JPS645443B2 - - Google Patents
Info
- Publication number
- JPS645443B2 JPS645443B2 JP57209343A JP20934382A JPS645443B2 JP S645443 B2 JPS645443 B2 JP S645443B2 JP 57209343 A JP57209343 A JP 57209343A JP 20934382 A JP20934382 A JP 20934382A JP S645443 B2 JPS645443 B2 JP S645443B2
- Authority
- JP
- Japan
- Prior art keywords
- coil
- magnetic field
- coil side
- terminal
- terminal transition
- 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
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
- Magnetic Resonance Imaging Apparatus (AREA)
- Paper (AREA)
- Particle Accelerators (AREA)
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は磁場発生装置に係り、特に磁場によつ
てプラズマを閉じ込める方式の核融合装置に用い
て好適の磁場発生装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a magnetic field generator, and particularly to a magnetic field generator suitable for use in a nuclear fusion device that confines plasma using a magnetic field.
従来のこの種の磁場発生装置は、プラズマに対
しトーラス方向に垂直な磁場を発生させるコイル
を備えており、そのコイルは第1図に示すような
スパイラルコイル、または第3図に示すようなス
リツトコイルが周知である。 Conventional magnetic field generators of this type are equipped with a coil that generates a magnetic field perpendicular to the torus direction of the plasma, and the coil can be a spiral coil as shown in Figure 1 or a slit coil as shown in Figure 3. is well known.
第1図は従来のスパイラルコイルの配置を示す
平面図であり、第2図は第1図のトーラスを示す
断面図である。図に示す如くスパイラルコイル1
及び2は、プラズマ3を封入する真空容器4の外
周面上にトーラス方向に連続して配設され、これ
らのコイル1及び2と前記同様に配設された乱流
加熱コイル5との外側にトロイダルコイル6が設
けられている。尚、符号10及び20は、スパイ
ラルコイル1及び2に電流を供給するためのフイ
ーダであり、またOはトーラス中心を、Tはトー
ラス方向をそれぞれ示す。 FIG. 1 is a plan view showing the arrangement of a conventional spiral coil, and FIG. 2 is a sectional view showing the torus of FIG. 1. Spiral coil 1 as shown in the figure
and 2 are arranged continuously in the torus direction on the outer peripheral surface of the vacuum vessel 4 that encloses the plasma 3, and on the outside of these coils 1 and 2 and the turbulent flow heating coil 5 arranged in the same manner as above. A toroidal coil 6 is provided. Reference numerals 10 and 20 are feeders for supplying current to the spiral coils 1 and 2, O indicates the center of the torus, and T indicates the direction of the torus, respectively.
かかる構成の磁場発生装置によると、スパイラ
ルコイル1及び2がトーラス方向に連続している
ため、これらコイル1及び2をトロイダルコイル
6の内径内に組込むことが難しく、また乱流加熱
コイル5の電流等による漏れ磁場と鎖交するため
大きな電圧がコイル端子間に誘起する欠点があ
る。 According to the magnetic field generator having such a configuration, since the spiral coils 1 and 2 are continuous in the toroidal direction, it is difficult to incorporate these coils 1 and 2 into the inner diameter of the toroidal coil 6, and the current of the turbulent heating coil 5 is There is a drawback that a large voltage is induced between the coil terminals due to linkage with the leakage magnetic field caused by etc.
かかる欠点を解消するものとして、第3図に示
すような磁場発生装置が提供されている。すなわ
ち、この磁場発生装置は、所定の径の半円弧状の
コイル辺70と、これとは異径の小さい半円弧状
のコイル辺71とを各コイル70及び71の端部
にて終端渡り部72及び73をもつて接続して前
記両コイル辺70及び71をほぼ一定間隔で配設
し、該コイル辺70の一部より該コイル辺70及
び71に電流iA,iBを供給するためのフイーダ7
4を設けてなる半円弧状コイル装置7Aと、上記
同様の構成を有する半円弧状コイル装置7Bとが
二個円形になるように組み合せて構成されてい
る。かかる構成を有する磁場発生装置とすれば、
分割可能なので、前記2つの欠点は解消するもの
のトーラス方向に連続ではないため、第4図に示
すように終端渡り部72及び73でトーラス方向
に不連続電流iA及びiBが流れ、プラズマ3に対し
不整磁場Beを発生するという欠点があつた。 In order to overcome this drawback, a magnetic field generator as shown in FIG. 3 has been provided. That is, this magnetic field generating device has a semicircular arc-shaped coil side 70 with a predetermined diameter and a semicircular arc-shaped coil side 71 with a smaller diameter different from the coil side 70 at the ends of each coil 70 and 71. 72 and 73, the coil sides 70 and 71 are arranged at a substantially constant interval, and currents i A and i B are supplied from a part of the coil side 70 to the coil sides 70 and 71. feeder 7
4 and a semicircular arc coil device 7B having the same configuration as described above are combined to form a circular shape. If the magnetic field generator has such a configuration,
Since it can be divided, the above two drawbacks can be solved, but since it is not continuous in the torus direction, discontinuous currents i A and i B flow in the torus direction at the terminal transition parts 72 and 73 as shown in FIG. 4, and the plasma 3 However, it has the disadvantage of generating an asymmetric magnetic field Be.
本発明の目的は、上述した従来技術の欠点を解
消し、トロイダルコイル内径内への組込みを容易
とすると共に、終端渡り部電流に上る不整磁場の
少ない磁場発生装置を提供することにある。
It is an object of the present invention to provide a magnetic field generating device which eliminates the above-mentioned drawbacks of the prior art, which can be easily incorporated into the inner diameter of a toroidal coil, and which generates less irregular magnetic field that increases in the terminal transition portion current.
本発明は、上記目的を達成するため、コイル辺
端部の終端渡り部を重ね合せることにより、不整
磁場の発生を抑制したことを特徴とする。
In order to achieve the above object, the present invention is characterized in that generation of an irregular magnetic field is suppressed by overlapping the terminal transition portions of the coil side ends.
以下、本発明の実施例を図面に従つて説明す
る。第5図は、本発明に係る磁場発生装置の第1
実施例を示す平面図であり、第6図は第5図を矢
符P方向からみた拡大正面図である。本発明の実
施例において、従来例と同一構成要素には同一符
号を付して説明を省略する。本発明に係る第1実
施例が第3図に示す従来例と異なるところは、ス
プリツトコイル7A及び7Bの終端渡り部72′
及び73′を高さ方向に積み重ねた点にあり、他
の構成には変更はない。さらに詳細には、第6図
に示すように、渡り部72′及び73′を高さ方向
に積み重ねるには渡り部72′及び73′を重ね合
せた厚み2dが全体としてコイル辺70または7
1の高さHとほぼ同じ位にする方が望ましい。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 5 shows the first magnetic field generator according to the present invention.
FIG. 6 is a plan view showing the embodiment, and FIG. 6 is an enlarged front view of FIG. 5 viewed from the direction of arrow P. In the embodiment of the present invention, the same components as in the conventional example are given the same reference numerals, and the description thereof will be omitted. The difference between the first embodiment of the present invention and the conventional example shown in FIG. 3 is that the terminal transition portions 72' of the split coils 7A and 7B
and 73' are stacked in the height direction, and there is no other change in the structure. More specifically, as shown in FIG. 6, in order to stack the transition portions 72' and 73' in the height direction, the thickness 2d of the overlapping transition portions 72' and 73' is the entire coil side 70 or 73'.
It is preferable that the height be approximately the same as the height H of 1.
かかる構成したことにより第4図にて説明した
不正磁場起磁力Beの発生を無くすことができる。 With this configuration, the generation of the irregular magnetic field magnetomotive force Be explained in FIG. 4 can be eliminated.
第7図は本発明の他の実施例であり、終端渡り
部72′及び73′の変形例を示したものである。
第7図において、二組の終端渡り部72′及び7
3′のうち、一方を、例えば終端渡り部73′をコ
イル辺の厚み方向に二分割した終端渡り部73
0′とし、他方の終端渡り部72′を前記終端渡り
部730′に挾み込んで互に重ね合せ構成したも
のである。 FIG. 7 shows another embodiment of the present invention, showing a modification of the terminal transition portions 72' and 73'.
In FIG. 7, two sets of terminal transition parts 72' and 7
3', for example, the terminal transition part 73' is divided into two in the thickness direction of the coil side.
0', and the other end transition portion 72' is sandwiched between the end transition portion 730' and overlapped with each other.
かかる構成によれば、さらに不正磁場を少なく
できるものである。 According to this configuration, it is possible to further reduce illegal magnetic fields.
ここで、終端渡り部の不正磁場発生について検
討してみる。第6図において、終端渡り部直下A
点に終端渡り部72′及び73′に流れる電流が与
える不整磁場Beは、その大きさをBe1とすると、
大略第(1)式で与えられる。 Here, let's consider the generation of an illegal magnetic field at the terminal transition section. In Figure 6, right below the terminal transition part A
The irregular magnetic field Be given by the current flowing through the terminal transition portions 72' and 73' at a point is expressed as follows :
It is roughly given by equation (1).
Be1=K(1/d−1/d+t) ……(1)
ここで、K:比例定数
d:距離
t:終端渡り部導体厚み
この(1)式で与えられる不正磁場Beは第4図に
示した発生機構によるものではなく、電流源の距
離の違いにより生ずるものである。 Be 1 = K (1/d-1/d+t) ... (1) where, K: proportionality constant d: distance t: thickness of the conductor at the terminal transition section The irregular magnetic field Be given by this equation (1) is shown in Figure 4. This is not caused by the generation mechanism shown in Figure 1, but is caused by the difference in the distance between the current sources.
また、第7図の如くコイルを配列したときの、
この種の不正磁場の大きさは下記第(2)式で与えら
れる。 Also, when the coils are arranged as shown in Figure 7,
The magnitude of this type of irregular magnetic field is given by the following equation (2).
Be2=K(1/2d−1/d+0.75t
+1/2(d+1.5t)) ……(2)
ここで一例としてd=4〔cm〕、t=1〔cm〕と
して(1),(2)式を数値計算してみる。 Be 2 = K (1/2d-1/d+0.75t +1/2(d+1.5t)) ...(2) Here, as an example, assuming d = 4 [cm] and t = 1 [cm], (1), Let's try to calculate equation (2) numerically.
(1)式より、Be1=50.0×10-3K
(2)式より、Be2=5.4×10-3K
以上の如く第7図に示す如く配設すると、より
一層不正磁場を低減することができることが理解
できる。 From equation (1), Be 1 = 50.0×10 -3 K From equation (2), Be 2 = 5.4×10 -3 K If the arrangement is as shown in Figure 7, the irregular magnetic field will be further reduced. I can understand that it is possible.
第8図及び第9図は本発明のさらに他の実施例
であり、第7図に示す構成のものと同一作用効果
をもたらすものである。第8図の実施例は、コイ
ル辺7の片側をターンコイルとなし、これを図示
の如くサンドイツチ状に配設して構成したもので
ある。 FIGS. 8 and 9 show still other embodiments of the present invention, which provide the same effects as the configuration shown in FIG. 7. In the embodiment shown in FIG. 8, one side of the coil side 7 is formed into a turn coil, which is arranged in the shape of a sanderch as shown in the figure.
第9図において、スプリツトコイルの終端渡り
部について、一方の渡り部730″を、環状に形
成すると共に、その内部に他方の渡り部72′を
その環状内に配設して同軸構造としたものであ
る。 In FIG. 9, regarding the terminal transition part of the split coil, one transition part 730'' is formed in an annular shape, and the other transition part 72' is arranged inside the annular shape to form a coaxial structure. It is something.
以上説明したように本発明によれば、半円弧状
のコイル装置を二個組み合せて円形状の磁場発生
装置とすると共に、コイル辺の終端渡り部を互に
重ね合せるようにしたので、不正磁場の発生がな
くなるという効果がある。
As explained above, according to the present invention, two semicircular arc-shaped coil devices are combined to form a circular magnetic field generating device, and the terminal transition portions of the coil sides are overlapped with each other, so that irregular magnetic fields can be generated. This has the effect of eliminating the occurrence of
第1図は従来の磁場発生装置を示す平面図、第
2図は第1図のトーラスの断面図、第3図は従来
の別の磁場発生装置の例を示す平面図、第4図は
第3図の終端渡り部で電流による不整磁場起磁力
が発生する機構を説明する説明図、第5図は本発
明に係る磁場発生装置の一実施例を示す平面図、
第6図は第5図の終端渡り部をトーラス外径側よ
りみた拡大正面図、第7図は本発明の他の実施例
を示す正面図、第8図は本発明のさらに他の実施
例を示す正面図、第9図は本発明の同他の実施例
を示す正面図である。
70……コイル辺、71……コイル辺、72及
び73……終端渡り部、74……フイーダ、Be
……不整磁場起磁力、iA及びiB……電流。
FIG. 1 is a plan view showing a conventional magnetic field generator, FIG. 2 is a cross-sectional view of the torus in FIG. 1, FIG. 3 is a plan view showing another example of a conventional magnetic field generator, and FIG. FIG. 3 is an explanatory diagram illustrating a mechanism in which an irregular magnetic field magnetomotive force is generated by a current at the terminal transition portion; FIG. 5 is a plan view showing an embodiment of the magnetic field generator according to the present invention;
FIG. 6 is an enlarged front view of the terminal transition portion of FIG. 5 viewed from the outside diameter side of the torus, FIG. 7 is a front view showing another embodiment of the present invention, and FIG. 8 is a further embodiment of the present invention. FIG. 9 is a front view showing another embodiment of the present invention. 70...Coil side, 71...Coil side, 72 and 73...Terminal transition portion, 74...Feeder, Be
...irregular magnetic field magnetomotive force, i A and i B ... current.
Claims (1)
れとは異径の半円弧状の第2のコイル辺とを両コ
イル辺の端部にて終端渡り部をもつて接続して前
記両コイル辺をほぼ一定間隔で配設し、前記コイ
ル辺の外側コイル辺の一部より該両コイル電流を
供給するためのフイーダを設けてなる半円弧状コ
イル装置を、二個円形に組み合せてなる磁場発生
装置において、二組の終端渡り部を該コイル辺の
厚み方向に互い重ね合せてなることを特徴とする
磁場発生装置。 2 特許請求の範囲第1項記載の磁場発生装置に
おいて、二組の終端渡り部のうち、一方の終端渡
り部をコイル辺の厚み方向に二分割し、他方の終
端渡り部を前記一方の終端渡り部に挾み込んで互
に重ね合せてなることを特徴とする磁場発生装
置。[Scope of Claims] 1. A first coil side having a semicircular arc shape with a predetermined diameter and a second coil side having a semicircular arc shape having a different diameter from the first coil side having a terminal transition portion at the ends of both coil sides. A semicircular arc coil device is provided, in which both coil sides are connected at approximately constant intervals, and a feeder is provided for supplying current to both coils from a part of the outer coil side of the coil side. A magnetic field generating device comprising two pieces combined in a circular shape, characterized in that two sets of terminal transition portions are overlapped with each other in the thickness direction of the coil sides. 2. In the magnetic field generating device according to claim 1, one of the two sets of terminal transition portions is divided into two in the thickness direction of the coil side, and the other terminal transition portion is connected to the one terminal end. A magnetic field generator characterized by being sandwiched between transition parts and stacked on top of each other.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57209343A JPS59100890A (en) | 1982-12-01 | 1982-12-01 | magnetic field generator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57209343A JPS59100890A (en) | 1982-12-01 | 1982-12-01 | magnetic field generator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59100890A JPS59100890A (en) | 1984-06-11 |
| JPS645443B2 true JPS645443B2 (en) | 1989-01-30 |
Family
ID=16571374
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57209343A Granted JPS59100890A (en) | 1982-12-01 | 1982-12-01 | magnetic field generator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59100890A (en) |
-
1982
- 1982-12-01 JP JP57209343A patent/JPS59100890A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59100890A (en) | 1984-06-11 |
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