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JPH0263146B2 - - Google Patents
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JPH0263146B2 - - Google Patents

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Publication number
JPH0263146B2
JPH0263146B2 JP9041585A JP9041585A JPH0263146B2 JP H0263146 B2 JPH0263146 B2 JP H0263146B2 JP 9041585 A JP9041585 A JP 9041585A JP 9041585 A JP9041585 A JP 9041585A JP H0263146 B2 JPH0263146 B2 JP H0263146B2
Authority
JP
Japan
Prior art keywords
refrigerant
condenser
heat exchanger
refrigeration circuit
compressor
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
JP9041585A
Other languages
Japanese (ja)
Other versions
JPS61250457A (en
Inventor
Susumu Kanashiki
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.)
Subaru Corp
Original Assignee
Fuji Heavy Industries 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 Fuji Heavy Industries Ltd filed Critical Fuji Heavy Industries Ltd
Priority to JP9041585A priority Critical patent/JPS61250457A/en
Publication of JPS61250457A publication Critical patent/JPS61250457A/en
Publication of JPH0263146B2 publication Critical patent/JPH0263146B2/ja
Granted legal-status Critical Current

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  • Compression-Type Refrigeration Machines With Reversible Cycles (AREA)
  • Devices That Are Associated With Refrigeration Equipment (AREA)
  • Cold Air Circulating Systems And Constructional Details In Refrigerators (AREA)

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は車輛用冷房装置やルームクーラー等に
使用される冷房装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a cooling device used for a vehicle cooling device, a room cooler, or the like.

〔発明の技術的背景〕[Technical background of the invention]

冷房装置においては、従来から、蒸発器の効率
を向上させるため、冷媒を分流器を通して多数の
管路に分流させた後、蒸発器内に送入し、通風フ
アンから送りこまれる通風との間で熱交換を行な
うようにしている。
Conventionally, in cooling equipment, in order to improve the efficiency of the evaporator, refrigerant is divided into multiple pipes through a flow divider, and then introduced into the evaporator, which is then separated from the draft air sent from the ventilation fan. It is designed to perform heat exchange.

第3図は従来の冷房装置における冷凍サイクル
を例示するもので、圧縮機1で圧縮され、昇温し
た気相冷媒は凝縮器2内に導入され、フアン3に
よる通風Aとの熱交換によつて冷却され、液化し
て受液器4に送入される。
FIG. 3 shows an example of a refrigeration cycle in a conventional cooling system. Gaseous refrigerant that has been compressed by a compressor 1 and heated up is introduced into a condenser 2, and is exchanged with ventilation A by a fan 3. The liquid is then cooled, liquefied, and sent to the liquid receiver 4.

受液器4に入つた液化冷媒は比重差によつて気
体と液体に分離し、液相冷媒は底部に一端が開口
する管路を通して汲み上げられ過冷却熱交換器5
に導入される。
The liquefied refrigerant that has entered the receiver 4 is separated into gas and liquid due to the difference in specific gravity, and the liquid refrigerant is pumped up through a pipe with one end open at the bottom and transferred to the supercooling heat exchanger 5.
will be introduced in

過冷却熱交換器5は前述のフアン3によつて流
れる通風Aの方向に対し、凝縮器2よりも上流側
に配置されており、過冷却熱交換器5内を流過す
る液化冷媒は通風Aとの熱交換によつて過冷却さ
れる。
The supercooling heat exchanger 5 is arranged upstream of the condenser 2 with respect to the direction of the draft A flowing by the fan 3 described above, and the liquefied refrigerant flowing through the supercooling heat exchanger 5 is It is supercooled by heat exchange with A.

過冷却熱交換器5によつて過冷却された液化冷
媒は膨脹弁6に導入され、減圧・霧化された後、
分流器7を通り、多数本の管路8a〜8n内を分
流して蒸発器に送入される。
The liquefied refrigerant supercooled by the supercooling heat exchanger 5 is introduced into the expansion valve 6, and after being depressurized and atomized,
The water passes through the flow divider 7, is divided into a large number of pipe lines 8a to 8n, and is sent to the evaporator.

通風フアン10による通風Bは蒸発器9内を流
れる冷媒との熱交換によつて冷却され、冷気とし
て車内あるいは室内の冷房に供される。
The ventilation B generated by the ventilation fan 10 is cooled by heat exchange with the refrigerant flowing in the evaporator 9, and is used as cold air to cool the interior of the vehicle or the room.

一方、蒸発器9内を流過する際に通風Bによつ
て加熱された冷媒は蒸発し、蒸発器9の出口で集
合され、管路11を通して圧縮機1に環流し、冷
凍サイクルを完了する。
On the other hand, the refrigerant heated by the ventilation B while flowing through the evaporator 9 evaporates, collects at the outlet of the evaporator 9, and flows back to the compressor 1 through the pipe 11 to complete the refrigeration cycle. .

なお、蒸発器9の出口には管路11内に流入す
る冷媒の温度を検出する感温筒12が取付けられ
ている。
Note that a temperature sensing cylinder 12 is attached to the outlet of the evaporator 9 to detect the temperature of the refrigerant flowing into the pipe line 11.

膨脹弁6は感温筒12からの温度信号と、圧力
信号により弁開度を調節する。この膨脹弁6の開
度調節は通常、蒸発器内の飽和圧力に対して感温
筒12の温度が5℃程度過熱された状態となるよ
う、つまり5℃以上では弁開作動、5℃未満では
弁閉作動するよう設定されている。
The expansion valve 6 adjusts its opening degree based on the temperature signal from the temperature sensing tube 12 and the pressure signal. Normally, the opening degree of the expansion valve 6 is adjusted so that the temperature of the thermosensor cylinder 12 is overheated by about 5 degrees Celsius relative to the saturation pressure in the evaporator. The valve is set to close.

従つて、冷媒が流れすぎ、蒸発器9内での蒸発
が完了しない状態になると、冷媒は飽和状態のま
ま感温筒12内を流過するようになるから、過熱
度は上述の5℃より小さくなり、膨脹弁6は絞り
こまれ、冷媒流量を減少させる。
Therefore, if the refrigerant flows too much and evaporation in the evaporator 9 is not completed, the refrigerant will flow through the temperature sensing tube 12 in a saturated state, and the degree of superheat will be lower than the above-mentioned 5°C. becomes smaller, and the expansion valve 6 is throttled to reduce the refrigerant flow rate.

一方、膨脹弁6を絞りすぎ、冷媒の蒸発が蒸発
器9の途中で完了してしまうような場合には過熱
度が上述の設定温度以上となるので、膨脹弁6は
開弁方向に作動し、冷媒流量を増加させる。
On the other hand, if the expansion valve 6 is throttled too much and evaporation of the refrigerant is completed in the middle of the evaporator 9, the degree of superheat will exceed the above-mentioned set temperature, and the expansion valve 6 will operate in the opening direction. , increase the refrigerant flow rate.

上述した膨脹弁6の開閉動作により冷媒は蒸発
器9内で適度に蒸発し、冷却風を供給することに
なる。
By opening and closing the expansion valve 6 described above, the refrigerant is appropriately evaporated in the evaporator 9, and cooling air is supplied.

第4図は第3図の冷凍サイクルをモリエル線図
上に示したものであり、iはエンタルピ、pは圧
力、tは温度を表す。
FIG. 4 shows the refrigeration cycle of FIG. 3 on a Mollier diagram, where i represents enthalpy, p represents pressure, and t represents temperature.

同図において、aは圧縮機1の入口での吸入ガ
スの状態を示しており、冷媒は圧縮機1で圧縮さ
れる結果、その出口では、bで示すようにエンタ
ルピi、圧力p、温度tは高くなつている。
In the figure, a indicates the state of the suction gas at the inlet of the compressor 1, and as a result of the refrigerant being compressed by the compressor 1, at the outlet, the enthalpy i, pressure p, temperature t is getting higher.

上記bの状態で凝縮器2内に送入された冷媒は
凝縮器内を流過する間に次第に冷却され、飽和点
cを過ぎると、液化を開始する。更に冷却される
と、飽和終了点dでは冷媒のほとんどが液化し、
受液器4に入る。
The refrigerant fed into the condenser 2 in the state b above is gradually cooled while flowing through the condenser, and when it passes the saturation point c, it starts to liquefy. When further cooled, most of the refrigerant liquefies at the saturation end point d,
Enters liquid receiver 4.

受液器4からは液相部分のみが過冷却熱交換器
5内に送入され、過冷却されて過冷却熱交換器5
の出口では状態eとなる。
From the liquid receiver 4, only the liquid phase portion is sent into the supercooling heat exchanger 5, where it is supercooled and transferred to the supercooling heat exchanger 5.
At the exit, the state is e.

過冷却熱交換器5を出た過冷却冷媒は膨脹弁6
に導入され、その絞り作用により減圧され、膨脹
の途中で気・液2相流となり、fの状態にて分流
器7に送入される。
The supercooled refrigerant leaving the supercooling heat exchanger 5 is passed through the expansion valve 6.
The gas is introduced into the air flow pipe, the pressure is reduced by the throttling action, the gas and liquid become a two-phase flow during expansion, and the flow is sent to the flow divider 7 in the state f.

分流器7により各管路8a〜8n内に分流した
冷媒は蒸発器9内を流過する間に蒸発を完了し、
h点以降は気相100%となつて昇温し、a状態に
て圧縮機1の入口に戻り、以後同様に冷凍サイク
ルを反復する。
The refrigerant divided into each of the pipes 8a to 8n by the flow divider 7 completes evaporation while flowing through the evaporator 9,
After point h, the temperature becomes 100% gas phase, the temperature rises, the temperature returns to the inlet of the compressor 1 in state a, and the refrigeration cycle is repeated in the same manner.

次に第3図に示す空冷式の凝縮器2を用いたバ
ス用冷房装置の場合を例につて、上記冷凍サイク
ルにおけるfの状態を説明すると、夏季、外気温
35℃のとき、凝縮器2の凝縮温度は60℃で圧力は
約15Kg/cm2G、過冷却熱交換器5による冷却量は
15deg.であり、冷媒の蒸発温度と圧力は約7℃、
2.9Kg/cm2Gである。
Next, the state of f in the refrigeration cycle will be explained using the case of a bus cooling system using an air-cooled condenser 2 shown in FIG. 3 as an example.
At 35℃, the condensation temperature of condenser 2 is 60℃, the pressure is about 15Kg/cm 2 G, and the amount of cooling by supercooling heat exchanger 5 is
15 degrees, and the refrigerant evaporation temperature and pressure are approximately 7 degrees Celsius.
It is 2.9Kg/cm 2 G.

膨脹弁6の入口における冷媒温度は過冷却によ
り45℃となつており、膨脹弁6出口では気体重量
約25%の湿り蒸気である。このときの圧力はゲー
ジ圧で2.9Kg/cm2であり、冷媒は重量比で25%が
ガス化している気・液2相流である。
The refrigerant temperature at the inlet of the expansion valve 6 is 45° C. due to supercooling, and the refrigerant temperature at the outlet of the expansion valve 6 is wet steam with a gas weight of about 25%. The pressure at this time was 2.9 kg/cm 2 in gauge pressure, and the refrigerant was a gas/liquid two-phase flow in which 25% by weight was gasified.

冷媒の容積は7℃の液状態では0.729/Kg、
ガス状態では45.83/Kgであるから、 液 量:0.729×0.75=0.546 ガス量:45.83×0.25=11.45 となり、体積比では液量1に対してガス量21とな
る。
The volume of refrigerant is 0.729/Kg in liquid state at 7℃,
In the gas state, it is 45.83/Kg, so liquid volume: 0.729 x 0.75 = 0.546 gas volume: 45.83 x 0.25 = 11.45, and the volume ratio is 1 liquid volume to 21 gas volume.

このように液量に対してガス量が圧倒的に多い
気・液2相流においては、管路の曲り部や分岐部
で重力、慣性力、表面張力等により冷媒液が管壁
に張りついたような偏つた流れを生じやすい。
In this two-phase flow of gas and liquid, where the amount of gas is overwhelmingly large compared to the amount of liquid, the refrigerant liquid sticks to the pipe wall at bends and branch points of the pipe due to gravity, inertial force, surface tension, etc. This tends to cause uneven flow.

なお、第4図のgは過冷却を行なわない場合を
示しており、この場合は冷媒の気相成分が重量比
で35%を占めることになるので、冷媒の偏りは一
層生じやすくなる。
Note that g in FIG. 4 shows the case where supercooling is not performed, and in this case, the gaseous phase component of the refrigerant will account for 35% by weight, so unevenness of the refrigerant is more likely to occur.

〔背景技術の問題点〕[Problems with background technology]

上述の如く、従来の冷房装置においては、分流
器によつて冷媒を多数の管路に分流させる際、冷
媒の液相部分が体積比で1/20〜1/30しかない
ため、流れの渦や管壁での表面張力により、分流
器からの配分に偏りが生じやすく、多数の管路に
冷媒を均一に配分することが困難である。
As mentioned above, in conventional cooling systems, when the refrigerant is divided into multiple pipes using a flow divider, the liquid phase portion of the refrigerant is only 1/20 to 1/30 by volume, so the vortex of the flow is generated. Due to surface tension on the walls of the pipes and pipes, the distribution from the flow divider tends to be uneven, making it difficult to uniformly distribute the refrigerant to a large number of pipes.

各管路に配分される冷媒にアンバランスが生じ
ると、液量の多い管路では出口部においても未だ
飽和状態であり、液が残つているにも拘らず、液
量の少ない管路では、出口端ですでに過熱ガスに
なつているという状態が生ずる。
If an imbalance occurs in the refrigerant distributed to each pipe, pipes with a large amount of liquid will still be saturated at the outlet, and pipes with a small amount of liquid will still be saturated, even though some liquid remains. A situation arises in which the gas is already superheated at the outlet end.

このような場合に、感温筒12で過熱度が0の
飽和状態を検知して膨脹弁6を絞ると、他の管路
の冷媒量も一緒に減少してしまうため、蒸発器9
の能力が大幅に低下するという欠点があつた。
In such a case, if the thermosensor cylinder 12 detects a saturated state with a superheat degree of 0 and throttles the expansion valve 6, the amount of refrigerant in other pipes will also decrease, so the evaporator 9
The disadvantage was that the performance of the system was significantly reduced.

〔発明の目的〕[Purpose of the invention]

本発明は背景技術における上述の如き欠点を除
去すべくなされたもので、冷媒の過冷却を大きく
とることができ、しかも冷媒の配分をより均一化
して効率の低下を防止した冷房装置を提供するこ
とを目的とする。
The present invention has been made in order to eliminate the above-mentioned drawbacks in the background art, and provides a cooling device that can achieve a large amount of supercooling of the refrigerant and furthermore evenly distributes the refrigerant to prevent a decrease in efficiency. The purpose is to

〔発明の概要〕[Summary of the invention]

本発明は冷房装置は、上述の目的を達成するた
め、圧縮機と、この圧縮機によつて圧縮され昇温
した冷媒を凝縮させる凝縮器と、この凝縮器から
送出される冷媒を受入れる受液器と、この受液器
から送出される液化冷媒を過冷却させる熱交換器
と、この熱交換器から送出される液化冷媒を複数
本の管路に分流させる分流器と、前記管路を通し
て導入される冷媒を蒸発させる蒸発器とから成る
冷凍回路と; 前記受液器の気相部分から送出される冷媒ガス
を冷却して凝縮させる凝縮器と、この凝縮器を出
た冷媒を膨脹させる膨脹装置と、前記熱交換器内
を流過して第1冷凍回路側の冷媒を過冷却させた
冷媒を前記圧縮機の入口側へ戻す管路とから成る
第2冷凍回路と; を備えたことを特徴とする。
In order to achieve the above-mentioned object, the present invention provides a cooling device that includes a compressor, a condenser that condenses refrigerant compressed by the compressor and heated up, and a liquid receiver that receives the refrigerant sent out from the condenser. a heat exchanger for subcooling the liquefied refrigerant sent out from the liquid receiver, a flow divider for dividing the liquefied refrigerant sent out from the heat exchanger into a plurality of pipes, and a flow divider for introducing the liquefied refrigerant through the pipes. a refrigeration circuit consisting of an evaporator that evaporates refrigerant; a condenser that cools and condenses the refrigerant gas sent out from the gas phase portion of the liquid receiver; and an expansion circuit that expands the refrigerant exiting the condenser. and a second refrigeration circuit comprising: a second refrigeration circuit that returns the refrigerant that has passed through the heat exchanger and supercooled the refrigerant on the first refrigeration circuit side to the inlet side of the compressor; It is characterized by

〔発明の実施例〕[Embodiments of the invention]

以下、図面を参照して本発明の実施例を説明す
る。
Embodiments of the present invention will be described below with reference to the drawings.

第1図は本発明を適用した冷房装置の冷凍サイ
クルを例示するもので、第3図におけると同一部
材は同一の記号で示さている。
FIG. 1 illustrates a refrigeration cycle of a cooling device to which the present invention is applied, and the same members as in FIG. 3 are indicated by the same symbols.

第1図において、圧縮機1で圧縮され、昇温し
た高圧の気相冷媒は凝縮器2内に導入され、通風
Aとの熱交換によつて冷却され、液化して受液器
4に送入される。
In FIG. 1, a high-pressure gaseous refrigerant that has been compressed by a compressor 1 and heated up is introduced into a condenser 2, cooled by heat exchange with ventilation A, liquefied, and sent to a liquid receiver 4. entered.

受液器4に入つた冷媒は比重差によつて気体と
液体に分離し、液相冷媒はそこに一端が開口する
管路を通して汲み上げられ過冷却熱交換器20に
導入される。
The refrigerant that has entered the liquid receiver 4 is separated into gas and liquid due to the difference in specific gravity, and the liquid refrigerant is pumped up through a pipe that is open at one end and introduced into the supercooling heat exchanger 20 .

過冷却熱交換器20によつて過冷却された液化
冷媒は膨脹弁6に導入され、減圧した後、分流器
7を通り、多数本の管路8a〜8n内を分流して
蒸発器9に送入される。
The liquefied refrigerant supercooled by the supercooling heat exchanger 20 is introduced into the expansion valve 6, and after being depressurized, passes through the flow divider 7, and is divided into multiple pipes 8a to 8n to reach the evaporator 9. sent.

通風フアン10による通風Bは蒸発器9内を流
れる冷媒との熱交換によつて冷却され、冷気とし
て車内あるいは室内の冷房に供される。
The ventilation B generated by the ventilation fan 10 is cooled by heat exchange with the refrigerant flowing in the evaporator 9, and is used as cold air to cool the interior of the vehicle or the room.

一方、蒸発器9内を流過する際に通風Bによつ
て加熱された冷媒は蒸発し、蒸発器9の出口で集
合され、管路11を通して圧縮機1に環流し、冷
凍サイクルを完了する。
On the other hand, the refrigerant heated by the ventilation B while flowing through the evaporator 9 evaporates, collects at the outlet of the evaporator 9, and flows back to the compressor 1 through the pipe 11 to complete the refrigeration cycle. .

上述の回路を本発明では第1冷凍回路という。 The above-mentioned circuit is referred to as a first refrigeration circuit in the present invention.

一方、受液器4の上部のガス部分に開口する管
路21には凝縮器22が接続されている。この凝
縮器は第1冷凍回路の凝縮器2に対し冷却風Aの
上流側に配置されており、凝縮器22内に送入さ
れた冷媒は冷却風Aとの熱交換によつて冷却液化
される。この液化冷媒は膨脹弁23またはキヤピ
ラリ管から成る膨張装置内に導入され、減圧膨脹
した後、過冷却熱交換器20内で第1回路側の冷
媒を過冷却し、自身は加熱されて蒸発し、管路2
4を経て圧縮機1に流入する。
On the other hand, a condenser 22 is connected to a conduit 21 that opens into the upper gas portion of the liquid receiver 4 . This condenser is placed upstream of the cooling air A with respect to the condenser 2 of the first refrigeration circuit, and the refrigerant fed into the condenser 22 is cooled and liquefied by heat exchange with the cooling air A. Ru. This liquefied refrigerant is introduced into an expansion device consisting of an expansion valve 23 or a capillary tube, and after being depressurized and expanded, the refrigerant on the first circuit side is supercooled in the subcooling heat exchanger 20, and the refrigerant itself is heated and evaporated. , conduit 2
4 and flows into the compressor 1.

本発明においては上記受液器4から管路21、
凝縮器22、膨脹弁23、過冷却熱交換器20、
管路24を経て圧縮機1に至る回路を第2冷凍回
路という。
In the present invention, from the liquid receiver 4 to the pipe line 21,
condenser 22, expansion valve 23, subcooling heat exchanger 20,
The circuit leading to the compressor 1 via the pipe line 24 is referred to as a second refrigeration circuit.

第2図は第1図の冷凍サイクルをモリエル線図
上に示したもので、状態aの冷媒は圧縮機1で圧
縮される結果、その出口では、bで示すようにエ
ンタルピi、圧力p、温度tはいずれも高くなつ
ている。
FIG. 2 shows the refrigeration cycle of FIG. 1 on a Mollier diagram. As a result of the refrigerant in state a being compressed by compressor 1, at its outlet, enthalpy i, pressure p, The temperature t is increasing in both cases.

上記bの状態で凝縮器2内に送入された冷媒は
凝縮器内を流過する間に次第に冷却され、飽和点
cを過ぎると液化を開始する。凝縮器2の出口で
はdのように冷媒のほとんどが液化し、受液器4
に入る。
The refrigerant fed into the condenser 2 in the state b above is gradually cooled while flowing through the condenser, and begins to liquefy after passing the saturation point c. At the outlet of the condenser 2, most of the refrigerant liquefies as shown in d, and the liquid receiver 4
to go into.

受液器4からは液相部分のみが過冷却熱交換器
20内に送入され、dからeまで過冷却される。
状態eで過冷却熱交換器20を出た過冷却冷媒は
膨脹弁6に導入され、その絞り作用により減圧さ
れ、eからfまで変化する。
Only the liquid phase portion is sent from the liquid receiver 4 into the supercooling heat exchanger 20, and is supercooled from d to e.
The supercooled refrigerant that exits the supercooling heat exchanger 20 in state e is introduced into the expansion valve 6, and its pressure is reduced by its throttling action, changing from e to f.

各管路8a〜8n内に分流した冷媒は蒸発器9
内を流過する間に蒸発を完了し、h点以降は気相
100%の冷媒として過熱され、圧縮機1の入口、
すなわちa状態に戻り、以後同様に冷凍サイクル
を反復する。
The refrigerant divided into each pipe line 8a to 8n is transferred to an evaporator 9.
Evaporation completes while flowing through the
The inlet of the compressor 1, which is superheated as 100% refrigerant,
That is, the state returns to state a, and the refrigeration cycle is repeated in the same manner thereafter.

上述のように本発明の冷房装置の第2冷凍回路
においては、受液器4の上部のガス部分から取出
された冷媒は第2冷凍回路の凝縮器22で冷却さ
れて液化し、膨脹弁23で減圧され、熱交換器2
0内で第1冷凍回路の冷媒を過冷却した後、圧縮
機1に吸入される。
As described above, in the second refrigeration circuit of the cooling device of the present invention, the refrigerant taken out from the upper gas portion of the liquid receiver 4 is cooled and liquefied in the condenser 22 of the second refrigeration circuit, and the refrigerant is liquefied by the expansion valve 23. The pressure is reduced by heat exchanger 2.
After the refrigerant in the first refrigeration circuit is subcooled within the refrigeration system 0, it is sucked into the compressor 1.

なお、上記第2冷凍回路の圧縮機への吸入口は
管路11の最も圧力の低い部分とする。これによ
り熱交換器20における第2冷凍回路の冷媒飽和
温度を最も低い温度とすることができる。従つ
て、第1冷凍回路の膨脹弁6に流入する液化冷媒
を第1冷凍回路の蒸発温度まで冷却することがで
きる。
Note that the suction port to the compressor of the second refrigeration circuit is the lowest pressure part of the pipe line 11. Thereby, the refrigerant saturation temperature of the second refrigeration circuit in the heat exchanger 20 can be set to the lowest temperature. Therefore, the liquefied refrigerant flowing into the expansion valve 6 of the first refrigeration circuit can be cooled to the evaporation temperature of the first refrigeration circuit.

このように、本発明においては、膨脹弁6に流
入する冷媒温度を予め蒸発器9の蒸発温度まで冷
却しているので、膨脹弁6で減圧しても気体相が
発生せず、仮りに発生してもその量は極めて僅か
である。従つて、分流器7における分流は均等に
行なわれる。
In this way, in the present invention, since the temperature of the refrigerant flowing into the expansion valve 6 is cooled in advance to the evaporation temperature of the evaporator 9, a gas phase is not generated even if the pressure is reduced by the expansion valve 6, and even if However, the amount is extremely small. Therefore, the flow in the flow divider 7 is evenly divided.

〔発明の効果〕〔Effect of the invention〕

上記の如く、本発明の冷房装置においては、分
流器に流入する冷媒温度が蒸発器における蒸発温
度まで低下しているので、気相の発生は僅小であ
り、ほとんどの冷媒は液相のままで分流器に流入
する。
As mentioned above, in the cooling device of the present invention, the temperature of the refrigerant flowing into the flow divider is lowered to the evaporation temperature in the evaporator, so the generation of gas phase is minimal, and most of the refrigerant remains in the liquid phase. flows into the flow divider.

従つて、分流器から各管路への冷媒配分量は均
一化し、蒸発器出口では全ての管路で冷媒の蒸発
が完了するので蒸発器の熱交換効率が向上する。
これに伴ない蒸発器の小形化が可能となり、原価
の低減、軽量化を実現できる上、著しい省エネル
ギー効果が得られる。
Therefore, the amount of refrigerant distributed from the flow divider to each pipe is made uniform, and the evaporation of the refrigerant is completed in all the pipes at the evaporator outlet, thereby improving the heat exchange efficiency of the evaporator.
This makes it possible to downsize the evaporator, which reduces cost and weight, and provides significant energy savings.

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

第1図は本発明の冷房装置の冷凍回路の実施例
を示す系統図、第2図はそのモリエル線図、第3
図は従来の冷房装置を例示する系統図、第4図は
そのモリエル線図である。 1……圧縮機、2,22……凝縮器、3,10
……通風フアン、4……受液器、5,20……過
冷却熱交換器、6,23……膨脹弁、7……分流
器、8a〜8n……管路、9……蒸発器、12…
…感温筒、20……熱交換器。
FIG. 1 is a system diagram showing an embodiment of the refrigeration circuit of the cooling device of the present invention, FIG. 2 is its Mollier diagram, and FIG.
The figure is a system diagram illustrating a conventional cooling device, and FIG. 4 is a Mollier diagram thereof. 1...Compressor, 2,22...Condenser, 3,10
... Ventilation fan, 4 ... Liquid receiver, 5, 20 ... Supercooling heat exchanger, 6, 23 ... Expansion valve, 7 ... Divider, 8a to 8n ... Pipe line, 9 ... Evaporator , 12...
...Thermosensitive tube, 20...Heat exchanger.

Claims (1)

【特許請求の範囲】 1 圧縮機と、この圧縮機によつて圧縮され昇温
した冷媒を凝縮させる凝縮器と、この凝縮器から
送出される冷媒を受入れる受液器と、この受液器
から送出される液化冷媒を過冷却させる熱交換器
と、この熱交換器から送出される液化冷媒を複数
本の管路に分流させる分流器と、前記管路を通し
て導入される冷媒を蒸発させる蒸発器とから成る
第1冷凍回路と; 前記受液器の気相部分から送出される冷媒ガス
を冷却して凝縮させる凝縮器と、この凝縮器を出
た冷媒を膨脹させる膨脹装置と、前記熱交換器内
を流過して第1冷凍回路側の冷媒を過冷却させた
冷媒を前記圧縮機の入口側へ戻す管路とから成る
第2冷凍回路と; を備えたことを特徴とする冷房装置。 2 第2冷凍回路の凝縮器が第1冷凍回路の凝縮
器に対して、通風の上流側に配置されていること
を特徴とする特許請求の範囲第1項記載の冷房装
置。
[Claims] 1. A compressor, a condenser that condenses refrigerant compressed and heated by the compressor, a liquid receiver that receives the refrigerant sent from the condenser, and a liquid receiver that receives the refrigerant from the liquid receiver. A heat exchanger that subcools the liquefied refrigerant sent out, a flow divider that divides the liquefied refrigerant sent out from the heat exchanger into a plurality of pipes, and an evaporator that evaporates the refrigerant introduced through the pipes. a first refrigeration circuit comprising; a condenser that cools and condenses refrigerant gas sent from the gas phase portion of the liquid receiver; an expansion device that expands the refrigerant exiting the condenser; and the heat exchanger. a second refrigeration circuit consisting of a conduit that returns the refrigerant that has passed through the container to supercool the refrigerant on the first refrigeration circuit side to the inlet side of the compressor; and a cooling device characterized by comprising: . 2. The cooling device according to claim 1, wherein the condenser of the second refrigeration circuit is arranged upstream of the ventilation with respect to the condenser of the first refrigeration circuit.
JP9041585A 1985-04-26 1985-04-26 Chilling unit Granted JPS61250457A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9041585A JPS61250457A (en) 1985-04-26 1985-04-26 Chilling unit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9041585A JPS61250457A (en) 1985-04-26 1985-04-26 Chilling unit

Publications (2)

Publication Number Publication Date
JPS61250457A JPS61250457A (en) 1986-11-07
JPH0263146B2 true JPH0263146B2 (en) 1990-12-27

Family

ID=13997960

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9041585A Granted JPS61250457A (en) 1985-04-26 1985-04-26 Chilling unit

Country Status (1)

Country Link
JP (1) JPS61250457A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH07189908A (en) * 1993-12-28 1995-07-28 Mitsubishi Electric Corp Accumulator and refrigeration cycle device

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012132586A (en) * 2010-12-20 2012-07-12 Calsonic Kansei Corp Refrigeration cycle device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH07189908A (en) * 1993-12-28 1995-07-28 Mitsubishi Electric Corp Accumulator and refrigeration cycle device

Also Published As

Publication number Publication date
JPS61250457A (en) 1986-11-07

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