JP3069914B2 - Fluid distribution method to heat absorbing wall in space environment test equipment - Google Patents
Fluid distribution method to heat absorbing wall in space environment test equipmentInfo
- Publication number
- JP3069914B2 JP3069914B2 JP2331731A JP33173190A JP3069914B2 JP 3069914 B2 JP3069914 B2 JP 3069914B2 JP 2331731 A JP2331731 A JP 2331731A JP 33173190 A JP33173190 A JP 33173190A JP 3069914 B2 JP3069914 B2 JP 3069914B2
- Authority
- JP
- Japan
- Prior art keywords
- heat absorbing
- absorbing wall
- space environment
- environment test
- test equipment
- 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 - Fee Related
Links
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B64—AIRCRAFT; AVIATION; COSMONAUTICS
- B64G—COSMONAUTICS; VEHICLES OR EQUIPMENT THEREFOR
- B64G7/00—Simulating cosmonautic conditions, e.g. for conditioning crews
- B64G2007/005—Space simulation vacuum chambers
Landscapes
- Testing Of Devices, Machine Parts, Or Other Structures Thereof (AREA)
- Devices For Use In Laboratory Experiments (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、宇宙環境と略同等の高真空,極低温の環境
を形成し、人工衛星等の宇宙空間で使用される各種機器
の試験を行う宇宙環境試験装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention forms a high-vacuum and cryogenic environment which is almost equivalent to the space environment, and is used for testing various devices used in space such as artificial satellites. Related to space environment test equipment.
宇宙環境試験装置(スペースチェンバー)は、一般
に、真空容器の内部にシュラウド又はシールドと呼ばれ
る熱吸収壁を設置して宇宙の冷暗黒を模擬するととも
に、真空容器の内部を真空ポンプで真空排気して宇宙の
高真空を模擬するものである。即ち、シュラウドを100K
以下に冷却して、宇宙の冷暗黒を模擬するのが一般的で
あり、その寒冷源としては、主に液体窒素が用いられて
きている。さらに、前記真空容器内に放出ガスの多い試
験体を収容して高真空に排気するためには、非常に大き
なポンプを用いて排気する必要があるが、このような場
合には、真空容器の内部、シュラウド内に極低温排気
面、即ちクライオパネルを組み込んで、該クライオパネ
ルを20K以下に冷却し、窒素等のガスを凝結排気するク
ライオポンプとして機能させる必要があった。このクラ
イオパネルの冷却源には、従来からヘリウム冷凍機から
供給されるヘリウムが用いられている。In general, a space environment test apparatus (space chamber) simulates the darkness and darkness of the universe by installing a heat absorbing wall called a shroud or a shield inside a vacuum vessel, and evacuating the inside of the vacuum vessel with a vacuum pump. It simulates the high vacuum of the universe. That is, shroud 100K
It is common to simulate the darkness and darkness of the universe by cooling below, and liquid nitrogen has been mainly used as the cold source. Furthermore, in order to accommodate a specimen with a large amount of released gas in the vacuum container and to evacuate it to a high vacuum, it is necessary to evacuate using a very large pump. It was necessary to incorporate a cryogenic exhaust surface, that is, a cryopanel inside the shroud, to cool the cryopanel to 20K or less, and to function as a cryopump for condensing and exhausting gas such as nitrogen. Helium supplied from a helium refrigerator is conventionally used as a cooling source for the cryopanel.
また、試験完了後に真空容器内を常温まで加温する際
には、一般に、窒素ガスをシュラウドに導入することに
より行われていた。In addition, when the inside of the vacuum vessel is heated to room temperature after the test is completed, it is generally performed by introducing nitrogen gas into the shroud.
このような宇宙環境試験装置において、前記シュラウ
ドやクライオパネルとしては、マニホールドと呼ばれる
集合管にフィン管を多数接合して形成したものが用いら
れている。In such a space environment test apparatus, a shroud or a cryopanel formed by joining a plurality of fin tubes to a collecting tube called a manifold is used.
しかしながら、上記多数のフィン管を用いたシュラウ
ド等に、液体窒素やヘリウムからなる冷流体を供給する
にあたっては、シュラウド等の中で熱負荷が最も多く、
最も大量に冷流体を必要とするフィン管の流量に合わせ
て全てのフィン管に冷流体を分配していた。また円盤状
のシュラウド等のようににフィン管の長さが異なるもの
においても、熱負荷が最も大きい長いフィン管に合わせ
て冷流体を供給するため、長さが短く流動抵抗の少ない
他のフィン管には無駄な量の冷流体が供給されることに
なり、必要以上に大量の冷流体を使用していた。However, when supplying a cold fluid such as liquid nitrogen or helium to a shroud using a large number of fin tubes, the heat load is the largest among the shrouds and the like.
The cold fluid was distributed to all the fin tubes according to the flow rate of the fin tubes requiring the largest amount of the cold fluid. In addition, even for fin tubes with different lengths, such as a disk-shaped shroud, other fins with a short length and low flow resistance are supplied because the cooling fluid is supplied according to the long fin tube with the largest heat load. An unnecessary amount of cold fluid was supplied to the tube, and an excessively large amount of cold fluid was used.
そこで本発明は、それぞれのフィン管が受ける熱負荷
に応じて冷流体を供給でき、上記冷流体の無駄を防止で
きる流体分配方法を提供することを目的としている。Therefore, an object of the present invention is to provide a fluid distribution method capable of supplying a cold fluid according to the heat load received by each fin tube and preventing the waste of the cold fluid.
上記した目的を達成するために、本発明の宇宙環境試
験装置における熱吸収壁への流体分配方法は、真空容器
の内部に多数のフィン管を併設した熱吸収壁を配設し、
該熱吸収壁のフィン管にマニホールドを介して冷流体を
供給し、前記真空容器内を冷却するにあたり、前記マニ
ホールドとフィン管との接合部に、それぞれのフィン管
に流入する冷流体の流量を制御する流量調整手段を設け
たことを特徴としている。In order to achieve the above object, a method for distributing fluid to a heat absorbing wall in the space environment test apparatus of the present invention includes disposing a heat absorbing wall provided with a number of fin tubes inside a vacuum vessel,
A cold fluid is supplied to the fin tubes of the heat absorbing wall through a manifold, and when cooling the inside of the vacuum vessel, the flow rate of the cold fluid flowing into each fin tube at a junction between the manifold and the fin tubes is reduced. It is characterized in that flow rate adjusting means for controlling is provided.
以下、本発明を図面に示す実施例に基づいて、さらに
詳細に説明する。Hereinafter, the present invention will be described in more detail based on embodiments shown in the drawings.
まず、第3図及び第4図に示すように、本実施例に示
す宇宙環境試験装置1は、真空容器2内に複数のブロッ
クに分割形成された胴部シュラウド3と容器両端の鏡部
シュラウド4とを配設したもので、各シュラウド3,4
は、それぞれに液体窒素導入用の入口マニホールド5と
出口マニホールド6とを備えており、各シュラウド3,4
の下部側に入口マニホールド5が、上部側に出口マニホ
ールド6が位置するように配置されている。First, as shown in FIGS. 3 and 4, a space environment test apparatus 1 according to this embodiment includes a body shroud 3 formed in a vacuum vessel 2 divided into a plurality of blocks and mirror shrouds at both ends of the vessel. 4 and each shroud 3,4
Is provided with an inlet manifold 5 and an outlet manifold 6 for introducing liquid nitrogen, respectively.
The inlet manifold 5 is located on the lower side of the device, and the outlet manifold 6 is located on the upper side.
上記シュラウド3,4は、第1図に示すように、管体の
両側に翼辺を一体に設けたフィン管7を隙間無く多数並
べたものであり、その両端は、それぞれベント管8,カッ
プリング9,10を介して前記入口マニホールド5又は出口
マニホールド6に接続している。As shown in FIG. 1, the shrouds 3 and 4 are formed by arranging a large number of fin tubes 7 integrally provided with wing sides on both sides of a tube without gaps. It is connected to the inlet manifold 5 or the outlet manifold 6 via rings 9 and 10.
そして、上記カップリング9,10の両方或いはいずれか
一方、好ましくは入口マニホールド5側のカップリング
9には、第2図に示すように、該カップリング9を流れ
る冷流体の流量を制御するためのオリフィス11が設けら
れている。このオリフィス11は、各フィン管7の状態に
よってその径、即ち流量が決定されるもので、フィン管
7の表面積,フィン管7の長さ,熱負荷,両マニホール
ドへの冷流体導入位置に対するフィン管7の取付け位置
等の各種条件に従って決定される。Then, as shown in FIG. 2, both or one of the couplings 9 and 10, preferably the coupling 9 on the inlet manifold 5 side, is used to control the flow rate of the cold fluid flowing through the coupling 9. Orifice 11 is provided. The diameter of the orifice 11, that is, the flow rate is determined by the state of each fin tube 7. It is determined according to various conditions such as the mounting position of the pipe 7.
例えば、第4図に示す円盤型シュラウドの場合には、
カップリング9のオリフィス11の径は、第5図に示すよ
うな分布を示す。即ち、中心部に位置し、長さが長く表
面積も大きなフィン管には多量の冷媒体を導入し、端部
側の長さが短く表面積も小さなフィン管には少量の冷媒
体を導入するように調整されている。For example, in the case of the disk type shroud shown in FIG.
The diameter of the orifice 11 of the coupling 9 shows a distribution as shown in FIG. That is, a large amount of refrigerant is introduced into a fin tube located at the center and having a long length and a large surface area, and a small amount of refrigerant is introduced into a fin tube having a short end surface and a small surface area. Has been adjusted.
オリフィス11の径を決定するためには、例えば、n本
の隣り合うフィン管間の圧力損失が等しいという条件
で、(n−1)個の連立方程式を立て、ニュートン−ラ
フソン(Newton−Raphson)法によって流量を求め、必
要流量に5%から20%程度を加えた範囲に冷流体を供給
するようにして決定することができる。In order to determine the diameter of the orifice 11, for example, under the condition that the pressure losses between n adjacent fin tubes are equal, (n-1) simultaneous equations are established and Newton-Raphson is determined. The flow rate is determined by the method, and the cooling fluid can be supplied in a range obtained by adding about 5% to 20% to the required flow rate.
尚、流量調整手段としては、上記のようにカップリン
グ9にオリフィス11を設けるほか、フィン管7に単にオ
リフィスを挿入する、前記ベント管の径や長さを変えて
流量調整機能を持たせる、マニホールドの接続口の径を
変えるなど、様々な手段で行うことが可能である。As the flow rate adjusting means, in addition to providing the orifice 11 in the coupling 9 as described above, simply inserting an orifice into the fin tube 7, and changing the diameter and length of the vent pipe to have a flow rate adjusting function. This can be performed by various means such as changing the diameter of the connection port of the manifold.
また、シュラウド等の細部の構造は、真空容器の大き
さやシュラウドの分割数等によって適宜最適な形状及び
組合わせを選択できる。Further, for the detailed structure of the shroud and the like, an optimal shape and combination can be appropriately selected depending on the size of the vacuum vessel, the number of divided shrouds and the like.
以上説明したように、本発明の宇宙環境試験装置にお
ける熱吸収壁への流体分配方法は、熱吸収壁の熱負荷や
流路抵抗に応じて最適な流量を設定できるので、ポン
プ,タンク等の給液設備の容量の低減、冷凍機設備の小
型化、消費エネルギーの低減等を図れる。As described above, in the method of distributing fluid to the heat absorbing wall in the space environment test apparatus of the present invention, the optimum flow rate can be set according to the heat load and the flow path resistance of the heat absorbing wall. The capacity of the liquid supply equipment can be reduced, the size of the refrigerator equipment can be reduced, and energy consumption can be reduced.
図は本発明の一実施例を示すもので、第1図はフィン管
の接続状態を示す側面図、第2図はフィン管の接続部の
拡大断面図、第3図はシュラウドの設置状態を示す概略
斜視図、第4図は円盤状シュラウドの正面図、第5図は
オリフィスの径分布を示す図である。 1……宇宙環境試験装置、2……真空容器、3……胴部
シュラウド、4……鏡部シュラウド、5……入口マニホ
ールド、6……出口マニホールド、7……フィン管、8
……ベント管、9,10……カップリング、11……オリフィ
スFIG. 1 shows an embodiment of the present invention. FIG. 1 is a side view showing a connection state of a fin tube, FIG. 2 is an enlarged sectional view of a connection portion of the fin tube, and FIG. FIG. 4 is a front view of a disk-shaped shroud, and FIG. 5 is a view showing a diameter distribution of an orifice. DESCRIPTION OF SYMBOLS 1 ... Space environment test apparatus, 2 ... Vacuum container, 3 ... Trunk shroud, 4 ... Mirror shroud, 5 ... Inlet manifold, 6 ... Outlet manifold, 7 ... Fin tube, 8
…… vent pipe, 9,10 …… coupling, 11 …… orifice
───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) B64G 7/00 ──────────────────────────────────────────────────続 き Continued on front page (58) Field surveyed (Int.Cl. 7 , DB name) B64G 7/00
Claims (1)
た熱吸収壁を配設し、該熱吸収壁のフィン管にマニホー
ルドを介して冷流体を供給し、前記真空容器内を冷却す
るにあたり、前記マニホールドとフィン管との接合部
に、それぞれのフィン管に流入する冷流体の流量を制御
する流量調整手段を設けたことを特徴とする宇宙環境試
験装置における熱吸収壁への流体分配方法。A heat absorbing wall provided with a number of fin tubes arranged inside a vacuum vessel, a cooling fluid is supplied to the fin tubes of the heat absorbing wall through a manifold, and the inside of the vacuum vessel is cooled. A flow control means for controlling a flow rate of a cold fluid flowing into each of the fin tubes at a joint portion between the manifold and the fin tubes. Method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2331731A JP3069914B2 (en) | 1990-11-29 | 1990-11-29 | Fluid distribution method to heat absorbing wall in space environment test equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2331731A JP3069914B2 (en) | 1990-11-29 | 1990-11-29 | Fluid distribution method to heat absorbing wall in space environment test equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04197900A JPH04197900A (en) | 1992-07-17 |
| JP3069914B2 true JP3069914B2 (en) | 2000-07-24 |
Family
ID=18246973
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2331731A Expired - Fee Related JP3069914B2 (en) | 1990-11-29 | 1990-11-29 | Fluid distribution method to heat absorbing wall in space environment test equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3069914B2 (en) |
-
1990
- 1990-11-29 JP JP2331731A patent/JP3069914B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04197900A (en) | 1992-07-17 |
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