JPH0326520B2 - - Google Patents
Info
- Publication number
- JPH0326520B2 JPH0326520B2 JP3811882A JP3811882A JPH0326520B2 JP H0326520 B2 JPH0326520 B2 JP H0326520B2 JP 3811882 A JP3811882 A JP 3811882A JP 3811882 A JP3811882 A JP 3811882A JP H0326520 B2 JPH0326520 B2 JP H0326520B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- water channel
- truncated conical
- cooling water
- conical column
- 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
- 239000000498 cooling water Substances 0.000 claims description 25
- 239000002245 particle Substances 0.000 claims description 14
- 230000001133 acceleration Effects 0.000 claims description 4
- 239000000463 material Substances 0.000 description 6
- 238000001816 cooling Methods 0.000 description 4
- 230000008646 thermal stress Effects 0.000 description 4
- 229910000831 Steel Inorganic materials 0.000 description 3
- 230000020169 heat generation Effects 0.000 description 3
- 239000010959 steel Substances 0.000 description 3
- 229910001369 Brass Inorganic materials 0.000 description 2
- 239000010951 brass Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
Landscapes
- Particle Accelerators (AREA)
Description
【発明の詳細な説明】
本発明は、粒子加速管中に整列して垂設される
粒子加速器の加速電極の冷却機構に特徴を有する
ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention is characterized by a cooling mechanism for accelerating electrodes of a particle accelerator arranged vertically in a particle accelerator tube.
従来の粒子加速器は、第1図に示すように大電
力の高周波を用いる粒子加速管1の内部に、多数
個の環状をなす加速電極2を、非常に高精度に芯
出しされた間隔、同心度、傾き等のアライメント
によつて一直線にライン状に位置決めし、一定間
隔毎に吊下げて配設した構造になつている。 As shown in Figure 1, a conventional particle accelerator has a large number of annular accelerating electrodes 2 arranged concentrically at very precisely centered intervals inside a particle accelerating tube 1 that uses high-power, high-frequency waves. The structure is such that they are positioned in a straight line by alignment such as angle and inclination, and are suspended at regular intervals.
また、前記のような粒子加速器においては、共
振周波数で高い加速電界を得るために、粒子加速
管1の内径Dと加速電極2の各部寸法(第2図に
示すD1,D2,D3,D4,T1,T2等)が電気的に自
ら決定されている。 In addition, in the above-mentioned particle accelerator, in order to obtain a high accelerating electric field at a resonant frequency, the inner diameter D of the particle accelerating tube 1 and the dimensions of each part of the accelerating electrode 2 (D 1 , D 2 , D 3 shown in FIG. , D 4 , T 1 , T 2 , etc.) are electrically determined by themselves.
さらに、前記の加速電極2は、外側の平円板部
A1と中心側の穴A′明き截頭円錐柱部A2(ノーズコ
ーン部)とからなる電極Aの部分を有しており、
該電極Aにおいては、大電力高周波の壁損失によ
る発熱を生じ、その発熱量は、第3図に示すよう
な発熱曲線となり、特に同図から明らかなように
第2図に示す截頭円錐柱部(ノーズコーン部)
A2の部分に高い発熱を生ずる。 Furthermore, the acceleration electrode 2 has an outer flat disk portion.
It has an electrode A portion consisting of A 1 and a truncated conical column portion A 2 (nose cone portion) with a hole A′ on the center side,
In the electrode A, heat is generated due to wall loss of high power and high frequency, and the amount of heat generated becomes a heat generation curve as shown in FIG. part (nose cone part)
A High heat generation occurs in the 2 part.
よつて、前記発熱による温度上昇を防ぐために
電極Aを冷却する必要があるが、粒子加速管1内
は超高真空に保持され、また、該電極Aは機能上
外表面から冷却することが不可能であるため、内
部に流体(一般的には純水)を流して温度を一定
にすることが必要となる。 Therefore, it is necessary to cool the electrode A in order to prevent the temperature from rising due to the heat generation, but the inside of the particle accelerator tube 1 is maintained at an ultra-high vacuum, and the electrode A cannot be cooled from the outer surface due to its function. Since this is possible, it is necessary to flow a fluid (generally pure water) inside to keep the temperature constant.
従つて、前記した条件下で加速電極2を冷却す
る従来の構造は、第4図、第5図に示すように電
極Aに併設されている支持首部A3に設けた入口
通路aから冷却水を流入し、截頭円錐柱部A2に
設けた半円弧状の両水路a2、および平円板部A1
に設けた半円弧状の両水路a1に矢示のように流通
せしめたのち、出口通路Sから排出するようにな
つている。 Therefore, the conventional structure for cooling the accelerating electrode 2 under the above conditions is to supply cooling water from the inlet passage a provided in the support neck A 3 attached to the electrode A, as shown in FIGS. 4 and 5. flows into semicircular arc-shaped both channels a 2 provided in the truncated conical column part A 2 , and the flat disc part A 1
After flowing as shown by the arrows through semicircular arc-shaped water channels a1 provided in the upper and lower sides, the water is discharged from an outlet passage S.
しかし、前記した従来の加速電極2においては
(1) 第4図、第5図に示すように平円板部A1に
おける水路が少なく、伝熱面積が小さいので、
平円板部A1の温度が高くなる。 However, in the conventional accelerating electrode 2 described above, (1) As shown in FIGS. 4 and 5, there are few water channels in the flat disk portion A1 , and the heat transfer area is small;
The temperature of the flat disk portion A1 increases.
(2) 穴明き截頭円錐柱部A2即ちノーズコーン部
の水路断面積が大きく、冷却水の流速が小さい
ので、流量一定の条件下では熱伝達率が小さく
なり、最も発熱が大きいノーズコーン部を効率
よく冷却することができない。(加速電極数が
非常に多く、ポンプの設備費が高くなるため実
際上流量の増加は望めない。)
などにより、加速電極の全面に亘つて、温度偏差
による熱応力および熱変形を生ずる欠点がある。(2) The perforated truncated conical column A 2 , that is, the nose cone, has a large waterway cross-sectional area and a low cooling water flow rate, so under a constant flow rate, the heat transfer coefficient is small, and the nose generates the most heat. The cone cannot be cooled efficiently. (Since the number of accelerating electrodes is very large, the equipment cost of the pump becomes high, so it is practically impossible to increase the flow rate.) Due to these reasons, there is a drawback that thermal stress and thermal deformation due to temperature deviation occur over the entire surface of the accelerating electrode. be.
本発明は、従来の粒子加速器の加速電極におけ
る前記したような欠点を解消するために開発され
たものであつて、外側の平円板部と中心側の穴明
き截頭円錐柱部とからなる電極内に截頭円錐柱部
のを中心とする略円形状あるいは半円弧状の水路
を多重に設けて、前記水路の隣接端部を屈曲通路
にて連結するとともに、前記電極に併設されてい
る支持首部内に設けた入口通路を前記水路の最内
側に直結しかつ前記入口通路を囲む出口通路を前
記水路の最外側に直結した冷却水路を設け、前記
截頭円錐柱部内における前記冷却水路を小断面積
にしかつ外表面に近接させて多数配設した点に特
徴を有し、その目的とする処は、第3図に示すよ
うな壁損失が与えられ、第2図に示すような加速
電極の諸寸法が電気的に決定され、かつ冷却水量
を極力少くしなければならない条件下で、
(イ) 冷却水が沸騰しないように加速電極の温度を
極力低くし、
(ロ) 加速電極の温度分布を極力均等にし、熱応力
度および局部変形を小さくするとともに、
(ハ) 加速電極を安価に製作するため、材料費およ
び加工費の安価な最も一般的な材料(鋼材)で
製作できるようにした、
粒子加速器の加速電極を供する点にある。 The present invention was developed to eliminate the above-mentioned drawbacks of accelerating electrodes of conventional particle accelerators. Multiple substantially circular or semi-circular water channels centered around the truncated conical column are provided in the electrode, and adjacent ends of the water channels are connected by a bent passage, and the channels are provided adjacent to the electrode. A cooling water channel is provided in which an inlet passage provided in the support neck part is directly connected to the innermost side of the water channel, and an outlet passage surrounding the inlet passage is directly connected to the outermost side of the water channel, and the cooling water channel in the truncated conical column part is provided. It is characterized in that it has a small cross-sectional area and is arranged in large numbers close to the outer surface, and its purpose is to provide a wall loss as shown in Fig. 3, and Under conditions where the dimensions of the accelerating electrode are determined electrically and the amount of cooling water must be kept as low as possible, (a) the temperature of the accelerating electrode is kept as low as possible so that the cooling water does not boil, and (b) the accelerating electrode In addition to making the temperature distribution as uniform as possible and minimizing thermal stress and local deformation, (c) the accelerating electrode can be manufactured at low cost, so it can be manufactured from the most common material (steel) with low material and processing costs. The purpose of this invention is to provide an accelerating electrode for a particle accelerator.
本発明は、前記の構成よりなつており、加速電
極の全面に亘つて合理的に冷却水路が配設され、
特に最も発熱量の大きい截頭円錐柱部における冷
却水路を小断面積にしかつ外表面に近接させて多
数配設しているので、截頭円錐柱部〔ノーズコー
ン部〕の温度を極めて効率よく低下させることが
できるとともに、全面に亘つて略一様に冷却する
ことができ、温度偏差による熱応力および熱変形
を著しく小さくすることができる。従つて、熱伝
導率の大きい高価な材料(例えば銅、黄銅)を使
用しないで、比較的に熱伝導率の小さい鋼材を使
用して安価な加速電極にすることが可能となる。 The present invention has the above-mentioned configuration, in which cooling channels are rationally arranged over the entire surface of the accelerating electrode,
In particular, the cooling channels in the truncated conical column, which generates the largest amount of heat, have a small cross-sectional area and are arranged in large numbers close to the outer surface, so the temperature of the truncated conical column (nose cone) can be controlled extremely efficiently. In addition, it is possible to cool substantially uniformly over the entire surface, and thermal stress and thermal deformation due to temperature deviation can be significantly reduced. Therefore, instead of using expensive materials with high thermal conductivity (such as copper and brass), it is possible to make an inexpensive accelerating electrode by using a steel material with relatively low thermal conductivity.
以下、本発明の実施例を図示について説明す
る。第6図ないし第11図に、第1図に示すよう
な粒子加速管1の内部に整列して垂設される本発
明の一実施例である加速電極12の各部を示して
おり、該加速電極12は、第7図に示すように外
側の平円板部A1と中心側の穴A′明きの截頭円錐
柱部A2とよりなる全体が略円環状の電極Aの部
分、および該電極Aに併設された支持首部A3(第
6図参照)からなつており、さらに、それらの内
部には後記するような全面に亘る冷却水路が配設
されている。 Hereinafter, embodiments of the present invention will be described with reference to the drawings. 6 to 11 show each part of an accelerating electrode 12, which is an embodiment of the present invention, which is aligned and vertically arranged inside the particle accelerating tube 1 as shown in FIG. As shown in FIG. 7, the electrode 12 is a portion of the electrode A that is generally annular in its entirety, consisting of an outer flat disk portion A 1 and a central truncated conical portion A 2 with a hole A′. and a support neck portion A 3 (see FIG. 6) attached to the electrode A, and a cooling water channel extending over the entire surface as described later is disposed inside them.
即ち、この実施例における冷却水路は、第6図
断面に示すように電極Aの外側の平円板部A1お
よび截頭円錐柱部A2の内部のいずれにおいても、
截頭円錐柱部の軸を中心とする略円形状あるいは
対の半円弧状の水路g〜m,m′を多重に設けて
水路間の半径方向の肉厚を薄くし、全面に亘つて
伝熱面積を大幅に増大し、水路g〜m′の隣接端
部を図示のように屈曲通路を介して連結するとと
もに、電極Aに併設されている支持首部A3に設
けた入口通路aを前記水路の最内側の端部に直結
し、かつ、入口通路aを囲むように支持首部A3
に設けた出口通路Sを前記水路の最外側の端部に
直結して、加速電極12の内部全面に亘る冷却水
路が配設されている。 That is , as shown in the cross- section in FIG.
Multiple approximately circular or paired semicircular arc-shaped waterways g to m, m' centered on the axis of the truncated conical column are provided to reduce the wall thickness in the radial direction between the waterways to ensure transmission over the entire surface. The thermal area is greatly increased, and the adjacent ends of the water channels g to m' are connected via the bent passage as shown in the figure, and the inlet passage a provided in the support neck A 3 attached to the electrode A is A support neck part A 3 is directly connected to the innermost end of the water channel and surrounds the inlet passage a.
A cooling water channel is provided over the entire interior of the accelerating electrode 12 by directly connecting the outlet passage S provided in the cooling water channel to the outermost end of the water channel.
さらに、前記の冷却水路は、ノーズコーン部即
ち截頭円錐柱部A2の内部において、第7図断面
にて示しさらに第8図ないし第10図断面に示す
ようになつており、全般的に水路が小断面積に形
成され、截頭円錐柱部A2の厚さ方向に3分割
(分割数を増すこともできる)にした両側の略形
状の水路m,m′および半円弧状の水路gにて形
成し、冷却水の流速を増大し熱伝達率を向上せし
め、冷却水と内壁との温度差を小さくしており、
さらに、外表面と水路との肉厚δを極力薄くし、
また穴A′に対しても近接させた構造として熱伝
等による温度差を小さくし、全体的には、截頭円
錐柱部A2の内部に配設されている冷却水路は、
第11図に示すような水路b〜m,m′の経路に
なつている。 Further, the above-mentioned cooling water channel is arranged inside the nose cone portion, that is, the truncated conical column portion A2 , as shown in the cross section of FIG. 7 and further shown in the cross sections of FIGS. 8 to 10, and generally The waterway is formed with a small cross-sectional area, and the truncated conical column part A2 is divided into three parts in the thickness direction (the number of divisions can be increased), and the approximately shaped waterways m and m' on both sides, and the semi-circular waterway. g, increases the flow rate of cooling water, improves the heat transfer coefficient, and reduces the temperature difference between the cooling water and the inner wall.
Furthermore, the wall thickness δ between the outer surface and the waterway is made as thin as possible,
In addition, the structure is placed close to the hole A' to reduce the temperature difference due to heat transfer, etc., and overall the cooling water channel arranged inside the truncated conical column part A2 is
The route is water channels b to m and m' as shown in Fig. 11.
第6図ないし第11図に示した本発明の一実施
例は、前記したようになつており、該加速電極1
2の内部に配設されている冷却水路の構造の詳述
を兼ねてその作用を説明する。 An embodiment of the present invention shown in FIGS. 6 to 11 is as described above, and the accelerating electrode 1
The structure of the cooling water channel disposed inside the cooling water passage 2 will be explained in detail as well as its function.
冷却水は、第6図に示す支持首部A3と平円板
部A1を貫く入口通路aから截頭円錐柱部A2内に
導入されて一部が水路a′に分流され、その分流量
は2分割となる。なお、水路a′側は分流水路a側
と同一構造になつているので、その説明は分流水
路a側の説明によつて一部省略する。 Cooling water is introduced into the truncated conical column part A 2 from the inlet passage a that passes through the support neck part A 3 and the flat disk part A 1 shown in FIG. The flow rate is divided into two. Note that since the water channel a' side has the same structure as the branch water channel a side, a portion of the explanation will be omitted in favor of the explanation of the branch water channel a side.
第8図断面に示す入口通路aの分流水路a中の
冷却水は、第9図断面に示す水路bを通つて第1
0図断面に示す水路cに出て、水路cを出た冷却
水は、水路mを経て水路eより第9図断面に示す
水路fを通り、第8図断面に示す水路gに出たの
ち、水路gを流れて第7図断面に矢示で示す水路
hを通り水路iに出る。ここで入口通路aから分
流した他方の水路a″から流れてきた(詳細は省
略、第11図参照)冷却水と合流し、再び半弧円
状の水路に分岐して水路i,j,k,lを経て出
口通路Sから排出される。 The cooling water in the branch waterway a of the inlet passage a shown in the cross-section of FIG. 8 passes through the waterway b shown in the cross-section of FIG.
The cooling water that exits the waterway c shown in the cross-section of Figure 0 passes through the waterway m, passes through the waterway e, passes through the waterway f shown in the cross-section of Figure 9, and exits the waterway g shown in the cross-section of Figure 8. , flows through waterway g, passes through waterway h shown by the arrow in the cross section of FIG. 7, and exits to waterway i. Here, it merges with the cooling water that has flowed from the other waterway a'' that has branched off from the inlet passage a (details are omitted, see Figure 11), and branches into a semicircular waterway again to form waterways i, j, and k. , l and is discharged from the outlet passage S.
従つて、前記した実施例においては、発熱量の
極めて大きい電極Aの截頭円錐柱部A2の内部に
おいて、小断面積に形成された略円形状の両水路
m,m′および中央部の半円弧状の対をなす水路
gに流通することになり、冷却水の流速が増大さ
れて熱伝導率が著しく向上されるとともに、厚み
方向の全面に亘つて均等に降温されかつ外表面の
降温も良好になつて、冷却水と内壁との温度差が
小さくなり、さらに、外側の平円板部A1におい
ても、多重に形成された対の半円弧状の水路によ
つて各水路間の半径方向の肉厚が薄くなり熱伝導
率が向上されて均一な降温効果が得られる。 Therefore, in the above-mentioned embodiment, inside the truncated conical column part A2 of the electrode A which generates an extremely large amount of heat, both the substantially circular water channels m and m' formed in a small cross-sectional area and the central part are formed. The cooling water flows through a pair of semicircular arc-shaped channels g, increasing the flow rate and significantly improving thermal conductivity, and lowering the temperature evenly over the entire surface in the thickness direction and lowering the temperature on the outer surface. The temperature difference between the cooling water and the inner wall becomes better, and the temperature difference between the cooling water and the inner wall becomes smaller.Furthermore, even in the outer flat disk part A1 , the multiple semicircular arc-shaped water channels form a plurality of pairs to reduce the temperature difference between each water channel. The wall thickness in the radial direction is thinner, the thermal conductivity is improved, and a uniform temperature-lowering effect can be obtained.
よつて、この実施例によれば、加速電極12の
全面に亘つて温度偏差による熱応力および熱変形
を著しく小さくすることができ、特に最高の発熱
量を生ずる截頭円錐柱部A2の降温も十分に達成
できるため、熱伝導率の大きい高価な材料(例え
ば銅、黄銅)を使用せずに、熱伝導率の小さい鋼
材を使用することが可能となり、安価な加速電極
を提供することができる。 Therefore, according to this embodiment, it is possible to significantly reduce thermal stress and thermal deformation due to temperature deviation over the entire surface of the accelerating electrode 12, and in particular, to reduce the temperature of the truncated conical column portion A2 that generates the highest amount of heat. This also makes it possible to use steel materials with low thermal conductivity instead of using expensive materials with high thermal conductivity (e.g. copper, brass), making it possible to provide inexpensive accelerating electrodes. can.
なお、前記実施例では截頭円錐柱部(ノーズコ
ーン部)の水路を、その厚み方向に3分割した状
態に構成しているが、本発明においては特に3分
割に限られるものではない。 In the above embodiment, the water channel of the truncated conical column (nose cone) is divided into three parts in the thickness direction, but the present invention is not limited to three parts.
以上本発明を実施例について説明したが、勿論
本発明はこのような実施例にだけ局限されるもの
ではなく、本発明の精神を逸脱しない範囲内で
種々の設計の改変を施しうるものである。 Although the present invention has been described above with reference to embodiments, it goes without saying that the present invention is not limited to such embodiments, and that various design modifications can be made without departing from the spirit of the present invention. .
第1図は従来の粒子加速器の概要を示す断面
図、第2図は従来の加速電極の電極部分のみを示
す縦断面形状図、第3図A,Bは、第2図の電極
の部分ポジシヨン図および発熱量の状態図、第4
図は第2図の電極内部に配設した冷却水路の説明
図、第5図は第4図の−断面図、第6図は本
発明の一実施例を示す加速電極の断面図(第5図
と同様な断面)、第7図は第6図の−断面図、
第8図は第7図の−断面図、第9図は第7図
の−断面図、第10図は第7図の−断面
図、第11図は実施例の截頭円錐柱部における水
路の状態を示す見取図である。
1:粒子加速管、12:加速電極、A:電極、
A1:平円板部、A2:截頭円錐柱部、A3:支持首
部、A′:穴、a:入口通路、b〜m,m′:水路、
S:出口通路。
Figure 1 is a cross-sectional view showing an overview of a conventional particle accelerator, Figure 2 is a longitudinal cross-sectional view showing only the electrode portion of a conventional accelerating electrode, and Figures 3A and B are partial positions of the electrode in Figure 2. Figure and state diagram of calorific value, 4th
The figure is an explanatory diagram of the cooling water channel arranged inside the electrode in Figure 2, Figure 5 is a cross-sectional view of Figure 4, and Figure 6 is a cross-sectional view of an accelerating electrode showing an embodiment of the present invention (Figure 5). Figure 7 is a cross-sectional view of Figure 6.
8 is a sectional view of FIG. 7, FIG. 9 is a sectional view of FIG. 7, FIG. 10 is a sectional view of FIG. 7, and FIG. 11 is a water channel in the truncated conical column of the embodiment. FIG. 1: particle acceleration tube, 12: acceleration electrode, A: electrode,
A 1 : flat disk part, A 2 : truncated conical column part, A 3 : support neck part, A': hole, a: entrance passage, b to m, m': water channel,
S: Exit passage.
Claims (1)
部とからなる電極内に截頭円錐柱部の軸を中心と
する略円形状あるいは半円弧状の水路を多重に設
けて、前記水路の隣接端部を屈曲通路にて連結す
るとともに、前記電極に併設されている支持首部
内に設けた入口通路を前記水路の最内側に直結し
かつ前記入口通路を囲む出口通路を前記水路の最
外側に直結した冷却水路を設け、前記截頭円錐柱
部内における前記冷却水路を小断面積にしかつ外
表面に近接させて多数配設したことに特徴を有す
る粒子加速管中に整列して垂設される粒子加速器
の加速電極。1. Multiple approximately circular or semi-circular water channels centered around the axis of the truncated conical column are provided in an electrode consisting of an outer flat disk portion and a perforated truncated conical column portion at the center. , the adjacent ends of the water channel are connected by a bent passage, an inlet passage provided in a support neck attached to the electrode is directly connected to the innermost side of the water channel, and an outlet passage surrounding the inlet passage is connected to the outlet passage. A cooling water channel directly connected to the outermost side of the water channel is provided, and the cooling water channels in the truncated conical column part have a small cross-sectional area and are arranged in large numbers in close proximity to the outer surface of the particle acceleration tube. Accelerating electrode of a particle accelerator installed vertically.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3811882A JPS58155700A (en) | 1982-03-12 | 1982-03-12 | Accelerating electrode for particle accelerator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3811882A JPS58155700A (en) | 1982-03-12 | 1982-03-12 | Accelerating electrode for particle accelerator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58155700A JPS58155700A (en) | 1983-09-16 |
| JPH0326520B2 true JPH0326520B2 (en) | 1991-04-11 |
Family
ID=12516547
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3811882A Granted JPS58155700A (en) | 1982-03-12 | 1982-03-12 | Accelerating electrode for particle accelerator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58155700A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CA2911525A1 (en) | 2013-05-17 | 2014-11-20 | Martin A. Stuart | Dielectric wall accelerator utilizing diamond or diamond like carbon |
| JP6653650B2 (en) * | 2013-11-21 | 2020-02-26 | バーバラ スチュアート | Reactor |
-
1982
- 1982-03-12 JP JP3811882A patent/JPS58155700A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58155700A (en) | 1983-09-16 |
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