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JPS6042858B2 - air conditioner - Google Patents
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JPS6042858B2 - air conditioner - Google Patents

air conditioner

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Publication number
JPS6042858B2
JPS6042858B2 JP8811980A JP8811980A JPS6042858B2 JP S6042858 B2 JPS6042858 B2 JP S6042858B2 JP 8811980 A JP8811980 A JP 8811980A JP 8811980 A JP8811980 A JP 8811980A JP S6042858 B2 JPS6042858 B2 JP S6042858B2
Authority
JP
Japan
Prior art keywords
circuit
output
air conditioner
outputs
control circuit
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
JP8811980A
Other languages
Japanese (ja)
Other versions
JPS5714165A (en
Inventor
博 藤枝
勇 奥田
賢一郎 今須
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP8811980A priority Critical patent/JPS6042858B2/en
Publication of JPS5714165A publication Critical patent/JPS5714165A/en
Publication of JPS6042858B2 publication Critical patent/JPS6042858B2/en
Expired legal-status Critical Current

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  • Air Conditioning Control Device (AREA)

Description

【発明の詳細な説明】 本発明は圧縮機、熱交換器、電気信号によりその弁開
度を調節し得る電気式膨張弁等より冷凍サイクルを形成
してなる空気調和装置に関し、特に前記電気式膨張弁の
制御の信頼性を高めることを目的とする。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an air conditioner in which a refrigeration cycle is formed by a compressor, a heat exchanger, an electric expansion valve whose valve opening degree can be adjusted by an electric signal, and more particularly to The purpose is to improve the reliability of expansion valve control.

従来より電気式膨張弁としては、ヒータとバイメタルを
組合せ、ヒータへの通電量によりその発熱量を調節し、
バイメタルの変位置を変化させてその弁開度を調節する
もの、あるいはモータにより弁開度を調節するものなど
があつた。
Conventionally, electric expansion valves combine a heater and a bimetal, and adjust the amount of heat generated by the amount of electricity applied to the heater.
There were some that adjusted the valve opening by changing the position of a bimetal, and others that used a motor to adjust the valve opening.

電気式膨張弁を用いた冷凍サイクルの概略構成を第9図
に示す。第9図で、1は圧縮機、2は凝縮器、3は電気
式膨張弁、4は蒸発器である。5Aは蒸発器3の中間部
(入口側でもよい)に設けた第1の温度センサ、5Bは
蒸発器3の出口側に設けた第2の温度センサで、それぞ
れの温度センサ5A,5Bにて検出する温度差SH″が
一定になるよう、制御回路5は電気式膨張弁3の弁開度
を制御する電気信号を出力している。
FIG. 9 shows a schematic configuration of a refrigeration cycle using an electric expansion valve. In FIG. 9, 1 is a compressor, 2 is a condenser, 3 is an electric expansion valve, and 4 is an evaporator. 5A is a first temperature sensor provided at the middle part (or the inlet side) of the evaporator 3, and 5B is a second temperature sensor provided at the outlet side of the evaporator 3. The control circuit 5 outputs an electric signal to control the valve opening degree of the electric expansion valve 3 so that the detected temperature difference SH'' becomes constant.

ここで前記温度?H″は蒸発器4内の冷媒圧力降下がゼ
ロであれば、過熱度SHとなるが、冷媒圧力降下がゼロ
でなければ圧力降下相当分の温度ΔTを過熱際Hから引
いた値、すなわちSH″=SH−ΔTとなる。したがつ
てΔTがSHに比して無視し得る程度に小さいかまたは
ΔTが一定であれば温度差SH″は過熱度SHまたはS
Hに一定値を引いたSH相応の値となり、温度差SH″
を略々一定に維持することにより、過熱度SH一定の冷
凍サイクルの最適運転状態を実現できる。第10図は電
気式膨張弁3の弁開度PVに対する温度差SH″の関係
を示す。今冷凍サイクルがサイクル1の曲線上で運転さ
れてい.るとすれば、サイクル最適過熱度SH″1を得
るための弁開度0Vは0V1である。また例えば圧縮機
1の容量変化や内外気温の変化や凝縮器2あるいは蒸発
器4の送風ファン(図示せず)の速度変化などがあつて
、冷凍サイクルがサイクル2の曲線!上で運転されれば
、最適過熱度SH]を得るための弁開度0Vは0V2で
ある。冷凍サイクル1の状態で運転しており、そのとき
弁開度0Vが0V1に制御され、SH″がSH″1に制
御されているとする。この状態からサイクル2に急変し
たとき、冷・凍サイクル状態検出器としての第1,第2
の温度センサの応答遅れのために、この変化を認識でき
ず、あるいは変化を検出し弁開度0Vを0V1から0■
2へ変える信号を出力しても、電気式膨張弁3の応答遅
れのため、弁開度0Vは0V1から0V2へすぐ変化し
ない。そこでサイクル2で弁開度0Vが0V1のままで
あれば、温度差SH″はSH″2となる。この温度はS
H″2〈SH″1であるから、制御回路5はサイクル2
の点Cとの区別がつかないため、弁開度p■を小さくし
て温度差SH″を大きくしようとする。ところが現在の
動作点は点Bであるから、これから更に弁開度0Vが小
さくなるから、ますます温度差SH″は小となり、これ
に”よりさらに弁開度PVを小さくしようとする。この
ような状態では結局電気式膨張弁3の開度はφまでいつ
てしまい、冷凍サイクル2の状態での最適状態(A″点
)が得られない。サイクル1からサイクル2への変化は
上述したように様々な要因により変化するから、冷凍サ
イクル制御上は、弁開度PVの制御によつてサイクルを
正常に制御できる範囲、すなわちサイクル1では弁開度
PVを0VM1以上、サイクル2では弁開度0Vを0V
M2以上の範囲で弁開度PVを制御しなければならず、
もしも上述したように弁開度0Vの制御によつて冷凍サ
イクルを最適状態に制御できない場合は何らかの方法に
より弁開度QVを正常範囲に修正する必要がある。従来
の制御回路ではこのような機能がなかつたので一度上述
した制御不能範囲に入つてしまえば、そこから脱出する
ことができず、正常な空調運転がなされなくなつてしま
うという不都合を生じていた。本発明は上記従来例の欠
点を解消し、もしも上述した制御不能範囲に入つたとき
は、弁開度0Vの強制修正動作を行なわせ、正常範囲に
復帰させる機能を有した制御装置を有する空気調和装置
を提供するものである。
Said temperature here? H'' is the degree of superheating SH if the refrigerant pressure drop in the evaporator 4 is zero, but if the refrigerant pressure drop is zero, it is the value obtained by subtracting the temperature ΔT equivalent to the pressure drop from the H during superheating, that is, SH ″=SH−ΔT. Therefore, if ΔT is negligibly small compared to SH or ΔT is constant, the temperature difference SH'' will be the superheat degree SH or S.
The value corresponding to SH is obtained by subtracting a certain value from H, and the temperature difference SH''
By keeping SH substantially constant, an optimal operating state of the refrigeration cycle in which the degree of superheating SH is constant can be realized. FIG. 10 shows the relationship between the temperature difference SH'' and the valve opening degree PV of the electric expansion valve 3.If the refrigeration cycle is currently operated on the curve of cycle 1, then the cycle optimum superheat degree SH''1 The valve opening degree 0V to obtain is 0V1. Also, for example, due to changes in the capacity of the compressor 1, changes in the internal and external temperatures, and changes in the speed of the blower fan (not shown) of the condenser 2 or evaporator 4, the refrigeration cycle changes to the cycle 2 curve! If the engine is operated above, the valve opening degree 0V to obtain the optimum superheat degree SH is 0V2. It is assumed that the refrigeration cycle 1 is being operated, and that the valve opening degree 0V is controlled to 0V1 and SH'' is controlled to SH''1. When there is a sudden change from this state to cycle 2, the first and second refrigeration cycle state detectors
Due to the delay in the response of the temperature sensor, this change cannot be recognized, or the change is detected and the valve opening degree is changed from 0V1 to 0.
Even if a signal to change the value to 2 is output, the valve opening degree 0V does not immediately change from 0V1 to 0V2 due to the response delay of the electric expansion valve 3. Therefore, if the valve opening degree 0V remains 0V1 in cycle 2, the temperature difference SH'' becomes SH''2. This temperature is S
Since H″2<SH″1, the control circuit 5 is in cycle 2.
Since the valve opening cannot be distinguished from point C, an attempt is made to reduce the valve opening p■ to increase the temperature difference SH''.However, since the current operating point is point B, the valve opening 0V will become smaller from now on. Therefore, the temperature difference SH'' becomes smaller and smaller, which causes the valve opening PV to be further reduced.In such a state, the opening of the electric expansion valve 3 ends up reaching φ, and the refrigeration The optimum state (point A'') in the state of cycle 2 cannot be obtained. The change from cycle 1 to cycle 2 changes due to various factors as described above, so in terms of refrigeration cycle control, the cycle can be normally controlled by controlling the valve opening degree PV, that is, in cycle 1, the valve opening is degree PV is 0VM1 or more, and in cycle 2, the valve opening degree is 0V.
The valve opening PV must be controlled in a range of M2 or more,
If the refrigeration cycle cannot be controlled to the optimum state by controlling the valve opening degree 0V as described above, it is necessary to correct the valve opening degree QV to a normal range by some method. Conventional control circuits did not have such a function, so once they entered the above-mentioned uncontrollable range, there was no way out and normal air conditioning operation was no longer possible. . The present invention solves the drawbacks of the conventional example, and if the above-mentioned uncontrollable range is entered, the valve opening is forcibly corrected to 0 V, and the air conditioner is equipped with a control device that has the function of returning the valve to the normal range. It provides a harmonization device.

このような制御を実現するためには、(1)弁開度0V
の制御では温度差SH″が制御できない制御不能状態か
否かの検出、(2)検出結果としてもしも制御不能状態
のときの制御の内容、(3)前記制御不能状態が前記の
制御により制御可能状態となつたときの状態の検出と強
制修正制御の終了という三つの要素を実現する必要があ
る。
In order to realize such control, (1) the valve opening degree is 0V;
Detection of whether the temperature difference SH'' is in an uncontrollable state that cannot be controlled by the control of It is necessary to realize three elements: detection of the condition when the condition occurs and termination of forced correction control.

(1)制御不能状態の検出。(1) Detection of an uncontrollable state.

制御不能状態の検出方法としては次の三つが考えられる
。(1−1) 電気式膨張弁3への制御回路5の出力信
号。
The following three methods can be considered for detecting an uncontrollable state. (1-1) Output signal of control circuit 5 to electric expansion valve 3.

ヒータとバイメタルを組合せた熱電式膨張弁(通電
閉形)の印加電圧VTと弁開度0Vとの関係を第1図に
示す。
FIG. 1 shows the relationship between the applied voltage VT and the valve opening degree of 0 V of a thermoelectric expansion valve (energized closed type) that combines a heater and a bimetal.

冷凍サイクルの変化を考えて、弁開度0Vとしては0V
min〜0Vmaxであり、相当する電圧をVTmin
とVTmaxとする。今第10図のサイクルがサイクル
1で0V1=0Vminとする。このとき印加電圧■T
は■τMaxである。もしもサイクル1から2へ変化し
たときは、上述したように制御回路5は弁開度0Vを小
さくする方向すなわちVTmaxよりも大きな電圧を出
力す1る。そこで、V,maxよりも大きな適当な電圧
VD〉■Tmaxよりも、■,が大きくなつた場合は明
らかに制御不能範囲であるから、これにより不能状態の
検出ができる。これは電気回路的には、例えば第2図に
示す回路で容1易に実現できる。第2図で、50は制御
回路で、第1の温度センサ5Aとしてのサーミスタ5A
1第2の温度センサ5Bとしてのサーミスタ5Bで検出
する温度の差により、熱電式膨張弁3の印加電圧■ァを
制御し、前記温2度差を略々一定に保つ。60は検出回
路で、抵抗6B,6Cで電圧■。
Considering changes in the refrigeration cycle, the valve opening degree is 0V.
min to 0Vmax, and the corresponding voltage is VTmin
and VTmax. Now assume that the cycle in FIG. 10 is cycle 1 and 0V1=0Vmin. At this time, the applied voltage ■T
is ■τMax. If the cycle changes from cycle 1 to cycle 2, the control circuit 5 outputs a voltage larger than VTmax in the direction of decreasing the valve opening degree 0V, as described above. Therefore, if the appropriate voltage VD larger than V,max>2 becomes larger than Tmax, it is clearly in the uncontrollable range, so that an uncontrollable state can be detected. In terms of an electrical circuit, this can be easily realized using, for example, the circuit shown in FIG. In FIG. 2, 50 is a control circuit, and a thermistor 5A as a first temperature sensor 5A.
1. Based on the temperature difference detected by the thermistor 5B as the second temperature sensor 5B, the voltage applied to the thermoelectric expansion valve 3 is controlled to keep the temperature difference of 2 degrees approximately constant. 60 is a detection circuit, and voltage ■ is generated by resistors 6B and 6C.

を得て、電圧比較器6Aで電圧■。と電圧VTとを比較
し、もしも■。〉■T(正常)なら電圧比較器6A出力
はHi(この場合出力形式はオープンコレク2夕),■
oく■T(異常)なら6A出力はbとなる。この実施例
では、異常の場合、制御回路5の出力電圧=熱電式膨張
弁3の印加電圧TVを強制的にφ■にし、その弁開度を
全開としている。この実施例では極めて簡単な回3路で
確実に異常を検出できる。(1−2)蒸発器温度TOV
AO 蒸発器4の第1の温度センサ5Aで検している温度すな
わち蒸発器温度TEVAは通常の正常運転中は冷媒が気
液二相状態となつてい3るので比較的低温となつている
The voltage comparator 6A gives the voltage ■. Compare and voltage VT, and if ■. 〉■ If T (normal), the voltage comparator 6A output is Hi (in this case, the output format is open collector 2), ■
If it is T (abnormal), the 6A output will be b. In this embodiment, in the case of an abnormality, the output voltage of the control circuit 5 = the applied voltage TV of the thermoelectric expansion valve 3 is forcibly set to φ■, and the valve opening degree is set to be fully open. In this embodiment, an abnormality can be reliably detected using three extremely simple circuits. (1-2) Evaporator temperature TOV
The temperature detected by the first temperature sensor 5A of the AO evaporator 4, that is, the evaporator temperature TEVA, is relatively low during normal operation because the refrigerant is in a gas-liquid two-phase state.

然るに、電気式膨張弁3の弁開度不足が発生すれば冷媒
循環量が不足し、そのために冷媒は蒸発器4の入口部付
近で全部蒸発してしまい、これにより、蒸発器温度TO
ぃが上昇する。サイク4ルの正常な運転時の蒸発器温度
TEVAのとり得る範囲の最大値TEVAmaxよりも
、現在の蒸発器温度TεVAが高くなれば、これは異常
状態である。この方法を具体的に実現する電気回路の一
例として第3図の回路がある。51は制御回路5の実施
例で、この回路では第1の温度センサとしてサーミスタ
5Aで検出する温度TEVAと図中の電圧■Eとは抵抗
5Cを適当に選べば、所定の温度範囲で直線関係となる
However, if the electric expansion valve 3 is insufficiently opened, the amount of refrigerant circulated will be insufficient, and the refrigerant will all evaporate near the inlet of the evaporator 4, causing the evaporator temperature TO to decrease.
i rises. If the current evaporator temperature TεVA is higher than the maximum value TEVAmax of the possible range of the evaporator temperature TEVA during normal operation of cycle 4, this is an abnormal state. An example of an electric circuit that specifically implements this method is the circuit shown in FIG. 51 is an embodiment of the control circuit 5. In this circuit, the temperature TEVA detected by the thermistor 5A as the first temperature sensor and the voltage E in the figure have a linear relationship within a predetermined temperature range if the resistor 5C is appropriately selected. becomes.

すなわち次式で表わせる。そこで、A:比例定数B:定
数 ときの電圧VOは次のようになる。
In other words, it can be expressed by the following equation. Therefore, the voltage VO when A: proportionality constant and B: constant is as follows.

この電圧 ▼P−1し11141f116V^11μ
′lll υよりも電圧■。が小さくなれば、蒸発器温
度TEVAがTBVA>TIll:VAmaxとなる。
61は検出回路で、電源を抵抗61A,61Bによつて
分割して電圧■5minを得て、この電圧Tlll:M
in<5TEとを電圧比較器61Cにより比較し、TE
>Tε而n(正常)なら電圧比較器61C出力はHi.
.TIll:くTOmin(異常)なら電圧比較器61
C出力はbとなり、この実施例では膨張弁3の印加電圧
を強制的にゼロとし、弁開度を全開とする。
This voltage ▼P-111141f116V^11μ
Voltage ■ than ′llll υ. If becomes smaller, the evaporator temperature TEVA becomes TBVA>TIll:VAmax.
61 is a detection circuit, which divides the power supply by resistors 61A and 61B to obtain a voltage of 5 min, and this voltage Tllll:M
in<5TE by the voltage comparator 61C, and TE
> Tε n (normal), the voltage comparator 61C output is Hi.
.. TIll: If TOmin (abnormal), voltage comparator 61
The C output becomes b, and in this embodiment, the applied voltage to the expansion valve 3 is forcibly set to zero, and the valve opening degree is set to be fully open.

この実施例では蒸発器4の動作状態に応じてサイクルの
異常/正常を検出するため状態検出が極めて確実に行な
える。(1−3) 制御回路出力とサイクル応答との関
係。
In this embodiment, since abnormality/normality of the cycle is detected according to the operating state of the evaporator 4, the state can be detected extremely reliably. (1-3) Relationship between control circuit output and cycle response.

例えば第2図で、もしも第1第2の温度センサで検出す
る各温度の温度?βH″が所定の温度差SHRよりも大
きければ、膨張弁印加電圧■τが小さくなり、弁開度0
■を広くし温度差SH″を小さくしようとする。
For example, in Figure 2, what is the temperature of each temperature detected by the first and second temperature sensors? If βH'' is larger than the predetermined temperature difference SHR, the expansion valve applied voltage ■τ becomes small and the valve opening becomes 0.
(2) is widened to try to reduce the temperature difference SH''.

サイクルの正常な動作では、この動作により温度?H″
は小さくなる。しかし異常時は第10図に示すように弁
開度0■を広くすれば温度差SH″は大きくなる。した
がつて現在の状態の正常または異常の判別は制御回路5
の出力の方向に対する温度差SH″の方向によつて判別
できる。具体的には第4図に示すような実施例で実現で
きる。52は制御回路5の他の実施例で、52Aはアナ
ログマルチプレクサ、52Bはアナログマルチプレクサ
52Aで選択した第1または第2の温度センサ5A,5
Bのアナログ出力をデジタル量に変換するA/Dコンバ
ータ、52CはA/Dコンバータ52Bの出力を受け、
前記温度差SH″が一定となる制御をプログラム的に実
現しているマイクロコンピュータで、制御結果を出力し
52DなるD/Aコンバータにてアナログ量に変換し膨
張弁3に出力する。
In normal operation of the cycle, this operation causes temperature? H″
becomes smaller. However, in the event of an abnormality, as shown in Fig. 10, if the valve opening degree 0 is widened, the temperature difference SH'' will increase.
This can be determined based on the direction of the temperature difference SH'' with respect to the direction of the output of , 52B is the first or second temperature sensor 5A, 5 selected by the analog multiplexer 52A.
An A/D converter 52C that converts the analog output of B into a digital quantity receives the output of the A/D converter 52B,
A microcomputer that programmatically implements control to keep the temperature difference SH'' constant outputs the control result, converts it into an analog quantity with a 52D D/A converter, and outputs it to the expansion valve 3.

ここで、温度差SH″を一定のサンプリング周期Tsに
したがつて求め、サンプリングとサンプリングの間出力
を保持する。
Here, the temperature difference SH'' is determined according to a constant sampling period Ts, and the output is held between samplings.

あるサンプリング時点TSiで電圧VTi>VTi−1
(■Ti−1は1サンプリング前の時点TSO−1での
出力)を出力したとき1サンプリング後の時点TSI+
1で測定した温度差SH″i+1がサンプリング時点T
Siでの温度差SH″iと、SH″+1〉SH″iの関
係を満足していれば正常、そうでなければ異常と判別で
きる。以上述べた手順は全てマイクロコンピュータ52
C内部のプログラムによつて処理することができる。し
たがつて上述した検出回路はマイクロコンピュータ52
C内にプログラム的に実現されている。この方法では制
御出力に対する応答の合理性を判定するのでサイクルの
異常状態を確実に検出できる。(2)異常時制御。
At a certain sampling point TSi, voltage VTi>VTi-1
(■Ti-1 is the output at time TSO-1 one sampling before) When outputting, the time TSI+ after one sampling
The temperature difference SH″i+1 measured at 1 is the sampling time T
If the relationship between the temperature difference SH″i in Si and SH″+1>SH″i is satisfied, it can be determined to be normal, and if not, it can be determined to be abnormal. All the steps described above are performed by the microcomputer 52
It can be processed by a program inside C. Therefore, the above-mentioned detection circuit is implemented by the microcomputer 52.
It is implemented programmatically in C. Since this method determines the rationality of the response to the control output, it is possible to reliably detect abnormal conditions in the cycle. (2) Abnormality control.

既に第2図および第3図の実施例で示したように、弁開
度PVの強制修正動作として弁開度0Vを全開とする制
御がある。ここでは異常を検出する検出回路と、検出回
路出力により制御回路出力を制御する出力制御回路とが
兼用されている。この回路では、図示したように極めて
簡単でしかも安価な回路で出力を制御できる。弁開度Q
Vを全開にしないで、冷凍サイクルを正常状態に戻す場
合、少くとも0Vmaxにすればよい。
As already shown in the embodiments of FIGS. 2 and 3, as a forced correction operation of the valve opening degree PV, there is control to fully open the valve opening degree 0V. Here, the detection circuit that detects an abnormality and the output control circuit that controls the control circuit output based on the detection circuit output are used. With this circuit, the output can be controlled with an extremely simple and inexpensive circuit as shown. Valve opening Q
When returning the refrigeration cycle to a normal state without fully opening V, it is sufficient to set it to at least 0Vmax.

このような制御を実現する回路例を第5図示す。第5図
で、第2図と異なるのは制御回路53にはアナログスイ
ッチ53Aが付加され、検出回路62は電圧比較器出力
にプルアップ抵抗が付加され、さらに出力制御回路70
が付加されている。正常状態では検出回路62の出力は
Hiで、アナログスイッチ53Aのみがオンし、温度差
SH″に基づく制御をしている。もしもサイクルが異常
となり、検出回路62の出力がLOとなると、出力制御
回路70のインバータ70A出力がHiとなり、アナロ
グスイッチ70Bがオンし、出力制御回路70の出力は
電源70Cの電圧■Tminとなる。一方アナログスイ
ッチ53Aはオフしているので、膨張弁3の印加電圧■
TはVTminとなり、弁開度0Vは0Vmaxとなる
。弁開度0■を0Vmaxにすることの利点は膨張弁3
が活性の状態のままなので後述ザる復帰回路により正常
の制御に復帰したときの立上り速度が速くなることであ
る。またサイクルの状態によつては弁開度0Vが全開で
は液状態のままで圧縮機に冷媒が戻るいわゆる液バック
が発生する危険性があるが、弁開度PVを0Vminに
保つことによつてその危険性を減少できる。3)正常動
作への復帰。
FIG. 5 shows an example of a circuit that realizes such control. 5, the difference from FIG. 2 is that an analog switch 53A is added to the control circuit 53, a pull-up resistor is added to the voltage comparator output of the detection circuit 62, and an output control circuit 70 is added to the detection circuit 62.
is added. In a normal state, the output of the detection circuit 62 is Hi, only the analog switch 53A is turned on, and control is performed based on the temperature difference SH''. If the cycle becomes abnormal and the output of the detection circuit 62 becomes LO, the output control is disabled. The output of the inverter 70A of the circuit 70 becomes Hi, the analog switch 70B turns on, and the output of the output control circuit 70 becomes the voltage ■Tmin of the power supply 70C.On the other hand, since the analog switch 53A is off, the voltage applied to the expansion valve 3 ■
T becomes VTmin, and the valve opening degree 0V becomes 0Vmax. The advantage of setting the valve opening degree from 0■ to 0Vmax is that the expansion valve 3
Since the control remains active, the rise speed becomes faster when normal control is restored by the return circuit described below. Also, depending on the cycle condition, if the valve opening PV is fully open, there is a risk that so-called liquid back may occur, where the refrigerant returns to the compressor in a liquid state.However, by keeping the valve opening PV at 0Vmin, You can reduce that risk. 3) Return to normal operation.

(3−1) タイマ。(3-1) Timer.

異常を検出して膨張弁への出力制御開始時から所定の時
間が経過すれば、どのようなサイクル状態でも正常動作
範囲に復帰する。
If a predetermined time period elapses from the time when an abnormality is detected and the output control to the expansion valve is started, the normal operating range will be restored regardless of the cycle state.

ある状態では、上述したように液バックが発生する。液
バックが発生しても、そこでは温度差SH″により膨張
弁3を制御することにより、温度差SH″を所定の温度
差別?に制御できるので、正常動作範囲といえる。それ
で、出力の制御から所定時間経過したら、制御を温度差
SH″による制御に復帰させる。これは例えば第6図の
回路で実現できる。63は検出回路60に逆流防止用ダ
イオード63Aを付加したものである。
In certain conditions, liquid backing occurs as described above. Even if a liquid back-up occurs, the expansion valve 3 is controlled based on the temperature difference SH'', so that the temperature difference SH'' is adjusted to a predetermined temperature difference. This can be said to be within the normal operating range. Then, after a predetermined period of time has elapsed from the output control, the control is returned to control based on the temperature difference SH''. This can be realized, for example, by the circuit shown in FIG. It is.

80は復帰回路で、検出回路63が異常を検出してLO
を出力するとトランジスタ80Aがオフし、コンデンサ
が充電を開始し、所定時間が経過すると電圧比較器80
Bの出力が肪となり、検出回路63の電圧比較器6Aの
非反転入力はほぼ−Vccとなり、電圧比較器6Aの出
力はHiの正常出力が復帰される。
80 is a recovery circuit, in which the detection circuit 63 detects an abnormality and outputs LO.
When the transistor 80A is output, the transistor 80A turns off, the capacitor starts charging, and after a predetermined period of time, the voltage comparator 80A turns off.
The output of the voltage comparator 6A of the detection circuit 63 becomes approximately -Vcc, and the output of the voltage comparator 6A returns to the normal output of Hi.

このときトランジスタ80Aはオンし、これにより電圧
比較器80Bの出力はHiとなる。このようにタイマに
より強制復帰させることにより、異常動作を終了させる
ことができるが、この方法は回路80の多少の変更によ
り検出回路61にも適用可能だし、また第4図のように
マイクロコンピュータを用いたものにあつてはさらに容
易に実現できる。(3−2) 蒸発器温度TIll:V
AO異常動作により、弁開度0Vを全開または所定の開
度に制御すれば蒸発器温度T。
At this time, the transistor 80A is turned on, so that the output of the voltage comparator 80B becomes Hi. The abnormal operation can be terminated by forcing a return using a timer, but this method can also be applied to the detection circuit 61 by making some changes to the circuit 80, and can also be applied to the detection circuit 61 as shown in FIG. This can be realized even more easily if the method is used. (3-2) Evaporator temperature TIll:V
If the valve opening degree 0V is controlled to be fully open or to a predetermined opening degree due to the abnormal AO operation, the evaporator temperature T will be maintained.

VAは低下してくる。それで、正常動作をし得る温度T
EVANMに達したとき、異常動作を終了すればよい、
この回路例を第7図に示す。64は検出回路61に逆流
防止用ダイオード64Aを付加した検出回路である。
VA is decreasing. Therefore, the temperature T at which normal operation can occur
When EVANM is reached, the abnormal operation should be terminated.
An example of this circuit is shown in FIG. 64 is a detection circuit in which a backflow prevention diode 64A is added to the detection circuit 61.

81は復帰回路で、トランジスタ81B1抵抗81C等
から成りいわゆるヒステリシス回路となつている。
Reference numeral 81 denotes a recovery circuit, which is composed of a transistor 81B, a resistor 81C, etc., and is a so-called hysteresis circuit.

異常動作となり、電圧比較器61Cがノ肪出力となると
トランジスタ81Bがオンし、電圧比較器61CはTE
.VANM相当の電圧とTEVAとを比較し、異常動作
によりT[11:VAが低下し)TεVA<TIll:
VANM(くTEVAmaX)となると、電圧比較器6
1C出力はHiとなり、正常動作に復帰する。
When an abnormal operation occurs and the voltage comparator 61C becomes a normal output, the transistor 81B turns on and the voltage comparator 61C becomes TE.
.. Compare the voltage equivalent to VANM and TEVA and find that T[11:VA decreases due to abnormal operation] TεVA<TIll:
When it comes to VANM (TEVAmaX), voltage comparator 6
The 1C output becomes Hi and normal operation is restored.

この方法は制御回路50を適当に変更することにより、
検出回路60に対しても使用可能であり、また第4図に
示したように、マイクロコンピュータを使用するものに
あつてはプログラムにより容冫易に実現できる。これは
蒸発器温度という状態に応じた復帰を行なうので、液戻
りに至る前に復帰させることができるという利点がある
。(3−3) 温度差SH″。
This method is achieved by appropriately modifying the control circuit 50.
It can also be used for the detection circuit 60, and as shown in FIG. 4, if a microcomputer is used, it can be easily realized by a program. This has the advantage that it can be restored before the liquid returns because it is restored in accordance with the state of the evaporator temperature. (3-3) Temperature difference SH''.

異常動作により弁開度を所定の弁開度にすることにより
、蒸発器が湿つた状態に戻り、温度差SH″は除々に大
きくなり、さらに湿り液バック方向になり、再び温度差
SH″は低下していく。
By adjusting the valve opening to a predetermined valve opening due to abnormal operation, the evaporator returns to a wet state, the temperature difference SH'' gradually increases, and the damping liquid backs up further, and the temperature difference SH'' increases again. It continues to decline.

そこで、第1の方法としては温度差SH″の時間勾配が
負すなわち温度差SH″が減少傾向になつたとき、異常
動作を終了させる。第2の方法としては温度差SH″が
ある大きさまで戻つた状態で異常動昨を終了させる。
Therefore, the first method is to terminate the abnormal operation when the time gradient of the temperature difference SH'' is negative, that is, when the temperature difference SH'' tends to decrease. The second method is to terminate the abnormal movement when the temperature difference SH'' has returned to a certain level.

まず前者の方法の実現にあつては、第4図に示すマイク
ロコンピュータを使つたものが有利であり、例えば異常
動作に入つたあと、適当な時間間隔にて温度差SWを測
定し、ある時点の温度差SH″iと一測定時間間隔後の
温度?Hi+1とが、SH″i>SH″i+1なる関係
を満足したときに異常動作を終了すればよい。
First, in realizing the former method, it is advantageous to use the microcomputer shown in Fig. 4. For example, after entering abnormal operation, the temperature difference SW is measured at appropriate time intervals, and The abnormal operation may be terminated when the temperature difference SH"i and the temperature ?Hi+1 after one measurement time interval satisfy the relationship SH"i>SH"i+1.

これによれば温度差βH″に基いて異常動作を終了する
ので最も確実に正常動作範囲に戻つたことを検出できる
。後者の方法の実施例を第8図に示す。65は検出回路
60に逆流防止用ダイオード65Aを付加した検出回路
、82は復帰回路で、抵抗82Aと逆流防止用ダイオー
ド82Bよりなるいわゆるヒス テリシス回路を形成し
ている。
According to this method, since the abnormal operation is terminated based on the temperature difference βH'', the return to the normal operating range can be detected most reliably. An embodiment of the latter method is shown in FIG. A detection circuit 82 includes a backflow prevention diode 65A, and a return circuit 82 forms a so-called hysteresis circuit consisting of a resistor 82A and a backflow prevention diode 82B.

異常動作時は検出回路65の電圧比較器出力は肪とな
り、抵抗6Bに並列に抵抗6Cが接続され、温度差SW
が適当な大きさSH″RSTに達する と、制御回路5
0のオペアンプ出力■OはSH′RSTに対応する電圧
■0RSTまで低下し、そのために電圧比較器6A出力
はHiとなり、異常動作が終了する。
During abnormal operation, the voltage comparator output of the detection circuit 65 becomes red.
A resistor 6C is connected in parallel to the resistor 6B, and the temperature difference SW
When reaches an appropriate size SH″RST, the control circuit 5
The operational amplifier output 0 of 0 falls to the voltage 0RST corresponding to SH'RST, so the output of the voltage comparator 6A becomes Hi, and the abnormal operation ends.

この方法を(1−1)の異常検出回路と組合せて用いれ
ば極めて簡単に復帰回路を構成できる。以上述べた説明
では各々単独に説明したが、これらを適宜組合せること
も容易に行なえる。
If this method is used in combination with the abnormality detection circuit (1-1), a recovery circuit can be constructed extremely easily. In the above explanation, each of them has been explained individually, but they can also be easily combined as appropriate.

また復帰の場合タイマと温度差βH″とを組合せるなど
ということも本発明の範囲に属する。以上詳述したよう
に、本発明によれば、何らかの原因で冷凍サイクルが異
常状態になつたとき、これを検出回路で検出し、制御回
路の出力を制御して、強制的に正常状態に復帰させ、冷
凍サイクルが正常動作範囲に入つたことを検出して、先
の異常動作を終了させた正常動作に復帰させるので、従
来例に見られる欠点を排除した極めて動作信頼性の高い
膨張弁制御装置が得られ、異常動作範囲に入つてしまつ
た場合でも復帰できるので、従来例の欠点を排除した空
気調和装置が得られる優れた効果を奏するものである。
Furthermore, in the case of recovery, it also falls within the scope of the present invention to combine a timer and the temperature difference βH''.As detailed above, according to the present invention, when the refrigeration cycle becomes abnormal for some reason, , this was detected by the detection circuit, the output of the control circuit was controlled to force a return to the normal state, and the previous abnormal operation was terminated by detecting that the refrigeration cycle had entered the normal operating range. Since it returns to normal operation, it is possible to obtain an expansion valve control device with extremely high operating reliability that eliminates the drawbacks seen in conventional examples.Even if it enters the abnormal operating range, it can be restored, eliminating the drawbacks of conventional examples. The air conditioner has excellent effects.

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

第1図は通電閉形熱電膨張弁の印加電圧と弁開度の関係
を示す特性図、第2図は本発明の空気調和装置の実施例
における制御回路と検出回路を示す図、第3図は本発明
の他の実施例の制御回路と検出回路を示す図、第4図は
本発明の他の実施例の制御回路のブロック図、第5図は
本発明の出力制御回路を示す図、第6図は本発明の復帰
回路の実施例を示す図、第7図は同他の実施例を示す図
、第8図は同他の実施例を示す図、第9図は従ノ来の冷
凍サイクルの説明図、第10図は膨張弁の開度に対する
温度差SH″の関係を説明する特性図である。 3・・・・・・電気式膨張弁、4・・・・・・蒸発器、
5,50,51,52,53・・・・・制御回路、60
,61,62,63,64,65・・・・・・検出回路
、70・・・・出力制御回路、80,81,82・・・
・・復帰回路。
FIG. 1 is a characteristic diagram showing the relationship between the applied voltage and the valve opening degree of the energized closed thermoelectric expansion valve, FIG. 2 is a diagram showing the control circuit and detection circuit in an embodiment of the air conditioner of the present invention, and FIG. FIG. 4 is a block diagram of a control circuit according to another embodiment of the present invention, FIG. 5 is a diagram showing an output control circuit of the present invention, and FIG. 6 is a diagram showing an embodiment of the recovery circuit of the present invention, FIG. 7 is a diagram showing another embodiment, FIG. 8 is a diagram showing another embodiment, and FIG. 9 is a diagram showing a conventional refrigeration circuit. An explanatory diagram of the cycle, FIG. 10 is a characteristic diagram illustrating the relationship between the temperature difference SH'' and the opening degree of the expansion valve. 3...Electric expansion valve, 4...Evaporator ,
5, 50, 51, 52, 53...control circuit, 60
, 61, 62, 63, 64, 65... detection circuit, 70... output control circuit, 80, 81, 82...
...Return circuit.

Claims (1)

【特許請求の範囲】 1 電気信号によりその弁開度を調節し得る電気式膨張
弁3と、冷凍サイクルの状態に応じて前記電気式膨張弁
3へ弁開度を制御する電気信号を出力し冷凍サイクルを
略々最適状態に維持する制御回路5と、前記制御回路5
の動作にも拘らず冷凍サイクルを最適化できない状態で
あることを検出し、そのとき異常信号を出力する検出回
路と、前記検出回路の出力に応じて、前記制御回路5の
出力電気信号を制御する出力制御回路70と、冷凍サイ
クルが前記制御回路5により最適化できる状態であるこ
とを検出し、前記検出回路の出力または前記出力制御回
路70を制御する正常信号を出力する復帰回路80〜8
2とを具備したことを特徴とする空気調和装置。 2 検出回路は制御回路5の出力電気信号が所定の範囲
を越えたとき異常信号を出力する回路60である特許請
求の範囲第1項記載の空気調和装置。 3 検出回路は空気調和装置の蒸発器温度が所定の温度
以上になつたとき異常信号を出力する回路61である特
許請求の範囲第1項記載の空気調和装置。 4 制御回路5は空気調和装置の蒸発器の入口側または
蒸発器中間部に設けた第1の冷媒温度センサ5Aと、出
口側に設けた第2の冷媒温度センサ5Bと、前記第1の
冷媒温度センサ5Aと前記第2の冷媒温度センサ5Bと
の出力の差に応じて前記電気式膨張弁3へ制御信号を出
力し、前記出力の差を略々一定に維持する回路であり、
検出回路は前記電気式膨張弁3への制御信号の増減に対
する前記出力の差の増減の関係を検出し、前記関係が所
定の関係になつたとき異常信号を出力する回路である特
許請求の範囲第1項記載の空気調和装置。 5 出力制御回路70は前記検出回路が異常信号を出力
したとき、前記電気式膨張弁3の弁開度が所定の開度と
なるよう前記制御回路5の出力電気信号を制御する回路
である特許請求の範囲第1項記載の空気調和装置。 6 復帰回路は前記検出回路が異常信号を出力してから
所定時間経過後に正常信号を出力する回路である特許請
求の範囲第1項記載の空気調和装置。 7 復帰回路は空気調和装置の蒸発器4の温度が所定温
度以下のとき正常信号を出力する回路である特許請求の
範囲第1項記載の空気調和装置。 8 復帰回路は前記出力制御回路70が前記制御回路5
の出力を制御中に、冷凍サイクルの過熱度または相応の
温度差の変化が所定の関係を満足したとき正常信号を出
力する回路である特許請求の範囲第1項記載の空気調和
装置。
[Scope of Claims] 1. An electric expansion valve 3 whose opening degree can be adjusted by an electric signal, and an electric signal which outputs an electric signal to control the valve opening degree to the electric expansion valve 3 according to the state of a refrigeration cycle. a control circuit 5 that maintains the refrigeration cycle in a substantially optimal state; and the control circuit 5.
a detection circuit that detects that the refrigeration cycle cannot be optimized despite the operation of the refrigeration cycle and outputs an abnormal signal at that time, and controls the output electric signal of the control circuit 5 according to the output of the detection circuit. and recovery circuits 80 to 8 that detect that the refrigeration cycle is in a state that can be optimized by the control circuit 5 and output a normal signal that controls the output of the detection circuit or the output control circuit 70.
An air conditioner characterized by comprising: 2. 2. The air conditioner according to claim 1, wherein the detection circuit is a circuit 60 that outputs an abnormal signal when the output electric signal of the control circuit 5 exceeds a predetermined range. 3. The air conditioner according to claim 1, wherein the detection circuit is a circuit 61 that outputs an abnormal signal when the evaporator temperature of the air conditioner exceeds a predetermined temperature. 4. The control circuit 5 includes a first refrigerant temperature sensor 5A provided at the inlet side of the evaporator of the air conditioner or an intermediate portion of the evaporator, a second refrigerant temperature sensor 5B provided at the outlet side, and the first refrigerant temperature sensor 5B provided at the outlet side. A circuit that outputs a control signal to the electric expansion valve 3 according to the difference in output between the temperature sensor 5A and the second refrigerant temperature sensor 5B, and maintains the difference in output substantially constant,
The detection circuit is a circuit that detects the relationship between the increase and decrease of the difference in the output with respect to the increase and decrease of the control signal to the electric expansion valve 3, and outputs an abnormal signal when the relationship becomes a predetermined relationship. The air conditioner according to item 1. 5. The output control circuit 70 is a circuit that controls the output electric signal of the control circuit 5 so that the valve opening of the electric expansion valve 3 becomes a predetermined opening when the detection circuit outputs an abnormal signal. An air conditioner according to claim 1. 6. The air conditioner according to claim 1, wherein the recovery circuit is a circuit that outputs a normal signal after a predetermined time has elapsed after the detection circuit outputs the abnormal signal. 7. The air conditioner according to claim 1, wherein the return circuit is a circuit that outputs a normal signal when the temperature of the evaporator 4 of the air conditioner is below a predetermined temperature. 8 The recovery circuit is such that the output control circuit 70 is connected to the control circuit 5.
The air conditioner according to claim 1, which is a circuit that outputs a normal signal when a change in the degree of superheating of the refrigeration cycle or a corresponding temperature difference satisfies a predetermined relationship while controlling the output of the air conditioner.
JP8811980A 1980-06-27 1980-06-27 air conditioner Expired JPS6042858B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8811980A JPS6042858B2 (en) 1980-06-27 1980-06-27 air conditioner

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8811980A JPS6042858B2 (en) 1980-06-27 1980-06-27 air conditioner

Publications (2)

Publication Number Publication Date
JPS5714165A JPS5714165A (en) 1982-01-25
JPS6042858B2 true JPS6042858B2 (en) 1985-09-25

Family

ID=13934004

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8811980A Expired JPS6042858B2 (en) 1980-06-27 1980-06-27 air conditioner

Country Status (1)

Country Link
JP (1) JPS6042858B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58133570A (en) * 1982-02-01 1983-08-09 松下電器産業株式会社 Controller for refrigeration cycle

Also Published As

Publication number Publication date
JPS5714165A (en) 1982-01-25

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