, a magnetic circuit has a certain degree of magnetic permeability in space, so even if a part of the iron core is magnetically blocked, magnetic flux passing through the space remains. . This residual adsorption force is a major problem with this electromagnet. This is because in order to reliably disconnect the control rod, the suction force after disconnection must be sufficiently small compared to the control rod's own weight.

周囲温度がキュリー点を超えていない場合と超えた場合
の磁束分布のシミュレーシッン結果の例を第8図A、B
に示す、なお図面を簡略化するため磁束分布については
右半分のみ表示しである。キュリー温度を超えて感温磁
性材16が磁性を失い磁気回路の一部が磁気的に遮断さ
れた場合、磁束は磁気抵抗の大きな感温磁性材16の近
傍で大量に空間に洩れることになる。
Figures 8A and B show examples of simulation results of magnetic flux distribution when the ambient temperature does not exceed the Curie point and when it exceeds the Curie point.
To simplify the drawing, only the right half of the magnetic flux distribution is shown. If the temperature-sensitive magnetic material 16 loses its magnetism and a part of the magnetic circuit is magnetically cut off by exceeding the Curie temperature, a large amount of magnetic flux will leak into space near the temperature-sensitive magnetic material 16 with high magnetic resistance. .

−a的には、コイル14に近い部分は磁束密度が大きく
、遮断部に近いほど小さくなる。吸着力は吸着面を通過
する磁束密度に依存するため、吸着面と遮断部及びコイ
ルの相対的な位置関係によって、遮断後の吸着力は異な
ることになる。
In terms of -a, the magnetic flux density is large in a portion close to the coil 14, and becomes smaller as it is closer to the cutoff portion. Since the attraction force depends on the magnetic flux density passing through the attraction surface, the attraction force after interruption will vary depending on the relative positional relationship between the attraction surface, the interruption section, and the coil.

従来形状の場合、吸着面Yはコイル16から遠く又遮断
部に近いため磁束密度は小さいが、分割面Xはコイル1
4に近く遮断部から遠いため磁束密度はかなり大きく残
留している。その結果、キュリー点を超えてもかなり大
きな吸着力が残ることになり、炉停止機構としての信頼
性に問題が生じる。
In the case of the conventional shape, the magnetic flux density is small because the attracting surface Y is far from the coil 16 and close to the cutoff part, but the dividing surface X is far from the coil 16.
Since it is close to 4 and far from the cutoff part, the magnetic flux density remains quite large. As a result, a considerably large adsorption force remains even beyond the Curie point, which poses a problem in reliability as a reactor shutdown mechanism.

この残留吸着力を下げるためには、中央脚部の鉄芯断面
積を小さくしたり、吸着面間に間隙を設ける等の方法が
考えられるが、それでは磁気回路全体の磁気抵抗が大き
くなり、キュリー点未満の定常運転状態での吸着力も低
下することになる。アンペア・ターン数を減らす方法も
同様に定常運転状態での吸着力が低下することになる。
In order to reduce this residual adsorption force, methods such as reducing the cross-sectional area of the iron core in the central leg or creating a gap between the adsorption surfaces can be considered, but this would increase the magnetic resistance of the entire magnetic circuit, making the Curie The adsorption force under the steady state of operation below the point also decreases. A method of reducing the number of ampere turns will similarly reduce the suction force under steady operating conditions.

従って従来技術のような基本構造を有する限り、キュリ
ー温度での吸着力を犠牲にすることなくキュリー点以上
での吸着力を小さくすることができなかった。
Therefore, as long as the basic structure as in the prior art is used, it has not been possible to reduce the adsorption force above the Curie temperature without sacrificing the adsorption force at the Curie temperature.

本発明の目的は、上記のような従来技術の欠点を解消し
、キュリー点未満での吸着力は十分大きく、しかもキュ
リー点以上での吸着力を十分小さくして定常運転中は誤
動作の心配がなく、温度異常上昇時は確実に制御棒の切
り離し動作を行わせることができるような制御棒保持機
構用の自己作動型電磁石を提供することにある。
The purpose of the present invention is to eliminate the above-mentioned drawbacks of the prior art, and to provide a system in which the suction force below the Curie point is sufficiently large, and the suction force above the Curie point is sufficiently small, so that there is no fear of malfunction during steady operation. The object of the present invention is to provide a self-actuating electromagnet for a control rod holding mechanism that can reliably disconnect the control rods when the temperature rises abnormally.

[課題を解決するための手段] 上記のような目的を達成できる本発明は、二分割可能な
構造の鉄芯とコイルとを具備し、鉄芯の一部に感温磁性
材を組み込み周囲温度に応じて二つの鉄芯の吸着−切り
離しにより制御棒の保持−切り離しを行う電磁石におい
て、コイルを装着する方の鉄芯の全ての吸着面とコイル
取付は部との間にそれぞれ感温磁性材を設けた制御棒保
持機構用の自己作動型電磁石である。
[Means for Solving the Problems] The present invention, which can achieve the above objects, includes an iron core and a coil with a structure that can be divided into two, and a temperature-sensitive magnetic material is incorporated into a part of the iron core to adjust the ambient temperature. In an electromagnet that holds and disconnects the control rod by adsorbing and separating the two iron cores, a temperature-sensitive magnetic material is placed between all the adsorption surfaces of the iron core on which the coil is attached and the coil mounting part. This is a self-actuated electromagnet for the control rod holding mechanism.

例えば、一方の鉄芯を円柱体の中央で切り欠いたような
全体はぼU字型の構造とし、その両脚部にそれぞれコイ
ルを巻装し、両コイル巻き付は個所と両吸着面との間に
感温磁性材を設け、それに対してアーマチェアとなる他
方の鉄芯を円板状にする構造が好ましい。
For example, one iron core is cut out at the center of a cylindrical body to create a roughly U-shaped structure, and a coil is wound around each leg of the core, and the winding of both coils is done at a certain point and on both suction surfaces. It is preferable to have a structure in which a temperature-sensitive magnetic material is provided in between, and the other iron core serving as the armchair is shaped like a disk.

[作用] 上記のような構造では、周囲温度が感温磁性材のキュリ
ー点以上になるとコイルと全ての吸着面が直接鉄芯で磁
気的に短絡されず、全ての吸着面はコイルから遮断され
る。このため全ての吸着面の磁束密度は遮断部感温磁性
材のコイル側から空間に漏れた磁束の一部だけとなり、
極めて小さく吸着力は殆ど発生しない、従ってキュリー
点前後での吸着力の変化が極めて大きくなり定常運転中
の誤動作の可能性は殆どなくなり、しかも異常発生時に
おける切り離し動作の信幀性が高くなる。
[Function] With the above structure, when the ambient temperature rises above the Curie point of the temperature-sensitive magnetic material, the coil and all attraction surfaces are not directly magnetically short-circuited by the iron core, and all attraction surfaces are cut off from the coil. Ru. Therefore, the magnetic flux density of all the attraction surfaces is only a part of the magnetic flux that leaked into the space from the coil side of the temperature-sensitive magnetic material of the interrupting part.
The suction force is extremely small and almost no suction force is generated.Therefore, the change in suction force before and after the Curie point is extremely large, so there is almost no possibility of malfunction during normal operation, and the reliability of the disconnection operation when an abnormality occurs is increased.

[実施例] 第1図は本発明に係る自己作動型電磁石の一実施例を示
す断面図である。また第2図A、  Bはキュリー点未
満での磁束分布とキュリー点以上での磁束分布を示す説
明図であり、図面を簡略化するため磁束分布は右半分の
み描いである。
[Embodiment] FIG. 1 is a sectional view showing an embodiment of a self-actuating electromagnet according to the present invention. Further, FIGS. 2A and 2B are explanatory diagrams showing the magnetic flux distribution below the Curie point and the magnetic flux distribution above the Curie point, and in order to simplify the drawings, only the right half of the magnetic flux distribution is drawn.

第1の鉄芯20は回転対称体であり、中央脚部20aと
外周円筒部20bとが上部で連続したような構造をなし
、中央脚部20aにコイル24が巻装されている。中央
脚部20aと外周円筒部20bの下端面がそれぞれ吸着
面となり、アーマチュアとなる円板状の第2の鉄芯22
を吸着する。なお図示するのを省略するが、実際には従
来同様、第2の鉄芯22からは制御棒が吊設される。
The first iron core 20 is a rotationally symmetric body, and has a structure in which a central leg portion 20a and an outer peripheral cylindrical portion 20b are continuous at the upper portion, and a coil 24 is wound around the central leg portion 20a. The lower end surfaces of the central leg portion 20a and the outer cylindrical portion 20b serve as suction surfaces, respectively, and a disk-shaped second iron core 22 serves as an armature.
adsorbs. Although not shown in the drawings, a control rod is actually suspended from the second iron core 22 as in the conventional case.

この電磁石では、第1の鉄芯20のコイル取付は部と吸
着面との間にそれぞれ感温磁性材26a、26bを設ケ
チイル。
In this electromagnet, temperature-sensitive magnetic materials 26a and 26b are installed between the coil attachment portion of the first iron core 20 and the attraction surface, respectively.

第2図Aからも判るように、キュリー温度に達しない場
合には、感温磁性材26a、26bは強磁性体であるか
ら、コイル24で発生した磁束は殆ど全て磁気回路内を
通り、吸着面X。
As can be seen from FIG. 2A, when the Curie temperature is not reached, since the temperature-sensitive magnetic materials 26a and 26b are ferromagnetic, almost all the magnetic flux generated in the coil 24 passes through the magnetic circuit and is attracted. Face X.

Yでは磁束密度が大きく十分な吸着力が働く。At Y, the magnetic flux density is large and sufficient adsorption force is exerted.

これによって制御棒は保持される。This holds the control rod in place.

周囲温度がキュリー点を超えると感温磁性材26a、2
6bはその磁性を失う、すると第2図Bに示すように、
磁束が吸着面の手前でバイパスする形となるため吸着面
X、Yでの磁束密度は大幅に低下する。このため吸着力
が低下し、制御棒の自重によって第2の鉄芯22は切り
離されて落下し原子炉を停止させる。
When the ambient temperature exceeds the Curie point, the temperature-sensitive magnetic materials 26a, 2
6b loses its magnetism, then as shown in Figure 2B,
Since the magnetic flux is bypassed before the attracting surface, the magnetic flux density at the attracting surfaces X and Y is significantly reduced. As a result, the adsorption force decreases, and the second iron core 22 is separated and falls due to the control rod's own weight, stopping the reactor.

ところでこのような構造の場合には、中央脚部に設置し
た感温磁性材26aは外周円筒部に設置した感温磁性材
26bに比べて温度応答性が劣る問題がある。迅速な動
作が要求される場合に、より好ましい構造を第3図〜第
5図に示す、なお第4図は第3図におけるIV−IV断
面を示し、第5図は第3図におけるV−V断面を示す。
However, in the case of such a structure, there is a problem that the temperature-sensitive magnetic material 26a installed in the central leg portion has inferior temperature responsiveness compared to the temperature-sensitive magnetic material 26b installed in the outer peripheral cylindrical portion. When quick operation is required, a more preferable structure is shown in FIGS. 3 to 5. FIG. 4 shows the IV-IV cross section in FIG. 3, and FIG. 5 shows the V-IV cross section in FIG. 3. A V cross section is shown.

この実施例では、第1の鉄芯30は基本的には円柱体の
中央に溝状の切り欠きを設けたような形状をなし、両側
の脚部30a、30bが上部で連続している構造である
。そしてそれぞれの脚部30a、30bにコイル34a
、34bが巻装される0両脚部30a、30bの先端吸
着面でアーマチュアとなる円板状の第20鉄芯32を吸
着する0両脚部30a、30bのコイル取付は部と両級
着面との間に感温磁性材36a、36bが組み込まれる
In this embodiment, the first iron core 30 basically has the shape of a cylindrical body with a groove-like cutout in the center, and has a structure in which the legs 30a and 30b on both sides are continuous at the upper part. It is. A coil 34a is attached to each leg 30a, 30b.
, 34b are wound on the end suction surfaces of the two legs 30a, 30b, which attract the disc-shaped 20th iron core 32, which becomes the armature. Temperature-sensitive magnetic materials 36a and 36b are incorporated between them.

またキュリー点前後における磁束分布を第6図A、Bに
示す0周囲温度がキュリー点未満の場合には磁束は殆ど
全てが磁気回路を流れ、吸着面での磁束密度は高く十分
大きな吸着力を発生する(第6図A参照)、それに対し
て周囲温度がキュリー点を超えると、発生した磁束は空
間を漏れてバイパスするため、吸着面には空間に漏れた
磁束の掻く一部だけが流れるに過ぎず、吸着面での磁気
的吸着力は極めて小さくなる(第6図B参照)、またこ
の実施例において、感温磁性材36a、36bをより長
くするが、あるいは両方の感温磁性材36a、36bの
間の寸法をより狭くすれば、キュリー点を超えた場合に
おける吸着面での磁束密度を更に小さくすることができ
る。
In addition, the magnetic flux distribution before and after the Curie point is shown in Figure 6A and B. When the ambient temperature is below the Curie point, almost all of the magnetic flux flows through the magnetic circuit, and the magnetic flux density on the attraction surface is high enough to generate a sufficiently large attraction force. On the other hand, when the ambient temperature exceeds the Curie point, the generated magnetic flux leaks through the space and bypasses it, so only a portion of the magnetic flux leaking into the space flows through the attraction surface. However, in this embodiment, the temperature-sensitive magnetic materials 36a and 36b are made longer, or both temperature-sensitive magnetic materials are made longer. If the dimension between 36a and 36b is narrower, the magnetic flux density on the attraction surface when the Curie point is exceeded can be further reduced.

[発明の効果] 本発明では上記のようにコイルと全ての吸着面の間にそ
れぞれ感温磁性材が組み込まれているから、周囲温度が
キュリー点を超えた場合には全ての吸着面がコイルから
隔絶されるため、全ての吸着面で磁束密度が非常に小さ
くなり吸着力は殆ど発生せず異常時における切り離しの
信頬性は著しく向上する。またアンペア・ターン数や鉄
芯の断面積を大きくとることでキュリー点未満での吸着
力を十分大きくできるため、定常運転中の誤動作の可能
性は低減し自己作動型電磁石としての信鎖性は著しく向
上する。
[Effects of the Invention] In the present invention, as described above, temperature-sensitive magnetic materials are incorporated between the coil and all the attraction surfaces, so when the ambient temperature exceeds the Curie point, all the attraction surfaces are connected to the coil. Since the magnetic flux density is extremely small on all attraction surfaces, almost no attraction force is generated, and the reliability of disconnection in the event of an abnormality is significantly improved. In addition, by increasing the number of ampere turns and the cross-sectional area of the iron core, the adsorption force below the Curie point can be sufficiently increased, reducing the possibility of malfunction during steady operation and ensuring reliability as a self-operating electromagnet. Significantly improved.

特に一方の鉄芯をU字型構造とすると、全ての感温磁性
材が外側に位置するため温度応答性が良好となり好まし
い、また第1の鉄芯の外形を円柱体に近い構造とし、そ
れに対応してアーマチェアとなる第2の鉄芯を円板状に
すれば、制御棒落下後のリセット作業等の場合に第1の
鉄芯と第2の鉄芯との相対的な回転等を考慮する必要が
なくなり、作業性に支障を及ぼすこともない。
In particular, it is preferable to make one of the iron cores have a U-shaped structure, since all the temperature-sensitive magnetic materials are located on the outside, resulting in good temperature response. Correspondingly, if the second iron core that serves as the armchair is made into a disk shape, the relative rotation between the first iron core and the second iron core can be taken into consideration when resetting the control rod after it falls. There is no need to do this, and there is no problem with workability.

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

第1図は本発明に係る自己作動型電磁石の一実施例を示
す概略構成図、第2図A、Bはそのキュリー点前後にお
ける磁束分布を示す説明図、第3図は本発明の他の実施
例を示す説明図、第4図はそのrV−IV断面図、第5
図はそのv−■断面図、第6図A、Bはそのキュリー点
前後における磁束密度分布を示す説明図である。 また第7図は従来技術の一例を示す断面図、第8図A、
Bはそのキュリー点前後における磁束密度分布を示す説
明図である。 10.20.30・・・第1の鉄芯、12,22゜32
・・・第2の鉄芯、14,24.34a、34b ・・
・コイル、16,26a、26b、36a。 36b・・・感温磁性材。 特許出願人 動力炉・核燃料開発事業団代  理  人
     茂  見     穣第1IIA 2゜ 第31!! 第4図 第5図 第 図 第 図
FIG. 1 is a schematic configuration diagram showing one embodiment of a self-actuating electromagnet according to the present invention, FIGS. 2A and B are explanatory diagrams showing the magnetic flux distribution before and after the Curie point, and FIG. An explanatory diagram showing an example, FIG. 4 is its rV-IV sectional view, and FIG.
The figure is a v--■ cross-sectional view, and FIGS. 6A and 6B are explanatory diagrams showing the magnetic flux density distribution before and after the Curie point. In addition, FIG. 7 is a sectional view showing an example of the prior art, FIG. 8A,
B is an explanatory diagram showing the magnetic flux density distribution before and after the Curie point. 10.20.30...first iron core, 12,22°32
...Second iron core, 14, 24.34a, 34b...
- Coils, 16, 26a, 26b, 36a. 36b...Temperature-sensitive magnetic material. Patent applicant: Power Reactor and Nuclear Fuel Development Corporation Representative, Shigeru Miyoshi 1st IIA 2゜31st! ! Figure 4 Figure 5 Figure Figure

Claims (1)

【特許請求の範囲】 1、二分割可能な構造の鉄芯とコイルとを具備し、鉄芯
の一部に感温磁性材を組み込み周囲温度に応じて二つの
鉄芯の吸着−切り離しにより制御棒の保持−切り離しを
行う電磁石において、コイルを装着する方の鉄芯の全て
の吸着面とコイル取付け部との間にそれぞれ感温磁性材
を設けたことを特徴とする制御棒保持機構用の自己作動
型電磁石。 2、一方の鉄芯は円柱体の中央を切り欠いた全体をほぼ
U字型の構造とし、その両脚部にそれぞれコイルを巻装
し、両コイル取付け部と両吸着面との間に感温磁性材を
設け、アーマチュアとなる他方の鉄芯は円板状をなして
いる請求項1記載の自己作動型電磁石。
[Claims] 1. Equipped with an iron core and a coil with a structure that can be divided into two, a temperature-sensitive magnetic material is incorporated into a part of the iron core, and control is achieved by attracting and separating the two iron cores according to the ambient temperature. A control rod holding mechanism for an electromagnet for holding and separating rods, characterized in that a temperature-sensitive magnetic material is provided between all adsorption surfaces of the iron core on which the coil is attached and the coil attachment part. Self-actuated electromagnet. 2. One of the iron cores has a roughly U-shaped structure, with the center of the cylindrical body cut out, and coils are wound around each of its legs, and a temperature-sensitive sensor is installed between both coil attachment parts and both adsorption surfaces. 2. A self-actuating electromagnet according to claim 1, wherein a magnetic material is provided and the other iron core serving as the armature has a disk shape.
JP63212114A 1988-08-26 1988-08-26 Self-actuation type electromagnet for control rod holding mechanism Granted JPH0261593A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63212114A JPH0261593A (en) 1988-08-26 1988-08-26 Self-actuation type electromagnet for control rod holding mechanism

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63212114A JPH0261593A (en) 1988-08-26 1988-08-26 Self-actuation type electromagnet for control rod holding mechanism

Publications (2)

Publication Number Publication Date
JPH0261593A true JPH0261593A (en) 1990-03-01
JPH0559400B2 JPH0559400B2 (en) 1993-08-30

Family

ID=16617109

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63212114A Granted JPH0261593A (en) 1988-08-26 1988-08-26 Self-actuation type electromagnet for control rod holding mechanism

Country Status (1)

Country Link
JP (1) JPH0261593A (en)

Also Published As

Publication number Publication date
JPH0559400B2 (en) 1993-08-30

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