JPS608778A - Nuclear fusion device - Google Patents

Nuclear fusion device

Info

Publication number
JPS608778A
JPS608778A JP58115932A JP11593283A JPS608778A JP S608778 A JPS608778 A JP S608778A JP 58115932 A JP58115932 A JP 58115932A JP 11593283 A JP11593283 A JP 11593283A JP S608778 A JPS608778 A JP S608778A
Authority
JP
Japan
Prior art keywords
magnetic field
field coil
fusion device
nuclear fusion
coil
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
JP58115932A
Other languages
Japanese (ja)
Inventor
石塚 達郎
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 JP58115932A priority Critical patent/JPS608778A/en
Publication of JPS608778A publication Critical patent/JPS608778A/en
Pending legal-status Critical Current

Links

Classifications

    • Y—GENERAL 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
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E30/00—Energy generation of nuclear origin
    • Y02E30/10—Nuclear fusion reactors

Landscapes

  • Discharge Heating (AREA)
  • Lining Or Joining Of Plastics Or The Like (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〕 本発明は核融合装置に係シ、特にドーナツ状の真空容器
に沿って配置され、真空容器に直接支持されるボロイダ
ル磁場コイルを、vmえた核融合装置に閏する。
[Detailed Description of the Invention] [Field of Application of the Invention] The present invention relates to a nuclear fusion device, and in particular, a voloidal magnetic field coil disposed along a donut-shaped vacuum vessel and directly supported by the vacuum vessel. Leap into the fusion device.

〔発明の背景〕[Background of the invention]

核融合装置は磁場を用いて真空容器内部に高温プラズマ
を容器壁面から離してW]じ込めるもので、トーラス型
核融合装置においては、この磁場の壁を作るために高磁
場を発生するトロイダル磁場コイル、及び高温プラズマ
の安定保持、あるいは位置制御のためのポロイダル磁場
コイルを備えている。このトロイダル、及びボロイダル
磁場コイルを備えている核融合装置の概略を第1図、及
び第2図に示す。
Nuclear fusion devices use a magnetic field to trap high-temperature plasma inside a vacuum container, separating it from the container wall. In torus-type fusion devices, a toroidal magnetic field that generates a high magnetic field is used to create a wall of this magnetic field. It is equipped with a poloidal magnetic field coil for stable maintenance of high-temperature plasma or position control. The outline of a nuclear fusion device equipped with this toroidal and voloidal magnetic field coil is shown in FIGS. 1 and 2.

読図において、2は厚肉部3とベローズ4を交互に配置
してほぼドーナツ状に形成される真壁容器で、その内部
にはプラズマ1が閉じ込められる。
In the drawing, reference numeral 2 denotes a solid-walled container formed into a substantially doughnut-like shape by alternately arranging thick-walled portions 3 and bellows 4, and plasma 1 is confined inside the container.

トロイダル磁場コイル5は真空容器2を取り囲み、かつ
、トーラス周方向に所定間隔をもって複数個配置されて
いる。一方、ポロイダル磁場コイル6は、真空容器2と
トロイダル磁場コイル5との間に、真空容器2に沿って
配置されている。伺、8は真空容器2内を真空排気する
真空排気装置、9はトロイダル磁場コイル5をサポート
を介して支持する上、下架台である。
A plurality of toroidal magnetic field coils 5 surround the vacuum vessel 2 and are arranged at predetermined intervals in the circumferential direction of the torus. On the other hand, the poloidal magnetic field coil 6 is disposed along the vacuum vessel 2 between the vacuum vessel 2 and the toroidal magnetic field coil 5. 8 is a vacuum evacuation device for evacuating the inside of the vacuum container 2, and 9 is an upper and lower pedestal that supports the toroidal magnetic field coil 5 via a support.

このように構成される核融合装置において、ポロイダル
磁場コイル6は、真空容器2内のプラズマ1に磁場を印
加しなければならないので、真空容器2からできる限シ
小さな距離をもって設置される方が、プラズマ1との結
合性の面でも、ポロイダル磁場コイル6の電源容量の面
でも、更には限られた空間を節約する面でも有利である
。このため、通常、ポロイダル磁場コイル6は、第3図
、及び第4図に示す如く真空容器2の外壁に直接取付け
られておシ、第5図にその取付構造の詳細を示す如く、
ポロイダル磁場コイル6は、トーラス周方向の所定位置
で支持部材12によシ真空容器2に固定的に支持されて
いる。
In the nuclear fusion device configured in this way, the poloidal magnetic field coil 6 must apply a magnetic field to the plasma 1 in the vacuum vessel 2, so it is better to install it at the smallest possible distance from the vacuum vessel 2. This is advantageous in terms of coupling with the plasma 1, power capacity of the poloidal magnetic field coil 6, and saving limited space. For this reason, the poloidal magnetic field coil 6 is normally attached directly to the outer wall of the vacuum vessel 2 as shown in FIGS. 3 and 4, and the details of the mounting structure are shown in FIG.
The poloidal magnetic field coil 6 is fixedly supported on the vacuum vessel 2 by a support member 12 at a predetermined position in the circumferential direction of the torus.

しかしながら、従来のこのような構成だと、ベーキング
等によシ真空容器2が昇温すると、この真空容器2は第
6図に示す様に実線から点線の状態に変形してしまう。
However, with such a conventional structure, when the temperature of the vacuum container 2 increases due to baking or the like, the vacuum container 2 deforms from the solid line to the dotted line as shown in FIG.

これによシボロイダル磁場コイル6の取付点10が11
に移動する。このようにポロイダル磁場コイル6に変形
、変位を生じた場合には、それらの相対変位によシボロ
イダル磁場コイル6に強制変位が加わってしまい、この
時、ポロイダル磁場コイル6に発生する応力、歪が過大
になる恐れがあるという強度の面%、らの問題があった
。
As a result, the attachment point 10 of the Shiboloidal magnetic field coil 6 is set to 11.
Move to. When deformation and displacement occur in the poloidal magnetic field coil 6 in this way, forced displacement is applied to the ciboloidal magnetic field coil 6 due to these relative displacements, and at this time, the stress and strain generated in the poloidal magnetic field coil 6 increase. There was a problem with the strength, which could become excessive.

〔発明の目的〕[Purpose of the invention]

本発明はこれに鑑みなされたもので、その目的とすると
ころは、ポロイダル磁場コイルに作用する真空容器との
相対熱変位が小さな核融合装置を提供するにある。
The present invention has been made in view of this, and its purpose is to provide a nuclear fusion device in which the relative thermal displacement between the poloidal magnetic field coil and the vacuum vessel acting on the poloidal magnetic field coil is small.

〔発明の概要〕[Summary of the invention]

本発明は内部にプラズマを収納するほぼドーナツ状の真
空容器のトーラス周方向に沿って設けられたポロイダル
磁場コイルの電気抵抗を純銅より大きい導体により構成
し、真空容器の昇降温に併せて該コイルを熱膨張させ、
該コイルと真空容器の熱変位差を極小にし、所謂の目的
を達成するように成したものである。
In the present invention, the electric resistance of the poloidal magnetic field coil provided along the circumferential direction of the torus of a nearly donut-shaped vacuum vessel that stores plasma therein is made of a conductor larger than that of pure copper, and the coil thermally expand,
This is designed to minimize the difference in thermal displacement between the coil and the vacuum vessel to achieve the so-called purpose.

本発明の詳細な説明する。各記号をそれぞれΔRv真空
容器の主半径方向熱変位 ΔRcコイルの主半径方向熱変位 Δtv真空容器の昇温温度 Δtcコイルの昇温温度 Rv 真空容器の着目点の主半径 FLc コイルの着目点の主半径 αV、真空容器の線膨張率 αCコイルの線膨張率 とする。
The present invention will be described in detail. Each symbol is ΔRv Main radial thermal displacement of the vacuum vessel ΔRc Main radial thermal displacement of the coil Δtv Temperature rise of the vacuum vessel Δtc Temperature rise of the coil Rv Main radius of the point of interest of the vacuum vessel FLc Main of the point of interest of the coil The radius αV is the linear expansion coefficient of the vacuum vessel and the linear expansion coefficient αC of the coil.

真空容器2の昇温時に発生するポロイダル磁場コイル6
の熱応力は、両者間の変位差に起因する。
Poloidal magnetic field coil 6 generated when the temperature of the vacuum container 2 increases
The thermal stress of is caused by the displacement difference between the two.

ここで、それぞれのトーラス主半径方向変位は、ΔRv
−Δtv−L(v・αV ΔRc−Δtc−ルc・αC で記述されるので、 Rv=Rc とすれば、変位差ΔRは ΔR−ΔRv−ΔELc =(Δtv(Iv−Δtcαc ) Rvとなり、ポロ
イダル磁場コイル6の熱応力を小さくするにはΔtvα
VとΔtcαCを極力等しくすればよいことがわかる。
Here, each torus principal radial displacement is ΔRv
-Δtv-L(v・αV ΔRc−Δtc−ruc・αC, so if Rv=Rc, the displacement difference ΔR becomes ΔR−ΔRv−ΔELc=(Δtv(Iv−Δtcαc) Rv, which is a poloidal To reduce the thermal stress of the magnetic field coil 6, Δtvα
It can be seen that V and ΔtcαC should be made as equal as possible.

このためには、真空容器2とポロイダル磁場コイル6の
線膨張係数を一致させることと、両者の温度を等しくす
ることが、最も効果的でちる。
For this purpose, it is most effective to match the coefficients of linear expansion of the vacuum vessel 2 and the poloidal magnetic field coil 6, and to equalize their temperatures.

本発明は、この点に着目しなされたものである。The present invention has been made with this point in mind.

真空容器2に取付けられたポロイダル磁場コイル6が、
真空容器2と一体に十分に保温されているとすれば、真
空容器2のベーキング時には、真空容器からの熱伝導に
よシ両者の温度は等しくなるので、線膨張係数をほぼ等
しくすることで、ポロイダル磁場コイル6には、応力が
ほとんど発生せず、良好な核融合装置が得られる。
The poloidal magnetic field coil 6 attached to the vacuum container 2 is
Assuming that the vacuum container 2 and the vacuum container 2 are sufficiently heat-insulated, when the vacuum container 2 is baked, the temperature of both will be equal due to heat conduction from the vacuum container, so by making the coefficients of linear expansion approximately equal, Almost no stress is generated in the poloidal magnetic field coil 6, and a good nuclear fusion device can be obtained.

一方、ポロイダル磁場コイル6の保温が十分でない場合
には、真空容器からの熱伝導によるポロイダル磁場コイ
ル6の加熱は期待できないのでコイル自体に通電するこ
とにより昇温させることか、必要である。
On the other hand, if the heat retention of the poloidal magnetic field coil 6 is insufficient, heating of the poloidal magnetic field coil 6 by heat conduction from the vacuum container cannot be expected, so it is necessary to raise the temperature by energizing the coil itself.

ところが、通常の真空容器2のベーキングによる昇温は
、100C以上であるので、従来の様な銅導体を用いた
ボロイダル磁場コイルでは、大電流を長時間流さない限
シ、目的を達成できない。
However, since the temperature rise due to normal baking of the vacuum container 2 is 100 C or more, a conventional voloidal magnetic field coil using a copper conductor cannot achieve its purpose unless a large current is passed for a long time.

これは、前記コイルの従来の設計思想が、ジュール損を
小さくすることにあったためである。
This is because the conventional design concept of the coil was to reduce Joule loss.

本発明では、ボロイダル磁場コイルを構成する導体に純
銅より電気抵抗の大きな材料を用いているため、従来構
成のコイルと比べ、同じ昇温を得るのに純銅との電気抵
抗比の平方根分の一以下の電流を流せば良く、その分、
発生する電磁力を低減できる。
In the present invention, since a material with higher electrical resistance than pure copper is used for the conductor constituting the voloidal magnetic field coil, compared to the conventionally configured coil, it is necessary to obtain the same temperature rise by only one square root of the electrical resistance ratio with pure copper. All you need to do is to flow the following current, and by that amount,
The electromagnetic force generated can be reduced.

例えば、真空容器およびボロイダル磁場コイルが5US
304で構成されている場合、電気抵抗は、電気銅の約
35倍であるので、通電昇温させる場合のコイル電流は
、従来の銅コイルの場合に比べ約1/6で済む。
For example, if the vacuum vessel and voloidal magnetic field coil are 5US
304, the electrical resistance is about 35 times that of electrolytic copper, so the coil current when energized and heated is about 1/6 of that of a conventional copper coil.

〔発明の効果〕〔Effect of the invention〕

以上説明した本発明の核融合装置によれば、ドーナツ状
の真空容器のトーラス周方向に沿って設けられたボロイ
ダル磁場コイルの熱変位の小さな核融合装置を得ること
ができる。
According to the nuclear fusion device of the present invention described above, it is possible to obtain a nuclear fusion device in which the thermal displacement of the voloidal magnetic field coil provided along the circumferential direction of the torus of the donut-shaped vacuum container is small.

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

第1図はトーラス型核融合装置の概略を一部断面して示
す平面図、第2図はそのA−A断面図、第3図はボロイ
ダル磁場コイルを11mえた真空容器の平面図、第4図
はそのB−B断面図、第5図は従来のボロイダル磁場コ
イルの取付状態を示す真空容器の断面図、第6図はその
変位後の状態を示す図である。 1・・・プラズマ、2・・・真空容器、5・・・トロイ
ダル磁第 I 図 第 2 図 第 3 図 第 4 図 第5図 幣 611
Figure 1 is a partially sectional plan view of a torus-type fusion device, Figure 2 is a sectional view taken along line A-A, Figure 3 is a plan view of a vacuum vessel with a voloidal magnetic field coil placed 11 meters away, and Figure 4 The figure is a cross-sectional view taken along line BB, FIG. 5 is a cross-sectional view of the vacuum container showing the state in which a conventional voloidal magnetic field coil is attached, and FIG. 6 is a view showing the state after displacement. 1... Plasma, 2... Vacuum vessel, 5... Toroidal magnetism Figure I Figure 2 Figure 3 Figure 4 Figure 5 611

Claims (1)

【特許請求の範囲】 1、内部にプラズマを収納するほぼドーナツ状の真空容
器と、該真空容器を取シ囲み、かつ、トーラス周方向に
所定間隔をもって複数個配置されたトロイダル磁場コイ
ルと、前記真空容器のトーラス周方向に沿って設けられ
たポロイダル磁場コイルとを備えた核融合装置において
、前記ボロイダル磁場コイルは、純銅より覗気抵抗が大
きい導体を用いて構成されていることを特徴とする核融
合装置。 2、前記ボロイダル@楊コイルの導体は、前記真空容器
を構成している材料とほぼ等しい線膨張係数を有してい
ることを特徴とする特許請求の範囲第1項記載の核融合
装置。
[Scope of Claims] 1. A substantially donut-shaped vacuum container containing plasma therein, a plurality of toroidal magnetic field coils surrounding the vacuum container and arranged at predetermined intervals in the circumferential direction of the torus; A nuclear fusion device comprising a poloidal magnetic field coil provided along the circumferential direction of a torus of a vacuum vessel, characterized in that the voloidal magnetic field coil is constructed using a conductor having a higher resistance to peeking than pure copper. Nuclear fusion device. 2. The nuclear fusion device according to claim 1, wherein the conductor of the voloidal @Yang coil has a linear expansion coefficient substantially equal to that of the material constituting the vacuum vessel.
JP58115932A 1983-06-29 1983-06-29 Nuclear fusion device Pending JPS608778A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58115932A JPS608778A (en) 1983-06-29 1983-06-29 Nuclear fusion device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58115932A JPS608778A (en) 1983-06-29 1983-06-29 Nuclear fusion device

Publications (1)

Publication Number Publication Date
JPS608778A true JPS608778A (en) 1985-01-17

Family

ID=14674752

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58115932A Pending JPS608778A (en) 1983-06-29 1983-06-29 Nuclear fusion device

Country Status (1)

Country Link
JP (1) JPS608778A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20190046627A (en) 2017-10-25 2019-05-07 유하미카쿠토 가부시키가이샤 Croquette-like snacks

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20190046627A (en) 2017-10-25 2019-05-07 유하미카쿠토 가부시키가이샤 Croquette-like snacks
KR20200071723A (en) 2017-10-25 2020-06-19 유하미카쿠토 가부시키가이샤 Snack sweets of croquette style

Similar Documents

Publication Publication Date Title
JPS61113218A (en) Superconductive magnet
JPS6362138A (en) Deflection yoke for oscilloscope with heat radiation mechanism
FR2592745B1 (en) STATOR WITH SUPERPHOTOUS THREE PHASE WINDINGS
US4430600A (en) Modular low aspect ratio-high beta torsatron
JPH0622965Y2 (en) Superconducting coil device
JPS6119089B2 (en)
JPS608390Y2 (en) heating device
JPH02108998A (en) Heat-resisting driving coil and control rod driving device
JP3294068B2 (en) High temperature operation type battery with heat conduction plate
JP2739159B2 (en) Toroidal magnet
JPS6032149B2 (en) nuclear fusion device
JPS6119091B2 (en)
JPS6222117B2 (en)
JPH0458190A (en) Electromagnetic force support device
JPS6028102Y2 (en) Superconducting toroidal magnetic field device
JPS58186914A (en) Superconductive magnet apparatus
JPS633275B2 (en)
JPS59114499A (en) Heat transfer flow simulation testing device of reactor core
JP3068922B2 (en) Superconducting magnet
JPS62183503A (en) Very low temperature container
JPS5913718B2 (en) Fusion device upper mount
JPS61102584A (en) Torus type fusion device
JPS5946577A (en) Coil in vacuum vessel for nuclear fusion device
JP2000188215A (en) Radiation shield plate
JPS6078382A (en) Tokamak type nuclear fusion device