JPS5942484A - Nuclear fusion device - Google Patents
Nuclear fusion deviceInfo
- Publication number
- JPS5942484A JPS5942484A JP57152513A JP15251382A JPS5942484A JP S5942484 A JPS5942484 A JP S5942484A JP 57152513 A JP57152513 A JP 57152513A JP 15251382 A JP15251382 A JP 15251382A JP S5942484 A JPS5942484 A JP S5942484A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- voloidal
- fusion device
- stepped part
- field 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.)
- Granted
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
- Plasma Technology (AREA)
- Lining Or Joining Of Plastics Or The Like (AREA)
- Discharge Heating (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に係り、特にそのボロイダル磁場コ
イル間の渡り部構造に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a nuclear fusion device, and particularly to a structure of a transition portion between boroidal magnetic field coils.
核融合装置は真空容器内に磁界の壁を作り、この磁界の
壁の内部にプラズマを閉じ込めるもので、この磁界の発
生方式により種々の型がある。例えば、トーラス形核融
合装置では真空容器の周方向に沿ってこれを取り囲むよ
うに巻回配置された複数個のトロイダル磁場コイルによ
り真空容器の周方向に沿う磁界ケ加えて、真空容器内に
プラズマ全閉じ込めているが、さらに真空容器と同心円
状に配置された種々のボロイダル磁場コイルにより円心
磁界を発生させてプラズマの位置などを制御している。A nuclear fusion device creates a magnetic field wall in a vacuum container and confines plasma within the magnetic field wall, and there are various types depending on the method of generating this magnetic field. For example, in a torus-shaped fusion device, a plurality of toroidal magnetic field coils are wound around the vacuum vessel to apply a magnetic field along the circumference of the vacuum vessel, creating a plasma inside the vacuum vessel. Although the plasma is completely confined, various voloidal magnetic field coils placed concentrically with the vacuum vessel generate a circular magnetic field to control the plasma position.
ところで、この種トーラス形核融合装置において小形の
ものでは、第1図に示すように、そのボロイダル磁場コ
イル1が、真空容器2全取り囲むトロイダル磁場コイル
3の外側に配置されているのが普通である。なお図中、
C−C線はトーラス中心を示す。したがって、ボロイダ
ル磁場コ′イル1の占有空間を比較的大きくとることが
できるので、その構造に特別な考慮を払う必要はない。By the way, in a small toroidal fusion device of this type, the voloidal magnetic field coil 1 is usually placed outside the toroidal magnetic field coil 3 that completely surrounds the vacuum vessel 2, as shown in FIG. be. In addition, in the figure,
The C-C line indicates the center of the torus. Therefore, since the voloidal magnetic field coil 1 can occupy a relatively large space, there is no need to pay special consideration to its structure.
しかし、強磁場を発生させる大形の装管ともなると、第
1図に示す様な構造では装置全体が大形化し、構造上お
よび価格面からも得策ではない。However, when it comes to a large tube that generates a strong magnetic field, the structure shown in FIG. 1 increases the size of the entire device, which is not a good idea from both a structural and cost standpoint.
そこで、第2図に示すように、真空容器2とトロイダル
磁場コイル3との間の空間を有効に利用してボロイダル
磁場コイル1i1B、・・・・・・全配置することが行
なわれるが、この様に配置すると、次のような空間上の
問題がある。Therefore, as shown in FIG. 2, the space between the vacuum container 2 and the toroidal magnetic field coil 3 is effectively used to arrange all the voloidal magnetic field coils 1i1B. If they are arranged in the same way, the following spatial problems arise.
すなわち、種々のポロイダル磁場コイルがプラズマ制御
のために磁場分布を考慮し夫々の目的に応じて配置され
ているが、同一種類のポロイダル磁場コイルにおいては
空間の有効利用のために、例えばコイルINからコイル
IBへと順次接続される。第3図はこの接続部分を拡大
して示す斜視図、第4図は第3図のA矢視図である。こ
れらの図からも分るように、各コイルIA、IBの端部
la、lb間を渡り線4で接続する渡り部Xでは、その
他の部分に比べて1タ−y分の高さ寸法りだけ余分な空
間が必要となり、渡り部での電流による不要な磁界を打
ち消すだめの巻戻し線5をも考慮すれば、約2ターン分
の高さ寸法だけ余分な空間が必要となる。すなわち、各
コイル間の渡り部Xではその他の部分よシ少なくとも1
タ一ン分の高さ寸法だけ余分の空間が必要となるためt
真空容器2とトロイダル磁場コイル3との間の狭い空間
にポロイダル磁場コイル1を有効に配置することが困難
で、コイルlによる制御特性が低下するという欠点があ
った。In other words, various poloidal magnetic field coils are arranged according to their respective purposes in consideration of the magnetic field distribution for plasma control, but in order to make effective use of space, in the same type of poloidal magnetic field coils, for example, from coil IN to It is sequentially connected to coil IB. FIG. 3 is an enlarged perspective view of this connecting portion, and FIG. 4 is a view taken along arrow A in FIG. 3. As can be seen from these figures, at the transition section X where the ends la and lb of each coil IA and IB are connected by the crossover wire 4, the height dimension is 1 tera-y compared to the other sections. If the unwinding wire 5 for canceling the unnecessary magnetic field caused by the current at the transition section is also considered, an extra space corresponding to the height of about two turns is required. In other words, at the transition section X between each coil, at least one
Because extra space is required for the height of the tan
It is difficult to effectively arrange the poloidal magnetic field coil 1 in a narrow space between the vacuum vessel 2 and the toroidal magnetic field coil 3, and there is a drawback that the control characteristics by the coil 1 are deteriorated.
本発明の目的は、上記した従来技術の欠点金なくシ、ボ
ロイダル磁場コイル間を接続する渡9部の占有空間全減
少し得る核融合装置を提供することにある。SUMMARY OF THE INVENTION An object of the present invention is to provide a nuclear fusion device that eliminates the drawbacks of the prior art described above and can reduce the total space occupied by the bridge connecting the voloidal magnetic field coils.
この目的を達成するため、本発明は、トロイダル磁場コ
イルのターンに形成された傾斜段落し部の位置において
渡υ線をポロイダル磁場コイルの端部に接続するととも
に、この渡シ線の接続端部における傾斜段落し部に面す
る側を、この傾斜段落し部の傾斜面に沿うデーバー状に
形成し、渡り線を傾斜段落し部とほぼ面一に配置して渡
り線のだめの特別ガ占有空間を不要にしたことを特徴と
する。To achieve this object, the present invention connects a crossing wire to an end of a poloidal magnetic field coil at the position of an inclined step formed in a turn of a toroidal magnetic field coil, and also connects a connecting end of this crossing wire to an end of a poloidal magnetic field coil. The side facing the inclined stepped part is formed in a shape of a debar along the slope of the inclined stepped part, and the crossover wire is arranged almost flush with the inclined stepped part to create a special space occupied by the connecting wire. It is characterized by eliminating the need for
以下、本発明を図示の実施例について説明する。Hereinafter, the present invention will be described with reference to illustrated embodiments.
(75図は本発明の一実施例に係る核融合装置のポロイ
ダル磁場コイルにおける渡り部の斜視図。(Figure 75 is a perspective view of a transition section in a poloidal magnetic field coil of a nuclear fusion device according to an embodiment of the present invention.
第6図は第5図のB矢視図である。これらの図に卦いて
、一方のポロイダル磁場コイルIAの端部1aに一端が
接続された渡り綜4は、他方のポロイダル磁場コイルI
Bのターンに形成された傾斜段落し部6の位置において
、その他端がコイルIBの端部1bに接続されるととも
に、この接続端部における傾斜段落し部6に面する側が
傾斜段落し部6の傾斜面に沿うテーパー状に形成され、
これにより傾斜段落し部6とほぼ面一となるように配置
されている。FIG. 6 is a view taken along arrow B in FIG. In these figures, the crossover heel 4 whose one end is connected to the end 1a of one poloidal magnetic field coil IA is connected to the other poloidal magnetic field coil IA.
At the position of the inclined stepped part 6 formed in the turn B, the other end is connected to the end part 1b of the coil IB, and the side of this connection end facing the inclined stepped part 6 is connected to the inclined stepped part 6. It is formed in a tapered shape along the slope of the
As a result, it is arranged so as to be substantially flush with the inclined stepped part 6.
したがって、従来必要としていた渡9線4のための1タ
一ン分の旨さ寸法の空間が不要となシ。Therefore, there is no longer a need for a space with the size of 1 tanner for 9 wires 4, which was required in the past.
渡り部の占有空間を減少することができる。その結果、
真望容器2とトロイダル磁場コイル3との間の狭い空間
を有効に利用してポロイダル磁場コイル1を配置し、プ
ラズマ領域での不整磁場を極力小さくして制御特性を向
上することが可能となる。The space occupied by the transition section can be reduced. the result,
It becomes possible to arrange the poloidal magnetic field coil 1 by effectively utilizing the narrow space between the maze container 2 and the toroidal magnetic field coil 3, thereby minimizing the irregular magnetic field in the plasma region and improving the control characteristics. .
・!お、渡り部でも電流による不要な磁界を打ち消すた
めに巻戻し線5全設けるのは従来例と同じである。・! Also, as in the conventional example, all unwinding wires 5 are provided in the transition section to cancel out unnecessary magnetic fields caused by current.
第7図は本発明の他の実施例に係る核融合装置のポロイ
ダル磁場コイルにおける渡り部の側面図、第8図は第7
図のD −D断面図である。第5図および第6図の実施
例が同一面上にある各ボロイダル磁場コイル間を接続す
る場合の適用例であるのに対し、この実施例はポロイダ
ル磁場コイルIAとIBが異なる面上に位置し、かつこ
れらコイルIA、IB間に異種のポロイダル磁場コイル
7が介在している場合の適用例である。FIG. 7 is a side view of a transition section in a poloidal magnetic field coil of a nuclear fusion device according to another embodiment of the present invention, and FIG.
It is a sectional view taken along the line D-D in the figure. While the embodiments shown in FIGS. 5 and 6 are application examples for connecting voloidal magnetic field coils on the same plane, this embodiment has poloidal magnetic field coils IA and IB located on different planes. However, this is an application example in which different types of poloidal magnetic field coils 7 are interposed between these coils IA and IB.
この場合においても、渡υ線4を異種のポロイダル磁場
コイル7全跨いで設けるとともに、コイルIA、IBの
各端部1a、lbにそれぞれ接続される渡9線4の両接
続端部を各コイルI A、 IBのターンに形成された
傾斜段落し部6の位置に配置し、かつこの接続端部にお
ける傾斜段落し部6に面する側音傾斜段落し部6の傾斜
面に沿うテーパー状に形成することにより、前記実施例
と同様の効果が得られる。In this case as well, the crossing wire 4 is provided across all of the different types of poloidal magnetic field coils 7, and both connecting ends of the crossing wire 4 connected to the ends 1a and lb of the coils IA and IB are connected to each coil. It is arranged at the position of the inclined stepped part 6 formed in the turns of IA and IB, and is tapered along the slope of the side inclined stepped part 6 facing the inclined stepped part 6 at this connection end. By forming this, the same effects as in the embodiment described above can be obtained.
また、第9図は本発明のさらにfl、!の実施例に係る
核ji;i1合装置6fのボロイダル磁場コイルにおけ
る渡り部の側面図、第10図は第9図のE−E断面図で
ある。この実施例では、渡り線4が傾斜段落し部6の頑
斜介とほぼ直角の方向に延び、さらにこの渡り線4に沿
って巻戻し’、:、!5が並設されているが、ボロイダ
ル磁場コイル111の端部1bと渡り線4との接続構造
は前記実施例と同様である。したがって、この実施例に
おいても、前記実施例と同様な効果が得られる。Moreover, FIG. 9 shows further fl,! of the present invention. FIG. 10 is a side view of the transition portion in the voloidal magnetic field coil of the nuclear ji;i1 combining device 6f according to the embodiment, and FIG. In this embodiment, the connecting wire 4 extends in a direction substantially perpendicular to the oblique cutout of the inclined step section 6, and is further unwound along the connecting wire 4', :,! 5 are arranged in parallel, but the connection structure between the end portion 1b of the voloidal magnetic field coil 111 and the crossover wire 4 is the same as in the previous embodiment. Therefore, in this embodiment as well, the same effects as in the previous embodiment can be obtained.
なお、ボロイダル磁場コイルを真空容器とトロイダル磁
場コイルとの間の狭い空間に配置する場合について述べ
たが1本発明はこれに限らず、小形の核融合装置の様に
ボロイダル磁場コイルを真空容器およびトロイダル磁場
コイルの外側に配置する場合でも、ボロイダル磁場コイ
ルの渡り部の占有空間を小さくしようとするときには、
同様に適用することができる。Although we have described the case in which the voloidal magnetic field coil is placed in a narrow space between the vacuum vessel and the toroidal magnetic field coil, the present invention is not limited to this, and the voloidal magnetic field coil is placed in the vacuum vessel and the toroidal magnetic field coil, such as in a small nuclear fusion device. Even when placed outside the toroidal magnetic field coil, when trying to reduce the space occupied by the transition section of the boroidal magnetic field coil,
The same can be applied.
以上説明したように、本発明によれば、ボロイダル磁場
コイル間を接続する渡9部の占有空間を減少し得るので
、真空容器とトロイダル磁場コイルとの間などの狭い空
間を有効て利用してボロイダル磁場コイルを配置するこ
とができ、ボロイダル磁場コイルによる制御特性を向上
することが可能となる。As explained above, according to the present invention, it is possible to reduce the space occupied by the bridge connecting the voloidal magnetic field coils, so that narrow spaces such as between the vacuum container and the toroidal magnetic field coils can be effectively utilized. A voloidal magnetic field coil can be arranged, and control characteristics by the voloidal magnetic field coil can be improved.
第1図は小形の核融合装置の概略構成を示す断面図、第
2図は大形の核融合装置の概略構成を示す右半部断面図
、第3図は従来のボロイダル磁場コイル間の渡り部を示
す斜視図、第4図は第3図のA矢視図、第5図〜第10
図は本発明の各実施例に係るボロイダル磁場コイル間の
渡り部を示すもので、第5図は斜視図、第6図は第5図
のB矢視図、第7図は側面図、第8図は第7図のD −
1)断面図、第9図は側面図、第10図は第9図のE−
E断面図である。Figure 1 is a cross-sectional view showing the schematic configuration of a small fusion device, Figure 2 is a cross-sectional view of the right half showing the schematic configuration of a large fusion device, and Figure 3 is a cross-sectional view of a conventional voloidal magnetic field coil. FIG. 4 is a perspective view showing the section, FIG. 4 is a view from arrow A in FIG. 3, and FIGS.
The figures show the transition portion between the voloidal magnetic field coils according to each embodiment of the present invention, and FIG. 5 is a perspective view, FIG. Figure 8 is D- of Figure 7.
1) Cross-sectional view, Figure 9 is a side view, Figure 10 is E- in Figure 9.
It is an E sectional view.
Claims (1)
空容器の周方向に沿って真空容器を取り囲むように巻回
配置された複数個のトロイダル磁場コイルと、前記真空
容器と同心円状に配置された複数個のボロイダル磁場コ
イルとを備え、前記ボロイダル磁場コイルは傾斜段落し
部が形成されたターンを有し、各ボロイダル磁場コイル
間を渡り線により接続した核融合装置において、前記渡
り線を前記傾斜段落し部の位置において前記ボロイダル
磁場コイルの端部に接続するとともに、この渡り線の接
続端部における前記傾斜段落し部に面する側を、この傾
斜段落し部の傾斜面に沿うテーパー状に形成したことを
特徴とする核融合装置。1. An annular vacuum container that stores plasma, a plurality of toroidal magnetic field coils that are wound around the vacuum container along the circumferential direction of the vacuum container, and a plurality of toroidal magnetic field coils that are arranged concentrically with the vacuum container. A nuclear fusion device comprising a plurality of voloidal magnetic field coils, each of which has a turn with an inclined stepped part formed therein, and each of the voloidal magnetic field coils is connected by a crossover wire. It is connected to the end of the voloidal magnetic field coil at the position of the inclined stepped part, and the side of the connecting end of the crossover wire facing the inclined stepped part is tapered along the inclined surface of the inclined stepped part. A nuclear fusion device characterized by being formed.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57152513A JPS5942484A (en) | 1982-09-03 | 1982-09-03 | Nuclear fusion device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57152513A JPS5942484A (en) | 1982-09-03 | 1982-09-03 | Nuclear fusion device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5942484A true JPS5942484A (en) | 1984-03-09 |
JPH0318158B2 JPH0318158B2 (en) | 1991-03-11 |
Family
ID=15542087
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57152513A Granted JPS5942484A (en) | 1982-09-03 | 1982-09-03 | Nuclear fusion device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5942484A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63189002A (en) * | 1987-01-15 | 1988-08-04 | ボール、コーパレイシヤン | Wide band microstrip antenna and manufacture of the same |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS54111597U (en) * | 1978-01-26 | 1979-08-06 |
-
1982
- 1982-09-03 JP JP57152513A patent/JPS5942484A/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS54111597U (en) * | 1978-01-26 | 1979-08-06 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63189002A (en) * | 1987-01-15 | 1988-08-04 | ボール、コーパレイシヤン | Wide band microstrip antenna and manufacture of the same |
Also Published As
Publication number | Publication date |
---|---|
JPH0318158B2 (en) | 1991-03-11 |
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