JPH0114554B2 - - Google Patents
Info
- Publication number
- JPH0114554B2 JPH0114554B2 JP58148114A JP14811483A JPH0114554B2 JP H0114554 B2 JPH0114554 B2 JP H0114554B2 JP 58148114 A JP58148114 A JP 58148114A JP 14811483 A JP14811483 A JP 14811483A JP H0114554 B2 JPH0114554 B2 JP H0114554B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- cooling
- limiter
- poloidal
- discharge pipe
- 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
- Plasma Technology (AREA)
Description
【発明の詳細な説明】
本発明は核融合装置用磁気リミツタ冷却装置に
関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic limiter cooling device for a nuclear fusion device.
従来の核融合装置の概要とその問題点を第1図
〜第5図に基づいて説明する。第1図はその一部
を切り欠いた核融合装置の平面図、第2図は第1
図の−断面図、第3図は真空容器の縦断端面
図である。プラズマ1を保持するための真空容器
2は厚肉部2Aとベローズ部2Bからなる環状体
で、多数のトロイダル磁場コイル3内に配置さ
れ、その内部は真空排気装置4によつて真空にさ
れる。容器外ポロイダル磁場コイル5A,5Bは
プラズマ中に環状放電電流を発生させる1次巻線
の役割を果し、容器内ポロイダル磁場コイル6
A,6B,6Cはセパラトリツクス磁気面7を作
りプラズマ1へ流入する不純物を外部へ除去する
役割を果す。セパラトリツクス磁気面7にはプラ
ズマ1の一部が巻き付いてくるため、セパラトリ
ツクス磁気面7の端部は磁気リミツタ冷却ダクト
8A,8Bにより冷却する必要がある。このため
に磁気リミツタ冷却ダクト8A,8Bにはパイプ
9A,9Bにより冷媒が流される。なお、10は
変流器、11A,11Bはベースである。 An overview of conventional nuclear fusion devices and their problems will be explained based on FIGS. 1 to 5. Figure 1 is a partially cutaway plan view of the nuclear fusion device, and Figure 2 is the top view of the fusion device.
FIG. 3 is a vertical cross-sectional view of the vacuum container. A vacuum container 2 for holding plasma 1 is an annular body consisting of a thick wall portion 2A and a bellows portion 2B, and is arranged within a large number of toroidal magnetic field coils 3, and the inside thereof is evacuated by a vacuum evacuation device 4. . The outer poloidal magnetic field coils 5A and 5B serve as primary windings that generate an annular discharge current in the plasma, and the inner poloidal magnetic field coils 6
A, 6B, and 6C form a separatrix magnetic surface 7 and serve to remove impurities flowing into the plasma 1 to the outside. Since a portion of the plasma 1 wraps around the separatrix magnetic surface 7, the ends of the separatrix magnetic surface 7 must be cooled by the magnetic limiter cooling ducts 8A and 8B. For this purpose, refrigerant is flowed through the magnetic limiter cooling ducts 8A, 8B through pipes 9A, 9B. Note that 10 is a current transformer, and 11A and 11B are bases.
ところで磁気リミツタ冷却ダクト8A,8B
は、第4図に示す真空容器2の一部切り欠き平面
図および第5図に示すその拡大平面図(第2図の
−断面に相当)から明らかなように、それぞ
れ真空容器2のトーラス方向に所定のピツチで分
割されて全周に配置されている。そしてトーラス
方向に所定の間隔をもつて磁気リミツタ冷却ダク
ト8Aに結合した供給パイプ9A1と排出パイプ
9A2を真空容器2の壁を貫通して外部へ導出し、
このパイプ9A1,9A2を介して磁気リミツタ冷
却ダクト8Aに冷媒を流すようにしている。しか
しこのように冷媒流路を構成すると、真空容器2
と磁気リミツタ冷却ダクト8Aとパイプ9A1,
9A2とを要素として第5図に示す点A,B,C,
Dを通る電気的な閉回路が構成され、ポロイダル
磁場コイル5A,5B,6A〜6Cにより発生す
る鉛直方向の磁束12がこの閉回路内を通過す
る。このためプラズマ発生時にはこの閉回路に起
電力が生じて循環電流が流れ、この電流とポロイ
ダル磁場との相互作用により供給パイプ9A1と
排出パイプ9A2には過大な電磁力が発生して磁
気リミツタ冷却機構を破壊する危険がある。 By the way, magnetic limiter cooling ducts 8A and 8B
As is clear from the partially cutaway plan view of the vacuum container 2 shown in FIG. 4 and the enlarged plan view shown in FIG. 5 (corresponding to the − section in FIG. 2), It is divided at predetermined pitches and placed around the entire circumference. Then, the supply pipe 9A 1 and the discharge pipe 9A 2 connected to the magnetic limiter cooling duct 8A at a predetermined interval in the torus direction are led out through the wall of the vacuum vessel 2, and
The refrigerant is made to flow into the magnetic limiter cooling duct 8A through these pipes 9A 1 and 9A 2 . However, if the refrigerant flow path is configured in this way, the vacuum container 2
and magnetic limiter cooling duct 8A and pipe 9A 1 ,
Points A, B, C, shown in Figure 5 with 9A 2 as elements,
An electrical closed circuit is formed through D, and the vertical magnetic flux 12 generated by the poloidal magnetic field coils 5A, 5B, 6A to 6C passes through this closed circuit. Therefore, when plasma is generated, an electromotive force is generated in this closed circuit and a circulating current flows, and due to the interaction between this current and the poloidal magnetic field, an excessive electromagnetic force is generated in the supply pipe 9A 1 and the discharge pipe 9A 2 , causing a magnetic limiter. There is a risk of destroying the cooling mechanism.
従つて本発明の目的は、前記したような核融合
装置用磁気リミツタ冷却装置の循環電流の発生を
防止あるいは軽減して磁気リミツタ冷却機構の破
壊を防止することにある。 SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to prevent or reduce the generation of circulating current in a magnetic limiter cooling device for a nuclear fusion device as described above, thereby preventing destruction of the magnetic limiter cooling mechanism.
この目的を達成するため、本発明では、プラズ
マ中の不純物を除去するためのセパラトリツクス
磁気面の端部に配置される磁気リミツタ冷却ダク
ト内を、ポロイダル磁場の磁束の流れ方向に仕切
壁で仕切つて2つの冷却室とし、該各冷却室を両
端部で連通すると共に、この冷却室の一方に前記
供給パイプを、他方の冷却室に前記排出パイプを
結合し、かつ、この供給パイプと排出パイプを、
ポロイダル磁場の磁束の方向に対する直角方向の
位置と等しくしたことを特徴とする。 In order to achieve this objective, in the present invention, the inside of the cooling duct of the magnetic limiter placed at the end of the magnetic surface of the separator for removing impurities in the plasma is partitioned by a partition wall in the flow direction of the magnetic flux of the poloidal magnetic field. Two cooling chambers are provided, each cooling chamber is connected at both ends, and the supply pipe is connected to one of the cooling chambers, and the discharge pipe is connected to the other cooling chamber, and the supply pipe and the discharge pipe are connected to each other. ,
It is characterized in that the position is equal to the position in the direction perpendicular to the direction of the magnetic flux of the poloidal magnetic field.
以下、本発明を図示の実施例に基づいて説明す
る。第6図は磁気リミツタ冷却装置の縦断端面
図、第7図は第6図の−断面図で、これらは
片側の磁気リミツタ冷却ダクトを示しているが他
側の磁気リミツタ冷却ダクトも同様に構成され
る。 Hereinafter, the present invention will be explained based on illustrated embodiments. Fig. 6 is a longitudinal cross-sectional view of the magnetic limiter cooling device, and Fig. 7 is a cross-sectional view of the magnetic limiter cooling device in Fig. 6. These show the magnetic limiter cooling duct on one side, but the magnetic limiter cooling duct on the other side has the same structure. be done.
磁気リミツタ冷却ダクト13内は仕切壁13A
によつてポロイダル磁場の磁束の流れ方向に区切
られて両端部で連通する冷却室13B,13Cが
形成される。供給パイプ14Aは冷却室13Bに
連通し、排出パイプ14Bは冷却室13Cに連通
するように磁気リミツタ冷却ダクト13に結合さ
れる。なおこのとき供給パイプ14Aと排出パイ
プ14Bの位置は、ポロイダル磁場の磁束の方向
に対する直角方向の位置を等しくして、真空容器
2と磁気リミツタ冷却ダクト13と供給パイプ1
4Aと排出パイプ14Bによつて構成される電気
的な閉回路がポロイダル磁場コイル6B等により
発生する磁束と交差しないようにする。 Inside the magnetic limiter cooling duct 13 is a partition wall 13A.
Thus, cooling chambers 13B and 13C are formed which are separated in the flow direction of the magnetic flux of the poloidal magnetic field and communicated at both ends. The supply pipe 14A is connected to the cooling chamber 13B, and the discharge pipe 14B is connected to the magnetic limiter cooling duct 13 so as to communicate with the cooling chamber 13C. At this time, the positions of the supply pipe 14A and the discharge pipe 14B are made equal in the direction perpendicular to the direction of the magnetic flux of the poloidal magnetic field, so that the positions of the supply pipe 14A and the discharge pipe 14B are the same in the direction perpendicular to the direction of the magnetic flux of the poloidal magnetic field.
4A and the discharge pipe 14B so as not to intersect with the magnetic flux generated by the poloidal magnetic field coil 6B or the like.
このようにすることにより供給パイプ14Aか
ら冷却室13Bに供給された冷媒は冷却室13B
内を分流した後にその両端から冷却室13Cに流
入し、その後排出パイプ14Bから排出される流
路で流れ磁気リミツタ冷却ダクト13を冷却す
る。そして前記したように真空容器2と磁気リミ
ツタ冷却ダクト13と供給パイプ14Aと排出パ
イプ14Bによつて構成される電気的閉回路がポ
ロイダル磁場コイル6B等により発生する磁束と
交差しないので、プラズマ発生時に前記閉回路に
起電力が発生して循環電流が流れることがなく、
従つて電磁力による磁気リミツタ冷却機構の破壊
を防止することができる。 By doing this, the refrigerant supplied from the supply pipe 14A to the cooling chamber 13B is
After dividing the flow, it flows into the cooling chamber 13C from both ends, and then flows through a flow path that is discharged from the discharge pipe 14B to cool the magnetic limiter cooling duct 13. As described above, the electrical closed circuit constituted by the vacuum vessel 2, the magnetic limiter cooling duct 13, the supply pipe 14A, and the discharge pipe 14B does not intersect with the magnetic flux generated by the poloidal magnetic field coil 6B, etc., so that when plasma is generated, No electromotive force is generated in the closed circuit and no circulating current flows,
Therefore, destruction of the magnetic limiter cooling mechanism due to electromagnetic force can be prevented.
以上説明した本発明の核融合装置用磁気リミツ
タ冷却装置によれば、プラズマ中の不純物を除去
するためのセパラトリツクス磁気面の端部に配置
される磁気リミツタ冷却ダクト内を、ポロイダル
磁場の磁束の流れ方向に仕切壁で仕切つて2つの
冷却室とし、該各冷却室を両端部で連通すると共
に、この冷却室の一方に前記供給パイプを、他方
の冷却室に前記排出パイプを結合し、かつ、この
供給パイプと排出パイプを、ポロイダル磁場の磁
束の方向に対する直角方向の位置と等しくしたも
のであるから、真空容器と磁気リミツタ冷却ダク
ト、及びパイプによる閉回路がポロイダルコイル
により発生する磁束と交差しないため、循環電流
の発生を防止、あるいは軽減することができるの
で、磁気リミツタ冷却機構の破壊を防止すること
ができるという効果がある。 According to the magnetic limiter cooling device for a nuclear fusion device of the present invention described above, the magnetic flux of the poloidal magnetic field flows through the magnetic limiter cooling duct arranged at the end of the magnetic surface of the separator for removing impurities in plasma. The cooling chambers are partitioned in the direction by a partition wall to form two cooling chambers, each of the cooling chambers is communicated at both ends, and the supply pipe is connected to one of the cooling chambers, and the discharge pipe is connected to the other cooling chamber, and Since the supply pipe and the discharge pipe are placed at the same position perpendicular to the direction of the magnetic flux of the poloidal magnetic field, the closed circuit formed by the vacuum vessel, magnetic limiter cooling duct, and pipe does not intersect with the magnetic flux generated by the poloidal coil. Since the generation of circulating current can be prevented or reduced, the magnetic limiter cooling mechanism can be prevented from being destroyed.
第1図〜第5図は従来の核融合装置を示すもの
で、第1図はその一部を切り欠いた核融合装置の
平面図、第2図は第1図の−断面図、第3図
は真空容器の縦断端面図、第4図は真空容器の一
部切り欠き平面図、第5図はその拡大平面図であ
る。第6図および第7図は本発明の一実施例を示
すもので、第6図は核融合装置用磁気リミツタ冷
却装置の縦断端面図、第7図はその−断面図
である。
13……磁気リミツタ冷却ダクト、14A……
供給パイプ、14B……排出パイプ。
Figures 1 to 5 show conventional nuclear fusion devices. Figure 1 is a partially cutaway plan view of the fusion device, Figure 2 is a cross-sectional view of Figure 1, and Figure 3 is a cross-sectional view of Figure 1. 4 is a partially cutaway plan view of the vacuum container, and FIG. 5 is an enlarged plan view thereof. 6 and 7 show one embodiment of the present invention, FIG. 6 being a longitudinal sectional end view of a magnetic limiter cooling device for a nuclear fusion device, and FIG. 7 being a sectional view thereof. 13... Magnetic limiter cooling duct, 14A...
Supply pipe, 14B...Discharge pipe.
Claims (1)
トリツクス磁気面の端部に配置される磁気リミツ
タ冷却ダクトと、この磁気リミツタ冷却ダクトに
冷媒を流す供給パイプ、および排出パイプとを備
えた核融合装置用磁気リミツタ冷却装置におい
て、前記磁気リミツタ冷却ダクト内を、ポロイダ
ル磁場の磁束の流れ方向に仕切壁で仕切つて2つ
の冷却室とし、該各冷却室を両端部で連通すると
共に、この冷却室の一方に前記供給パイプを、他
方の冷却室に前記排出パイプを結合し、かつ、こ
の供給パイプと排出パイプを、ポロイダル磁場の
磁束の方向に対する直角方向の位置と等しくした
ことを特徴とする核融合装置用磁気リミツタ冷却
装置。1. A magnetic fusion device equipped with a magnetic limiter cooling duct arranged at the end of a separatrix magnetic surface for removing impurities in plasma, a supply pipe for flowing a coolant into the magnetic limiter cooling duct, and a discharge pipe. In the limiter cooling device, the inside of the magnetic limiter cooling duct is divided into two cooling chambers by a partition wall in the flow direction of the magnetic flux of the poloidal magnetic field, and each cooling chamber is communicated at both ends, and one of the cooling chambers is For a nuclear fusion device, characterized in that the supply pipe is coupled to the other cooling chamber and the discharge pipe is arranged at the same position in the direction perpendicular to the direction of the magnetic flux of the poloidal magnetic field. Magnetic limiter cooling device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58148114A JPS6040989A (en) | 1983-08-15 | 1983-08-15 | Magnetic limiter cooling device for fusion device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58148114A JPS6040989A (en) | 1983-08-15 | 1983-08-15 | Magnetic limiter cooling device for fusion device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6040989A JPS6040989A (en) | 1985-03-04 |
| JPH0114554B2 true JPH0114554B2 (en) | 1989-03-13 |
Family
ID=15445561
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58148114A Granted JPS6040989A (en) | 1983-08-15 | 1983-08-15 | Magnetic limiter cooling device for fusion device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6040989A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56160685A (en) * | 1980-05-16 | 1981-12-10 | Hitachi Ltd | Divertor for nuclear fusion equipment |
| JPS5777992A (en) * | 1980-11-04 | 1982-05-15 | Hitachi Ltd | Divertor for nuclear fusion device |
-
1983
- 1983-08-15 JP JP58148114A patent/JPS6040989A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6040989A (en) | 1985-03-04 |
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