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JP3799372B2 - Liquid target temperature measurement channel - Google Patents
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JP3799372B2 - Liquid target temperature measurement channel - Google Patents

Liquid target temperature measurement channel Download PDF

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Publication number
JP3799372B2
JP3799372B2 JP2001332320A JP2001332320A JP3799372B2 JP 3799372 B2 JP3799372 B2 JP 3799372B2 JP 2001332320 A JP2001332320 A JP 2001332320A JP 2001332320 A JP2001332320 A JP 2001332320A JP 3799372 B2 JP3799372 B2 JP 3799372B2
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JP
Japan
Prior art keywords
liquid metal
target
liquid
flow
temperature
Prior art date
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JP2001332320A
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Japanese (ja)
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JP2003139900A (en
Inventor
邦明 三浦
千明 山村
竜太郎 日野
雅紀 神永
勝洋 羽賀
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Sukegawa Electric Co Ltd
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Sukegawa Electric Co Ltd
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Description

【0001】
【発明の属する技術分野】
ターゲット容器の中を流れる液体金属に荷電粒子ビームを照射し、核破砕により液体金属中に中性子を発生させる液体ターゲットにおいて、ターゲット容器の中を流れる液体金属の温度を測定する液体ターゲット温度測定用チャンネルに関する。
【0002】
【従来の技術】
これまでの核破砕中性子源用液体ターゲットの構造は、流体の再循環流や流れの停滞域が生じて部分的な温度上昇(ホットスポット)が起こらないようにするため、ターゲット容器形状やその内部に配置される分配整流板の位置や形状が検討されてきた。しかし、ターゲット容器の中を流れる液体金属の温度測定のための検討は遅れていた。
【0003】
核破砕中性子源用液体ターゲットのターゲット容器の中を流れる液体金属に荷電粒子ビームを照射し、核破砕により液体金属中から中性子を発生させる場合、荷電粒子の衝突と核破砕反応により、液体金属が猛烈に発熱する。この猛烈に発熱するターゲット容器内を流れる液体金属の温度を測定するには、ナトリウムループ等で実績のあるシース型熱電対を使用するのが適当である。すなわち、シース型熱電対を使用し、その先端の測温点をターゲット容器内の液体金属の流れの中におき、ターゲット容器内を流れる液体金属の温度を測定するものである。
【0004】
【発明が解決しようとしている課題】
シース型熱電対の使用強度の観点からすると、シース型熱電対はターゲット容器の中を流れる液体金属に曝されるので、強度やエロージョン(潰食)を考慮するとシースは肉厚で太径にしなければならない。或いはウエル(鞘管)等でシース型熱電対を保護しなければならない。
【0005】
しかしこのような構造にすると、シース型熱電対の温度に対する測定値の応答速度が鈍化し、また液体金属の流れが阻害されてしまう。このため、測定値の応答速度や液体金属の流れに対する影響を考慮すると、シース型熱電対を細径にしてターゲット容器内の壁面に沿わせる構造が考えられる。
【0006】
しかしこのような構造にすると、今度は流体の温度を正確に測定することが出来ず、結果としてターゲット容器の内壁面の温度を測定する結果となってしまう。
これらのことから、シース型熱電対が液体金属の流れを阻害せずに、なお且つ液体金属の温度を正確に測定できるシース型熱電対の取付構造が要請される。
【0007】
本発明は、このような核破砕中性子源用液体ターゲットのターゲット容器内を流れる液体金属の温度を測定する場合の課題に鑑み、その目的は、シース型熱電対がターゲット容器内を流れる液体金属の流れを阻害せず、なお且つ液体金属の温度を正確に測定できる液体ターゲット温度測定用チャンネルを提供することにある。
【0008】
【課題を解決するための手段】
本発明では、前記の目的を達成するため、シース型熱電対6を液体金属が流れるターゲット容器1の壁面に取り付けるのではなく、ターゲット容器1の中に配置され、ターゲット容器1の中に流れる液体金属の流れを調整する分配整流板5にシース型熱電対6を取り付け、その測温接点7をこの分配整流板5から液体金属の流れの中に突出させるようにしたものである。
【0009】
すなわち、本発明による液体ターゲット温度測定用チャンネルは、ターゲット容器1の中を流れる液体金属に荷電粒子ビームを照射し、核破砕により液体金属中から中性子を発生させる場合に、ターゲット容器1の中を流れる液体金属の温度を測定するため、ターゲット容器1の中に配置され、ターゲット容器1の中に流れる液体金属の流れを調整する分配整流板5にシース型熱電対6を取り付け、このシース型熱電対6の測温点7を分配整流板5の表面から突出させて配置したものである。そのために、分配整流板5の全体または一部を中空にすると共に、その表面に中空な錘状の突起8を設け、分配整流板5の内部からシース型熱電対6の先端の測温点7を突起8の先端に導出し、その測温点7を突起8の先端でシールする。
【0010】
錘状の突起8は、分配整流板5から立ち上がった基部が太く、強度を有する一方、先端は容積が小さい。このため、シース型熱電対6の測温点7を保持する突起8の強度の確保が可能であると共に、測温点7付近の熱容量を小さくし、温度測定の応答性を確保することができる。
【0011】
また、突起8が液体金属の流れに強い抵抗を与えると、液体金属の流れが乱れ、突起8の背後にカルマンの渦列等を生じる原因となる。そこで、突起8が液体金属の流れにできるだけ影響を与えないように、突起8は流れの方向に対して長い扁平形状或いは流線型状とするのがよい。他方、シース型熱電対6により応答性よく液体金属の温度を測定するためには、その測温点7の部分では、突起8の容積が小さい方がよい。そこで、突起8はその立ち上がり部分の基部側を液体金属の流れの方向に長い扁平とし、シース型熱電対6の測温点7がシールされた突起8の頂点側を小径の円錐状とするのがよい。
【0012】
さらに、突起8が液体金属の流れに与える影響を出来るだけ小さくするため、分配整流板5の表面に複数の突起8が設けられ、且つそれらの突起8のうち液体金属の流れの方向に隣接するものは、液体金属の流れの方向に重ならないように、液体金属の流れと直交する方向にずらして配置するのがよい。
【0013】
このようにして、液体ターゲット温度測定用チャンネルを核破砕中性子発生用のターゲット容器1の内部に取付けて配置することによって、ターゲット容器1の中を流れる液体金属の流れに大きな影響を与えることなく、荷電粒子ビームが液体金属に照射される際に生じる液体金属の温度の変動が応答性よく測定できる。
【0014】
【発明の実施の形態】
次に、図面を参照しながら、本発明の実施の形態について、具体的且つ詳細に説明する。
核破砕中性子源用液体ターゲットの形状はこれまで様々な形状が提案されている。その一部の例を図1〜図3に示す。
【0015】
これらの液体ターゲットに共通したところは、ターゲット容器1が液体金属の入口2と出口3を有しており、流体の再循環流や流れの停滞域が生じて部分的な温度上昇(ホットスポット)が起こらないようにするため、ターゲット容器1の中に分配整流板5が配置してあることである。入口2からターゲット容器1に流入した液体金属が出口3側へ反転する箇所がターゲット部4であり、そこに太い矢印で示すように荷電粒子ビームが照射される。
【0016】
図1に示した液体ターゲットは、ターゲット容器1のターゲット部4の内部に対称に3枚ずつの分配整流板5を配置している。図2に示した液体ターゲットは、ターゲット容器1の入口2と出口3を仕切る中空の壁から延長してターゲット部4の内部に対称に1枚ずつのスリット付の分配整流板5を配置している。さらに、図3に示した液体ターゲットは、ターゲット容器1を二重管構造とし、外周側を入口2に、内周側を出口3とし、それら入口2と出口3を仕切る内部の管を分配整流板5としている。
【0017】
図4と図5に示すように、分配整流板5は基本的に板状であり、分配整流板5の内部を中空として、外表面の一部に中空状の突起8を形成する。少なくとも図4に矢印で示す液体金属の流れの方向に対して前後に隣接する突起8が液体金属の流れの方向に重ならないように、その流れの方向に直交する方向にずらして配置する。図示の例では、3つの全ての突起8、8…が液体金属が流れる方向に重ならないように、つまり突起8、8…が液体金属が流れる方向と直交する方向に互いにずれて配置されている。
【0018】
この突起8の基部側は、図4に矢印で示す液体金属の流れの方向に長い扁平形状或いは流線形状である。例えば、液体金属の流れの方向に長軸を有する楕円状である。他方、突起8の頂点は錘状に狭まって円形である。従ってこれらの突起8は、変則的な楕円錘及び円錐である。このため、突起8は全体として液体金属の流れの方向に長い扁平であるが、先端は円形で容積が小さい。
【0019】
中空な分配整流板5の内部と錐状の突起8の先端までは通じており、分配整流板5の内部から突起8の先端にシース型熱電対6を通す。そして、シース型熱電対6の一対の導電線の先端を接合した測温点7を突起8の先端部に配置し、この測温点7と共に突起8の先端部を溶接等で封止する。図5において、シース型熱電対6の引出線側は省略されている。
【0020】
このようにして分配整流板5の表面からシース型熱電対6の測温点7を液体金属の流れの中に突出し、分配整流板5そのものを液体ターゲット温度測定用チャンネルとする。すなわち、突起8の頂点にシース型熱電対6の測温点7を封止した分配整流板5を図1〜図3に示すようにしてターゲット容器1のターゲット部4の内部に配置し、ターゲット容器1のターゲット部4の中を流れる液体金属の温度を測定する。
【0021】
図6と図7は本発明の他の実施形態による分配整流板5を示す。分配整流板5の基本形状は板状であり、それらは液体金属の流れにより外力を受ける。そのため、強度等の理由で分配整流板5を中空にできない場合は、分配整流板5の表面の全部または一部に、中空状のチャンネル板10を取り付ける。このチャンネル板10の内部から突起8の先端にシース型熱電対6を通す。そして、シース型熱電対6の一対の導電線の先端を接合した測温点7を突起8の先端部に配置し、この測温点7と共に突起8の先端部を溶接等で封止する。図7においても、シース型熱電対6の引出線側は省略されている。
【0022】
このようにして分配整流板5の表面からシース型熱電対6の測温点7を液体金属の流れの中に突出し、分配整流板5を液体ターゲット温度測定用チャンネルとする。このような分配整流板5を図1〜図3に示すようにしてターゲット容器1のターゲット部4の内部に配置し、液体金属の温度を測定する。
【0023】
【発明の効果】
以上説明した通り、本発明による液体ターゲット温度測定用チャンネルでは、これを核破砕中性子発生用のターゲット容器1に取付けることによって、ターゲット容器1内を流れる液体金属の流れに対して大きな影響を与えることなく、ターゲット容器1内を流れる液体金属の温度を応答性よく測定することができる。従って、荷電粒子ビームがターゲット容器1内の液体金属に照射される際に生じる液体金属の温度が測定でき、発生中性子強度や液体ターゲット構造の除熱性能等の工学的データが取得できる。
【図面の簡単な説明】
【図1】本発明の実施形態による液体ターゲット温度測定用チャンネルを使用するターゲット容器の例を示す概略縦断側面図である。
【図2】本発明の実施形態による液体ターゲット温度測定用チャンネルを使用するターゲット容器の他の例を示す概略縦断側面図である。
【図3】本発明の実施形態による液体ターゲット温度測定用チャンネルを使用するターゲット容器の他の例を示す概略縦断側面図である。
【図4】本発明の一実施形態による液体ターゲット温度測定用チャンネルを示す概略平面図である。
【図5】図4のA−A線断面図である。
【図6】本発明の他の実施形態による液体ターゲット温度測定用チャンネルを示す概略平面図である。
【図7】図6のB−B線断面図である。
【符号の説明】
1 ターゲット容器
5 分配整流板
6 シース型熱電対
7 シース型熱電対の測温点
8 分配整流板の突起
[0001]
BACKGROUND OF THE INVENTION
Liquid target temperature measurement channel that measures the temperature of the liquid metal flowing in the target container in a liquid target that irradiates the liquid metal flowing in the target container with a charged particle beam and generates neutrons in the liquid metal by nuclear fragmentation. About.
[0002]
[Prior art]
The structure of the liquid target for the nuclear spallation neutron source so far does not cause a partial temperature rise (hot spot) due to the recirculation flow of the fluid or the stagnation region of the flow. The position and shape of the distribution rectifier plate arranged in the box have been studied. However, studies for measuring the temperature of liquid metal flowing in the target container have been delayed.
[0003]
When a charged metal beam is irradiated to a liquid metal flowing in the target vessel of a liquid target for a spallation neutron source and neutrons are generated from the liquid metal by spallation, the liquid metal is Fever fever. In order to measure the temperature of the liquid metal flowing in the target container that generates heat extremely, it is appropriate to use a sheathed thermocouple that has a proven record in a sodium loop or the like. That is, a sheath type thermocouple is used, a temperature measuring point at the tip thereof is placed in the flow of the liquid metal in the target container, and the temperature of the liquid metal flowing in the target container is measured.
[0004]
[Problems to be solved by the invention]
From the viewpoint of the strength of use of the sheathed thermocouple, the sheathed thermocouple is exposed to the liquid metal flowing in the target container, so the sheath must be thick and thick in consideration of strength and erosion. I must. Alternatively, the sheath type thermocouple must be protected by a well (sheath tube) or the like.
[0005]
However, with such a structure, the response speed of the measured value with respect to the temperature of the sheath type thermocouple is slowed, and the flow of the liquid metal is hindered. For this reason, considering the response speed of the measurement value and the flow of the liquid metal, a structure in which the sheath-type thermocouple is made thin along the wall surface in the target container can be considered.
[0006]
However, with such a structure, the temperature of the fluid cannot be accurately measured this time, and as a result, the temperature of the inner wall surface of the target container is measured.
For these reasons, there is a need for a sheathed thermocouple mounting structure in which the sheathed thermocouple can accurately measure the temperature of the liquid metal without hindering the flow of the liquid metal.
[0007]
In view of the problem of measuring the temperature of the liquid metal flowing in the target vessel of the liquid target for the spallation neutron source, the present invention aims at the liquid metal flowing in the target vessel by the sheath type thermocouple. An object of the present invention is to provide a liquid target temperature measurement channel that can accurately measure the temperature of the liquid metal without impeding the flow.
[0008]
[Means for Solving the Problems]
In the present invention, in order to achieve the above-mentioned object, the sheath-type thermocouple 6 is not attached to the wall surface of the target container 1 through which the liquid metal flows, but is disposed in the target container 1 and flows into the target container 1. A sheath type thermocouple 6 is attached to the distribution rectifying plate 5 for adjusting the metal flow, and the temperature measuring contact 7 is projected from the distribution rectifying plate 5 into the liquid metal flow.
[0009]
That is, the liquid target temperature measurement channel according to the present invention irradiates a liquid metal flowing in the target container 1 with a charged particle beam and generates neutrons from the liquid metal by nuclear fragmentation. In order to measure the temperature of the flowing liquid metal, a sheath type thermocouple 6 is attached to a distribution rectifying plate 5 which is arranged in the target container 1 and adjusts the flow of the liquid metal flowing into the target container 1, and this sheath type thermoelectric. The pair of temperature measuring points 7 are arranged so as to protrude from the surface of the distribution rectifying plate 5. For this purpose, the distribution rectifying plate 5 is entirely or partially hollowed, and a hollow weight-like projection 8 is provided on the surface thereof, and the temperature measuring point 7 at the tip of the sheath-type thermocouple 6 is provided from the inside of the distribution rectifying plate 5. Is led to the tip of the protrusion 8, and the temperature measuring point 7 is sealed with the tip of the protrusion 8.
[0010]
The weight-shaped protrusion 8 has a thick base and rises from the distribution rectifying plate 5, and has a small volume at the tip. For this reason, it is possible to ensure the strength of the protrusion 8 that holds the temperature measuring point 7 of the sheathed thermocouple 6 and to reduce the heat capacity in the vicinity of the temperature measuring point 7 and to ensure the responsiveness of temperature measurement. .
[0011]
Further, when the protrusion 8 gives a strong resistance to the flow of the liquid metal, the flow of the liquid metal is disturbed, which causes a Kalman vortex street or the like behind the protrusion 8. Therefore, it is preferable that the protrusion 8 has a flat shape or a streamline shape that is long in the flow direction so that the protrusion 8 does not affect the flow of the liquid metal as much as possible. On the other hand, in order to measure the temperature of the liquid metal with high responsiveness using the sheath type thermocouple 6, it is preferable that the volume of the protrusion 8 is small at the temperature measuring point 7. Therefore, the protrusions 8 a base side of the rising portion and a long flat in the direction of the liquid metal flow to the apex side of the projections 8 which temperature measuring point 7 of the sheath-type thermocouple 6 is sealed with the small diameter of the conical Is good.
[0012]
Furthermore, in order to minimize the influence of the protrusion 8 on the flow of the liquid metal, a plurality of protrusions 8 are provided on the surface of the distribution rectifying plate 5, and the protrusion 8 is adjacent to the liquid metal flow direction. It is preferable to dispose the object in a direction perpendicular to the liquid metal flow so as not to overlap the liquid metal flow direction.
[0013]
In this way, by arranging the liquid target temperature measurement channel inside the target container 1 for generating spallation neutrons, without greatly affecting the flow of the liquid metal flowing in the target container 1, Variations in the temperature of the liquid metal that occur when the charged particle beam is irradiated onto the liquid metal can be measured with good responsiveness.
[0014]
DETAILED DESCRIPTION OF THE INVENTION
Next, embodiments of the present invention will be described specifically and in detail with reference to the drawings.
Various shapes of the liquid target for the spallation neutron source have been proposed so far. Some examples are shown in FIGS.
[0015]
The common place for these liquid targets is that the target container 1 has an inlet 2 and an outlet 3 for liquid metal, and a recirculation flow of the fluid and a stagnation region of the flow occur, resulting in a partial temperature rise (hot spot). The distribution rectifying plate 5 is arranged in the target container 1 in order to prevent the occurrence of this. A portion where the liquid metal flowing into the target container 1 from the inlet 2 is reversed to the outlet 3 side is the target portion 4 where a charged particle beam is irradiated as indicated by a thick arrow.
[0016]
In the liquid target shown in FIG. 1, three distribution rectifying plates 5 are arranged symmetrically inside the target portion 4 of the target container 1. The liquid target shown in FIG. 2 extends from a hollow wall that partitions the inlet 2 and the outlet 3 of the target container 1, and has a distribution rectifying plate 5 with slits arranged symmetrically inside the target portion 4. Yes. Furthermore, the liquid target shown in FIG. 3 has a double-tube structure for the target container 1, the outer peripheral side is the inlet 2, the inner peripheral side is the outlet 3, and the inner pipe that partitions the inlet 2 and outlet 3 is distributed and rectified. The plate 5 is used.
[0017]
As shown in FIGS. 4 and 5, the distribution rectifying plate 5 is basically plate-shaped, and the inside of the distribution rectifying plate 5 is hollow, and a hollow protrusion 8 is formed on a part of the outer surface. At least the protrusions 8 adjacent in the front-rear direction with respect to the flow direction of the liquid metal indicated by arrows in FIG. 4 are arranged so as to be shifted in a direction perpendicular to the flow direction of the liquid metal. In the illustrated example, all the three protrusions 8, 8... Are arranged so as not to overlap each other in the direction in which the liquid metal flows, that is, the protrusions 8, 8,. .
[0018]
The base side of the protrusion 8 has a flat shape or a streamline shape that is long in the direction of the liquid metal flow indicated by an arrow in FIG. For example, an ellipse having a major axis in the direction of the flow of the liquid metal. On the other hand, the apex of the protrusion 8 is circular and narrowed to a weight. These protrusions 8 are therefore irregular elliptical cones and cones. Therefore, although the projection 8 is longer flat in the direction of the overall liquid metal flow, the tip is small volumes circular.
[0019]
The inside of the hollow distribution rectifying plate 5 communicates with the tip of the conical protrusion 8, and the sheath type thermocouple 6 is passed from the inside of the distribution rectifying plate 5 to the tip of the protrusion 8. Then, a temperature measuring point 7 where the tips of the pair of conductive wires of the sheath type thermocouple 6 are joined is arranged at the tip of the protrusion 8, and the tip of the protrusion 8 is sealed together with the temperature measuring point 7 by welding or the like. In FIG. 5, the lead wire side of the sheath type thermocouple 6 is omitted.
[0020]
In this way, the temperature measuring point 7 of the sheath type thermocouple 6 protrudes from the surface of the distribution rectifying plate 5 into the flow of the liquid metal, and the distribution rectifying plate 5 itself is used as a liquid target temperature measurement channel. That is, the distribution rectifying plate 5 in which the temperature measuring point 7 of the sheathed thermocouple 6 is sealed at the apex of the protrusion 8 is disposed inside the target portion 4 of the target container 1 as shown in FIGS. The temperature of the liquid metal flowing through the target portion 4 of the container 1 is measured.
[0021]
6 and 7 show a distribution rectifying plate 5 according to another embodiment of the present invention. The basic shape of the distribution rectifying plate 5 is plate-like, and they receive external force due to the flow of liquid metal. Therefore, when the distribution rectifying plate 5 cannot be made hollow for reasons such as strength, the hollow channel plate 10 is attached to all or a part of the surface of the distribution rectifying plate 5. The sheath type thermocouple 6 is passed from the inside of the channel plate 10 to the tip of the protrusion 8. Then, a temperature measuring point 7 where the tips of the pair of conductive wires of the sheath type thermocouple 6 are joined is arranged at the tip of the protrusion 8, and the tip of the protrusion 8 is sealed together with the temperature measuring point 7 by welding or the like. Also in FIG. 7, the lead wire side of the sheath type thermocouple 6 is omitted.
[0022]
In this way, the temperature measuring point 7 of the sheath type thermocouple 6 protrudes from the surface of the distribution rectifying plate 5 into the flow of the liquid metal, and the distribution rectifying plate 5 is used as a liquid target temperature measurement channel. Such a distribution rectifying plate 5 is disposed inside the target portion 4 of the target container 1 as shown in FIGS. 1 to 3, and the temperature of the liquid metal is measured.
[0023]
【The invention's effect】
As described above, in the liquid target temperature measurement channel according to the present invention, by attaching it to the target container 1 for generating spallation neutrons, the flow of the liquid metal flowing in the target container 1 is greatly affected. In addition, the temperature of the liquid metal flowing in the target container 1 can be measured with good responsiveness. Therefore, the temperature of the liquid metal generated when the charged metal beam is irradiated onto the liquid metal in the target container 1 can be measured, and engineering data such as the generated neutron intensity and the heat removal performance of the liquid target structure can be acquired.
[Brief description of the drawings]
FIG. 1 is a schematic longitudinal side view showing an example of a target container using a liquid target temperature measurement channel according to an embodiment of the present invention.
FIG. 2 is a schematic longitudinal side view showing another example of a target container using a liquid target temperature measurement channel according to an embodiment of the present invention.
FIG. 3 is a schematic longitudinal sectional side view showing another example of the target container using the liquid target temperature measurement channel according to the embodiment of the present invention.
FIG. 4 is a schematic plan view showing a liquid target temperature measurement channel according to an embodiment of the present invention.
5 is a cross-sectional view taken along line AA in FIG.
FIG. 6 is a schematic plan view showing a liquid target temperature measurement channel according to another embodiment of the present invention.
7 is a cross-sectional view taken along line BB in FIG.
[Explanation of symbols]
1 Target container 5 Distribution rectifying plate 6 Sheath type thermocouple 7 Temperature measuring point of sheath type thermocouple 8 Projection of distribution rectifying plate

Claims (3)

ターゲット容器(1)の中を流れる液体金属に荷電粒子ビームを照射し、核破砕により液体金属中から中性子を発生させる液体ターゲットに使用され、ターゲット容器(1)の中を流れる液体金属の温度を測定する液体ターゲット温度測定用チャンネルにおいて、ターゲット容器(1)の中に配置され、ターゲット容器(1)の中に流れる液体金属の流れを調整する分配整流板(5)の全体または一部を中空にすると共に、その表面に中空な錘状の突起(8)を設け、分配整流板(5)の内部からシース型熱電対(6)の先端の測温点(7)を突起(8)の先端に導出し、その測温点(7)を突起(8)の先端でシールすることにより、シース型熱電対(6)の測温点(7)を分配整流板(5)の表面から突出させて配置したことを特徴とする液体ターゲット温度測定用チャンネル。The liquid metal flowing in the target container (1) is irradiated with a charged particle beam and used for a liquid target that generates neutrons from the liquid metal by nuclear fragmentation. The temperature of the liquid metal flowing in the target container (1) is adjusted. In the liquid target temperature measurement channel to be measured, the distribution rectifying plate (5), which is arranged in the target container (1) and adjusts the flow of the liquid metal flowing in the target container (1), is entirely or partially hollow. In addition, a hollow spindle-shaped projection (8) is provided on the surface, and the temperature measuring point (7) at the tip of the sheath-type thermocouple (6) is provided from the inside of the distribution rectifying plate (5) to the projection (8). The temperature measuring point (7) of the sheath type thermocouple (6) protrudes from the surface of the distribution rectifying plate (5) by leading to the tip and sealing the temperature measuring point (7) with the tip of the protrusion (8). It is characterized by having arranged Liquid target for temperature measurement channel. 突起(8)の立ち上がり部分の基部側が液体金属の流れの方向に長い扁平形状または流線形状であり、シース型熱電対(6)の測温点(7)がシールされた突起(8)の頂点側が円錐状であることを特徴とする請求項1に記載の液体ターゲット温度測定用チャンネル。The base side of the rising portion of the protrusion (8) has a flat shape or a streamline shape that is long in the direction of the liquid metal flow, and the temperature measuring point (7) of the sheath type thermocouple (6) is sealed. The liquid target temperature measurement channel according to claim 1, wherein the apex side has a conical shape. 分配整流板(5)の表面に複数の突起(8)が設けられ、且つそれらの突起(8)のうち液体金属の流れの方向に前後に隣接するものは、液体金属の流れと直交する方向にずらして配置されていることを特徴とする請求項1または2に記載の液体ターゲット温度測定用チャンネル。  A plurality of projections (8) are provided on the surface of the distribution rectifying plate (5), and those projections (8) adjacent to the front and rear in the flow direction of the liquid metal are perpendicular to the flow of the liquid metal. The liquid target temperature measurement channel according to claim 1, wherein the channel is used for shifting the liquid target temperature.
JP2001332320A 2001-10-30 2001-10-30 Liquid target temperature measurement channel Expired - Fee Related JP3799372B2 (en)

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