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JPS5819014B2 - Heat pipe for solar collector - Google Patents
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JPS5819014B2 - Heat pipe for solar collector - Google Patents

Heat pipe for solar collector

Info

Publication number
JPS5819014B2
JPS5819014B2 JP54162575A JP16257579A JPS5819014B2 JP S5819014 B2 JPS5819014 B2 JP S5819014B2 JP 54162575 A JP54162575 A JP 54162575A JP 16257579 A JP16257579 A JP 16257579A JP S5819014 B2 JPS5819014 B2 JP S5819014B2
Authority
JP
Japan
Prior art keywords
heat
heat pipe
collector
solar
loss
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
JP54162575A
Other languages
Japanese (ja)
Other versions
JPS5685652A (en
Inventor
赤地久輝
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.)
Oki Electric Cable Co Ltd
Original Assignee
Oki Electric Cable Co 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 Oki Electric Cable Co Ltd filed Critical Oki Electric Cable Co Ltd
Priority to JP54162575A priority Critical patent/JPS5819014B2/en
Publication of JPS5685652A publication Critical patent/JPS5685652A/en
Publication of JPS5819014B2 publication Critical patent/JPS5819014B2/en
Expired legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F24HEATING; RANGES; VENTILATING
    • F24SSOLAR HEAT COLLECTORS; SOLAR HEAT SYSTEMS
    • F24S10/00Solar heat collectors using working fluids
    • F24S10/90Solar heat collectors using working fluids using internal thermosiphonic circulation
    • F24S10/95Solar heat collectors using working fluids using internal thermosiphonic circulation having evaporator sections and condenser sections, e.g. heat pipes
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/40Solar thermal energy, e.g. solar towers
    • Y02E10/44Heat exchange systems

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Sustainable Development (AREA)
  • Sustainable Energy (AREA)
  • Thermal Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)

Description

【発明の詳細な説明】 本発明は太陽熱コレクターに於ける太陽熱エネルギの吸
収構造及び該熱エネルギー移送構造の改善に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a solar thermal energy absorption structure and a thermal energy transfer structure in a solar collector.

太陽熱コレクターにおける太陽熱エネルギー吸収構造及
び移送構造としては各種のものがあるが何れも熱効率が
悪かったり構造が複雑であったり倒れも一長一短である
There are various types of solar energy absorption and transfer structures in solar collectors, but all of them have advantages and disadvantages, such as poor thermal efficiency, complicated structures, and the possibility of collapse.

最も一般的なものとして平板型コレクターがある。The most common type is a flat collector.

これは金属平板の片側平面に太陽熱吸収膜を形成し、そ
の裏面に金属管を形成又は接着してあり、吸収膜面から
吸収した熱エネルギーを熱伝導に依り金属管を加熱し、
その内壁にて水等の熱媒液と熱交換するものである。
In this method, a solar heat absorption film is formed on one side of a flat metal plate, and a metal tube is formed or glued on the back side of the metal plate, and the heat energy absorbed from the absorption film surface is heated to the metal tube by thermal conduction.
It exchanges heat with a heat medium liquid such as water on its inner wall.

これは受光面のエネルギー密度が小さいから高温度が得
られない。
This is because the energy density of the light-receiving surface is low, so high temperatures cannot be obtained.

従って断熱材に依り保温したとしても受光面の背面から
の放散、散失するエネルギーが大きい。
Therefore, even if heat is maintained using a heat insulating material, a large amount of energy is dissipated and dissipated from the back side of the light receiving surface.

水又は熱媒液を循環させるための循環装置が必須である
A circulation device for circulating water or heat transfer fluid is essential.

太陽熱コレクター全体として構造が複雑なため故障が多
い等の問題点かあ・つた。
The structure of the solar collector as a whole is complex, which causes problems such as frequent failures.

他の太陽熱コレクターの方式としてプラスチック管受光
型のものがある。
Another type of solar collector is the plastic tube type.

これは太陽熱吸収性の良い大口径管の中に貯水してあり
、プラスチック管表面で吸熱したエネルギーを管の内壁
で直接熱交換し、温水を得る方式で構造が極めて簡単な
利点がある反面、プラスチックの熱伝導率が悪いので受
光開始から熱交換開始迄の応答時間が遅い、熱吸収効率
が低く、受光エネルギー密度が小さいので高温が得られ
ない、等が問題点である。
This system stores water in large-diameter pipes that have good solar heat absorption, and the energy absorbed on the surface of the plastic pipe is directly exchanged with the inner wall of the pipe to obtain hot water, which has the advantage of an extremely simple structure. Problems include that the response time from the start of light reception to the start of heat exchange is slow due to the poor thermal conductivity of plastic, and that high temperatures cannot be obtained because the heat absorption efficiency is low and the received light energy density is low.

更に太陽熱コレクターの熱エネルギー吸収構造として真
空硝子管式受光管がある。
Furthermore, there is a vacuum glass tube type receiver tube as a thermal energy absorbing structure of a solar collector.

これは金属フィン付金属管を真空硝子管中に封じ込めた
構造であり、空気の対流に依る熱損失が無い、受光面の
裏面からの損失も極めて少い上に硝子管内面における再
反射に依る裏面からの熱吸収も追加される等の利点があ
る。
This has a structure in which a metal tube with metal fins is enclosed in a vacuum glass tube, so there is no heat loss due to air convection, loss from the back side of the light receiving surface is extremely small, and heat is absorbed by re-reflection on the inner surface of the glass tube. It has the advantage of additional heat absorption from the back side.

この構造は通常の平板型コレクターに比較して効率が良
く、硝子管のレンズ効果もあり、内面再反射もあるため
受光熱エネルギー密度が高いので・高温度が得られる。
This structure is more efficient than a normal flat collector, and because of the glass tube's lens effect and internal re-reflection, the received heat energy density is high and high temperatures can be obtained.

通常の平板型受光面で60℃位の温水が得られるのに対
し80℃位の高温水が得られるのでヒートポンプ等の補
助が無くても冷暖房にも利用出来るものである。
While hot water of about 60°C can be obtained with a normal flat light receiving surface, hot water of about 80°C can be obtained, so it can be used for air conditioning without the aid of a heat pump or the like.

然し構造が複雑であり又水又は熱媒液の循環装置も平板
型と同様に必須である。
However, the structure is complicated, and a circulation device for water or heat transfer fluid is also essential as in the flat plate type.

更に問題点としては真空硝子管は運搬、据付に細心の注
意を要すると共に、太陽熱コレクターシステム稼働後も
常に破損の危険に晒されている点である。
Another problem is that vacuum glass tubes require great care when transporting and installing them, and are always at risk of breakage even after the solar collector system is in operation.

平板型コレクターにおいても保護硝子板を有する構造の
場合、強風時等に飛来する物体に依る破損の危険が伴な
うものであるが保護硝子の破損はシステム稼働上は支障
は無いものである。
If a flat collector has a structure with a protective glass plate, there is a risk of damage due to flying objects during strong winds, but damage to the protective glass does not pose a problem in system operation.

然し真空管式の場合は真空硝子管の破損は受光エネルギ
ー密度の減小、対流熱損失の激増を意味するものでシス
テムとしては致命的な傷害となる。
However, in the case of a vacuum tube type, damage to the vacuum glass tube means a decrease in the received light energy density and a drastic increase in convective heat loss, resulting in fatal damage to the system.

真空硝子管は対流損失が無いので受光面であるフィンに
は何等の断熱保温手段が設けられて居らず従って一旦硝
子真空管が破損した場合は管内の空気対流だけでなく、
コレクター外部からの風の影響も受けて吸収熱エネルギ
ーの殆どが放散して了うに至る。
Vacuum glass tubes have no convection loss, so the fins that are the light-receiving surface are not provided with any kind of insulation and heat-retention means.
Most of the absorbed heat energy is dissipated due to the influence of wind from outside the collector.

又真空硝子管の完全破損だけでなく、強風に依る振動、
凍結に依る装着の狂い等に依る真空度の低下だけでも著
しい機能低下の恐れがある。
In addition to complete damage to the vacuum glass tube, vibrations caused by strong winds,
Even a decrease in the degree of vacuum due to incorrect installation due to freezing may lead to a significant decrease in functionality.

真空硝子管式熱エネルギー吸収方式の更に改善された構
造としてフィン付ヒートパイプを封入した方式がある。
A further improved structure of the vacuum glass tube thermal energy absorption method is a method in which a finned heat pipe is enclosed.

この場合ヒートパイプの秀れた熱移送能力に依って通常
の真空管式に比較して更に熱効率が向上し、又水又は熱
媒液の循環は装置が簡略化出来る利点がある。
In this case, due to the excellent heat transfer ability of the heat pipe, the thermal efficiency is further improved compared to the usual vacuum tube type, and the circulation of water or heat medium liquid has the advantage that the device can be simplified.

然し強風、台風等に対する脆弱さの点では通常の真空硝
子管式コレクターと同様である。
However, it is similar to ordinary vacuum glass tube collectors in terms of vulnerability to strong winds, typhoons, etc.

更に他の方式の太陽熱コレクターとして熱媒液を200
℃以上の高温に加熱し太陽熱発電等に利用する為のヒー
トパイプを熱エネルギー吸収及び熱移送として用いる太
陽光集束方式の真空硝子管式コレクターがある。
Furthermore, as another type of solar heat collector, heat transfer liquid can be used as a solar heat collector.
There is a vacuum glass tube type collector that uses a solar light focusing method that uses a heat pipe to absorb and transfer heat energy and heat it to a high temperature of ℃ or higher and use it for solar power generation.

これは動物線状曲面の反射板の焦点にヒートパイプを支
持した構造であり、ヒートパイプの全表面には耐熱性太
陽熱吸収膜が形成されである。
This is a structure in which a heat pipe is supported at the focal point of a reflective plate with an animal linear curved surface, and a heat-resistant solar heat absorbing film is formed on the entire surface of the heat pipe.

この方式は熱効率も良く高温度が容易に得られる利点が
あるが問題点としては受光面積に比較してヒートパイプ
の直径が小さい為、ヒートパイプ表面に太陽光を集光す
る為には抛物線曲面の反射鏡又は反射板の曲面構造を精
密に製作する必要があるので設備費も高価となる。
This method has the advantage of good thermal efficiency and can easily reach high temperatures, but the problem is that the diameter of the heat pipe is small compared to the light receiving area, so in order to concentrate sunlight on the surface of the heat pipe, it is necessary to use a parabolic curved surface. Since it is necessary to precisely manufacture the curved structure of the reflecting mirror or reflecting plate, the equipment cost is also high.

又有効に太陽光をヒートパイプ表面に集光せしめる為に
は精密に太陽光の方角追尾をする必要があるのも問題点
である。
Another problem is that in order to effectively focus sunlight on the surface of the heat pipe, it is necessary to precisely track the direction of sunlight.

本発明に係る太陽熱コレクター用ヒートパイプは上述の
如き従来の太陽熱コレクターに用いられた太陽熱吸収及
び移送構造の問題点を改善し、効率の高い且つ簡潔な構
造を提供せんとするものである。
The heat pipe for a solar heat collector according to the present invention is intended to improve the problems of the solar heat absorption and transfer structure used in the conventional solar heat collector as described above, and to provide a highly efficient and simple structure.

前述の如く平板型コレクターは受光平面から吸収した太
陽熱エネルギーを受光平面の裏面に接着した金属管に伝
導し、金属管内壁に於いてその中を循環する水又は熱媒
液と熱交換するものであり、水又は熱媒液循環の為の複
雑な配管及び加圧ポンプ及び動力を必要とするものであ
った。
As mentioned above, the flat plate type collector conducts the solar heat energy absorbed from the light receiving plane to the metal tube bonded to the back side of the light receiving plane, and exchanges heat with the water or heat transfer liquid circulating inside the metal tube on the inner wall of the metal tube. However, it required complicated piping, pressure pumps, and power for circulating water or heat transfer fluid.

これを簡素化する為に金属管の代りにヒートパイプを用
いることに依り少くも太陽熱受光平面の裏配管はこれを
大巾に簡素化することが出来る。
In order to simplify this, by using a heat pipe instead of a metal tube, at least the back piping of the solar heat receiving plane can be greatly simplified.

即ちヒートパイプはコンテナー内の作動液の作用に依り
何等の動力や装置の助けも必要とせず極めて効率良く熱
吸収部から放熱部に熱エネルギーを移送することが可能
となる。
That is, the heat pipe can transfer thermal energy from the heat absorbing section to the heat dissipating section extremely efficiently without requiring any power or the aid of any equipment due to the action of the working fluid in the container.

然し受光平面の裏面における金属管間又はヒートパイプ
間の金属面からの放射損失を防ぐことは不可能で何れの
場合も同様である。
However, it is impossible to prevent radiation loss from the metal surface between the metal tubes or between the heat pipes on the back side of the light-receiving plane, and the same is true in both cases.

通常の平板型コレクターの場合この損失を防ぐ為に断熱
材で保温しであるが、如伺に優秀な断熱材を用いたとし
ても相当の損失は免れ難いものである。
In order to prevent this loss, ordinary flat collectors are insulated with heat insulating material, but even if excellent heat insulating material is used, considerable loss is inevitable.

この損失を無くする為に真空管式コレクターが考案され
たのであるが、それもなお若干の問題点を残しているの
は前述の通りである。
A vacuum tube type collector was devised to eliminate this loss, but as mentioned above, it still has some problems.

以下図面に依って本発明に係る太陽熱吸収及び移送構造
である新しい型のヒートパイプについて詳述する。
A new type of heat pipe, which is a solar heat absorption and transfer structure according to the present invention, will be described in detail below with reference to the drawings.

第1図は本発明に係る太陽熱コレクター用ヒートパイプ
の外観図で第2図はその断面図である。
FIG. 1 is an external view of a heat pipe for a solar collector according to the present invention, and FIG. 2 is a sectional view thereof.

1はヒートパイプ本体の熱吸収部で本実施例ではコンテ
ナー外周に3枚の熱吸収フィン2が溶接しである。
Reference numeral 1 denotes a heat absorbing portion of the heat pipe body, and in this embodiment, three heat absorbing fins 2 are welded to the outer periphery of the container.

該熱吸収フィンはヒートパイプの熱吸収部Aの全長にわ
たり連続的に併動に設けである。
The heat absorbing fins are provided in continuous motion over the entire length of the heat absorbing portion A of the heat pipe.

更に該熱吸収フィン2の先端部は隣接するフィンの所定
の位置に気密に熔接されて全体として図面の如く中空円
柱状構造3に成形しである。
Furthermore, the tips of the heat absorbing fins 2 are hermetically welded to predetermined positions of adjacent fins, and the entire structure is formed into a hollow cylindrical structure 3 as shown in the drawings.

該円柱状構造の両端には蓋9,9′が気密に熔接し密封
されである。
At both ends of the cylindrical structure, lids 9, 9' are hermetically welded and sealed.

又その外周全表面には太陽熱吸収膜4が設けである。Further, a solar heat absorbing film 4 is provided on the entire outer surface.

この吸収膜は塗布、焼付、又は化学処理に依り表面に形
成する等何れの方法で設けても良い。
This absorption film may be provided by any method such as coating, baking, or forming on the surface by chemical treatment.

吸収膜4は太陽熱吸収効率の良い黒色ペイントでも良い
が、太陽光の殆んどを吸収し、赤外線を殆んど輻射しな
い選択性吸収膜であれば更に良好な特性を得ることが出
来る。
The absorbing film 4 may be a black paint with good solar heat absorption efficiency, but even better characteristics can be obtained if it is a selective absorbing film that absorbs most of the sunlight and emits almost no infrared rays.

1は通気孔で太陽熱吸収作動中や作動停止時における中
空柱状構造部内の空気の膨張及び収縮に依る中空柱状構
造の変形を防止する為内外間に僅かな通気性を与える為
の手段として設けであるものである。
1 is a ventilation hole, which is provided as a means to provide slight ventilation between the inside and outside in order to prevent deformation of the hollow columnar structure due to expansion and contraction of air within the hollow columnar structure during solar heat absorption operation and when the operation is stopped. It is something.

通気孔7は必ずしも図示の位置に限らず蓋9,9′等に
設けても良い。
The ventilation holes 7 are not necessarily provided in the illustrated positions, but may be provided in the lids 9, 9', etc.

5はヒートパイプ本体の放熱部、6は放熱フィンである
5 is a heat radiation part of the heat pipe main body, and 6 is a heat radiation fin.

8は熱移送部からの熱損失を防ぐための断熱層である。8 is a heat insulating layer for preventing heat loss from the heat transfer section.

以上本発明に係る太陽熱コレクター用ヒートパイプの一
実施例について述べたのであるが、その断面形状は必ず
しも第2図の如く中空円柱状構造である必要はない。
Although one embodiment of the heat pipe for a solar heat collector according to the present invention has been described above, its cross-sectional shape does not necessarily have to be a hollow cylindrical structure as shown in FIG.

適用される太陽熱コレクターの設計に応じて各種の形状
の中空柱状構造を採用してもよい。
Hollow columnar structures of various shapes may be employed depending on the design of the applied solar collector.

第3図a、b、c、dは夫々各種の断面形状を示しであ
る。
Figures 3a, b, c, and d show various cross-sectional shapes, respectively.

c、dについては熱吸収フィンの先端部とヒートパイプ
本体に対する溶接部との区別が明瞭でない特殊形状をし
て居るのが特徴である。
The features of c and d are that they have a special shape in which the tip of the heat absorbing fin and the welded part to the heat pipe body are not clearly distinguishable.

第4図は本発明に係るヒートパイプを太陽熱コレクター
に適用した場合の一実施例断面図である。
FIG. 4 is a sectional view of an embodiment in which the heat pipe according to the present invention is applied to a solar collector.

図に於いて11は本発明に係るヒートパイプ、12は太
陽光をヒートパイプの中空柱状構造部に反射投入するた
めの抛物線曲面をした反射板又は反射鏡である。
In the figure, 11 is a heat pipe according to the present invention, and 12 is a reflecting plate or reflecting mirror having a parabolic curved surface for reflecting sunlight into the hollow columnar structure of the heat pipe.

コレクターの受光平面の面積に比較して中空円柱状構造
部が充分に大きな外面積を占めているので抛物線曲面は
精密な曲面である必要はない。
Since the hollow cylindrical structure occupies a sufficiently large external area compared to the area of the light-receiving plane of the collector, the parabolic curved surface does not need to be a precise curved surface.

又同じ理由から矢印で示した太陽光が必ずしも垂直方向
から投射されなくても反射光は確実に中空円柱状構造部
表面に反射投入されるのも大きな特徴となっている。
For the same reason, another major feature is that even if the sunlight indicated by the arrow is not necessarily projected from the vertical direction, the reflected light is certainly reflected onto the surface of the hollow cylindrical structure.

13は断熱層、14は保護硝子板、15はコレクター保
護板である。
13 is a heat insulating layer, 14 is a protective glass plate, and 15 is a collector protection plate.

本発明に係る太陽熱コレクター用ヒートパイプは以上の
如き構造であり又第4図使用例の如く使用されるので、
次に述べる如き独特の作用効果を発揮する。
The heat pipe for solar heat collector according to the present invention has the above-described structure and is used as shown in the usage example in Fig. 4.
It exhibits the following unique functions and effects.

説明の便の為に第4図の如き太陽熱コレクターで冷暖房
給湯システムに応用するものとし、ヒートパイプは銅コ
ンテナー水作動液型としヒートパイプ本体の直径13m
m、中空円柱状構造部の直径50−太陽光受光平面の中
即ち反射鏡の入口中を300rrrrnと想定してその
作用を説明する。
For convenience of explanation, we will assume that a solar collector as shown in Figure 4 is applied to an air-conditioning, heating, and hot water supply system, and the heat pipe is a copper container water-operated type with a diameter of 13 m.
The operation will be explained assuming that the diameter of the hollow cylindrical structure is 50 m and the diameter of the sunlight receiving plane, that is, the entrance of the reflecting mirror is 300 rrrrn.

(1)表面温度が必要以上に高くならないので表面から
の放射損失が極めて少ない。
(1) Since the surface temperature does not become higher than necessary, radiation loss from the surface is extremely small.

運転中の冷暖房給湯システムでは熱媒体が水の場合は1
00℃以下、熱媒液の場合150℃であるからヒートパ
イプ吸熱部の加熱温度は200°C〜250℃で充分と
考えられる。
1 if the heating medium is water in an operating air conditioning, heating, and hot water system.
Since the temperature is 00°C or less, and 150°C in the case of a heat transfer liquid, it is considered that a heating temperature of 200°C to 250°C for the heat pipe heat absorption section is sufficient.

宇宙空間における地球表面に対する太陽光の輻射熱量は
電力量換算で毎平方m当り1.35KW/h年平均であ
ると言われる。
It is said that the amount of heat radiated from sunlight to the earth's surface in outer space is 1.35 KW/h per square meter per year in terms of electric energy.

この熱量は地表に到達する迄に地域、季節に依り異なる
が約50%が大気、塵挨その他に吸収されて太陽熱コレ
クターに到達する太陽光の輻射熱量は電力量換算で年平
均平方m当りは”650w/h位であると推定されてい
る。
This amount of heat varies depending on the region and season before it reaches the earth's surface, but approximately 50% of it is absorbed by the atmosphere, dust, etc., and the amount of radiant heat from sunlight that reaches the solar collector is equivalent to the amount of electricity per square meter per year. ``It is estimated to be around 650w/h.

平板型太陽熱コレクターに於いて、実効太陽熱吸収量は
一般的には300W/h 〜400W/h毎平方m位と
考えられる。
In a flat solar collector, the effective amount of solar heat absorption is generally considered to be about 300 W/h to 400 W/h per square meter.

これは反射板の有無、反射板の性能、コレクター自身の
熱効率に依って大巾に相異する。
This varies widely depending on the presence or absence of a reflector, the performance of the reflector, and the thermal efficiency of the collector itself.

通常の平板型コレクターでは50°C〜65℃前後の温
水を得る運転状態で平板平面の表面温度は80℃〜90
℃位になるものと考えられる。
In a normal flat plate type collector, the surface temperature of the flat plate is 80°C to 90°C when operating to obtain hot water of around 50°C to 65°C.
It is thought that the temperature will be around ℃.

(但し運転停止状態では180℃〜190℃にも到達す
る。
(However, when the operation is stopped, the temperature reaches 180°C to 190°C.

)太陽光受光平面中300mの場合、ヒートパイプ本体
で直接集束受光する場合の太陽エネル00 ギー密度は「5 = 7.35倍に達し表面温度は数1
00℃に達することが考えられる。
) At a distance of 300 m from the sunlight receiving plane, the solar energy density when the heat pipe directly focuses and receives the light is 5 = 7.35 times, and the surface temperature is several 1
It is conceivable that the temperature will reach 00°C.

ヒートパイプ表面に選択吸収膜が形成されている場合吸
収膜が銅の表面に形成された黒色酸化膜である場合10
0℃以下で太陽光の90%を吸収し、赤外線の8%を放
射するに過ぎない(米国エネルギー研究開発庁)が温度
が高くなると共に放射損失が増加し450℃で損益分岐
温度に達する(同庁)即ち数100℃に表面温度が達す
ると放射熱損失の方が多くなって太陽光集束の効果を失
って了うに至る。
When a selective absorption film is formed on the surface of the heat pipe When the absorption film is a black oxide film formed on the surface of copper 10
At temperatures below 0°C, 90% of sunlight is absorbed and only 8% of infrared radiation is emitted (U.S. Energy Research and Development Agency), but as the temperature rises, radiation loss increases and reaches the break-even temperature at 450°C (the agency). ) That is, when the surface temperature reaches several 100 degrees Celsius, the radiation heat loss becomes greater and the solar light focusing effect is lost.

これを防ぐためにはヒートパイプ拐質、選択吸収膜とし
て極めて高価なニッケルーブラックニッケルの如き組合
わせを必要とする。
In order to prevent this, extremely expensive combinations such as nickel-black nickel are required as heat pipe particles and selective absorption membranes.

又ヒートパイプとしての熱移送性能として銅コンテナー
水作動液型ヒートパイプの場合、200℃位が最も効率
が良く熱移送量も最大となりそれ以上では急激にその能
力を失い、250℃位で全く作動しなくなる。
In addition, in terms of heat transfer performance as a heat pipe, in the case of a copper container water-operated heat pipe, it is most efficient and the amount of heat transfer is maximum at around 200°C, and above that it rapidly loses its ability, and it does not work at all at around 250°C. I won't.

これは所甜ドライアンプ状態になり作動液の移動が不可
能となることに依る。
This is due to the fact that it becomes a dry amplifier state and the movement of the hydraulic fluid becomes impossible.

更に250℃位になると作動液の蒸気圧が高くなりヒー
トパイプの寿命が急激に低下する恐れがある。
Further, when the temperature reaches about 250° C., the vapor pressure of the working fluid increases, and there is a possibility that the life of the heat pipe will be rapidly reduced.

従ってヒートパイプの熱吸収部温度は約200°C以下
180℃以下にすることがあらゆる点から望ましい。
Therefore, it is desirable from all points of view that the temperature of the heat absorbing portion of the heat pipe is approximately 200° C. or less and 180° C. or less.

従って本発明に係る構造のヒートパイプの如く、フィン
の先端部を形成して直径501rrIrLの中空円柱状
構造とし、一旦この表面で太陽光を受けることに依リヒ
ートパイプの過熱を防ぐことが出来るものである。
Therefore, as in the heat pipe having the structure according to the present invention, the tip of the fin is formed into a hollow cylindrical structure with a diameter of 501rrIr, and once sunlight is received on this surface, the heat pipe can be prevented from overheating. It is.

中空円柱状構造部表面の選択吸収面の太陽熱エネルギー
密度はその集束度が300=300=1.9倍である5
0π 157 から平板型コレクターの吸収する太陽熱エネルギーの約
1.9倍となり、その表面温度は170℃位になるもの
と考えられる。
The degree of convergence of the solar thermal energy density on the selective absorption surface of the hollow cylindrical structure surface is 300 = 300 = 1.9 times5.
From 0π 157 , the solar thermal energy absorbed by the flat collector is about 1.9 times, and its surface temperature is considered to be about 170°C.

従ってこの程度の温度では表面からの熱放射損失は極め
て少ないものとなる。
Therefore, at this temperature, heat radiation loss from the surface is extremely small.

(2)平板型コレクターに比較して伝導熱損失が極めて
少ない。
(2) Compared to flat collectors, conductive heat loss is extremely low.

平板型コレクターは受光平面の裏面から断熱材を介して
熱伝導損失が避けられない。
In a flat collector, heat conduction loss cannot be avoided from the back side of the light-receiving plane through the heat insulating material.

本発明のヒートパイプの中空円柱状構造部はその全表面
が熱吸収平面即ち受光面であって何らの伝導熱損失がな
い。
The entire surface of the hollow cylindrical structure of the heat pipe of the present invention is a heat absorption plane, that is, a light receiving surface, and there is no conductive heat loss.

(3)平板型コレクターに比較して対流熱損失が極めて
少ない。
(3) Convection heat loss is extremely low compared to flat collectors.

同等の表面積の平板型に対し円柱体表面からの熱損失は
空気対流量が少なく従ってそのための損失も少ないもの
となる。
Compared to a flat plate type with the same surface area, the heat loss from the surface of the cylindrical body is smaller due to the smaller air flow rate.

(2)項及び(3)項の熱損失の少なさの影響に依り(
1)項記載の中空円柱状構造体の表面温度170℃(推
9の実際温度は200℃を越すことが測定されている。
Due to the effect of low heat loss in terms (2) and (3), (
The surface temperature of the hollow cylindrical structure described in item 1) is 170°C (the actual temperature of Inference 9 has been measured to exceed 200°C).

(4)中空円柱構造部の選択吸収膜で吸収した熱エネル
ギーは極めて効率良く殆んど損失無くヒートパイプに吸
収され殆んど損失無く放熱部に移送される。
(4) Thermal energy absorbed by the selective absorption film of the hollow cylindrical structure is absorbed by the heat pipe extremely efficiently with almost no loss, and is transferred to the heat radiation section with almost no loss.

その熱エネルギー伝達は次の通りに行なわれる。The thermal energy transfer takes place as follows.

[)フィンを通じて直接ヒートパイプに伝導し吸収され
る。
[) Conducted directly to the heat pipe through the fins and absorbed.

11)中空柱状構造部の内壁から輻射熱として直接ヒー
トパイプに吸収されるか、輻射熱としてフィンに吸収さ
れた後ヒートパイプに伝導されて吸収される。
11) The heat is directly absorbed by the heat pipe as radiant heat from the inner wall of the hollow columnar structure, or it is absorbed by the fins as radiant heat and then conducted to the heat pipe and absorbed.

面 中空柱状構造部の内壁とヒートパイプの外周の間に
密封状態になっている空気の激しい対流に依り中空柱状
構造部の熱エネルギーは急速Aこフィン及ヒートパイプ
に吸収される。
Due to the intense air convection sealed between the inner wall of the hollow columnar structure and the outer periphery of the heat pipe, the thermal energy of the hollow columnar structure is rapidly absorbed into the A-column and the heat pipe.

iV)上記の如く殆んど損失なくヒートパイプの熱吸収
部で吸収された熱エネルギーはヒートパイプ独特の熱移
送特性に依り、又銅コンテナー水作動液ヒートパイプの
最大能力を発揮し銅の熱伝導速度の数100倍の速度で
放熱部に移送される。
iV) As mentioned above, the thermal energy absorbed by the heat absorption part of the heat pipe with almost no loss is due to the unique heat transfer characteristics of the heat pipe, and the copper container water hydraulic fluid exerts its maximum capacity and the heat of the copper is absorbed by the heat absorption part of the heat pipe with almost no loss. The heat is transferred to the heat sink at a speed several hundred times faster than the conduction speed.

この移送には何等の動力も必要とせず従って何等の機械
的損失も生じない。
This transfer does not require any power and therefore does not result in any mechanical losses.

又平板型コレクター裏面の熱交換用金属細管と異なり最
短距離を、殆んど放熱損失を生ずる暇も無い早さで移送
される。
Also, unlike the thin metal tubes for heat exchange on the back side of the flat collector, it is transferred over the shortest distance at a speed with almost no time for heat radiation loss.

これはヒートパイプ内が高真空であり作動液は熱エネル
ギーを吸収した状態で放熱部に音速に近い速度で移動す
ることに依る。
This is because the inside of the heat pipe is in a high vacuum and the working fluid absorbs thermal energy and moves to the heat dissipation section at a speed close to the speed of sound.

以上(1) 、 (2) 、 (3) 、 (4)項を
総合して本発明に係る太陽熱コレクター用ヒートパイプ
はコレクターの熱エネルギーの吸収及び移送構造として
極めて優秀な効率を示すものでその損失は中空柱状構造
外表面に形成した太陽熱吸収膜の吸収損失と放射損失が
殆んどでありその他の損失としては平板型コレクターの
数分の−に過ぎない僅かな対流損失と反射板又は反射鏡
の吸収損失だけである。
Considering the above (1), (2), (3), and (4), the heat pipe for a solar collector according to the present invention exhibits extremely excellent efficiency as a collector thermal energy absorption and transfer structure. Most of the loss is due to absorption loss and radiation loss from the solar heat absorption film formed on the outer surface of the hollow columnar structure.Other losses include slight convection loss, which is only a few fractions of that of a flat collector, and reflection from the reflective plate. It is only the absorption loss of the mirror.

従って良好な特性の選択吸収膜と反射鏡の選定がなされ
るならば平板型コレクターよりはるかに効率の良い、真
空硝子管型コレクターに匹敵する効率を示すことが可能
なコレクターを構成することが出来るものである。
Therefore, if a selective absorption film and reflecting mirror with good characteristics are selected, it is possible to construct a collector that is far more efficient than a flat plate collector and comparable in efficiency to a vacuum glass tube collector. It is something.

本発明に係るヒートパイプは更に次の如き作用効果があ
る。
The heat pipe according to the present invention further has the following effects.

(5)ヒートパイプの外表面で直接に集束太陽光を受光
する場合より焦点が大きいので反射板又は反射鏡の反射
曲面は高精度を要求しないので製作が容易で安価である
(5) Since the focal point is larger than in the case of directly receiving focused sunlight on the outer surface of the heat pipe, high precision is not required for the reflective curved surface of the reflector or reflector, so manufacturing is easy and inexpensive.

(6)上記と同理由で太陽入射角度にも高い精度を要求
しないので太陽方向を追尾する場合の追尾装置も簡易な
装置で良い。
(6) For the same reason as above, high accuracy is not required for the angle of incidence of the sun, so a simple tracking device may be used to track the direction of the sun.

(7)熱膨張、収縮、其他外部からの衝撃、凍結等に依
る破損、特性低下の恐れが無い、真空硝子管型コレクタ
ーは優秀な特性を有するが、これ等の点が問題点として
残されていた。
(7) Vacuum glass tube type collectors have excellent properties as there is no risk of damage or property deterioration due to thermal expansion, contraction, other external shocks, freezing, etc. However, these points remain as problems. was.

この利点は又運搬時に破損の恐れが無いと言う利点をも
発揮するものである。
This advantage also provides the advantage that there is no risk of damage during transportation.

以上の如く本発明に係る新しい構造のヒートパイプは太
陽熱コレクターに適用してコレクターの性能改善に多く
の卓越した作用効果を発揮するもので太陽熱利用技術の
向上に貢献する所が大きいものと信じられる。
As described above, when the heat pipe of the new structure according to the present invention is applied to a solar heat collector, it exhibits many outstanding effects in improving the performance of the collector, and is believed to greatly contribute to the improvement of solar heat utilization technology. .

本発明は必ずしも特許請求の範囲1に記載の構造に限定
するものではない。
The present invention is not necessarily limited to the structure described in claim 1.

特許請求の範囲1では金属薄板製フィンをヒートパイプ
のコンテナーに溶接し、その先端部の成形に依って中空
柱状構造部を構成したのであるが、実用上は他の方法に
依っても同様な構造性能のヒートパイプを得ることが出
来る。
In claim 1, a thin metal plate fin is welded to a heat pipe container, and the hollow columnar structure is formed by forming the tip of the fin, but other methods may be used in practice. A heat pipe with structural performance can be obtained.

即ち金属薄板を成形し中空柱状構造体を先づ製作して置
き、又別途に単数又は複数本の周囲又は長手方向又はス
パイラル状の金属フィンを熱吸収部外周の全長にわたり
連続的又は非連続的に形成したヒートパイプを製作し、
該ヒートパイプを中空柱状構造体の内部に圧入又は挿入
し然る後中空柱状構造体の両端を封止することに依り特
許請求の範囲1に係るヒートパイプと全く同じ性能作用
効果を示すヒートパイプを得ることが出来る。
That is, a hollow columnar structure is first manufactured by forming a thin metal plate, and then one or more circumferential, longitudinal, or spiral metal fins are placed continuously or discontinuously over the entire length of the outer periphery of the heat absorbing part. We produced a heat pipe formed in
A heat pipe that exhibits exactly the same performance and effect as the heat pipe according to claim 1 by press-fitting or inserting the heat pipe into the hollow columnar structure and then sealing both ends of the hollow columnar structure. can be obtained.

この場合も何等かの手段に依って中空柱状構造体の内外
間に僅かな通気性を与える必要があることは云うまでも
ない。
Needless to say, in this case as well, it is necessary to provide a slight amount of air permeability between the inside and outside of the hollow columnar structure by some means.

この場合は中空柱状構造体内壁とフィン外縁との間に熱
抵抗が生じ伝導熱量が減少する。
In this case, thermal resistance occurs between the inner wall of the hollow columnar structure and the outer edge of the fin, reducing the amount of heat conducted.

然しそれと同量の熱エネルギー量だけ中空柱状構造体内
壁から輻射する熱エネルギー及び内部空気の対流に依る
熱伝達量が増加して、全体的には特許請求の範囲1に係
る構造のヒートパイプと全く同一性能を発揮することが
出来る。
However, by the same amount of thermal energy, the thermal energy radiated from the inner wall of the hollow columnar structure and the amount of heat transfer due to the convection of the internal air are increased, and the overall heat pipe has the structure according to claim 1. They can exhibit exactly the same performance.

又他の応用実施例としては第3図c、dの如く金属フィ
ンを省略し、中空柱状構造体の内部にヒートパイプを挿
入した構造であっても本発明の目的ははゾ達成すること
が出来るものである。
As another application example, the object of the present invention can still be achieved even if the metal fins are omitted and a heat pipe is inserted inside the hollow columnar structure as shown in FIGS. 3c and 3d. It is possible.

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

第1図は本発明の一実施例を説明する一部破断側面図、
第2図は縦断正面図、第3図a−dはヒートパイプの異
なった構造例を説明する断面図、第4図はコレクターに
適用した場合の構造例を示す縦断側面図、第5図はコレ
クターに適用した場合の他の構造例を説明する断面図で
ある。 1・・・・・・ヒートパイプ本体、2・・・・・・熱吸
収フィン、3・・・・・・熱吸収フィンの中空柱状構造
部、4・・・・・・太陽熱吸収膜、5・・・・・七−ト
パイプ本体放熱部、6・・・・・・放熱フィン、1・・
・・・・通気孔、A・・・・・・熱吸収部、B・・・・
・・熱移送部、C・・・・・・放熱部。
FIG. 1 is a partially cutaway side view illustrating an embodiment of the present invention;
Fig. 2 is a vertical front view, Fig. 3 a - d are sectional views explaining different structural examples of the heat pipe, Fig. 4 is a longitudinal side view showing a structural example when applied to a collector, and Fig. 5 is a longitudinal sectional view. It is a sectional view explaining other structural examples when applied to a collector. DESCRIPTION OF SYMBOLS 1...Heat pipe body, 2...Heat absorption fins, 3...Hollow columnar structure of heat absorption fins, 4...Solar heat absorption film, 5 ... 7-pipe body heat radiation part, 6 ... heat radiation fin, 1 ...
...Vent hole, A...Heat absorption part, B...
...Heat transfer section, C... Heat dissipation section.

Claims (1)

【特許請求の範囲】[Claims] 1 太陽熱コレクターに用いる太陽熱吸収用及び移送用
のヒートパイプであってそのコンテナーの外周には熱吸
収部の全長にわたり連続した複数の金属薄板製熱吸収フ
ィンが設けてあり、この熱吸収フィンのそれぞれの先端
部は折曲され、その折曲端部はそれぞれ所定の部分と溶
接又は接着し、全体として中空な柱状構造体に形成する
とともにその両端開口部は封止されてあり、又該中空柱
状構造体はその内外間に僅かな通気性を与える手段が設
けられてあり、さらにその外周面には全面にわたって塗
装焼付け、又は化学処理等の方法により太陽熱吸収膜を
形成しであることを特徴とする太陽熱コレクター用ヒー
トパイプ。
1 A heat pipe for absorbing and transferring solar heat used in a solar heat collector, in which a plurality of continuous heat absorption fins made of thin metal plates are provided on the outer periphery of the container over the entire length of the heat absorption part, and each of these heat absorption fins The tip of the hollow columnar structure is bent, and each of the bent ends is welded or glued to a predetermined part to form a hollow columnar structure as a whole, and the openings at both ends are sealed. The structure is provided with a means for providing slight air permeability between the inside and outside of the structure, and is further characterized in that a solar heat absorbing film is formed on the entire outer peripheral surface by a method such as painting or chemical treatment. Heat pipe for solar heat collector.
JP54162575A 1979-12-14 1979-12-14 Heat pipe for solar collector Expired JPS5819014B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP54162575A JPS5819014B2 (en) 1979-12-14 1979-12-14 Heat pipe for solar collector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP54162575A JPS5819014B2 (en) 1979-12-14 1979-12-14 Heat pipe for solar collector

Publications (2)

Publication Number Publication Date
JPS5685652A JPS5685652A (en) 1981-07-11
JPS5819014B2 true JPS5819014B2 (en) 1983-04-15

Family

ID=15757187

Family Applications (1)

Application Number Title Priority Date Filing Date
JP54162575A Expired JPS5819014B2 (en) 1979-12-14 1979-12-14 Heat pipe for solar collector

Country Status (1)

Country Link
JP (1) JPS5819014B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5923057U (en) * 1982-08-04 1984-02-13 日東工器株式会社 solar heat collector
JPS5923049U (en) * 1982-11-19 1984-02-13 白木金属工業株式会社 solar heat collector tube
US7971587B2 (en) * 2007-10-31 2011-07-05 The Regents Of The University Of California Apparatus and method for solar thermal energy collection

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4059093A (en) * 1975-09-22 1977-11-22 Grumman Aerospace Corporation Solar energy collector
JPS5320699A (en) * 1976-08-09 1978-02-25 Daido Steel Co Ltd Slowly descending apparatus

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JPS5685652A (en) 1981-07-11

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