JPH0318158B2 - - Google Patents

Info

Publication number
JPH0318158B2
JPH0318158B2 JP57152513A JP15251382A JPH0318158B2 JP H0318158 B2 JPH0318158 B2 JP H0318158B2 JP 57152513 A JP57152513 A JP 57152513A JP 15251382 A JP15251382 A JP 15251382A JP H0318158 B2 JPH0318158 B2 JP H0318158B2
Authority
JP
Japan
Prior art keywords
magnetic field
slope
field coil
poloidal magnetic
poloidal
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.)
Expired - Lifetime
Application number
JP57152513A
Other languages
Japanese (ja)
Other versions
JPS5942484A (en
Inventor
Hiroyuki Kamya
Yosuke Shimanuki
Takashi Shibata
Tsutomu Kanari
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 JP57152513A priority Critical patent/JPS5942484A/en
Publication of JPS5942484A publication Critical patent/JPS5942484A/en
Publication of JPH0318158B2 publication Critical patent/JPH0318158B2/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

  • Discharge Heating (AREA)
  • Lining Or Joining Of Plastics Or The Like (AREA)
  • Plasma Technology (AREA)

Description

【発明の詳細な説明】 本発明は核融合装置に係り、特にそのポロイダ
ル磁場コイル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 of a poloidal magnetic field coil.

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
方向に沿つ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を加えて、真空容器内にプラ
ズマを閉じ込めているが、さらに真空容器と同心
円状に配置された種々のポ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 magnetic field is applied along the circumferential direction of the vacuum vessel using multiple toroidal magnetic field coils wound around the vacuum vessel to generate plasma inside the vacuum vessel. In addition, various poloidal magnetic field coils arranged concentrically with the vacuum vessel generate a circular magnetic field to control the position of the plasma.

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、そのポ
ロイダル磁場コイル1が、真空容器2を取り囲む
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。したがつて、ポ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 poloidal magnetic field coil 1 is usually placed outside the toroidal magnetic field coil 3 surrounding the vacuum vessel 2, as shown in FIG. be. Note that in the figure, the line CC indicates the center of the torus. Therefore, since the space occupied by the poloidal magnetic field coil 1 can be relatively large, 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置ともな
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。
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との間の空気間を有効に利用
してポロイダル磁場コイル1A,1B,…を配置
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。
However, when it comes to a large-sized device 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.
Therefore, as shown in FIG. 2, poloidal magnetic field coils 1A, 1B, etc. are arranged by effectively utilizing the air space between the vacuum container 2 and the toroidal magnetic field coil 3. When placed,
There are the following spatial problems:

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1Aから1B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、同一水平面上に配されている2個
のコイル1A,1Bの端部1a,1b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ターン分の高さ寸法hだけ余分な空間が必要
となり、渡り部では電流による不要な磁界を打ち
消すための巻戻し線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
より少なくとも1ターン分の高さ寸法だけ余分の
空間が必要となるため、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
1による制御特性が低下するという欠点があつ
た。
In other words, various poloidal magnetic field coils are arranged according to their respective purposes in consideration of magnetic field distribution for plasma control, but in order to effectively utilize the space in the same type of poloidal magnetic field coils,
For example, the coils 1A to 1B are connected in sequence.
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 part X where the ends 1a and 1b of the two coils 1A and 1B arranged on the same horizontal plane are connected by the crossover wire 4, compared to other parts, An extra space corresponding to the height h for one turn is required, and if the unwinding wire 5 for canceling unnecessary magnetic fields due to current at the transition section is also taken into consideration, an extra space equal to the height dimension equivalent to approximately 2 turns is required. Is required. In other words, the transition part X between each coil requires an extra space with a height of at least one turn compared to other parts, so the poloidal magnetic field coil is installed in the narrow space between the vacuum vessel 2 and the toroidal magnetic field coil 3. 1 is difficult to effectively arrange, and the control characteristics of the coil 1 are deteriorated.

本発明の目的は、上記した従来技術の欠点をな
くし、同一水平面上に配されているポロイダル磁
場コイル相互間を接続する渡り部の占有空間を減
少し得る核融合装置を提供することにある。
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 space occupied by the transition section that connects poloidal magnetic field coils arranged on the same horizontal plane.

この目的を達成するため、同一水平面上に配さ
れている2個のポロイダル磁場コイルの一方に傾
斜断落し部が形成され、他方のポロイダル磁場コ
イルと前記一方のポロイダル磁場コイルを接続す
る渡り線の端部が前記傾斜断落し部の傾斜面に対
向するよう配されていると共に、前記渡り線にお
ける前記傾斜断落し部の傾斜面に対向する部位
に、前記傾斜落し部の傾斜面に沿う傾斜面が形成
されていることを特徴とする。
In order to achieve this purpose, a slope cutout is formed in one of the two poloidal magnetic field coils arranged on the same horizontal plane, and a crossover wire connecting the other poloidal magnetic field coil and the one poloidal magnetic field coil is formed. An inclined surface along the inclined surface of the inclined cut-off part is disposed such that an end thereof faces the slope of the inclined cut-off part, and a slope surface along the slope of the inclined cut-off part is provided at a portion of the crossover line that faces the slope of the inclined cut-off part. It is characterized by the formation of

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.

第5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、
第6図は第5図のB矢視図である。これらの図に
おいて、一方のポロイダル磁場コイル1Aの端部
1aに一端が接続された渡り線4は、他方のポロ
イダル磁場コイル1B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1
B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. 5 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;
FIG. 6 is a view taken along arrow B in FIG. In these figures, the crossover wire 4, one end of which is connected to the end 1a of one poloidal magnetic field coil 1A, has its other end connected to the inclined stepped portion 6 formed in the turn of the other poloidal magnetic field coil 1B. coil 1
B, and the side of this connection end facing the inclined stepped section 6 is formed in a tapered shape along the inclined surface of the inclined stepped section 6, so that it is almost connected to the inclined stepped section 6. They are arranged so that they are flush.

したがつて、従来必要としていた渡り線4のた
めの1ターン分の高さ寸法の空間が不要となり、
渡り部の占有空間を減少することができる。その
結果、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。
Therefore, the space with the height of one turn for the crossover wire 4, which was conventionally required, is no longer required.
The space occupied by the transition section can be reduced. As a result, it is possible to effectively utilize the narrow space between the vacuum vessel 2 and the toroidal magnetic field coil 3 to arrange the poloidal magnetic field coil 1, thereby minimizing the irregular magnetic field in the plasma region and improving control characteristics. becomes.

なお、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を設けるのは従来例と同じ
である。
Note that, as in the conventional example, the unwinding wire 5 is also provided at the transition portion in order to cancel out unnecessary magnetic fields caused by the current.

なお、ポ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、本発明はこれに限らず、小
形の核融合装置の様にポ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、ポ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 the case has been described in which the poloidal 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 poloidal 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 the present invention is arranged outside the toroidal magnetic field coil, it can be similarly applied when trying to reduce the space occupied by the transition portion of the poloidal magnetic field coil.

以上説明したように、本発明によれば、ポロイ
ダル磁場コイル間を接続する渡り部を占有空間を
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に利用してポロイ
ダル磁場コイルを配置することができ、ポロイダ
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 transition portion connecting between the poloidal magnetic field coils, so that the poloidal magnetic field coils can be A magnetic field coil can be arranged, and control characteristics by the poloidal magnetic field coil can be improved.

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

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図は従来のポロイダル磁場
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6図は本発明の各実施例
に係るポ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
図である。 1A,1B……ポロイダル磁場コイル、1a,
1b……コイル端部、4……渡り線、6……傾斜
段落し部。
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 poloidal magnetic field coil. FIG. 4 is a perspective view showing the A section in FIG. 3, and FIGS. is a perspective view, and FIG. 6 is a view taken along arrow B in FIG. 1A, 1B... Poloidal magnetic field coil, 1a,
1b... Coil end, 4... Crossover wire, 6... Inclined step part.

Claims (1)

【特許請求の範囲】 1 プラズマを収納する円環状の真空容器と、該
真空容器と同心円状に配されている複数のポロイ
ダル磁場コイルを備えている該融合装置におい
て、 複数の前記ポロイダル磁場コイルのうち、同一
水平面上に配されているいずれか2個のポロイダ
ル磁場コイルの少なくとも一方に傾斜断落し部が
形成され、 他方のポロイダル磁場コイルと一方のポロイダ
ル磁場コイルを接続する渡り線の端部が前記傾斜
断落し部の傾斜面に対向するよう配されていると
共に、前記渡り線における前記傾斜断落し部の傾
斜面に対向する部位に、前記傾斜断落し部の傾斜
面に沿う傾斜面が形成されていることを特徴とす
る核融合装置。
[Scope of Claims] 1. The fusion device includes an annular vacuum vessel containing plasma and a plurality of poloidal magnetic field coils arranged concentrically with the vacuum vessel, comprising: Among them, at least one of the two poloidal magnetic field coils arranged on the same horizontal plane is formed with an inclined cut-off part, and the end of the crossover wire connecting the other poloidal magnetic field coil and one poloidal magnetic field coil is Arranged to face the slope of the slope cut-off part, and forming an inclined surface along the slope of the slope cut-off part at a portion of the crossover wire that faces the slope of the slope cut-off part. A nuclear fusion device characterized by:
JP57152513A 1982-09-03 1982-09-03 Nuclear fusion device Granted JPS5942484A (en)

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 JPS5942484A (en) 1984-03-09
JPH0318158B2 true 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)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4835538A (en) * 1987-01-15 1989-05-30 Ball Corporation Three resonator parasitically coupled microstrip antenna array element

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54111597U (en) * 1978-01-26 1979-08-06

Also Published As

Publication number Publication date
JPS5942484A (en) 1984-03-09

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