JPS6040989A - Magnetic limiter cooling device for fusion device - Google Patents

Magnetic limiter cooling device for fusion device

Info

Publication number
JPS6040989A
JPS6040989A JP58148114A JP14811483A JPS6040989A JP S6040989 A JPS6040989 A JP S6040989A JP 58148114 A JP58148114 A JP 58148114A JP 14811483 A JP14811483 A JP 14811483A JP S6040989 A JPS6040989 A JP S6040989A
Authority
JP
Japan
Prior art keywords
magnetic
cooling
limiter
limiter cooling
vibe
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
JP58148114A
Other languages
Japanese (ja)
Other versions
JPH0114554B2 (en
Inventor
清水 正亜
中村 博雄
桝田 道雄
徹 清水
大和田 公郎
勝利 佐藤
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.)
Hitachi Ltd
Japan Atomic Energy Agency
Original Assignee
Hitachi Ltd
Japan Atomic Energy 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 Hitachi Ltd, Japan Atomic Energy Research Institute filed Critical Hitachi Ltd
Priority to JP58148114A priority Critical patent/JPS6040989A/en
Publication of JPS6040989A publication Critical patent/JPS6040989A/en
Publication of JPH0114554B2 publication Critical patent/JPH0114554B2/ja
Granted legal-status Critical Current

Links

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
    • Y02E30/10Nuclear fusion reactors

Landscapes

  • Plasma Technology (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 本発明は核融合装置用−気IJ 、?ツタ冷却装置に関
する。
[Detailed Description of the Invention] The present invention is for nuclear fusion devices - IJ, ? Regarding ivy cooling equipment.

従来の核融合装置の概要とその間jA点点記第1図〜第
5図基づいて説明する。第1図は七の一部を切り欠いた
核融合装置の平面図、第2図は8i¥1図の■−■町面
図、第3図は真空容器の縦断喝面図である。プラズマ1
を保持するだめの真空容器Zは厚肉部2Aとベローズ都
2Bからなる環状体で、多数のトロイダル磁場コイル3
内に配置され、その内部は真空排気装置4によって真空
にされる。
The outline of a conventional nuclear fusion device will be explained based on the dots jA in FIGS. 1 to 5. Figure 1 is a partially cutaway plan view of the fusion device, Figure 2 is a cross-sectional view of Figure 8i\1, and Figure 3 is a vertical sectional view of the vacuum vessel. plasma 1
The vacuum vessel Z that holds the
The inside thereof is evacuated by a vacuum evacuation device 4.

容器外ボロイダルla場コイルsA、sui’=プラズ
マ中に核状放電電流を発生させる1次巻總の役割を来し
、容器内ボロイダル磁場コイルfiA、6B。
Voloidal la field coils outside the container sA, sui' serve as primary windings to generate a nuclear discharge current in the plasma, and voloidal magnetic field coils inside the container fiA, 6B.

6Cldセパラトリックス磁気面7を作りプラズマ1へ
流入する不純物を外部へ除去する役割を果す。
The 6Cld separatrix creates a magnetic surface 7 and serves to remove impurities flowing into the plasma 1 to the outside.

セパラトリックス磁気面7にはプラズマ1の一部が巻き
付いてくるだめ、セパラトリックス磁気面7の端部は磁
気リミッタ冷却タフ)8A、814に146冷却する必
袂がある。このために磁気リミツク冷却ダク)8A、8
13にはバイブ9A、913によシ冷媒が流される。な
お、10は変流話、IIA。
Because part of the plasma 1 is wrapped around the separatrix magnetic surface 7, it is necessary to cool the ends of the separatrix magnetic surface 7 to the magnetic limiter cooling tough) 8A, 814. For this purpose magnetic limit cooling duct) 8A, 8
13, refrigerant is flowed through the vibrator 9A, 913. In addition, 10 is a strange story, IIA.

1111まペースである。The pace is 1111.

ところで−気リミッタ冷却ダクト8A(8B1μ、第4
図に示す真空容器2の一部切り欠き平面図および第5図
に示すその拡大平面図(第2図の■−v断面に相当)か
ら9」らかなように、それぞn真空容器2のトーラス方
向に所定のピッチで分割されて全周に配置されている。
By the way - air limiter cooling duct 8A (8B1μ, 4th
From the partially cutaway plan view of the vacuum container 2 shown in the figure and the enlarged plan view shown in FIG. They are divided at a predetermined pitch in the torus direction and arranged around the entire circumference.

そしてトーラス方向にlフ■定の間隔をもって磁気リミ
ツク冷却ダクト8Aに結合した供給パイプ9A、 とソ
ノト出パイプ9A2を真空容器2の壁を貫通して外部へ
導出し、このバイア’9A1.9A2を介して磁気リミ
ッタ冷却ダク)8Aに冷緑をUt、すようにしている。
Then, the supply pipe 9A and the output pipe 9A2, which are connected to the magnetic limit cooling duct 8A at a fixed interval in the torus direction, are led out through the wall of the vacuum vessel 2, and the vias 9A1 and 9A2 are connected to the magnetic limit cooling duct 8A. Through the magnetic limiter cooling duct) 8A, cool green is supplied.

しかしこのように冷媒流路をJ、l成すると、真空容器
2と磁気リミッタ冷却ダクト8Aとパイプ9 A+ 。
However, when the refrigerant flow paths are formed into J and L in this way, the vacuum vessel 2, the magnetic limiter cooling duct 8A, and the pipe 9A+ are formed.

9A2とを要素として855図に示ず点A 、 I:3
 、 C。
9A2 as an element, point A, I:3 not shown in the 855 diagram.
,C.

Dを通る電気的な閉回路が構成され、ボロイダル磁場コ
イル5 A 、513 、6 A〜6Cにより発生する
鉛直方向の磁束12がこのi71回路内を通過する。
An electrical closed circuit passing through D is constructed, and the vertical magnetic flux 12 generated by the voloidal magnetic field coils 5A, 513, 6A to 6C passes through this i71 circuit.

このためプラズマ発生時にはこの開回路に起?if力が
生じて循環電流が流れ、この電流とボロイダル磁場との
相互作用により供給バイブ9A1 ど排出パイプ9A、
には過大な電磁力が発生して磁気リミッタ冷却(幾栴を
破壊する危険がある。
For this reason, when plasma is generated, this open circuit occurs? If force is generated, a circulating current flows, and the interaction between this current and the voloidal magnetic field causes the supply vibe 9A1 and the discharge pipe 9A,
There is a danger that excessive electromagnetic force will be generated and destroy the magnetic limiter cooling.

従って本発明の目的は、前記しlこ工うな核1ml侶装
置用磁気リミッタ冷却装置の循狽電6f、の発生を防止
あるいは軽減して磁気リミッタ冷却機構の破壊を防止す
ることにある。
Therefore, an object of the present invention is to prevent or reduce the occurrence of the circulating current 6f in the magnetic limiter cooling device for a 1 ml nuclear device, thereby preventing destruction of the magnetic limiter cooling mechanism.

この目的を達成するため、本発明は、供llSパイプと
排出パイプをボロイダル磁場の磁束の方向に対する直角
方向の位置を等しくして磁気リミッタ冷却ダクトに結合
することによシ、真空容器と磁気リミッタ冷却ダクトと
バイブによる閉回路がボロイダルコイルにより発生する
磁束と交差しないようにして循環電流の発生を防止ある
いは軽減することを特徴とする。
To achieve this objective, the present invention combines the vacuum vessel and the magnetic limiter by connecting the supply pipe and the discharge pipe to the magnetic limiter cooling duct with equal positions perpendicular to the direction of the magnetic flux of the voloidal magnetic field. It is characterized in that the closed circuit formed by the cooling duct and the vibrator does not intersect with the magnetic flux generated by the voloidal coil, thereby preventing or reducing the generation of circulating current.

以下、本発明を白水の実施yIlに基づいて祝り」すゐ
。第6図は磁気リミッタ冷却層11の絃〜r端面図、4
7図は第6図のXU−■断面図で、これらは片側の磁気
リミッタ?tt 7i+1ダクトを示しているが他+1
1ilの磁気リミッタ冷却ダクトも同様に474成され
ん。
Hereinafter, the present invention will be celebrated based on Hakusui's implementation. FIG. 6 is an end view of the magnetic limiter cooling layer 11 from string to r.
Figure 7 is a cross-sectional view of XU-■ in Figure 6. Are these the magnetic limiters on one side? tt 7i+1 duct is shown, but other +1
A 1il magnetic limiter cooling duct is similarly constructed.

磁気リミッタ冷却ダクト13内は仕切疎13 Aによっ
てボロイダル磁場の磁束の流れ方向に区切られて両端部
で連通ずる冷却層13B、13Cが形成される。供に占
バイブ14Aは冷却m131Jに連通し、(ノド出バイ
114Bは冷却層13Cに連通するように磁気リミッタ
冷却メ″クト13に結合される。なおこのとき供給パイ
プ14Aと排出パイプ14Bの位置は、ボロイダル磁場
の磁束の方向に対する直角方向の位置を等しくして、真
空′4器2と磁気リミッタ冷却ダクト13としく給パイ
プ14Aと排出パイプ14Bによっても4成される電気
的な閉回路がボロイダル磁場コイル613等により発生
する磁束と交差しないようにする。
The inside of the magnetic limiter cooling duct 13 is divided by a sparse partition 13A in the flow direction of the magnetic flux of the voloidal magnetic field, and cooling layers 13B and 13C are formed which communicate at both ends. At the same time, the dipping vibrator 14A is connected to the cooling layer 131J, and the throat outlet vibrator 114B is connected to the magnetic limiter cooling member 13 so as to communicate with the cooling layer 13C. In this case, the positions in the direction perpendicular to the direction of the magnetic flux of the voloidal magnetic field are made equal, and an electrical closed circuit is formed by the vacuum unit 2, the magnetic limiter cooling duct 13, the supply pipe 14A, and the discharge pipe 14B. It should not intersect with the magnetic flux generated by the voloidal magnetic field coil 613 or the like.

このようにすることによりbIL給パイプ14Aから冷
却1(1313に供給された冷媒は冷却層13 II内
を分流した後にその両端から冷却層13cにoIL人し
、その駁わト出パイプ1413がら排出ざ7’Lる流路
で流れ磁気リミッタ冷却ダクト13を冷却する。
By doing this, the refrigerant supplied from the bIL supply pipe 14A to the cooling layer 1313 flows through the cooling layer 13 II, flows into the cooling layer 13c from both ends, and is discharged from the outlet pipe 1413. The magnetic limiter cooling duct 13 is cooled by flowing through a flow path extending from 7'L.

そして前記したように真空容器2と磁気リミソク冷却ダ
クト13と供給パイプ14Aと排出パイプ14Bによっ
て構成される電気的141回路がボロイダル磁場コイル
6B等により発生する磁束と交差しないので、プラズマ
発生時に前記閉回路に起蒐力が発生して循@電流が流れ
ることがなく、従って1磁力による磁気リミッタ冷却機
構の破壊を防止することができる。
As described above, the electrical 141 circuit constituted by the vacuum vessel 2, the magnetic rim cooling duct 13, the supply pipe 14A, and the discharge pipe 14B does not intersect with the magnetic flux generated by the voloidal magnetic field coil 6B, etc. No electromotive force is generated in the circuit and no circulating current flows, so it is possible to prevent the magnetic limiter cooling mechanism from being destroyed by a single magnetic force.

以上のように本発明によれば、供給バイブと排出パイプ
をボロイダル磁場の磁束の方向に対する直角方向の位置
を等しくして磁気リミッタ冷却ダクトに結合したことに
より、ボロイダル磁場コイルに、C#)発生する磁束と
の交差tなくシ、プラズマ発生時の循環電流の発生を防
止あるいは軽減したので、磁気リミッタ冷却機構の破壊
を防止することがでさる幼呆がある。
As described above, according to the present invention, the supply vibe and the discharge pipe are connected to the magnetic limiter cooling duct with the same positions perpendicular to the direction of the magnetic flux of the voloidal magnetic field, so that C#) is generated in the voloidal magnetic field coil. Since the generation of circulating current during plasma generation is prevented or reduced without intersecting with the magnetic flux, the magnetic limiter cooling mechanism can be prevented from being destroyed.

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

第1図〜第5図は従来の核融合装置aを示すもので、第
1図はその一部を切り欠い1こ核融合装置の平面図、粥
2図は第1図の■〜11断面図、第3図は真空容器の縦
断端面図、第4図は真壁容Rまの一部切シ欠き平面図、
第5図はその拡大半面図である。第6図およびL+47
図は本発明の一実施νりを示すもので、第6図は核融合
装置4用a気リミツタ冷却装置の縦期端面図、第7図は
七のM[−■断面図である。 13・・・磁気リミッタ冷却ダクト、14A・・・供給
パ第1 図 第3品 第4図 第5図 駆6図 第7図
Figures 1 to 5 show a conventional nuclear fusion device a. Figure 1 is a partially cutaway plan view of the fusion device, and Figure 2 is a cross section from ■ to 11 in Figure 1. Figure 3 is a vertical cross-sectional end view of the vacuum vessel, Figure 4 is a partially cutaway plan view of the true wall volume R,
FIG. 5 is an enlarged half view thereof. Figure 6 and L+47
The figures show one implementation of the present invention; FIG. 6 is a longitudinal end view of the a-air limiter cooling device for the fusion device 4, and FIG. 13... Magnetic limiter cooling duct, 14A... Supply port 1 Figure 3 Product Figure 4 Figure 5 Drive 6 Figure 7

Claims (1)

【特許請求の範囲】[Claims] 1、 プラズマ中の不純物を除去するためのセパラトリ
ックス磁気面の端部に配置される磁気リミッタ冷却ダク
トと、この磁気リミッタ冷力1ダクトに冷媒を流す供給
バイブおよび排出バイブとを備えた核融合装置用磁気リ
ミッタ冷却装置において、前記供給バイブと排出バイブ
全ポロイダル−楊の磁束の方向に対する直角方向の位置
を等しくして前記磁気リミッタ冷却ダクトに結合したこ
とケ特徴とする核融合装置用磁気リミッタ冷却装置。
1. A nuclear fusion device equipped with a magnetic limiter cooling duct placed at the end of the separatrix magnetic surface for removing impurities in the plasma, and a supply vibe and a discharge vibe that flow a coolant through the magnetic limiter cooling force 1 duct. A magnetic limiter cooling device for a nuclear fusion device, characterized in that the supply vibe and the discharge vibe are connected to the magnetic limiter cooling duct with equal positions in a direction perpendicular to the direction of magnetic flux of all poloidal beams. Cooling system.
JP58148114A 1983-08-15 1983-08-15 Magnetic limiter cooling device for fusion device Granted JPS6040989A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58148114A JPS6040989A (en) 1983-08-15 1983-08-15 Magnetic limiter cooling device for fusion device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58148114A JPS6040989A (en) 1983-08-15 1983-08-15 Magnetic limiter cooling device for fusion device

Publications (2)

Publication Number Publication Date
JPS6040989A true JPS6040989A (en) 1985-03-04
JPH0114554B2 JPH0114554B2 (en) 1989-03-13

Family

ID=15445561

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58148114A Granted JPS6040989A (en) 1983-08-15 1983-08-15 Magnetic limiter cooling device for fusion device

Country Status (1)

Country Link
JP (1) JPS6040989A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56160685A (en) * 1980-05-16 1981-12-10 Hitachi Ltd Divertor for nuclear fusion equipment
JPS5777992A (en) * 1980-11-04 1982-05-15 Hitachi Ltd Divertor for nuclear fusion device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56160685A (en) * 1980-05-16 1981-12-10 Hitachi Ltd Divertor for nuclear fusion equipment
JPS5777992A (en) * 1980-11-04 1982-05-15 Hitachi Ltd Divertor for nuclear fusion device

Also Published As

Publication number Publication date
JPH0114554B2 (en) 1989-03-13

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