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JPH0145560B2 - - Google Patents
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JPH0145560B2 - - Google Patents

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Publication number
JPH0145560B2
JPH0145560B2 JP55182901A JP18290180A JPH0145560B2 JP H0145560 B2 JPH0145560 B2 JP H0145560B2 JP 55182901 A JP55182901 A JP 55182901A JP 18290180 A JP18290180 A JP 18290180A JP H0145560 B2 JPH0145560 B2 JP H0145560B2
Authority
JP
Japan
Prior art keywords
heat
wick
heat pipe
magnetic material
section
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
Application number
JP55182901A
Other languages
Japanese (ja)
Other versions
JPS57108592A (en
Inventor
Kazuyasu Takahashi
Masataka Mochizuki
Koichi Masuko
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fujikura Cable Works Ltd
Original Assignee
Fujikura Cable Works Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Fujikura Cable Works Ltd filed Critical Fujikura Cable Works Ltd
Priority to JP55182901A priority Critical patent/JPS57108592A/en
Publication of JPS57108592A publication Critical patent/JPS57108592A/en
Publication of JPH0145560B2 publication Critical patent/JPH0145560B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Heat-Exchange Devices With Radiators And Conduit Assemblies (AREA)
  • General Induction Heating (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は熱伝達の制御できるヒートパイプに関
するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a heat pipe whose heat transfer can be controlled.

ヒートパイプは熱特性がすぐれていることか
ら、物の加熱、冷却についてあらゆる分野で利用
される。
Heat pipes have excellent thermal properties and are used in all fields for heating and cooling objects.

従来の技術 ヒートパイプは通常熱負荷に応じて熱輸送を行
つている。
Conventional technology Heat pipes usually transport heat according to the heat load.

これは、熱源・吸熱源の状態によつてヒートパ
イプの作動温度が定まり、熱輸送を行う媒体であ
る作動流体の気相、液相の繰返し変化が適切に行
なわれているからである。
This is because the operating temperature of the heat pipe is determined by the conditions of the heat source and heat absorption source, and the working fluid, which is the medium for heat transport, is repeatedly changed between the gas phase and the liquid phase in an appropriate manner.

しかし、ここで例えば熱負荷にとつて輸送され
る熱量が所望の価からはずれる事態が生じ、過熱
ないし過冷状態となる場合が生ずる。
However, here, for example, a situation occurs in which the amount of heat transported in response to a heat load deviates from a desired value, resulting in an overheating or undercooling state.

このような状態では当然輸送される熱は有効に
使われず、結局熱効率の低下をきたす。
Under such conditions, the transported heat is naturally not used effectively, resulting in a decrease in thermal efficiency.

発明が解決しようとする課題 本発明は以上の事情に鑑みてなされたもので、
熱源、吸熱源すなわち熱負荷の状態に応じて、伝
達される熱を制御し、ヒートパイプの熱輸送を有
効にし、被熱物の過熱、過冷を防ごうとするもの
である。
Problems to be Solved by the Invention The present invention has been made in view of the above circumstances.
The purpose is to control the transferred heat according to the state of the heat source and heat absorption source, that is, the heat load, to make the heat transport of the heat pipe effective, and to prevent the object to be heated from being overheated or overcooled.

発明が解決しようとする手段 中空棒状密封容器内壁にウイツクが設けられ、
かつ同容器内に作動流体が封入され、その流手方
向の一端部を蒸発部とし、中間部を断熱部とし、
他端部を凝縮部とするヒートパイプにおいて、前
記断熱部の位置のウイツクを積層金網状によつて
弾性磁性材とし、前記ヒートパイプ上の、前記磁
性材ウイツクに対応する位置に、ヒートパイプの
外方へ向つて放射状に、磁性材ウイツクに収縮力
を与える電気的磁界発生手段が設けられてなるヒ
ートパイプ。
Means to be Solved by the Invention A wick is provided on the inner wall of the hollow rod-shaped sealed container,
and a working fluid is sealed in the container, one end in the flow direction is an evaporation part, the middle part is a heat insulating part,
In a heat pipe in which the other end is a condensing part, the wick at the position of the heat insulating part is made of an elastic magnetic material in the form of a laminated wire mesh, and the heat pipe is placed at a position corresponding to the magnetic material wick on the heat pipe. A heat pipe that is provided with electric magnetic field generating means that applies a contraction force to a magnetic material radially outward.

作 用 ヒートパイプにおいて蒸発部に凝縮液化した作
動流体が溜つていて、これが加熱されると蒸発、
気化して断熱された中間部である断熱部を通過
し、熱負荷のある凝縮部に移動し、ここで吸熱さ
れて、凝縮液化し、毛細管作用をなすウイツクを
通つて再び蒸発部に移動し、ここで再び同じ液相
→気相→液相の相変化サイクルを繰返す。
Function In a heat pipe, condensed and liquefied working fluid accumulates in the evaporator section, and when it is heated, it evaporates.
It evaporates and passes through an insulated intermediate section, the adiabatic section, and moves to the condensing section, which has a heat load, where it absorbs heat, condenses and liquefies, and passes through the capillary action to the evaporating section again. , and here the same phase change cycle of liquid phase → gas phase → liquid phase is repeated again.

この状態において、ヒートパイプの断熱部の位
置のウイツクを積層された金網状の弾性磁性材か
らなるものとし、この磁性材ウイツクに毛細管作
用をなす空隙を持たせる。
In this state, the wick at the heat insulating part of the heat pipe is made of a laminated wire mesh-like elastic magnetic material, and this magnetic material wick is provided with a gap that acts as a capillary tube.

前記磁性材ウイツクにヒートパイプの外方へ向
つて放射状に磁力が作用すると、ウイツクの空隙
の密度を所望の密度にし、粗、密の程度に応じて
ウイツクを通る凝縮液化した作動流体の移動量が
制御され、その結果熱輸送量が適当な量に確保さ
れる。
When a magnetic force acts radially on the magnetic material wick toward the outside of the heat pipe, the density of the voids in the wick becomes the desired density, and the amount of movement of the condensed and liquefied working fluid through the wick changes depending on the degree of coarseness or density. is controlled, and as a result, an appropriate amount of heat transport is ensured.

実施例 本発明の実施例を図によつて説明すると(特に
第1図)、1は本発明に係るヒートパイプであつ
て、中空棒状密封容器であつて以下の構成からな
る。
Embodiment An embodiment of the present invention will be described with reference to the drawings (particularly FIG. 1). Reference numeral 1 is a heat pipe according to the present invention, which is a hollow rod-shaped sealed container having the following configuration.

すなわち、2は通常用いられる金網状の銅製の
ウイツクであり、ヒートパイプ1の内壁に設けら
れている。
That is, reference numeral 2 denotes a wire-mesh-like copper wick that is commonly used, and is provided on the inner wall of the heat pipe 1.

21は他の磁性材ウイツクであつて、磁性材例
えば鉄製の積層された金網状のウイツクであり、
ヒートパイプ1の長手方向一定の箇所すなわち断
熱部であつて、例えば中央附近に設けられてい
る。
21 is another magnetic material wick, which is a wire mesh-shaped wick made of a magnetic material such as iron and laminated;
It is a constant location in the longitudinal direction of the heat pipe 1, that is, a heat insulating portion, and is provided, for example, near the center.

この磁性材ウイツク21は適度な空隙を有し、
この空隙が粗、密の状態の繰返しが可能に復元力
が働く程度の弾性を持たせてある。
This magnetic material wick 21 has an appropriate gap,
These voids are made to have enough elasticity to exert a restoring force so that they can be repeatedly changed between sparse and dense states.

この磁性材ウイツク21を後述する作動流体が
毛細管作用によつて通るときに、磁性材ウイツク
21の空隙の粗、密状態に応じて、通過量が制御
される。
When a working fluid, which will be described later, passes through the magnetic material wick 21 by capillary action, the amount of passage is controlled depending on whether the gap in the magnetic material wick 21 is coarse or dense.

3はヒートパイプ1の外側で前記磁性材ウイツ
ク21の対応した位置に設けられた電気的磁界発
生用手段であつて巻線31より構成されている。
Reference numeral 3 denotes an electric magnetic field generating means provided outside the heat pipe 1 at a position corresponding to the magnetic material wick 21, and is composed of a winding 31.

巻線31はヒートパイプ1の外方へ向つて放射
状に、前記磁性材ウイツク21に収縮力を与える
作用が果せるように巻回されている。
The winding 31 is wound radially outward of the heat pipe 1 so as to exert a contraction force on the magnetic material wick 21.

すなわち、例えば、ヒートパイプ1の外側に長
手方向に直角にジグザグ状に周方向にわたつて巻
回されている。
That is, for example, it is wound around the outside of the heat pipe 1 in a zigzag shape at right angles to the longitudinal direction over the circumferential direction.

この巻線3に可変の直流電流を流せばヒートパ
イプの外方へ向つて放射状に磁力が生じ、磁性材
ウイツク21に上記方向に収縮力が働らく。
When a variable direct current is passed through this winding 3, a magnetic force is generated radially outward of the heat pipe, and a contraction force acts on the magnetic material wick 21 in the above direction.

4は蒸発部、5は断熱部、6は凝縮部であつ
て、上記ヒートパイプ1には作動流体7例えばア
ンモニヤが充填されている。
4 is an evaporation section, 5 is a heat insulating section, and 6 is a condensation section, and the heat pipe 1 is filled with a working fluid 7 such as ammonia.

作動流体7が凝縮液化して、上記蒸発部4に溜
つていると、蒸発部4の熱源で熱せられて、蒸発
気化し、上記断熱部5を通過して、上記凝縮部6
に移送される。
When the working fluid 7 is condensed and liquefied and accumulated in the evaporation section 4, it is heated by the heat source of the evaporation section 4, evaporates and vaporizes, passes through the insulation section 5, and becomes the condensation section 6.
will be transferred to.

凝縮部6で熱負荷に熱を与えると作動流体7は
凝縮液化して前記銅製のウイツク2、磁性材ウイ
ツク21を毛細管作用によつて移動する。
When heat is applied to the thermal load in the condensing section 6, the working fluid 7 is condensed and liquefied, and moves through the copper wick 2 and the magnetic material wick 21 by capillary action.

流動流体7が磁性材ウイツク21を移動する際
に一部上述したごとく磁性材ウイツク21の空隙
の粗、密の状態に応じて通過する液量が制御さ
れ、その結果、蒸発部4に溜まる液量が制御さ
れ、結局蒸発気化量も制御されるから熱輸送量が
熱負荷の状態に適合するよう制御される。
When the flowing fluid 7 moves through the magnetic material wick 21, the amount of liquid passing through the magnetic material wick 21 is controlled depending on the sparseness or density of the gaps in the magnetic material wick 21, as described in part above, and as a result, the amount of liquid that accumulates in the evaporator 4 is reduced. Since the amount of evaporation is controlled, and the amount of evaporation is also controlled, the amount of heat transport is controlled to match the state of heat load.

ここで上記方向に収縮力が働らくメカニズムを
第2図を用いて説明する。
Here, the mechanism by which the contraction force acts in the above direction will be explained using FIG. 2.

第2図は第1図をAA′に沿つて破断した破断断
面図であつて、それぞれ図の向きに、すなわちB
においては紙面に向かつて垂直方向に手前側に電
流が流れ、Cにおいては紙面に向かつて垂直方向
に向側に流れているとする。
FIG. 2 is a cutaway cross-sectional view of FIG.
It is assumed that in case C, the current flows vertically toward the front side toward the paper surface, and in C, the current flows vertically toward the paper surface toward the opposite side.

Bにおいては図のごとく左回りの磁界、Cにお
いては図のごとく右回りの磁界が生じる。矢印の
大きさは磁界の強さに比例した強さであることを
意味する。
At B, a counterclockwise magnetic field is generated as shown in the figure, and at C, a clockwise magnetic field is generated as shown. The size of the arrow means that the strength is proportional to the strength of the magnetic field.

Dにおいては、ヒートパイプ1の外方へ向つて
放射状に磁力が合成されて、この方向に磁力が生
ずる。同様にしてここで矢印の大きさは磁力の大
きさに比例した大きさを表わす意味である。一方
Eにおいては、上記と逆方向の磁力が生ずるが、
弾性磁性材ウイツク21はヒートパイプ1の内壁
に密着して装着されているので、内方への引張力
に働いても、殆んど伸張することがない。
At D, the magnetic forces are combined radially outward of the heat pipe 1, and a magnetic force is generated in this direction. Similarly, the size of the arrow here means the size proportional to the size of the magnetic force. On the other hand, at E, a magnetic force occurs in the opposite direction to the above, but
Since the elastic magnetic material wick 21 is attached closely to the inner wall of the heat pipe 1, it hardly stretches even if an inward tensile force is applied.

上記磁力が働いて磁性材ウイツク21がヒート
パイプ1の外方へ向つて放射状に収縮力を受けて
いる場合の概念を示す。
The concept is shown in which the magnetic material wick 21 receives a contracting force radially outward of the heat pipe 1 due to the above-mentioned magnetic force.

すなわち、Fにおいては収縮力が働らき、ヒー
トパイプ1の外方に収縮する。
That is, a contraction force acts at F, causing the heat pipe 1 to contract outward.

Hに磁性材ウイツク21が収縮した状態の概念
図を示す。
A conceptual diagram of the state in which the magnetic material wick 21 is contracted is shown in FIG.

Gにおいては引張力が働らくが、一部上述した
ごとく磁性材ウイツク21がヒートパイプ1の内
壁に固着されているので内方へは引張られず、し
たがつて空隙が現状より拡がることはない。
A tensile force acts at G, but as mentioned above, the magnetic material wick 21 is fixed to the inner wall of the heat pipe 1, so it is not pulled inward, and therefore the gap will not become wider than it is now. .

なお、ヒートパイプ1の磁性材ウイツク21に
磁力が働らかないときの磁性材ウイツク21の状
態を第2図中のKに示した。
The state of the magnetic material wick 21 when no magnetic force acts on the magnetic material wick 21 of the heat pipe 1 is shown at K in FIG.

次に本発明のヒートパイプについてその作用を
更に具体的に説明すると、例えば巻線31に
1.5A/mm2の電流密度の電流が流れ作動流体7が
移動して100℃の熱伝達が行なわれている場合、
100℃が過熱状態であり、80℃の熱伝達が所望の
価であれば電流密度を2.5A/mm2として磁力を強
めると鉄製のウイツク21の空隙が狭められて作
動流体7の移動流量が減少するので所望の温度の
熱伝達ができる。
Next, to explain the action of the heat pipe of the present invention in more detail, for example, the winding 31
When a current with a current density of 1.5 A/mm 2 flows and the working fluid 7 moves, heat transfer of 100°C occurs.
If 100°C is the overheating state and the desired heat transfer is 80°C, then if the current density is set to 2.5A/mm 2 and the magnetic force is strengthened, the gap in the iron wick 21 will be narrowed and the moving flow rate of the working fluid 7 will be reduced. Since the temperature decreases, heat transfer at the desired temperature can be achieved.

本発明は上記実施例に限定されるものではな
く、ウイツクは少くとも巻線に対応した部分は磁
性材である鉄製の金網であればよいが、他の部分
も同様のウイツクで構成されてよいことは勿論で
ある。
The present invention is not limited to the above-mentioned embodiments, and at least the part corresponding to the winding wire may be made of iron wire mesh made of magnetic material, but other parts may also be constructed of a similar wick. Of course.

更にヒートパイプの形状も中空円筒形、中空角
柱形を問わず、巻線も通常使用されるものであれ
ばこれに適用できる。
Further, the shape of the heat pipe can be either a hollow cylinder or a hollow prism, and the heat pipe can be applied to any commonly used winding wire.

発明の効果 以上述べたごとく本発明によればヒートパイプ
の断熱部の位置のウイツクを磁性材とし、これに
対応した位置のヒートパイプの外側に設けられた
巻線の直流電流を調節することによつてヒートパ
イプのウイツクの空隙を密にしたり粗にしたりす
ることによつて容易にヒートパイプの熱伝達を広
範囲に制御できる。
Effects of the Invention As described above, according to the present invention, the wires at the heat insulating portions of the heat pipes are made of magnetic material, and the DC current of the windings provided on the outside of the heat pipes at the corresponding positions is adjusted. Therefore, by making the gaps in the heat pipe dense or coarse, the heat transfer in the heat pipe can be easily controlled over a wide range.

又磁性材ウイツク21はヒートパイプの外方へ
向つて放射状に密、粗の動作をするのみで長手方
向に対しては密、粗の動作をしないので密、粗を
くり返すことによつて磁性材ウイツク21がヒー
トパイプの内壁からずり落ちることになる危険も
ない。
In addition, the magnetic material wick 21 only performs dense and coarse movements radially toward the outside of the heat pipe, but does not perform dense and coarse movements in the longitudinal direction, so repeating the dense and coarse movements makes it magnetic. There is no danger that the material wick 21 will slip off the inner wall of the heat pipe.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明のヒートパイプに関する一部切
裁断面図。第2図は本発明において磁性材ウイツ
ク21に収縮力が働くメカニズムの説明図。 図中 1……ヒートパイプ、2……銅製ウイツ
ク、21……鉄製の金網状の磁性材ウイツク、3
……電気的磁界発生用手段、31……巻線、4…
…蒸発部、5……断熱部、6……凝縮部、7……
作動流体である。
FIG. 1 is a partially cutaway sectional view of the heat pipe of the present invention. FIG. 2 is an explanatory diagram of the mechanism by which contractile force acts on the magnetic material wick 21 in the present invention. In the diagram: 1... Heat pipe, 2... Copper wick, 21... Iron wire mesh magnetic material wick, 3
...Electrical magnetic field generating means, 31...Winding, 4...
...Evaporation section, 5...Insulation section, 6...Condensation section, 7...
It is a working fluid.

Claims (1)

【特許請求の範囲】[Claims] 1 中空棒状密封容器内壁にウイツクが設けら
れ、かつ同容器内に作動流体が封入され、その長
手方向の一端部を蒸発部とし、中間部を断熱部と
し、他端部を凝縮部とするヒートパイプにおい
て、前記断熱部の位置のウイツクを積層金網状の
弾性磁性材とし、前記ヒートパイプ上の、前記磁
性材ウイツクに対応する位置に、ヒートパイプの
外方へ向つて放射状に、磁性材ウイツクに収縮力
を与える電気的磁界発生手段が設けられてなるヒ
ートパイプ。
1 A heat device in which a hollow rod-shaped sealed container is provided with a wick on the inner wall, a working fluid is sealed in the container, one longitudinal end of the container serves as an evaporation section, the middle section serves as a heat insulating section, and the other end serves as a condensation section. In the pipe, the wick at the position of the heat insulating part is made of an elastic magnetic material in the form of a laminated wire mesh, and the magnetic material wick is placed on the heat pipe at a position corresponding to the magnetic material wick in a radial direction toward the outside of the heat pipe. A heat pipe that is equipped with an electric magnetic field generating means that applies a contraction force to the heat pipe.
JP55182901A 1980-12-25 1980-12-25 Heat pipe Granted JPS57108592A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP55182901A JPS57108592A (en) 1980-12-25 1980-12-25 Heat pipe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55182901A JPS57108592A (en) 1980-12-25 1980-12-25 Heat pipe

Publications (2)

Publication Number Publication Date
JPS57108592A JPS57108592A (en) 1982-07-06
JPH0145560B2 true JPH0145560B2 (en) 1989-10-04

Family

ID=16126356

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55182901A Granted JPS57108592A (en) 1980-12-25 1980-12-25 Heat pipe

Country Status (1)

Country Link
JP (1) JPS57108592A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWM264484U (en) * 2004-10-27 2005-05-11 Jia-Hau Li Forming structure of heat-pipe multi-layered capillary constitution

Also Published As

Publication number Publication date
JPS57108592A (en) 1982-07-06

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