JPS6080787A - Torus-shaped fusion device - Google Patents

Torus-shaped fusion device

Info

Publication number
JPS6080787A
JPS6080787A JP58188302A JP18830283A JPS6080787A JP S6080787 A JPS6080787 A JP S6080787A JP 58188302 A JP58188302 A JP 58188302A JP 18830283 A JP18830283 A JP 18830283A JP S6080787 A JPS6080787 A JP S6080787A
Authority
JP
Japan
Prior art keywords
plasma
magnetic field
radiation shield
coil
torus
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
JP58188302A
Other languages
Japanese (ja)
Other versions
JPH0472199B2 (en
Inventor
進 佐藤
井村 泰也
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
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP58188302A priority Critical patent/JPS6080787A/en
Publication of JPS6080787A publication Critical patent/JPS6080787A/en
Publication of JPH0472199B2 publication Critical patent/JPH0472199B2/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

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  • 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】 〔発明の利用分野〕 本発明はプラズマ容器内にプラズマを閉じ込めるトロイ
ダル磁場コイルを超電導コイルで414成するようにし
たトーラス形核融合盛kK関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a toroidal fusion stack kK in which a toroidal magnetic field coil for confining plasma in a plasma container is formed of superconducting coils.

〔発明の背景〕[Background of the invention]

第1図は従来のトーラス形核融合装置6.0縦断面図で
ある。超高温のプラズマ1を1イJじ込める円環状のプ
ラズマ容器2は、その内部が高真空状態に保持されてい
る。このプラズマ容器2の外周には、プラズマ閉じ込め
用の磁場を発生する俵数個の常11L導コイルからなる
トロイダル磁場コイル3が、等間隔で、全体としてトー
ラス状となるように配置i(’aれている。これらのト
ロイダル磁場コイル3は上ペース4と下ベース5とによ
って支持され、またプラズマ割出1用の垂直磁場を発生
する内部ボロイダル磁場コイル6および外部ボロイダル
磁場コイル7は、プラズマ容器2とトロイダル蛾場コイ
ル3との間、および架構8の上下にそれぞれ配置され(
いる。また、プラズマ容器2内に閉じ込められたプラズ
マ1を加熱するための変流器コイル9は中央主柱10の
周りに装着されている。
FIG. 1 is a longitudinal sectional view of a conventional torus-shaped fusion device 6.0. An annular plasma container 2 that can contain 1 J of ultra-high temperature plasma 1 is maintained in a high vacuum state inside. Around the outer periphery of this plasma container 2, toroidal magnetic field coils 3 consisting of several 11L conductive coils that generate a magnetic field for plasma confinement are arranged at equal intervals so as to form a torus shape as a whole. These toroidal magnetic field coils 3 are supported by an upper pace 4 and a lower base 5, and an internal voloidal magnetic field coil 6 and an external voloidal magnetic field coil 7, which generate a vertical magnetic field for plasma indexing 1, are attached to the plasma vessel. 2 and the toroidal moth field coil 3, and above and below the frame 8 (
There is. Further, a current transformer coil 9 for heating the plasma 1 confined within the plasma container 2 is mounted around the central main column 10.

このようにトーラス形核−j合裟直においては、そのト
ロイダル磁場コイルとして、従来は常電導コイルが用い
られていたが、発生させるべきトロイダル磁場の増強と
使用′電力量低減の観点から、最近超畦尋コイルの使用
が望まれている。
In this way, in the torus-shaped core, a normal conducting coil has conventionally been used as the toroidal magnetic field coil, but from the viewpoint of increasing the toroidal magnetic field to be generated and reducing the amount of electric power used, it has recently been It is desired to use a super-furrowed coil.

ところで、トーラス形核融合皺直では削1尼トロイダル
磁場コイルと共にプラズマ答器内のプラズマを制御1−
るボロイダル山場コイルの設置か不ば1欠である。
By the way, in the toroidal fusion reactor, the plasma in the plasma reactor is controlled together with the toroidal magnetic field coil.
The only thing missing is the installation of a boroidal mountain coil.

しかしなから、トロイダル磁場コイルを超市害形にした
場合、この超電導コイルは極低(晶(42°IOであり
、またボロイダル(M Wコイルは常温であり、更に高
真空状態に推持されたプラズマ答器内のプラズマは超高
温であって、11(I記トロイタル脩楊コイルを極低溝
にして超市得状悪を保持するには、如何K 4sシール
ドイト」成をプ鋤9J K行うかが大きな課題で一般に
超′亀7!4装置に用いられる熱輻射シールドは熱バラ
ンスのため熱伝4を率の良い鋼板やアルミ板等が採用さ
れている。しかるにトーラス形核融合装置には前記した
ようにプラズマを1tid (11したり安定化させる
ためのボロイダル磁場コイル群ヲ備えており、これらの
ポロイダルイ1h場コイルにはパルス状通亀を行ない、
これによって発生する磁界をプラズマに作用させる必要
がある。疲って従来一般に採用されている熱伝倫、率の
良い1なわち′屯気伝尋の良好な銅板やアルミ板を使用
する場合には、ボロイダル磁楊コイル忙よる(W界が熱
¥j+’+躬シールド産より遮敵されプラズマに作用し
なくなる。
However, when a toroidal magnetic field coil is made into a superconducting type, this superconducting coil has an extremely low crystalline (42°IO) and a voloidal (MW coil is at room temperature, and is maintained in a high vacuum state). The plasma in the plasma reactor is extremely high temperature, so in order to make the troutal coil into an extremely low groove and keep it in a very poor condition, the plasma in the plasma reactor is extremely hot. This is a major issue, and the thermal radiation shields used in the Super 7!4 device generally use steel plates, aluminum plates, etc. that have a good heat transfer rate for heat balance.However, in the torus-shaped fusion device, As mentioned above, it is equipped with a group of voloidal magnetic field coils to stabilize the plasma, and these poloidal 1h field coils are passed through in a pulsed manner.
It is necessary to cause the magnetic field generated by this to act on the plasma. When using a copper plate or aluminum plate with a good rate of heat conduction, which has been commonly used in the past, it is necessary to use a voloidal magnetic coil (W field is heat conduction). It is shielded from the enemy by the j+'+mugi shield and no longer affects plasma.

つまり市気伝冑、の良い熱輻射シールドを用いた場合に
は、ボロイダル++b k’Jコイルの(lb界によっ
て熱りにA射シールドに両市IAtが発生しこれによる
反抗磁界によってプラズマに作用するtI94界が弱く
なりボロイダル磁場コイルの磁界が有効に作用しない欠
点が生じるものと考えられる。
In other words, when using a thermal radiation shield with good energy transmission, IAt is generated in the A radiation shield due to the heat of the voloidal ++b k'J coil, and the resulting repulsive magnetic field acts on the plasma. This is considered to be a drawback in that the tI94 field becomes weak and the magnetic field of the voloidal magnetic field coil does not work effectively.

〔発ψ」の目的〕[Purpose of emitting ψ]

本発明はこの点VC所みてなされたもので、その目的は
、超’lJf尋トロイダル磁場コイルを極低温状態に1
呆持し、かつボロイダル価場コイルによル発生磁界をプ
ラズマに有効に作用させて、プラズマを安定に制御し得
るトーラス形核融合装飯を提供することにある。
The present invention was made in consideration of this point, and its purpose is to bring an ultra-1Jf toroidal magnetic field coil to an extremely low temperature.
It is an object of the present invention to provide a torus-shaped nuclear fusion device that can stably control a plasma by effectively acting on the plasma with a magnetic field generated by a voloidal field coil.

〔づt勤1明のイ!↓L要 〕 この目的を達成するために本発明は、超lt!、纏トロ
イダルm J19コイルを包囲して設けた熱輻射シール
ドのうち、少1.cくともプラズマK 4.も近接する
熱輻射シールドを電気的高抵抗材で信成したことを特徴
とする。本発明の好猪しい実施の惑4j3?においては
、前記熱輻則シールドを籾数個に分割してボロイダル0
14 %コイルによる渦′v1.流の発生を更に抑制し
、史に分1!r11部分に山7気的絶縁′吻を配置自、
して熱遮蔽する。
[It's the first day of work! ↓L Required] To achieve this purpose, the present invention is extremely useful! Of the heat radiation shield provided surrounding the Toroidal M J19 coil, there is a small amount of 1. c Spider Plasma K 4. Another feature is that the adjacent thermal radiation shield is made of electrically high resistance material. Preferred implementation of the present invention 4j3? In this case, the heat radiation law shield is divided into several grains and the voloidal 0
14% vortex caused by coil'v1. Further suppressing the occurrence of water flow and reducing the number of times in history! A mountain 7 air insulation proboscis is placed on the r11 part.
and heat shield.

〔発明の笑施例)〕[Examples of inventions]

以下、本発明の一実施例を第2 t&1〜第1〜ス1に
ついて詳細VC説明する。なお、これら図中、第1図と
同−右号は同一物または相当物をネオ。
Hereinafter, an embodiment of the present invention will be explained in detail with respect to 2nd t&1 to 1st to s1. In addition, in these figures, the numbers on the right as in Figure 1 indicate the same or equivalent items.

この実施例が第1図の従来例と異なる点は、トロイダル
磁場コイルとして、従来の常電導コイルの代りに、液体
ヘリウムによりイ、超低温に冷却された超電導コイル■
1が用いられ、この超゛屯嚇トロイダル磁場コイル11
を極低温状態に保持するために、超電導トロイダル磁場
コイル11の口径内に円環状の熱輻射シールド管12が
、また超′亀導トロイダル磁塘らコイル11の外方にこ
れを曲むように内側PA輻射シールド筒工3、外側熱輻
射シールド筒14、上11+lI熱輻射シールドリンク
15、下cfil熱幅躬シールドリング16がそれぞれ
設けられ、さらに装胤全体が断熱真空容器17により覆
われて、真空状態に保持されていることである。なお、
容態輻射シールドには冷却管が装着されており、これに
液体窒素を流通させることにより作動される。
The difference between this embodiment and the conventional example shown in Fig. 1 is that the toroidal magnetic field coil is replaced by a superconducting coil cooled to an ultra-low temperature by liquid helium, instead of the conventional normal-conducting coil.
1 is used, and this ultra-thin toroidal magnetic field coil 11
In order to maintain the superconducting toroidal magnetic field coil 11 at an extremely low temperature, an annular thermal radiation shield tube 12 is installed within the diameter of the superconducting toroidal magnetic field coil 11, and an inner PA is installed so as to bend it outward of the superconducting toroidal magnetic field coil 11. A radiation shield tube 3, an outer heat radiation shield tube 14, an upper 11+lI heat radiation shield link 15, and a lower Cfil heat width shield ring 16 are provided, respectively, and the entire equipment is covered with an insulating vacuum container 17 to maintain a vacuum state. It is maintained in In addition,
The radiation shield is equipped with a cooling pipe, and is activated by flowing liquid nitrogen through it.

したがって、装置外部からの熱侵入は断熱具空容器17
により大部分が阻止され、かつ外部から真空容器17の
内抛まで侵入してきた熱や、外部ボロイダル磁場コイル
7および変θ1を器コイル9で発生する熱による輻射熱
は、内側、外側熱輻射シールド筒13 、14および上
側、下側熱幅射シールドリング15 、16により遮断
され、さらに超高温のプラズマlを閉じ込めたプラズマ
容器2や内部ボロイダル磁場コイル6からの輻射熱は熱
輻射シールド管12により遮断されるため、超電導トロ
イダル出湯コイル11は極低温状態に保持されることK
なる。
Therefore, heat intrusion from the outside of the device is prevented by
Most of the heat that has penetrated from the outside to the inside of the vacuum vessel 17 and the radiant heat generated by the external voloidal magnetic field coil 7 and the variable θ1 coil 9 are blocked by the inner and outer heat radiation shield cylinders. 13 , 14 and the upper and lower heat radiation shield rings 15 , 16 , and furthermore, the radiant heat from the plasma container 2 , which confines ultra-high temperature plasma L, and the internal voloidal magnetic field coil 6 is blocked by the heat radiation shield tube 12 . Therefore, the superconducting toroidal tapping coil 11 must be kept at an extremely low temperature.
Become.

また、前記各熱輻射シールドの拐料としては。Also, as a cleaning material for each of the heat radiation shields mentioned above.

′1a気抵抗が高くかつ熱遮蔽が良好な材料、例えばス
テンレス鋼・叡などを用いるのか望ましい。そして、プ
ラズマ容器最も近接して配(hされた熱輻射シールド看
J2は、第3図および第4図に示すようK、トーラス大
径の周方向K aパに分割され、かつ各分割部片12 
a間には合成樹脂1工どの昨気絶縁拐からなる断+mH
形の間隔片18か介挿されている。
It is desirable to use a material with high air resistance and good heat shielding, such as stainless steel or aluminum. As shown in FIGS. 3 and 4, the heat radiation shield J2, which is disposed closest to the plasma vessel, is divided into K and K in the circumferential direction of the large diameter of the torus, and each divided part is 12
Between a and 1, there is a break consisting of a synthetic resin layer and insulation layer + mH.
A shaped spacing piece 18 is inserted.

したがって、谷ホロイダル研場コイル6.7などのfr
R界によって各熱掘射シールドに発生する渦1イimp
、は大11〜in低減され、ポロイタル磁場コイルによ
り発生する磁界をプラズマIK月効に作用させてプラズ
マを安定K ’+ii’l I+T、IIすることがで
きる。
Therefore, the fr of valley holoidal research field coil 6.7 etc.
Vortex 1 imp generated in each thermal excavation shield by R field
, is reduced by 11~in, and the plasma can be stabilized by allowing the magnetic field generated by the poloidal magnetic field coil to act on the plasma IK moon effect.

〔発明の効果〕〔Effect of the invention〕

以上説明したように1本発明によ4は、トロイダル磁場
コイルとして超電導コイルを用いるにもかかわらず、こ
れを極低温状iff保持し、かつボロイダルh!t ’
4コイルで発生ずる磁界をノ°ラズマに有効に作用させ
てプラズマを安定に制(tll ’することができる。
As explained above, according to the present invention, the fourth aspect of the present invention is that although a superconducting coil is used as the toroidal magnetic field coil, it can be maintained at an extremely low temperature (if), and the voloidal h! t'
Plasma can be stably controlled (tll') by effectively applying the magnetic field generated by the four coils to the no-lasma.

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

第1図は従来のトーラス形核融合装置の縦〜[開園、第
2図は本発明の一実施例に係るトーラス形核融合装を奸
の縦1θr而図、第3図は熱輻射シールド管の平面図、
第4図ラス第3図のA部拡大図である。 2・・・・・・プラズマu 6% 6,7・・・・・・
ボロイダル磁場コイル% 11・・・・・・超電導トロ
イダル磁場コイル、12〜16・・・・・・mb II
MIl射シールド。 第1 店 第2図 16 5 / 第3図
Figure 1 shows a vertical view of a conventional torus-shaped fusion device [opening], Figure 2 shows a vertical 1θr view of a torus-shaped fusion device according to an embodiment of the present invention, and Figure 3 shows a thermal radiation shield tube. plan view of
FIG. 4 is an enlarged view of part A in FIG. 3. 2...Plasma u 6% 6,7...
Voloidal magnetic field coil% 11...Superconducting toroidal magnetic field coil, 12-16...mb II
MIl fire shield. 1st Store Figure 2 16 5 / Figure 3

Claims (1)

【特許請求の範囲】 1、 内部を高真空状fぷに保持された円環状のプラズ
マ容器と、このグラズマ容器内に発生ずるプラズマを閉
じ込める超電導トロイダル磁場コイルと、前記プラズマ
を制@1¥るボロイダル磁場コイルとを備えたものにお
いて、前記トロイダル磁場コイルを極低温に保持するよ
うにこのトロイダル磁場コイルを包囲する熱輻射シール
ドを設け、この熱輻射シールドのうち、少なくとも前記
プラズマに最も近接する熱幅躬シールドを電気的高抵抗
材で構成したことを特徴とするトーラス形核融合装揃。 2、特許請求の範囲第1.lI′Jにおいて、+iiJ
記プラズマに最も近接する熱輻射シールドは、MiJ記
プラズマ容器を取1+1jんで円環状に形成さね、かつ
l・−ラス太径周方向に沿って俵anfAに分割されて
いることを特徴とするトーラス形核融合装置Q。 3 %許請求の範囲第2項において、前記熱輻躬シール
ドの分割部片間K 電気的絶縁物を配tie、 シて熱
遮蔽したことを特徴とするトーラス形核融合装置4t。
[Claims] 1. An annular plasma vessel whose interior is kept in a high vacuum state, a superconducting toroidal magnetic field coil that confines plasma generated within the plasma vessel, and a voloidal coil that controls the plasma. A thermal radiation shield is provided surrounding the toroidal magnetic field coil so as to maintain the toroidal magnetic field coil at an extremely low temperature, and of the thermal radiation shield, at least a thermal radiation shield closest to the plasma is provided. A set of torus-shaped nuclear fusion equipment characterized by the fact that the shield is made of electrically high resistance material. 2. Scope of Claims No. 1. In lI′J, +iiJ
The thermal radiation shield closest to the plasma is formed into an annular shape by taking 1+1j of the MiJ plasma containers, and is divided into bales anfA along the large diameter circumferential direction. Torus-shaped fusion device Q. 3% The torus-shaped nuclear fusion device 4t according to claim 2, characterized in that an electrical insulator is disposed between the divided parts of the thermal radiation shield to provide thermal shielding.
JP58188302A 1983-10-11 1983-10-11 Torus-shaped fusion device Granted JPS6080787A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58188302A JPS6080787A (en) 1983-10-11 1983-10-11 Torus-shaped fusion device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58188302A JPS6080787A (en) 1983-10-11 1983-10-11 Torus-shaped fusion device

Publications (2)

Publication Number Publication Date
JPS6080787A true JPS6080787A (en) 1985-05-08
JPH0472199B2 JPH0472199B2 (en) 1992-11-17

Family

ID=16221232

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58188302A Granted JPS6080787A (en) 1983-10-11 1983-10-11 Torus-shaped fusion device

Country Status (1)

Country Link
JP (1) JPS6080787A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6395385A (en) * 1986-10-13 1988-04-26 株式会社日立製作所 Shield plate for nuclear fusion device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6395385A (en) * 1986-10-13 1988-04-26 株式会社日立製作所 Shield plate for nuclear fusion device

Also Published As

Publication number Publication date
JPH0472199B2 (en) 1992-11-17

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