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JP2551703B2 - Circulating method of working fluid in low boiling medium system - Google Patents
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JP2551703B2 - Circulating method of working fluid in low boiling medium system - Google Patents

Circulating method of working fluid in low boiling medium system

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Publication number
JP2551703B2
JP2551703B2 JP3218226A JP21822691A JP2551703B2 JP 2551703 B2 JP2551703 B2 JP 2551703B2 JP 3218226 A JP3218226 A JP 3218226A JP 21822691 A JP21822691 A JP 21822691A JP 2551703 B2 JP2551703 B2 JP 2551703B2
Authority
JP
Japan
Prior art keywords
working fluid
condenser
low boiling
liquid
gas
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
Application number
JP3218226A
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Japanese (ja)
Other versions
JPH0559909A (en
Inventor
起男 山崎
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.)
Hisaka Works Ltd
Original Assignee
Hisaka 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 Hisaka Works Ltd filed Critical Hisaka Works Ltd
Priority to JP3218226A priority Critical patent/JP2551703B2/en
Publication of JPH0559909A publication Critical patent/JPH0559909A/en
Application granted granted Critical
Publication of JP2551703B2 publication Critical patent/JP2551703B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、ヒ−トポンプやバイ
ナリ−サイクルのような低沸点媒体システムにおける作
動流体の循環方法に関し、特に、作動流体として二成分
系の非共沸混合媒体を使用する場合の性能向上を図るも
のである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for circulating a working fluid in a low boiling point medium system such as a heat pump or a binary cycle, and more particularly, to use a binary non-azeotropic mixture medium as the working fluid. In this case, the performance is improved.

【0002】[0002]

【従来の技術】低沸点媒体システムの一例として図3に
示されるバイナリー発電システムについて述べると、蒸
発器2、タービン4、凝縮器6およびポンプ8が直列に
接続されて閉ループ10を構成している。そして、その閉
ループ10内を循環する作動流体は、まず蒸発器2で熱源
流体から熱を奪って蒸発し、発生した蒸気はタービン4
に供給される。この蒸気はタービン4内で膨張して発電
機12を駆動する仕事をする。タービン4から排出された
蒸気は凝縮器6で冷却水に熱を奪われて凝縮する。凝縮
液はポンプ8で再び蒸発器2に送られる。
2. Description of the Related Art A binary power generation system shown in FIG. 3 as an example of a low boiling point medium system will be described. An evaporator 2, a turbine 4, a condenser 6 and a pump 8 are connected in series to form a closed loop 10. . The working fluid circulating in the closed loop 10 first removes heat from the heat source fluid in the evaporator 2 and evaporates, and the generated steam is the turbine 4
Is supplied to. This steam expands in the turbine 4 and serves to drive the generator 12. The steam discharged from the turbine 4 is deprived of heat by the cooling water in the condenser 6 and condensed. The condensate is sent to the evaporator 2 again by the pump 8.

【0003】ところで、このようなバイナリーサイクル
やヒートポンプ等の熱サイクルでは、効率の向上のため
作動流体に非共沸の混合媒体を用いてローレンツサイク
ルを構成させることがある。たとえばバイナリーサイク
ルは基本的にランキンサイクルであって、作動流体が単
一媒体のときは図4に示すようにTS線図の’−、
−がそれぞれ等温変化を示す。ところが、フロンR
123 とR22の混合のような混合媒体を作動流体として使
用すると、図5に示すように、同一圧力でも飽和温度が
変化し、蒸発器2では蒸発温度が上がり、凝縮器6では
凝縮温度が下がる。これによりローレンツサイクルが形
成され、システム効率が向上する。
By the way, in such a heat cycle such as a binary cycle or a heat pump, a Lorentz cycle may be constituted by using a non-azeotropic mixed medium as a working fluid in order to improve efficiency. For example, the binary cycle is basically a Rankine cycle, and when the working fluid is a single medium, as shown in FIG.
-Indicates isothermal changes. However, Freon R
When a mixed medium such as a mixture of 123 and R22 is used as the working fluid, the saturation temperature changes, the evaporation temperature rises in the evaporator 2 and the condensation temperature decreases in the condenser 6, as shown in FIG. . This forms a Lorentz cycle and improves system efficiency.

【0004】図6は最も簡単な二成分の液体−蒸気系の
温度−組成の関係を横軸に低沸成分のモル分率をとって
示したものである。GとLは単一相で、それぞれ気相と
液相、L+Gの領域は液体と蒸気が共存する二相領域で
ある。もし低沸成分の60モル%(モル分率=0.60)の液
体混合物の温度を、定圧下で上昇させたとすると、この
系の変化は直線ab'cd"e に沿って考えることができる。
低温では液相のみが存在するが、b'点で蒸気相が現われ
る。この蒸気相の組成はb"点で与えられ、2つの共役相
は図上の平衡連結線b"b'で結ばれている。さらに温度を
上げると、もっと多くの蒸気が生成するが、その場合、
蒸気中の低沸成分の濃度が高いので、液相ではこの成分
が相対的に減少し、液体の組成はb'c'd'に沿って変化
し、一方、蒸気の組成はb"c"d"に沿って変化する。温度
t℃では、二相領域にある系の全組成はc点で表される
が、蒸気組成、液体組成はそれぞれc点を通る平衡連結
線の両端、c"点とc'点で与えられる。二相の相対的な量
は、物理学のてこの原理から求められる。すなわち、蒸
気と液体のモル数の比はcc'と c"c の長さの比で表され
る。さらに温度を上げるとますます蒸気が生成し、d”
点になると液相はほとんどなくなり、これ以上温度が高
くなると、液相が消えて蒸気相(d"点)のみが残る。こ
れ以上は温度を(d"e に沿って)上げてもなにも起らな
い。
FIG. 6 shows the simplest temperature-composition relationship of a two-component liquid-vapor system with the horizontal axis representing the mole fraction of the low-boiling component. G and L are single phases, respectively, a gas phase and a liquid phase, and a region of L + G is a two-phase region where a liquid and a vapor coexist. If the temperature of a liquid mixture of 60 mol% (mol fraction = 0.60) of the low boilers is increased under constant pressure, the change in this system can be considered along a straight line ab'cd "e.
At low temperatures, only a liquid phase exists, but a vapor phase appears at point b '. The composition of this vapor phase is given by the point b ", and the two conjugate phases are connected by an equilibrium connection line b" b 'in the figure. Increasing the temperature will produce more steam, in which case
Due to the high concentration of low boiling components in the vapor, this component is relatively reduced in the liquid phase, the composition of the liquid changes along b'c'd ', while the composition of the vapor is b "c" It changes along the d ". At the temperature t ° C, the total composition of the system in the two-phase region is represented by the point c, but the vapor composition and the liquid composition are both ends of the equilibrium connecting line passing through the point c," Given by points and c'points. The relative amounts of the two phases are determined from the principle of leverage in physics. That is, the ratio of the number of moles of vapor to liquid is represented by the ratio of the length of cc 'to c "c. As the temperature is further increased, more and more vapor is generated, and d"
At the point, the liquid phase almost disappears, and when the temperature becomes higher than this, the liquid phase disappears and only the vapor phase (d "point) remains. Even if the temperature is further raised (along d" e) Does not happen.

【0005】[0005]

【発明が解決しようとする課題】凝縮器出口の作動流体
の気相では低沸成分の濃度が系内で最も高く、凝縮伝熱
面付近にも低沸成分のガスが滞留する。このため、図7
に示すように、低沸成分は凝縮器に対し物質移動および
熱移動を妨げる不凝縮ガスと同じような存在となり、伝
熱性能を低下させる。
In the vapor phase of the working fluid at the outlet of the condenser, the low boiling point component has the highest concentration in the system, and the gas having the low boiling point component stays near the condensation heat transfer surface. Therefore, in FIG.
As shown in (3), the low-boiling component exists in the condenser in the same manner as the non-condensable gas that impedes mass transfer and heat transfer, and reduces the heat transfer performance.

【0006】そこで、この発明の目的とするところは、
凝縮器の出口側で未凝縮の低沸成分ガスの濃度を下げ、
凝縮器伝熱性能を向上させることのできる二成分系の非
共沸混合媒体を作動流体として使用する低沸点媒体シス
テムにおける作動流体の循環方法を提供することにあ
る。
Therefore, the object of the present invention is to:
Decrease the concentration of uncondensed low-boiling component gas on the outlet side of the condenser,
It is an object of the present invention to provide a method for circulating a working fluid in a low boiling point medium system that uses a binary non-azeotropic mixed medium as a working fluid, which can improve heat transfer performance of a condenser.

【0007】[0007]

【課題を解決するための手段】 上述の目的を達成する
ために、この発明は、二成分系の非共沸混合媒体を作動
流体として使用する熱サイクルにおける作動流体の循環
方法において、凝縮器の出口側で作動流体を未凝縮ガス
と凝縮液とに分離し、その後、分離した未凝縮ガスを凝
縮液に混合して蒸発器に供給するようにしたものであ
る。未凝縮ガスを凝縮液に混合する手段としてはエジェ
クタを採用することができる。なお、ポンプやコンプレ
ッサーなど、液体に気体を吸引させる上でエジェクタと
同等の機能を発揮するその他の手段を採用することも可
能であるが、エジェクタは別段の動力を必要としない点
で有利である。
In order to achieve the above-mentioned object, the present invention provides a method for circulating a working fluid in a heat cycle in which a binary non-azeotropic mixed medium is used as a working fluid. The working fluid is separated into an uncondensed gas and a condensate on the outlet side, and then the separated uncondensed gas is mixed with the condensate and supplied to an evaporator. An ejector can be used as a means for mixing the uncondensed gas with the condensate. It should be noted that although it is possible to employ other means such as a pump or a compressor that exerts a function equivalent to that of the ejector when sucking gas into the liquid, the ejector is advantageous in that it does not require any additional power. .

【0008】[0008]

【作用】 非共沸混合媒体を作動流体とする熱サイクル
においては、蒸発器では低沸点成分が高沸点成分より先
に蒸発しやすく、凝縮器では高沸点成分よりも低沸点成
分が凝縮しにくいことから、凝縮器出口側の蒸気は入口
側よりも低沸点成分濃度が高く、凝縮液は高沸点成分濃
度が高いものであるところ、凝縮器の出口側で凝縮液か
ら分離した低沸点成分濃度の高い未凝縮ガスを高沸点成
分濃度の高い凝縮液に混合させることにより未凝縮ガス
が凝縮液に溶解される。その結果、凝縮器の作動流体出
口付近における未凝縮低沸点成分濃度が下がり、物質移
動および熱移動が容易になり凝縮器伝熱性能が向上す
る。また、低沸点成分ガス濃度の低下に伴い圧力も低下
する。したがって、凝縮圧が下がり、サイクルの効率向
上にも役立つ。
[Operation] In a heat cycle using a non-azeotropic mixed medium as a working fluid, a low boiling point component is likely to evaporate earlier in the evaporator than a high boiling point component, and a low boiling point component is less likely to be condensed in the condenser than a high boiling point component Therefore, the vapor on the outlet side of the condenser has a higher concentration of low-boiling components than the inlet side, and the condensate has a higher concentration of high-boiling components.The concentration of the low-boiling components separated from the condensate on the outlet side of the condenser By mixing the high-concentration uncondensed gas with the condensate having a high boiling point component concentration, the uncondensed gas is dissolved in the condensate. As a result, the concentration of uncondensed low boiling point components near the working fluid outlet of the condenser is reduced, mass transfer and heat transfer are facilitated, and heat transfer performance of the condenser is improved. Further, the pressure also decreases as the concentration of the low boiling point component gas decreases. Therefore, the condensing pressure is lowered, which also helps improve the efficiency of the cycle.

【0009】[0009]

【実施例】図3に示した上述のバイナリ−発電システム
に適用した場合を例にとって説明すると、図1に示すよ
うに、凝縮器6の出口側に未凝縮ガスを分離するための
ドレンポット14を設置し、凝縮器6の作動流体出口をこ
のドレンポット14に接続する。ドレンポット14の下部の
液相は循環ポンプ8に接続する。循環ポンプ8の吐出側
にエジェクタ16を取り付け、このエジェクタ16の吸引口
に、ドレンポット14の上部の気相を接続する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The case of application to the above-mentioned binary power generation system shown in FIG. 3 will be explained as an example. As shown in FIG. 1, a drain pot 14 for separating uncondensed gas is provided at the outlet side of the condenser 6. Is installed, and the working fluid outlet of the condenser 6 is connected to the drain pot 14. The liquid phase below the drain pot 14 is connected to the circulation pump 8. The ejector 16 is attached to the discharge side of the circulation pump 8, and the gas phase above the drain pot 14 is connected to the suction port of the ejector 16.

【0010】蒸発器2で発生した作動流体の蒸気は、タ
−ビン4に供給されて仕事をした後、凝縮器6で冷却水
に熱を奪われて凝縮する。凝縮ドレンと未凝縮ガスはド
レンポット14に流入する。ドレンポット14では液とガス
とに分離され、液は循環ポンプ8でエジェクタ16を経て
蒸発器2に送られる。ポンプ8から吐出された液がエジ
ェクタ16を通過する際にエジェクタ16ののど部に低圧部
が発生し、ドレンポット14からガスを吸引する。このよ
うにして吸引された低沸成分ガスは液中に巻き込まれて
吸収される。
The working fluid vapor generated in the evaporator 2 is supplied to the turbine 4 to perform work, and then the condenser 6 removes heat from the cooling water to condense it. The condensed drain and the uncondensed gas flow into the drain pot 14. In the drain pot 14, the liquid and the gas are separated, and the liquid is sent to the evaporator 2 via the ejector 16 by the circulation pump 8. When the liquid discharged from the pump 8 passes through the ejector 16, a low pressure portion is generated in the throat portion of the ejector 16 and sucks gas from the drain pot 14. The low-boiling component gas thus sucked is caught in the liquid and absorbed.

【0011】図2の気液平衡線図で説明すると、凝縮終
了温度Tcが同じ場合、エジェクタ16でドレンポット14
内の蒸気を吸引すれば蒸気中の低沸成分濃度が低下す
る。そして、蒸気の低沸成分濃度に平衡する形で液の低
沸成分濃度も低下する。図中の実線丸印から点線丸印へ
向かう矢印はこのことを表している。このようにして、
低沸成分濃度の低下した液と低沸成分濃度の高い蒸気と
が混合される結果、供給濃度Dと同じ濃度の液がエジェ
クタ16から排出される。このときの気相線および液相線
はそれぞれ点線位置にあり、圧力が低下した状態を示す
ことになる。
Explaining with the vapor-liquid equilibrium diagram of FIG. 2, when the condensation end temperature Tc is the same, the ejector 16 causes the drain pot 14 to operate.
If the vapor inside is sucked in, the concentration of the low boiling point component in the vapor will decrease. Then, the low boiling point component concentration of the liquid also decreases in a form of equilibrium with the low boiling point component concentration of the vapor. The arrow from the solid circle to the dotted circle in the figure indicates this. In this way,
As a result of mixing the liquid having a low low boiling point component concentration and the vapor having a high low boiling point component concentration, a liquid having the same concentration as the supply concentration D is discharged from the ejector 16. At this time, the vapor phase line and the liquid phase line are respectively located at dotted lines, which means that the pressure is reduced.

【0012】又、図8にヒ−トポンプを利用した場合の
実施例を示す。同図は、蒸発器2で発生した蒸気をコン
プレッサ−4′で加圧して凝縮器6に送り、高圧の液を
膨張弁16′で減圧し、蒸発器2で蒸発潜熱を奪うという
システムである。従って、蒸発器2の方が凝縮器6より
も低圧であるために、図1の実施例のように特にエジェ
クタ16を設ける必要はなく、膨張弁16′の二次側にドレ
ンポット14からの配管を接続するだけで図1の実施例の
場合と同様の作用が得られる。尚、この発明は、何ら上
記実施例にのみ制約されることなく、例えば凝縮器の出
口側において作動流体が未凝縮ガスと凝縮液とに十分に
分離されている場合にはドレンポットの使用を省略する
ことができる。又、分離された未凝縮ガスを吸引して凝
縮液に混合させることができれば、エジェクタ以外の手
段に置換することもできる。
FIG. 8 shows an embodiment in which a heat pump is used. This system is a system in which vapor generated in the evaporator 2 is pressurized by a compressor-4 'and sent to the condenser 6, high-pressure liquid is decompressed by an expansion valve 16', and latent heat of vaporization is taken by the evaporator 2. . Therefore, since the evaporator 2 has a lower pressure than the condenser 6, it is not necessary to provide the ejector 16 as in the embodiment of FIG. 1, and the drain pot 14 from the drain pot 14 is provided on the secondary side of the expansion valve 16 '. The same operation as in the case of the embodiment shown in FIG. 1 can be obtained simply by connecting the pipes. Incidentally, the present invention is not limited to the above-mentioned embodiment at all, and for example, when the working fluid is sufficiently separated into the uncondensed gas and the condensed liquid on the outlet side of the condenser, the use of the drain pot is not required. It can be omitted. Further, if the separated uncondensed gas can be sucked and mixed with the condensate, it can be replaced with a means other than the ejector.

【0013】[0013]

【発明の効果】 以上のように、この発明は、二成分系
の非共沸混合媒体を作動流体として使用する熱サイクル
における作動流体の循環方法において、凝縮器の出口側
で作動流体を未凝縮ガスと凝縮液とに分離し、その後、
分離した未凝縮ガスを凝縮液に混合して蒸発器に供給す
るものであるから、凝縮器出口付近における未凝縮低沸
点成分ガス濃度が下がり、物質移動及び熱移動を容易と
して凝縮器伝熱性能が向上する。また、凝縮器出口側の
低沸点成分ガス濃度の低下に伴い圧力も低下するので、
凝縮圧低下によるサイクル効率向上にも役立つ。
As described above, according to the present invention, in a working fluid circulation method in a heat cycle using a binary non-azeotropic mixed medium as a working fluid, the working fluid is not condensed on the outlet side of the condenser. Separated into gas and condensate, then
Since the separated uncondensed gas is mixed with the condensate and supplied to the evaporator, the concentration of the uncondensed low-boiling-point component gas near the condenser outlet decreases, facilitating mass transfer and heat transfer, and heat transfer performance of the condenser. Is improved. Further, since the pressure also decreases as the concentration of the low boiling point component gas on the outlet side of the condenser decreases,
It also helps improve cycle efficiency by reducing the condensation pressure.

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

【図1】この発明の実施例を示すバイナリー発電システ
ムのフローシートである。
FIG. 1 is a flow sheet of a binary power generation system showing an embodiment of the present invention.

【図2】凝縮器における作動流体の気液平衡線図であ
る。
FIG. 2 is a vapor-liquid equilibrium diagram of a working fluid in a condenser.

【図3】従来例を示すバイナリー発電システムのフロー
シートである。
FIG. 3 is a flow sheet of a binary power generation system showing a conventional example.

【図4】ランキンサイクルのTS線図である。FIG. 4 is a TS diagram of Rankine cycle.

【図5】ローレンツサイクルのTS線図である。FIG. 5 is a TS diagram of the Lorentz cycle.

【図6】二成分系混合媒体の温度−組成の関係を示す気
液平衡線図である。
FIG. 6 is a vapor-liquid equilibrium diagram showing a temperature-composition relationship of a binary mixed medium.

【図7】凝縮伝熱面の断面図である。FIG. 7 is a cross-sectional view of a condensation heat transfer surface.

【図8】ヒートポンプのフローシートである。FIG. 8 is a flow sheet of a heat pump.

【符号の説明】[Explanation of symbols]

2 蒸発器 4 タービン 6 凝縮器 8 循環ポンプ 10 閉ループ 12 発電機 14 ドレンポット 16 エジェクタ 2 Evaporator 4 Turbine 6 Condenser 8 Circulation pump 10 Closed loop 12 Generator 14 Drain pot 16 Ejector

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 二成分系の非共沸混合媒体を作動流体と
して使用する熱サイクルにおける作動流体の循環方法に
おいて、凝縮器の出口側で作動流体を未凝縮ガスと凝縮
液とに分離し、その後、分離した未凝縮ガスを凝縮液に
混合して蒸発器に供給することを特徴とする低沸点媒体
システムにおける作動流体の循環方法。
1. A method of circulating a working fluid in a thermal cycle using a binary non-azeotropic mixed medium as a working fluid, wherein the working fluid is separated into an uncondensed gas and a condensed liquid at an outlet side of a condenser, Then, the separated non-condensed gas is mixed with a condensate and supplied to an evaporator.
【請求項2】 前記分離した未凝縮ガスを凝縮液に混合
する手段がエジェクタであることを特徴とする請求項1
記載の低沸点媒体システムにおける作動流体の循環方
法。
2. The ejector is a means for mixing the separated uncondensed gas with the condensate.
A method of circulating a working fluid in a low boiling medium system as described.
JP3218226A 1991-08-29 1991-08-29 Circulating method of working fluid in low boiling medium system Expired - Fee Related JP2551703B2 (en)

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JP2002303105A (en) * 2001-04-09 2002-10-18 Mayekawa Mfg Co Ltd Two-phase separation Rankine cycle
CN101839154A (en) * 2010-04-28 2010-09-22 北京力通高科技发展有限公司 Distributed type residual-heat/residual-pressure power generation system and distributed type residual-heat/residual-pressure power generation method

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JPS59153074A (en) * 1983-02-22 1984-08-31 松下電器産業株式会社 Refrigeration cycle equipment
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