JPH0221510B2 - - Google Patents
Info
- Publication number
- JPH0221510B2 JPH0221510B2 JP58230974A JP23097483A JPH0221510B2 JP H0221510 B2 JPH0221510 B2 JP H0221510B2 JP 58230974 A JP58230974 A JP 58230974A JP 23097483 A JP23097483 A JP 23097483A JP H0221510 B2 JPH0221510 B2 JP H0221510B2
- Authority
- JP
- Japan
- Prior art keywords
- refrigerant
- solenoid valve
- electric expansion
- main
- flow rate
- 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
Links
Landscapes
- Air Filters, Heat-Exchange Apparatuses, And Housings Of Air-Conditioning Units (AREA)
- Compression-Type Refrigeration Machines With Reversible Cycles (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
この発明は、冷凍サイクルの冷媒循環量を適正
に制御する冷媒流量制御装置を備えた空気調和装
置に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to an air conditioner equipped with a refrigerant flow rate control device that appropriately controls the amount of refrigerant circulated in a refrigeration cycle.
〔従来技術〕
通常、冷凍サイクルでは、蒸発温度によつて適
正冷媒流量が異なり、蒸発温度が高くなるに伴な
い、大きな冷媒流量が必要であるが、冷凍サイク
ルの減圧装置としてキヤピラリチユーブを用いた
ものでは、その冷媒流量の調整巾が小さく、蒸発
温度が高いときには、冷媒流量が不定し、蒸発器
出口冷媒の過熱度が大きくなりすぎて、圧縮機の
温度が上昇したり、蒸発温度が低いときには、冷
媒流量が過大になつて圧縮機に液もどりを生じた
りすることがある。従つて、これらの問題点を解
決するために第1図に示すような冷凍サイクルが
考えられる。すなわち、第1図において、1は圧
縮機、2は凝縮器、3は減圧装置で、第2図に示
すように、外管31内に、例えばキヤピラリーチ
ユーブを用いた主絞り部32を嵌挿し、巻回して
いる。そして、主絞り部32、及び、外管31と
主絞り部32との間の冷媒流通路33を互いに、
並列となるように入口管35,36及び出口管3
7を設け、この入口管35,36は、凝縮器2の
出口に、また出口管37は後述する蒸発器の入口
に接続し、入口管36に電気式膨脹弁38を設け
ることにより構成したものである。4は蒸発器
で、上述した機器1〜3と順次接続され、冷凍サ
イクルを形成している。従つて、圧縮機1及び凝
縮器2は通常の冷凍サイクルと同様に作用する
が、減圧装置3においては、凝縮器2から供給さ
れた液冷媒は、主絞り部32を流通して、減圧さ
れ、蒸発器4で蒸発して冷却作用をなす。また、
凝縮器2から供給された液冷媒の一部は、電気式
膨脹弁38で減圧され、冷媒流通路33内で蒸発
して、主絞り部32内を流通する冷媒を冷却する
ので、主絞り部32内の冷媒流量は増大する。す
なわち、主絞り部32内で発生している冷媒の2
相流中のガス含有量が冷却量が多くなるにしたが
つて、少なくなり、流体抵抗が減少するためであ
る。従つて、電気式膨脹弁38の開度を調整する
ことによつて主絞り部32内を流れる冷媒の冷却
量が変化して流体抵抗が増減するために、冷媒流
量が制御できるので、例えば蒸発器4の出入口の
温度を検出し、蒸発器4の出口温度がその入口温
度よりも常に少し高くなるように、電気式膨脹弁
38を制御すると、蒸発器4出口で冷媒が完全に
ガス化して、わずかに過熱度がつき、常に適正な
冷媒流量が冷凍サイクル内を循環させることがで
きる。ところで、第3図に示すように、冷凍負荷
によつて、最適冷媒循環量は変化する。第3図に
おいて、曲線ABは、冷凍負荷に対する最適冷媒
循環量を示す曲線ABB′によつて梱まれた範囲
は電気式膨脹弁38によつて確保される循環量、
及びAB′B″A′によつて梱まれた範囲は主絞り
部32によつて確保される循環量を示す。しかし
ながら、上述した冷凍サイクルでは主絞り部32
には、常に、凝縮器2からの液冷媒が流通してい
るので、たとえ電気式膨脹弁38を全閉したとし
てもAA′で示される冷媒循環量が流通している。
従つて、第3図におけるA点からB点における範
囲で最適冷媒循環量に制御されるが、さらに、冷
凍負荷の小さいA点からC点における範囲では、
最適冷媒循環量には、制御できない問題点があ
る。[Prior art] Normally, in a refrigeration cycle, the appropriate refrigerant flow rate varies depending on the evaporation temperature, and as the evaporation temperature increases, a larger refrigerant flow rate is required. If the refrigerant flow rate adjustment range is small and the evaporation temperature is high, the refrigerant flow rate becomes unstable and the degree of superheating of the refrigerant at the evaporator outlet becomes too large, causing the compressor temperature to rise and the evaporation temperature to rise. When it is low, the refrigerant flow rate becomes excessive and may cause liquid backflow in the compressor. Therefore, in order to solve these problems, a refrigeration cycle as shown in FIG. 1 can be considered. That is, in FIG. 1, 1 is a compressor, 2 is a condenser, and 3 is a pressure reducing device. As shown in FIG. Insert and turn. Then, the main constriction section 32 and the refrigerant flow passage 33 between the outer tube 31 and the main constriction section 32 are connected to each other.
The inlet pipes 35, 36 and the outlet pipe 3 are arranged in parallel.
7, the inlet pipes 35 and 36 are connected to the outlet of the condenser 2, the outlet pipe 37 is connected to the inlet of the evaporator described later, and the inlet pipe 36 is provided with an electric expansion valve 38. It is. Reference numeral 4 denotes an evaporator, which is sequentially connected to the devices 1 to 3 described above to form a refrigeration cycle. Therefore, the compressor 1 and the condenser 2 function in the same way as a normal refrigeration cycle, but in the pressure reducing device 3, the liquid refrigerant supplied from the condenser 2 flows through the main constriction section 32 and is depressurized. , is evaporated in the evaporator 4 and has a cooling effect. Also,
A part of the liquid refrigerant supplied from the condenser 2 is depressurized by the electric expansion valve 38 and evaporated within the refrigerant flow path 33 to cool the refrigerant flowing through the main throttle section 32. The refrigerant flow rate within 32 increases. In other words, 2 of the refrigerant generated within the main constriction section 32
This is because the gas content in the phase flow decreases as the amount of cooling increases, and the fluid resistance decreases. Therefore, by adjusting the opening degree of the electric expansion valve 38, the amount of cooling of the refrigerant flowing in the main constriction section 32 is changed, and the fluid resistance increases or decreases, so the flow rate of the refrigerant can be controlled. By detecting the temperature at the inlet and outlet of the evaporator 4 and controlling the electric expansion valve 38 so that the outlet temperature of the evaporator 4 is always slightly higher than the inlet temperature, the refrigerant is completely gasified at the evaporator 4 outlet. , the degree of superheating is slightly increased, and an appropriate flow rate of refrigerant can be constantly circulated within the refrigeration cycle. By the way, as shown in FIG. 3, the optimum refrigerant circulation amount changes depending on the refrigeration load. In FIG. 3, curve AB indicates the optimum refrigerant circulation amount for the refrigeration load.
The range enclosed by AB'B''A' indicates the circulation amount secured by the main throttle section 32. However, in the above-mentioned refrigeration cycle, the main throttle section 32
Since the liquid refrigerant from the condenser 2 is always flowing through the refrigerant, even if the electric expansion valve 38 is fully closed, the refrigerant circulation amount indicated by AA' is still flowing.
Therefore, the refrigerant circulation amount is controlled to the optimum amount in the range from point A to point B in FIG. 3, but furthermore, in the range from point A to point C where the refrigeration load is small,
There are problems with the optimal refrigerant circulation rate that cannot be controlled.
この発明は、上記実情に鑑がみなされたもの
で、冷凍サイクルの冷凍負荷の変動幅が大きい空
気調和装置においても常に最適冷媒循環量を得る
ことを目的とするものである。
This invention was made in consideration of the above-mentioned circumstances, and aims to always obtain the optimum amount of refrigerant circulation even in an air conditioner in which the refrigeration load of the refrigeration cycle fluctuates widely.
〔発明の実施例〕
以下、この発明の一実施例を第4図に示す。図
において、1は圧縮機、2は凝縮器、3は減圧装
置で、第2図に示す構成と同一であるが入口管3
5に電磁弁39を設けている。4は蒸発器であ
り、これらの機器1〜3と順次接続され、冷凍サ
イクルを形成している。また、電気式膨脹弁38
は凝縮器2及び蒸発器4の熱媒体温度を検出して
演算し、この演算値に応じて出力される信号によ
り、印加電圧を決定する制御器(図示せず)によ
り制御される。すなわち、電気式膨脹弁38は印
加電圧により、その弁開度が決定されるものであ
る。また、電磁弁39は蒸発器4出口側熱媒体温
度が所定値以下のとき閉路し、所定値以上のとき
は開路される。[Embodiment of the Invention] An embodiment of the invention is shown in FIG. 4 below. In the figure, 1 is a compressor, 2 is a condenser, and 3 is a pressure reducing device, which has the same configuration as shown in FIG. 2, but an inlet pipe 3.
5 is provided with a solenoid valve 39. 4 is an evaporator, which is sequentially connected to these devices 1 to 3 to form a refrigeration cycle. In addition, an electric expansion valve 38
is controlled by a controller (not shown) which detects and calculates the heat medium temperatures of the condenser 2 and evaporator 4, and determines the applied voltage based on a signal output according to the calculated values. That is, the opening degree of the electric expansion valve 38 is determined by the applied voltage. Further, the solenoid valve 39 is closed when the heat medium temperature on the outlet side of the evaporator 4 is below a predetermined value, and is opened when the temperature is above a predetermined value.
次に、作用について第4図及び第5図に基づい
て説明する。冷媒流れ方向を実線矢印にて示す。
通常負荷の場合について説明する。この場合、蒸
発器4出口側熱媒体温度が所定値以上ある為、電
磁弁39は開路している。圧縮機1より吐出され
た冷媒ガスは凝縮器2にて凝縮液化され減圧装置
3に導かれる。減圧装置3においては、凝縮器2
から供給された液冷媒は主絞り部32を流通し
て、減圧され、蒸発器4で蒸発して、冷却作用を
なす。また、凝縮器2から供給された液冷媒の一
部は、電気式膨脹弁38で減圧され、冷媒流通路
33内で蒸発して、主絞り部32内を流通する冷
媒を冷却するので、主絞り部32内の冷媒流量は
増大する。 Next, the operation will be explained based on FIGS. 4 and 5. The direction of refrigerant flow is indicated by solid arrows.
The case of normal load will be explained. In this case, the electromagnetic valve 39 is open because the temperature of the heat medium on the outlet side of the evaporator 4 is higher than the predetermined value. Refrigerant gas discharged from the compressor 1 is condensed and liquefied in a condenser 2 and guided to a pressure reducing device 3. In the pressure reducing device 3, the condenser 2
The liquid refrigerant supplied from the main throttle section 32 is depressurized and evaporated in the evaporator 4 to perform a cooling effect. Further, a part of the liquid refrigerant supplied from the condenser 2 is depressurized by the electric expansion valve 38 and evaporated in the refrigerant flow path 33 to cool the refrigerant flowing in the main constriction section 32. The flow rate of refrigerant in the throttle section 32 increases.
上記状態より、更に、負荷が減少した場合、電
気式膨脹弁38の開度は更に絞られる。従つて、
主絞り部32内を流通する冷媒の冷却量は少なく
なり、主絞り部32内の冷媒流量は減少する。更
に負荷が減少し、第5図に示すA′点の直前に到
達した時、電磁弁39の開度は全閉状態となり、
主絞り部32内を流通する冷媒の冷却量は0とな
り、完全なキヤピラリーチユーブ制御と同様とな
る。なお、更に、負荷が減少して、第5図に示す
A′点を下まわると、電磁弁39は閉路し同時に
電気式膨張弁38の開度は開状態となり、A−
A′で示される冷媒循環量はA′点直前と同量とな
る。更に、負荷が減少した場合(例えば第5図に
示すC′点)は、電気式膨張弁38の開度は減少
し、C−C′で示される冷媒循環量を流す。なお、
第5図中、CAA′C′によつて梱まれた範囲は電
気式膨脹弁38によつて確保される循環量を示し
ている。 When the load is further reduced from the above state, the opening degree of the electric expansion valve 38 is further reduced. Therefore,
The amount of cooling of the refrigerant flowing through the main constriction section 32 decreases, and the flow rate of the refrigerant within the main constriction section 32 decreases. When the load further decreases and reaches just before point A' shown in Fig. 5, the opening degree of the solenoid valve 39 becomes fully closed.
The amount of cooling of the refrigerant flowing through the main constriction section 32 becomes 0, which is similar to complete capillary reach tube control. Furthermore, the load is further reduced, as shown in Fig. 5.
When the temperature drops below point A', the solenoid valve 39 closes and at the same time, the electric expansion valve 38 becomes open, and A-
The amount of refrigerant circulation indicated by A' is the same as that just before point A'. Furthermore, when the load decreases (for example, at point C' shown in FIG. 5), the opening degree of the electric expansion valve 38 decreases, allowing a circulating amount of refrigerant shown by C-C' to flow. In addition,
In FIG. 5, the area enclosed by CAA'C' indicates the amount of circulation ensured by the electric expansion valve 38.
以上のように構成されているので、負荷の小さ
い運転状態においても、電磁弁の開閉、及び電気
式膨脹弁の開度調整により、最適冷媒循環量を確
保することが出来、比較的簡単な制御で巾広い運
転範囲を、しかも、最適制御出来、空気調和装置
の信頼性を向上させることが可能である。
With the above configuration, even in low-load operating conditions, the optimal refrigerant circulation amount can be ensured by opening and closing the solenoid valve and adjusting the opening of the electric expansion valve, allowing relatively simple control. This enables optimal control over a wide operating range and improves the reliability of the air conditioner.
第1図は、従来例を示す冷凍サイクル図、第2
図は減圧装置の構成を示す構成図、第3図は従来
例を示す、冷凍負荷と最適冷媒循環量との関係
図、第4図は本発明の一実施例を示す冷凍サイク
ル図、第5図は本発明の一実施例を示す冷凍負荷
と最適冷媒循環量との関係図である。
また、図中、1は圧縮機、2は凝縮器、3は減
圧装置、4は蒸発器、32は主絞り部、38は電
気式膨脹弁、39は電磁弁である。なお、図中、
同一符号同一記号は、同一部分及び相当部分を示
す。
Figure 1 is a refrigeration cycle diagram showing a conventional example;
Figure 3 is a configuration diagram showing the configuration of a pressure reducing device, Figure 3 is a diagram showing the relationship between refrigeration load and optimal refrigerant circulation amount, which shows a conventional example, Figure 4 is a refrigeration cycle diagram showing an embodiment of the present invention, and Figure 5 The figure is a diagram showing the relationship between the refrigeration load and the optimum refrigerant circulation amount, showing one embodiment of the present invention. Further, in the figure, 1 is a compressor, 2 is a condenser, 3 is a pressure reducing device, 4 is an evaporator, 32 is a main throttle section, 38 is an electric expansion valve, and 39 is a solenoid valve. In addition, in the figure,
The same reference numerals indicate the same parts and corresponding parts.
Claims (1)
らの液冷媒を減圧する主絞り部と上記電磁弁およ
び上記主絞り部と並列に設けられ、上記凝縮器か
らの液冷媒の一部により上記主絞り部を冷却する
と共に冷却後の冷媒は上記主絞り部を流通した冷
媒と合流するように配設されたバイパス路と冷凍
サイクルの運転状態に応じて上記バイパス路の冷
媒流量を加減して上記主絞り部の冷却量を変える
電気式膨脹弁とからなる冷媒流量制御装置を備
え、上記冷凍サイクルの冷凍負荷の小さいときは
上記電磁弁を閉路して上記電気式膨脹弁のみによ
り冷媒流量を制御し、上記冷凍サイクルの冷凍負
荷の大きいときは上記電磁弁を開路して電磁弁お
よび上記電気式膨脹弁により冷媒流量を制御する
ようにしたことを特徴とする空気調和装置。1. A solenoid valve and a main constriction section for reducing the pressure of the liquid refrigerant from the condenser flowing through the solenoid valve, and a main constriction section provided in parallel with the solenoid valve and the main constriction section, and a part of the liquid refrigerant from the condenser The main throttle section is cooled, and the refrigerant after cooling is adjusted to adjust the refrigerant flow rate in the bypass channel according to the operating state of the bypass channel and the refrigeration cycle arranged so that the cooled refrigerant merges with the refrigerant that has passed through the main throttle section. A refrigerant flow control device includes an electric expansion valve that changes the amount of cooling in the main throttle section, and when the refrigeration load of the refrigeration cycle is small, the solenoid valve is closed and the refrigerant flow rate is controlled only by the electric expansion valve. An air conditioning apparatus characterized in that when the refrigeration load of the refrigeration cycle is large, the solenoid valve is opened and the refrigerant flow rate is controlled by the solenoid valve and the electric expansion valve.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58230974A JPS60122871A (en) | 1983-12-05 | 1983-12-05 | Air conditioner |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58230974A JPS60122871A (en) | 1983-12-05 | 1983-12-05 | Air conditioner |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60122871A JPS60122871A (en) | 1985-07-01 |
| JPH0221510B2 true JPH0221510B2 (en) | 1990-05-15 |
Family
ID=16916237
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58230974A Granted JPS60122871A (en) | 1983-12-05 | 1983-12-05 | Air conditioner |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60122871A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0737106Y2 (en) * | 1989-06-09 | 1995-08-23 | タバイエスペック株式会社 | Expansion device in refrigeration circuit |
-
1983
- 1983-12-05 JP JP58230974A patent/JPS60122871A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60122871A (en) | 1985-07-01 |
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