JPH0674573A - Method for controlling expansion valve in vapor-compression refrigerating apparatus - Google Patents
Method for controlling expansion valve in vapor-compression refrigerating apparatusInfo
- Publication number
- JPH0674573A JPH0674573A JP4243989A JP24398992A JPH0674573A JP H0674573 A JPH0674573 A JP H0674573A JP 4243989 A JP4243989 A JP 4243989A JP 24398992 A JP24398992 A JP 24398992A JP H0674573 A JPH0674573 A JP H0674573A
- Authority
- JP
- Japan
- Prior art keywords
- expansion valve
- control
- opening
- refrigerant
- temperature
- 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.)
- Pending
Links
Landscapes
- Air Conditioning Control Device (AREA)
Abstract
(57)【要約】
【目的】 設置場所により冷媒配管の長さが異なっても
安定した制御をする。
【構成】 冷媒配管を循環する冷媒流量を増減させる膨
張弁の開閉度を蒸発器の内部の温度状態に基づいて制御
部が出力する操作量に応じて制御する蒸気圧縮式冷凍装
置の膨張弁制御方法において、蒸発器の内部の温度状態
の変化から冷媒配管の長さを類推し、類推された冷媒配
管の長さに対応した最適な制御パラメータを制御部に設
定し、膨張弁を制御するようにした。(57) [Summary] [Purpose] Stable control is performed even if the length of the refrigerant pipe varies depending on the installation location. [Composition] Expansion valve control of a vapor compression refrigeration system for controlling the degree of opening / closing of an expansion valve for increasing / decreasing the flow rate of a refrigerant circulating in a refrigerant pipe in accordance with an operation amount output by a control unit based on a temperature state inside an evaporator In the method, the length of the refrigerant pipe is inferred from the change in the temperature state inside the evaporator, and the optimum control parameter corresponding to the inferred length of the refrigerant pipe is set in the control unit to control the expansion valve. I chose
Description
【0001】[0001]
【産業上の利用分野】本発明は、冷媒流量制御用の膨張
弁の開閉度を適切に制御する蒸気圧縮式冷凍装置の膨張
弁制御方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for controlling an expansion valve of a vapor compression refrigeration system, which appropriately controls the opening / closing degree of an expansion valve for controlling the flow rate of a refrigerant.
【0002】[0002]
【従来の技術】一般に、室内空調に利用する蒸気圧縮式
冷凍機では、室内温度が設定温度となるように一定に制
御され、その際、冷凍機自身が所有する冷房能力を最大
限に活用し、かつ、冷凍機内部の冷媒状態を安定に保つ
ために、冷媒流量の制御を行う。例えば、冷房の場合で
は冷凍機が室内から熱を蒸発器の内部の冷媒に吸収し、
凝縮器から室内外に放出されており、室内温度が設定温
度より高いとき冷凍機を最大限に運転し、室内温度が設
定温度より低くなったときコンプレッサの運転を停止し
て室内外の熱交換を停止している。この場合、冷凍機の
内部冷媒状態を安定に保たなければ室内外の熱交換が安
定に行われず、冷凍機の内部状態を安定に保つことで、
結果として室内温度が安定に保たれる。2. Description of the Related Art Generally, in a vapor compression refrigerator used for indoor air conditioning, the indoor temperature is constantly controlled so as to reach a set temperature, and at that time, the cooling capacity of the refrigerator itself is utilized to the maximum extent. In addition, in order to keep the refrigerant state inside the refrigerator stable, the refrigerant flow rate is controlled. For example, in the case of cooling, the refrigerator absorbs heat from the room into the refrigerant inside the evaporator,
Heat is discharged indoors and outdoors from the condenser, and when the room temperature is higher than the set temperature, the refrigerator is operated to the maximum, and when the room temperature is lower than the set temperature, the compressor operation is stopped and the indoor and outdoor heat exchange is performed. Have stopped. In this case, unless the internal refrigerant state of the refrigerator is kept stable, indoor and outdoor heat exchange is not performed stably, and by keeping the internal state of the refrigerator stable,
As a result, the indoor temperature is kept stable.
【0003】一般に、冷凍機の冷媒流量を制御する手段
として膨張弁の開閉度を制御することが行われている。
このための制御手段は原理的なものの分類でも数多く存
在するが、その一例として蒸発器の内部の温度状態の検
知に基づいて制御を行うSuper Heat制御(以
下「SH制御」という)について具体的に説明する。Generally, the opening / closing degree of an expansion valve is controlled as a means for controlling the refrigerant flow rate of a refrigerator.
There are many control means for this purpose even if they are in principle, but one example thereof is the Super Heat control (hereinafter referred to as “SH control”) that performs control based on the detection of the temperature state inside the evaporator. explain.
【0004】図12に、蒸気圧縮式冷凍機の冷媒回路の
概念図を示す。図において、1は蒸発器、2は凝縮器、
3はコンプレッサ、4は膨張弁で、この図は室内冷房機
の場合に適用しており、5は室外機、6は室内機とを示
している。室外機5と室内機6の内部の実線7は、冷媒
が内部を移動する冷媒配管を示しており、点線8は、そ
の冷媒配管7の内で特に室外機5と室内機6とを接続す
るための配管を示している。ここで、冷媒は配管の中を
図示矢印の方向に流れる。図12では、コンプレッサ3
は室外機側にあるが、室内機側にあってもよい。FIG. 12 shows a conceptual diagram of a refrigerant circuit of a vapor compression refrigerator. In the figure, 1 is an evaporator, 2 is a condenser,
3 is a compressor, 4 is an expansion valve, and this drawing is applied to the case of an indoor air conditioner, 5 is an outdoor unit, and 6 is an indoor unit. A solid line 7 inside the outdoor unit 5 and the indoor unit 6 indicates a refrigerant pipe through which the refrigerant moves, and a dotted line 8 connects the outdoor unit 5 and the indoor unit 6 in the refrigerant pipe 7 in particular. Shows the piping for. Here, the refrigerant flows through the pipe in the direction of the arrow in the figure. In FIG. 12, the compressor 3
Is on the outdoor unit side, but may be on the indoor unit side.
【0005】また、冷凍機を室内冷暖房機として使用す
る場合には、コンプレッサ3の出口に四方弁を設けて、
冷媒の流れる向きを切替えることで行われる。図12が
暖房機として動作する場合には、蒸発器1と凝縮器2の
役割は逆転する。蒸発器1と凝縮器2の内部では冷媒配
管7がジグザグに交差しているため、外気に触れる配管
表面積が大きくなり、空気と冷媒との熱交換率が良くな
っている。ここでは、図12を室内冷房機として、SH
制御では、蒸発器内部の冷媒温度、例えば、出口位置a
にある配管内部の冷媒温度と中間位置bにあたる配管内
部の冷媒温度を測定し、その温度差が一定値ecになる
ように制御する。これにより、冷媒機全体の内部状態を
安定にし、かつ高い冷凍能力を引き出す。SH制御で
は、蒸発器単体での情報のみで制御を行えるため、凝縮
器2やコンプレッサ3等の状態を計測することが物理的
に困難、あるいはコスト的に困難な場合に有効な制御手
段である。When the refrigerator is used as an indoor air conditioner, a four-way valve is provided at the outlet of the compressor 3,
This is done by switching the direction in which the refrigerant flows. When FIG. 12 operates as a heater, the roles of the evaporator 1 and the condenser 2 are reversed. Since the refrigerant pipes 7 intersect in a zigzag manner inside the evaporator 1 and the condenser 2, the surface area of the pipes exposed to the outside air is increased and the heat exchange rate between air and the refrigerant is improved. Here, as shown in FIG. 12 as an indoor air conditioner, the SH
In the control, the temperature of the refrigerant inside the evaporator, for example, the outlet position a
The temperature of the refrigerant inside the pipe at and the temperature of the refrigerant inside the pipe corresponding to the intermediate position b are measured, and the temperature difference is controlled to be a constant value ec. As a result, the internal state of the entire refrigerant machine is stabilized and a high refrigerating capacity is brought out. Since the SH control can be controlled only by the information of the evaporator itself, it is an effective control means when it is physically difficult or costly to measure the states of the condenser 2, the compressor 3, and the like. .
【0006】ところで、冷媒流量制御用の膨張弁4は、
一般に電動式のもので、その開閉度を離散的に制御で
き、制御パルスを入力することにより、単位操作量とし
て1開閉ステップ量を変化させることができる。つま
り、例えば、完全閉状態での開閉度を0、完全開状態で
の開閉度を500とすると、その間の開閉度を500ス
テップ分割した値に制御できる。このため、一般に、電
動弁はステッピングモータと同等の構造を有しており駆
動方式もほぼ同一である。なお、冷凍機は室内機および
室外機をユーザー先の設置環境に応じて、設置可能な適
切な場所に取り付けて使用される。By the way, the expansion valve 4 for controlling the flow rate of the refrigerant is
Generally, it is an electric type, and its opening / closing degree can be discretely controlled, and by inputting a control pulse, one opening / closing step amount can be changed as a unit operation amount. That is, for example, if the degree of opening / closing in the fully closed state is 0 and the degree of opening / closing in the fully opened state is 500, the degree of opening / closing during that period can be controlled to a value divided into 500 steps. Therefore, generally, the motor-operated valve has a structure similar to that of a stepping motor, and the drive system is almost the same. The refrigerator is used by installing the indoor unit and the outdoor unit in an appropriate place where they can be installed according to the installation environment of the user.
【0007】[0007]
【発明が解決しようとする課題】しかしながら、上記し
た蒸気圧縮式冷凍装置の膨張弁制御方法では、次の問題
がある。However, the above expansion valve control method for a vapor compression refrigeration system has the following problems.
【0008】まず、第1には、室内機6と室外機5とを
接続する配管8の長さは冷凍機の設置場所毎により異な
るからSH制御の安定性に大きな影響を与えるという問
題がある。すなわち、従来の方法では、予め標準の配管
長に応じた制御パラメータが設定され、この状態で納入
されていたからユーザ先での配管長が標準と異なれば、
膨張弁の開閉度の変化量に対する応答特性も異なり、冷
凍機の内部状態を安定に制御できなかった。この場合
に、実際に配管長を計測することも考えられるが、メジ
ャー等で計測することは、現実的な手法と言えず、設置
場所によっては配管長の計測が困難な場合もある。First, since the length of the pipe 8 connecting the indoor unit 6 and the outdoor unit 5 differs depending on the installation location of the refrigerator, there is a problem that the stability of SH control is greatly affected. . That is, in the conventional method, the control parameters according to the standard pipe length are set in advance, and since the control parameters are delivered in this state, if the pipe length at the user's end is different from the standard,
The response characteristics to the amount of change in the opening / closing degree of the expansion valve were also different, and the internal state of the refrigerator could not be controlled stably. In this case, it is possible to actually measure the pipe length, but measuring with a measure or the like cannot be said to be a realistic method, and it may be difficult to measure the pipe length depending on the installation location.
【0009】第2には、従来の膨張弁の開閉度を微妙に
調節するだけの方法では、1ステップ(単位操作量)が
大きいから冷凍機の内部の状態を精度よく安定状態に維
持することは困難であるという問題がある。この問題を
図13を参照して説明すると、時刻t1までSH制御に
よって温度検出信号d1と温度検出信号d2とは安定
し、温度差ecも目標値となっており変動していない。
ところが、時刻t1以降に変化要因、例えば、負荷変動
や外乱が生じ温度検出信号d1が低下して目標温度差よ
り小さくなると、膨張弁の開閉度を1ステップ(単位操
作量)安定方向へ減少させる。これによって、冷凍機の
内部状態も変化して温度検出信号d1と温度検出信号d
2とが変化するが、時刻t3に温度差e’c’の状態で
定常状態となる。この場合に、次の制御タイミングで上
記温度差e’c’を温度差ecに戻すべく膨張弁4の制
御が行われるが、温度差ecの安定状態に戻すまで長時
間を要し、振動的になることがある。Second, in the conventional method of only finely adjusting the opening / closing degree of the expansion valve, one step (unit operation amount) is large, so that the internal state of the refrigerator can be accurately maintained in a stable state. Has the problem of being difficult. This problem will be described with reference to FIG. 13. Until the time t1, the SH control stabilizes the temperature detection signal d1 and the temperature detection signal d2, and the temperature difference ec is a target value and does not change.
However, after the time t1, when a change factor, for example, load fluctuation or disturbance occurs and the temperature detection signal d1 decreases and becomes smaller than the target temperature difference, the opening / closing degree of the expansion valve is decreased by one step (unit operation amount) stable direction. . As a result, the internal state of the refrigerator also changes and the temperature detection signal d1 and the temperature detection signal d
2 changes, but becomes a steady state at the time t3 with the temperature difference e'c '. In this case, the expansion valve 4 is controlled to return the temperature difference e'c 'to the temperature difference ec at the next control timing, but it takes a long time to return the temperature difference ec to a stable state, and vibration May become.
【0010】このような状態となる理由は、冷凍機の内
部状態が安定状態から不安定状態に移行したとき、上記
した変化状態を抑え、あるいは元の状態を復元するため
1ステップ(単位操作量)、つまり、膨張弁4を絞る
が、1ステップの絞りの最小変化量が大きいため冷媒流
量の変化が大きく、復元する方向にオーバーシュートが
生じ、結果的に目的とは逆に不安定の状態へ移行させて
しまうからである。The reason for such a state is that when the internal state of the refrigerator shifts from a stable state to an unstable state, one step (unit operation amount) is used to suppress the above-mentioned changed state or restore the original state. ) That is, the expansion valve 4 is throttled, but since the minimum change amount of the throttle in one step is large, the change in the refrigerant flow rate is large and an overshoot occurs in the restoring direction, resulting in an unstable state contrary to the purpose. Because it will be transferred to.
【0011】従来、上記問題のため、ある範囲で安定が
得られる場合には、できるだけ膨張弁4を開閉度の変化
をさせないようにして安定を保つようにしているが、従
来の方法では、変化を抑えるため膨張弁4を制御しても
応答が遅いため、結果的に精度の良い安定な制御が得ら
れない。この場合、膨張弁4の1ステップ(単位操作
量)を小さくすることも考えられるが、コストが大幅に
増加することになると言う問題がある。Conventionally, due to the above problems, when stability is obtained within a certain range, the expansion valve 4 is kept as stable as possible by keeping the opening / closing degree unchanged. Even if the expansion valve 4 is controlled to suppress the above, the response is slow, and as a result, stable control with high accuracy cannot be obtained. In this case, it is conceivable to reduce one step (unit operation amount) of the expansion valve 4, but there is a problem that the cost will increase significantly.
【0012】そこで、本発明は、冷媒配管の長さに対応
して最適な制御パラメータを設定し、膨張弁の単位操作
量が大きいために起因する問題を解決し、精度の良い安
定な制御が得られる蒸気圧縮式冷凍装置の膨張弁制御方
法を提供することを目的とする。Therefore, the present invention solves the problem caused by the large unit operation amount of the expansion valve by setting the optimum control parameter corresponding to the length of the refrigerant pipe, and provides stable and accurate control. It is an object of the present invention to provide an expansion valve control method for a vapor compression refrigeration system obtained.
【0013】[0013]
【課題を解決するための手段】請求項1の発明は、コン
プレッサと凝縮器と膨張弁と蒸発器とを冷媒配管で循環
接続すると共に、冷凍機内部の冷媒温度の状態に基づき
制御演算して操作量を求め、求めた操作量に応じて前記
膨張弁の開閉度を制御する蒸気圧縮式冷凍装置の膨張弁
制御方法において、冷凍機内部の冷媒温度の状態の変化
から冷媒配管の長さを類推し、類推した冷媒配管の長さ
に対応した最適な制御演算パラメータを設定して膨張弁
を制御するようにしたものである。According to a first aspect of the present invention, a compressor, a condenser, an expansion valve and an evaporator are circulated and connected by a refrigerant pipe, and a control calculation is performed based on a state of a refrigerant temperature inside a refrigerator. In the expansion valve control method of the vapor compression type refrigerating apparatus for controlling the opening / closing degree of the expansion valve according to the operation amount obtained, the operation amount is determined, and the length of the refrigerant pipe is changed from the change in the state of the refrigerant temperature inside the refrigerator. The expansion valve is controlled by analogizing and setting the optimum control calculation parameter corresponding to the analogized length of the refrigerant pipe.
【0014】請求項2の発明は、コンプレッサと凝縮器
と膨張弁と蒸発器とを冷媒配管で循環接続すると共に、
冷凍機内部の冷媒温度の状態に基づき制御演算して操作
量を求め、求めた操作量に応じて前記膨張弁の開閉度を
単位ステップ量ずつ変えることにより制御する蒸気圧縮
式冷凍装置の膨張弁制御方法において、操作量に基づい
て膨張弁の開閉度を単位ステップ量変えると冷媒温度の
安定状態からの変化が大きく、逆に冷媒温度が不安定状
態となる場合に、その不安定状態を抑制するために膨張
弁の開閉度を単位ステップ変えた後、所定時間経過後に
膨張弁の開閉度を変えた方向と逆方向へ膨張弁の開閉度
を単位ステップ変えるようにしたものである。According to a second aspect of the present invention, the compressor, the condenser, the expansion valve and the evaporator are circulated and connected by a refrigerant pipe, and
An expansion valve for a vapor compression refrigeration system that controls the operation amount based on the state of the refrigerant temperature inside the refrigerator to obtain an operation amount and changes the opening / closing degree of the expansion valve by a unit step amount in accordance with the operation amount thus obtained. In the control method, if the opening / closing degree of the expansion valve is changed by a unit step amount based on the operation amount, the change in the refrigerant temperature from the stable state is large, and conversely, if the refrigerant temperature becomes unstable, the unstable state is suppressed. In order to achieve this, after changing the opening / closing degree of the expansion valve by a unit step, the opening / closing degree of the expansion valve is changed by a unit step in a direction opposite to the direction in which the opening / closing degree of the expansion valve is changed after a lapse of a predetermined time.
【0015】[0015]
【作用】請求項1の発明では、類推された冷媒配管の長
さに対応した最適な制御パラメータが設定され、設置場
所の如何にかかわらず蒸気圧縮式冷凍装置の内部状態を
安定して制御ができる。According to the first aspect of the present invention, the optimum control parameter corresponding to the length of the estimated refrigerant pipe is set, and the internal state of the vapor compression refrigeration system can be controlled stably regardless of the installation location. it can.
【0016】請求項2の発明では、操作量が単位2ステ
ップ量を発生させる量に満たないとき、膨張弁を単位ス
テップ量変化させた後に、適当なタイミングで逆方向に
開閉度を単位ステップ量変化させる。これにより、単位
操作量を出力すると逆に内部の温度状態が不安定となる
わずかな変化のときにも、対応して安定した制御ができ
る。According to the second aspect of the present invention, when the manipulated variable is less than the amount for generating the unit 2 step amount, the expansion valve is changed by the unit step amount, and then the opening / closing degree is changed in the reverse direction at an appropriate timing. Change. As a result, when the unit operation amount is output, conversely, stable control can be performed even when there is a slight change in which the internal temperature state becomes unstable.
【0017】[0017]
【実施例】以下、本発明の実施例を図面を参照して説明
する。Embodiments of the present invention will be described below with reference to the drawings.
【0018】図1は、本発明の第1実施例を示す構成図
である。図中、4は図12で説明した膨張弁、9は図1
2に示す蒸発器1の内部のa点の温度を検出し、温度検
出信号d1を出力する温度検出器、10は図12に示す
蒸発器1の内部のb点の温度を検出し、温度検出信号d
2を出力する温度検出器、11は温度検出信号d1と温
度検出信号d2の差が予め設定された値になるように制
御パラメータで操作量を求めその量を出力する制御部、
13は後に詳述する配管長を推論する推論部である。な
お、制御部11はファジィ推論で操作量を求めてもよ
く、推論部13はファジィ推論でなく類推する手法とし
てニューラルネットワークでもよい。FIG. 1 is a block diagram showing a first embodiment of the present invention. In the figure, 4 is the expansion valve explained in FIG. 12, and 9 is FIG.
2 detects the temperature at point a inside the evaporator 1 and outputs a temperature detection signal d1, and the temperature detector 10 detects the temperature at point b inside the evaporator 1 shown in FIG. Signal d
A temperature detector that outputs 2; 11 is a control unit that calculates a manipulated variable with a control parameter so that the difference between the temperature detection signal d1 and the temperature detection signal d2 is a preset value, and outputs the amount.
Reference numeral 13 is an inference unit for inferring the pipe length, which will be described in detail later. The control unit 11 may obtain the operation amount by fuzzy inference, and the inference unit 13 may be a neural network as a method of analogy rather than fuzzy inference.
【0019】本実施例は、冷媒の配管長と冷凍機の内部
状態の推移、つまり、冷凍機の内部の温度変化とが一定
の因果関係にあることに着目し、配管長を推論部13で
推論し、これによって、制御パラメータとして、例え
ば、PIDパラメータを設定するようにしている。In this embodiment, paying attention to the fact that there is a constant causal relationship between the refrigerant pipe length and the internal state of the refrigerator, that is, the internal temperature change of the refrigerator, and the inference unit 13 determines the pipe length. It is inferred that the PID parameter, for example, is set as the control parameter.
【0020】具体的に、蒸発器1の内部の温度の時間応
答を示す図2を参照して説明すると、時刻t1になるま
では温度検出信号d1と温度検出信号d2とが検出さ
れ、両者が制御部11で制御されており温度差も安定し
ている。この状態で時刻t1に何らかの原因で温度検出
信号d1が低下を開始すると、その状態が検出されて時
刻t2に制御部11により膨張弁4を操作して元の安定
を得る方向に制御がされる。この操作による時刻t2以
降での温度検出信号d1と温度検出信号d2と傾きは、
冷媒配管長による時間応答特性により異なる。すなわ
ち、冷媒配管長が大きければ、膨張弁4の開閉度を変化
した場合の応答が遅くなるから時刻t2で膨張弁4を操
作した後の温度検出信号d1と温度検出信号d2の変化
の立ち上がりが遅くなり、その傾きも小さく、逆に冷媒
配管が小さければ立ち上がりが早く、その傾きも大きく
なる。Specifically, referring to FIG. 2 showing the time response of the temperature inside the evaporator 1, the temperature detection signal d1 and the temperature detection signal d2 are detected until the time t1 and both of them are detected. The temperature difference is stable because it is controlled by the control unit 11. In this state, if the temperature detection signal d1 starts to decrease at time t1 for some reason, that state is detected, and the control unit 11 operates the expansion valve 4 at time t2 to perform control so as to obtain the original stability. . With this operation, the temperature detection signal d1 and the temperature detection signal d2 after time t2 and the slope are
Depends on the time response characteristics depending on the refrigerant pipe length. That is, if the length of the refrigerant pipe is large, the response when the opening / closing degree of the expansion valve 4 is changed is delayed. Therefore, the rise of the change of the temperature detection signal d1 and the temperature detection signal d2 after operating the expansion valve 4 at time t2. If the refrigerant pipe is small, the rise is quick and the inclination becomes large.
【0021】なお、実際には上記した蒸発器1の内部状
態以外のパラメータ、例えば、電源周波数、室内外の環
境温度、つまり、負荷等も前記した両者の因果関係に影
響を与えるから本実施例では、これらも考慮して配管長
の類推を実施している。In practice, parameters other than the internal state of the evaporator 1 described above, such as power supply frequency, indoor and outdoor environmental temperature, that is, load, etc., also affect the above-mentioned causal relationship between the two. Now, the analogy of the pipe length is carried out in consideration of these factors.
【0022】次に、本発明の配管長の類推方法としてフ
ァジィ推論を使用した場合について説明する。Next, a case where fuzzy inference is used as a pipe length analogy method of the present invention will be described.
【0023】まず、ファジィ推論の前件部メンバシップ
関数として膨張弁の開閉度、開閉度変化量、温度検出信
号d1の変化量、温度検出信号d2の変化量を定義し、
さらに、後件部メンバシップ関数として配管長を定義す
る。First, the opening / closing degree of the expansion valve, the opening / closing degree change amount, the change amount of the temperature detection signal d1 and the change amount of the temperature detection signal d2 are defined as the antecedent part membership function of the fuzzy inference.
Furthermore, the pipe length is defined as a consequent part membership function.
【0024】例えば、前件部メンバシップ関数としての
開閉度変化量は、図3に示す如く、ステップ2のとき正
しく中ぐらい、ステップ3以上のとき正しく大きいと定
義し、前件部メンバシップ関数としての温度検出信号d
1の変化量は図4に示す如く5℃のとき正しく中ぐら
い、7.5℃以上を正しく大きいと定義する。また、後
件部メンバシップ関数としての配管長は、図5に示す如
く12.5m以下は正しく短く、25mは正しく中ぐら
い、37.5m以上は正しく長いと定義する。For example, as shown in FIG. 3, the opening / closing degree change amount as the antecedent part membership function is defined to be correct and moderate in step 2, and large in steps 3 and above. Detection signal d as
As shown in FIG. 4, the change amount of 1 is defined as correct and medium when the temperature is 5 ° C. and correct and large when the temperature is 7.5 ° C. or higher. Further, as shown in FIG. 5, the pipe length as a consequent part membership function is defined as 12.5 m or less being correctly short, 25 m being properly medium, and 37.5 m or more being correctly long.
【0025】次に、実際には多くの場合のルールを記述
する必要があるが、ここでは簡単に説明するため、例え
ば、次の3ルールを考える。Next, in practice, it is necessary to describe rules in many cases, but here, for the sake of simplicity, consider the following three rules, for example.
【0026】まず、ルール(1)は「開閉度変化量が大
きくて、温度検出信号d1の変化量が中ぐらいならば、
配管長は長い」、ルール(2)は「開閉度変化量が大き
くて、温度検出信号d1の変化量が大きければ、配管長
は中ぐらい」、ルール(3)は「開閉度変化量が中ぐら
いで、温度検出信号d1の変化量が大きければ、配管長
は短い」とする。First, the rule (1) is that "if the opening / closing degree change amount is large and the change amount of the temperature detection signal d1 is medium,
The pipe length is long ", the rule (2) is" if the opening / closing degree change amount is large and the change amount of the temperature detection signal d1 is large, the pipe length is medium ", and the rule (3) is" openness degree change amount is medium ". If the amount of change in the temperature detection signal d1 is large, the pipe length is short. "
【0027】上記した定義により、例えば、ファジィ推
論への入力項として開閉度変化量はI1(3STE
P)、温度検出信号d1の変化量はJ1(6.25℃)
であった場合について、図6を参照して推論を説明す
る。According to the above definition, for example, the opening / closing degree change amount is I1 (3STE) as an input term to the fuzzy inference.
P), the change amount of the temperature detection signal d1 is J1 (6.25 ° C.)
The reasoning will be described with reference to FIG.
【0028】まず、ルール1では開閉度変化量I1の前
件部適合度は1、温度検出信号d1の変化量J1の前件
部適合度は0.5となる。そして、この2つの前件部
で、小さい方の適合度を前件部全体の適合度とすれば、
後件部適合度は0.5となる。次に、ルール2では開閉
度変化量I1の前件部は適合度は1、温度検出信号d1
の変化量J1の前件部適合度0.5となり、この2つの
前件部で小さい方をとると後件部適合度は0.5とな
る。最後にルール3では、開閉度変化量I1の前件部適
合度は0、温度検出信号d1の変化量J1の前件部適合
度は0.5となり、この場合に2つの前件部で小さい方
をとると後件部適合度は0となる。First, in rule 1, the antecedent conformity of the opening / closing degree change amount I1 is 1, and the antecedent conformance of the change amount J1 of the temperature detection signal d1 is 0.5. Then, in these two antecedents, if the smaller one is the fitness of the entire antecedent,
The consequent part conformance is 0.5. Next, in Rule 2, the antecedent part of the opening / closing degree change amount I1 has a compatibility of 1 and a temperature detection signal d1.
Of the change amount J1 is 0.5, and if the smaller of these two antecedents is taken, the congruence of the consequent is 0.5. Finally, in rule 3, the antecedent part conformity of the opening / closing degree change amount I1 is 0, and the antecedent part conformity of the change amount J1 of the temperature detection signal d1 is 0.5. In this case, the two antecedent parts are small. If the one is taken, the consequent part conformance becomes 0.
【0029】この結果、ルール1の後件部適合度は、
0.5で図示太線以下の台形の部分、ルール2の後件部
適合度は、0.5で図示太線以下の台形の部分、ルール
3の後件部適合度は、0で図示太線になる。これによっ
て、ルール1〜ルール3についてMINーMAX法を適
用すると、図6の右端に示す配管長の合成図形が得ら
れ、この合成図形から重心を求めると、重心H1が得ら
れる。この重心H1を配管長と推定する。As a result, the suitability of the consequent part of rule 1 is
A trapezoidal part below 0.5 in the drawing, the consequent part of rule 2 of the rule 2 is a trapezoidal part below 0.5 in the thick line, and a consequent part of rule 3 is 0 in the illustrated thick line. . As a result, when the MIN-MAX method is applied to the rules 1 to 3, a composite figure of the pipe length shown at the right end of FIG. 6 is obtained, and the center of gravity H1 is obtained by obtaining the center of gravity from this composite figure. This center of gravity H1 is estimated to be the pipe length.
【0030】同様にして入力として開閉度変化量がI
2、温度検出信号d1の変化量J1のとき図7に示すよ
うに後件部適合度は、ルール1で0、ルール2で0、ル
ール3で0.5となり、合成図形から重心を求めると、
配管長H2が得られる。Similarly, the opening / closing degree change amount is I as an input.
2. When the change amount J1 of the temperature detection signal d1 is shown in FIG. 7, the consequent part conformance is 0 in rule 1, 0 in rule 2, and 0.5 in rule 3, and when the center of gravity is obtained from the composite figure, ,
A pipe length H2 is obtained.
【0031】なお、メンバシップ関数と推論ルールは予
め実験的に求め、各変数の対応関係から定義する。ま
た、推定する配管長とそれに応じた適切な制御パラメー
タとは一対一に対応するから、後件部として配管長のか
わりに制御パラメータを定義することもできる。例え
ば、制御部11がPID制御の場合は比例項、積分項の
パラメータを推論部13で推論し変更し、制御部11が
ファジィ制御の場合には、メンバシップ関数の形状を変
えたり、ファジィ推論による開閉度操作量の出力結果に
直接重みを付ける。The membership function and the inference rule are experimentally obtained in advance, and are defined from the correspondence relation of each variable. Further, since the estimated pipe length and the appropriate control parameter corresponding thereto have a one-to-one correspondence, it is possible to define the control parameter instead of the pipe length as a consequent part. For example, when the control unit 11 is PID control, the parameters of the proportional term and the integral term are inferred and changed by the inference unit 13, and when the control unit 11 is fuzzy control, the shape of the membership function is changed or fuzzy inference is performed. The output result of the opening / closing degree manipulated variable by is directly weighted.
【0032】次に、本発明の配管長の類推手法としてニ
ューラルネットワークを使用した場合について図8のモ
デルを参照して説明する。Next, a case where a neural network is used as a pipe length analogy method of the present invention will be described with reference to the model of FIG.
【0033】ニューラルネットワーク(以下「NN」と
いう)の入力層は、図示するように膨張弁開閉度、室内
温度、温度検出信号d1の変化量、温度検出信号d2の
5変数の組合せとし、出力層は、配管長または複数の制
御パラメータa,b,cとする。The input layer of the neural network (hereinafter referred to as "NN") is a combination of five variables of the expansion valve opening / closing degree, the room temperature, the change amount of the temperature detection signal d1 and the temperature detection signal d2 as shown in the figure, and the output layer. Is the pipe length or a plurality of control parameters a, b, c.
【0034】まず、実験により求めた代表的ないくつか
の入力層の入力変数と出力層の出力値の因果関係のデー
タをNNに入力して、これを教師として繰り返しNNに
計算を行わせ内部での計算のための計算パラメータを変
更する学習をさせる。学習後は、NNは学習の際に教え
てない個々の入力の組合せにも対応して適切な配管長ま
たは制御パラメータが出力されて制御部11の制御パラ
メータが変更される。First, data of causal relationships between some input variables in the input layer and output values in the output layer obtained by experiments are input to the NN, and this is used as a teacher to repeatedly calculate the NN. Train students to change calculation parameters for calculations in. After learning, the NN outputs appropriate pipe lengths or control parameters corresponding to combinations of individual inputs that are not taught during learning, and the control parameters of the control unit 11 are changed.
【0035】具体的に図8の場合について説明すると、
最初に冷凍機での運転実験より、ある配管長、ある室内
温度、ある膨張弁開閉度、ある膨張弁開閉変化量の際の
温度検出信号d1と温度検出信号d2の変化量(つまり
傾き)を測定する。そして、この各々のパラメータをい
くつか変えて、また、測定する。この測定を各パラメー
タの代表的な値について行う。例えば、配管長について
は、5m,10m,15mなど、室内温度については2
0℃,25℃,30℃などについて、温度検出信号d1
と温度検出信号d2の変化量を測定する。こうして得ら
れた入出力のデータを教師としてNNに学習を行わせ
る。ただし、学習後のNNでは配管長などから温度検出
信号d1と温度検出信号d2の変化量を求めるのではな
く、温度検出信号d1と温度検出信号d2の変化量など
から配管長を求める。この場合、NNは、単に入出力変
数の組合せがどのようになっているかを学習するだけで
あるから、このようなことが可能となる。次に、学習後
はNNに学習させない場合の値、例えば、室内温度が2
2℃等を入力しても、その場合の全ての入力の組合せか
ら適切な配管長を推定出力する。このようにNNに学習
させることにより、入出力のすべての組合せを実験しな
くても、いくつかの代表的な実験を行えば、必要な配管
長の推定がされる。なお、図8では冷房の場合を述べて
いるからで室内温度となっているが、暖房の場合には、
室外温度となる。The case of FIG. 8 will be specifically described.
First, from an operation experiment in a refrigerator, a change amount (that is, a slope) of the temperature detection signal d1 and the temperature detection signal d2 at a certain pipe length, a certain room temperature, a certain expansion valve opening / closing degree, and a certain expansion valve opening / closing change amount is determined. taking measurement. Then, some of these parameters are changed and measured again. This measurement is performed for typical values of each parameter. For example, the pipe length is 5 m, 10 m, 15 m, etc., and the room temperature is 2
Temperature detection signal d1 for 0 ° C, 25 ° C, 30 ° C, etc.
And the amount of change in the temperature detection signal d2 is measured. The NN is made to learn by using the input / output data thus obtained as a teacher. However, in the NN after learning, the amount of change in the temperature detection signal d1 and the temperature detection signal d2 is not obtained from the pipe length, but the pipe length is obtained from the amount of change in the temperature detection signal d1 and the temperature detection signal d2. In this case, the NN simply learns what the combination of the input / output variables is, so that such a thing is possible. Next, after learning, the value when the NN is not allowed to learn, for example, the room temperature is 2
Even if 2 ° C or the like is input, an appropriate pipe length is estimated and output from all combinations of inputs in that case. By making the NN learn in this way, the required pipe length can be estimated by conducting some representative experiments without experimenting with all combinations of input and output. In addition, in FIG. 8, since the case of cooling is described, the room temperature is set, but in the case of heating,
It becomes the outdoor temperature.
【0036】ところで、電源周波数についてはNNの入
力変数としてもよいが60Hzの場合はそのまま、50
Hzの場合は予め実験により求められた係数を出力値に
掛けることで対応する。The power supply frequency may be an input variable of NN, but in the case of 60 Hz, it is 50
In the case of Hz, it is handled by multiplying the output value by a coefficient obtained in advance by an experiment.
【0037】なお、NNの学習では配管長について説明
したが、本発明の目的は、配管長の推定に応じて制御パ
ラメータを変えて、配管長に依存しない制御効果を得る
ことにある。配管長が判明すれば、そのときの制御パラ
メータは一意に決まるから、ファジィ推論を使用した場
合と同様にNNの学習を配管長を用いる代わりに制御パ
ラメータを用いても同様の結果が得られ、この場合、配
管長から制御パラメータへの変換の必要がないことにな
る。制御パラメータにはファジィ制御の場合ファジィ推
論の結果の膨張弁操作量に重み付けを行う係数などが、
PIDの制御の場合P、I、Dの各項が該当する。Although the pipe length has been described in the learning of the NN, the object of the present invention is to obtain a control effect that does not depend on the pipe length by changing the control parameter according to the estimation of the pipe length. If the pipe length is known, the control parameter at that time is uniquely determined. Therefore, similar to the case of using fuzzy inference, the same result can be obtained by using the control parameter instead of using the pipe length for learning NN. In this case, there is no need to convert the pipe length into control parameters. In the case of fuzzy control, the control parameters include a coefficient for weighting the expansion valve operation amount as a result of fuzzy inference.
In the case of PID control, the terms P, I, and D correspond.
【0038】上記した配管長の類推は、設置の際の試運
転時にのみ類推する手段を設けて類推結果を入力させ保
存させればよく、運転時に必ずしも必要はない。このよ
うに、冷凍機の設置時の配管長に応じて制御部11の制
御パラメータを変更するから蒸発器1の内部状態が安定
し、制御状態を安定にすることができる。The above-mentioned analogy of the pipe length may be established by providing means for analogy only during a trial run at the time of installation and inputting and saving the analogy result, which is not always necessary during operation. In this way, since the control parameter of the control unit 11 is changed according to the pipe length at the time of installing the refrigerator, the internal state of the evaporator 1 is stabilized and the control state can be stabilized.
【0039】本実施例では、SH制御の場合について説
明したが、他の制御手段にも配管長の類推の手法は応用
でき、また、ニューラルネットワークまたはファジィ推
論以外の類推手法でもよい。In this embodiment, the case of SH control has been described, but the pipe length analogy method can be applied to other control means, and analogy methods other than neural networks or fuzzy inference methods may be used.
【0040】次に、本発明の第2実施例について図面を
参照して説明する。Next, a second embodiment of the present invention will be described with reference to the drawings.
【0041】図9は本発明の第2実施例を示す構成図で
ある。図において、制御部14は、制御タイミング発生
部15と制御指令部16と駆動パルス発生部17と逆転
タイミング発生部18とから構成され、制御指令部16
には温度検出器9と温度検出器10が接続され、駆動パ
ルス発生部17には膨張弁4が接続されている。FIG. 9 is a block diagram showing the second embodiment of the present invention. In the figure, the control unit 14 includes a control timing generation unit 15, a control command unit 16, a drive pulse generation unit 17, and a reverse rotation timing generation unit 18.
Is connected to a temperature detector 9 and a temperature detector 10, and the drive pulse generator 17 is connected to the expansion valve 4.
【0042】本実施例は、冷凍機内部の冷媒温度安定状
態からの変化要因が、わずかの負荷変動や外乱の場合に
操作量に応じて膨張弁4を本来の安定する方向へ1ステ
ップ駆動させ、制御周期内の所定時間後に前記安定方向
と逆方向に1ステップ戻して内部状態変化による温度の
オーバーシュートを抑え、迅速に内部状態を安定に保つ
ようにしている。In the present embodiment, when the factor of change from the stable state of the refrigerant temperature inside the refrigerator is a slight load change or disturbance, the expansion valve 4 is driven one step in the original stable direction according to the manipulated variable. After a predetermined time within the control cycle, the temperature is overturned by one step in the opposite direction to the stable direction to suppress temperature overshoot due to a change in the internal state, and the internal state is quickly kept stable.
【0043】ここで、制御タイミング発生部15は一定
周期の制御タイミング信号を制御指令部16へ出力す
る。制御指令部16は制御タイミング信号を入力する
と、温度検出器9と温度検出器10とから温度検出信号
d1と温度検出信号d2とを取り込み、操作量をPID
等の制御パラメータにより演算する。Here, the control timing generation section 15 outputs a control timing signal of a constant cycle to the control command section 16. When the control command unit 16 receives the control timing signal, it takes in the temperature detection signal d1 and the temperature detection signal d2 from the temperature detector 9 and the temperature detector 10, and determines the manipulated variable as PID.
Calculate with control parameters such as.
【0044】駆動パルス発生部17は制御指令部16か
らの操作量に応じて膨張弁4へパルス信号を出力する。
逆転タイミング発生部18は、制御指令部16からの逆
転駆動の指令のときに安定方向へ1ステップ(単位操作
量)出力し、S1時間の計測の指令を入力し、S1時間
経過後に駆動パルス発生部17に対して安定方向と逆方
向へ1ステップ(単位操作量)逆転駆動の指令を出力す
る。The drive pulse generator 17 outputs a pulse signal to the expansion valve 4 according to the operation amount from the control commander 16.
The reverse rotation timing generation unit 18 outputs one step (unit operation amount) in the stable direction when the reverse rotation drive command is issued from the control command unit 16, inputs a measurement command for S1 time, and generates a drive pulse after S1 time has elapsed. A command for one-step (unit operation amount) reverse rotation drive is output to the unit 17 in the direction opposite to the stable direction.
【0045】次に、本実施例の制御部14の作用を図1
0を参照して説明する。Next, the operation of the control unit 14 of this embodiment will be described with reference to FIG.
This will be described with reference to 0.
【0046】まず、制御指令部16は制御タイミング発
生部15から制御タイミング信号を入力すると(10
1)、温度検出器9と温度検出器10とから温度検出信
号d1と温度検出信号d2とを読み込む(102)。制
御指令部16では、予め定められた目標値に対する温度
検出信号d1と温度検出信号d2との温度差に基づいて
制御パラメータにより操作量を演算する(103)。First, the control command section 16 receives a control timing signal from the control timing generation section 15 (10
1), the temperature detection signal d1 and the temperature detection signal d2 are read from the temperature detector 9 and the temperature detector 10 (102). The control command unit 16 calculates the manipulated variable by the control parameter based on the temperature difference between the temperature detection signal d1 and the temperature detection signal d2 with respect to a predetermined target value (103).
【0047】続いて、制御指令部16では、上記で演算
された操作量が、例えば、0.5ステップ未満のときは
実際のステップを0として駆動パルス発生部17へ駆動
パルスを出力せず(104)、0.5ステップ以上のと
きは逆転駆動か否かの判定をする(105)。この判定
で、逆転駆動でないとき、例えば、演算された操作量が
1.5ステップ以上のとき、1ステップ以上が駆動パル
ス発生部17へ出力される(106)。Subsequently, the control command section 16 does not output the drive pulse to the drive pulse generation section 17 by setting the actual step to 0 when the operation amount calculated above is, for example, less than 0.5 step ( 104) If the number of steps is 0.5 or more, it is determined whether or not reverse drive is performed (105). In this determination, when it is not the reverse drive, for example, when the calculated operation amount is 1.5 steps or more, one step or more is output to the drive pulse generation unit 17 (106).
【0048】上記判定で逆転駆動のとき、例えば、演算
された操作量が0.5ステップ以上で、かつ、1.5ス
テップ未満のとき制御指令部16は、ステップ1を安定
する方向へ駆動パルス発生部17へ出力するように指令
する一方、逆転タイミング発生部18へ一定時間S1の
計測の指令を出力する(107)。逆転タイミング発生
部18は、S1時間経過後に駆動パルス発生部17へ膨
張弁4の逆転駆動の指令を出力する(109)。続い
て、制御指令部16では、再び温度検出器9と温度検出
器10とから温度検出信号d1と温度検出信号d2とが
読み込まれ、操作量の演算が行われる(111)。この
結果、操作量を変化させる場合には、1ステップの駆動
指令を駆動パルス発生部17へ出力する(112)(1
13)。In the case of reverse rotation drive in the above determination, for example, when the calculated operation amount is 0.5 step or more and less than 1.5 step, the control command section 16 causes the drive pulse to stabilize Step 1. The generation unit 17 is instructed to output, while the reverse rotation timing generation unit 18 is output a measurement command for a fixed time S1 (107). The reverse rotation timing generation unit 18 outputs a command for reverse rotation drive of the expansion valve 4 to the drive pulse generation unit 17 after the lapse of S1 time (109). Subsequently, the control command unit 16 again reads the temperature detection signal d1 and the temperature detection signal d2 from the temperature detector 9 and the temperature detector 10, and calculates the manipulated variable (111). As a result, when the manipulated variable is changed, a drive command for one step is output to the drive pulse generator 17 (112) (1
13).
【0049】上記した逆転駆動の作用について図11を
参照して説明すると、時刻t1まで温度検出信号d1と
温度検出信号d2の温度差ecが目標値にほぼ一致し安
定している。この状態で時刻t1以降に外乱等で温度検
出信号d1がわずかに低下したとき、時刻t2に膨張弁
4を1ステップ閉方向、復元方向に操作する。次に、S
1時間後の時刻t3に膨張弁4を1ステップ開方向、つ
まり先ほどとは逆方向に操作する。これによって、図1
3と比較して判るように内部の状態が逆に不安定方向に
移行することなく、時刻t4に温度差ecを保ってわず
か上昇した状態で安定する。なお、逆転タイミング発生
部18が計測する一定時間S1は、予め実験によって最
適な時間を求め、設定しておく。また、逆転方向に膨張
弁を操作するので時刻t1とt4では開閉度が変化しな
いことになる。しかし、時刻t1以降での状態変化が大
きい場合には、やはり開閉度を1ステップ変化させなけ
ればならない場合があるから逆転パルス出力後にもう一
度温度検出信号d1と温度検出信号d2を読み込み、操
作量の演算を行い、1ステップ出力するかどうかを判定
する。このように、逆転パルスの出力は時刻t1での変
化が小さいときには安定な制御を得られるが、大きな変
化の場合には膨張弁操作による対応が遅れることにな
る。そこで、時刻t1での操作量演算結果が例えば1.
5ステップ以上のときには逆転駆動なしとすることで大
きな変化に対しても迅速な対応が可能となる。The operation of the above-described reverse drive will be described with reference to FIG. 11. Until the time t1, the temperature difference ec between the temperature detection signal d1 and the temperature detection signal d2 is substantially equal to the target value and stable. In this state, when the temperature detection signal d1 slightly decreases after time t1 due to disturbance or the like, the expansion valve 4 is operated in the one-step closing direction and the restoring direction at time t2. Then S
At time t3 one hour later, the expansion valve 4 is operated by one step in the opening direction, that is, in the direction opposite to the one before. As a result, FIG.
As can be seen from comparison with No. 3, the internal state does not shift to the unstable direction, but the temperature difference ec is maintained at time t4, and the internal state stabilizes in a slightly increased state. The fixed time S1 measured by the reverse rotation timing generator 18 is set by previously determining an optimum time by an experiment. Further, since the expansion valve is operated in the reverse direction, the opening / closing degree does not change at times t1 and t4. However, if the change in state after time t1 is large, the opening / closing degree may have to be changed by one step, so that the temperature detection signal d1 and the temperature detection signal d2 are read again after the reverse rotation pulse is output, and the operation amount A calculation is performed to determine whether to output one step. Thus, stable control of the output of the reverse rotation pulse can be obtained when the change at time t1 is small, but in the case of a large change, the response by the expansion valve operation is delayed. Therefore, the operation amount calculation result at time t1 is, for example, 1.
When the number of steps is 5 or more, no reverse rotation drive can be performed, which enables swift response to a large change.
【0050】このように本実施例では、安定状態からの
変化要因がわずかな外乱の場合に安定方向に1ステップ
操作量を変化させ所定時間後に逆方向に1ステップ操作
量を変化させるから1ステップ量が大きいことおよび操
作量の変化に対して応答が遅いことに起因するオーバー
シュートを防止し、精度のよい安定した制御ができる。As described above, in the present embodiment, when the change factor from the stable state is a slight disturbance, the one-step operation amount is changed in the stable direction, and the one-step operation amount is changed in the opposite direction after a predetermined time. It is possible to prevent overshoot due to a large amount and a slow response to a change in the operation amount, and to perform accurate and stable control.
【0051】なお、本実施例では、PID制御パラメー
タにより操作量を演算した例を説明したが、これに限ら
ず操作量をファジィ推論で推論する手法を用いてもよ
い。このファジィ推論にあたっては、温度検出信号d1
と温度検出信号d2の温度差と目標値ecとの偏差およ
び偏差の変化量をファジィ推論の入力とし膨張弁4の操
作量を推論する。例えば、目標値と温度検出信号d1と
温度検出信号d2との温度差が殆どないとき操作量は0
ステップ、上記目標値と上記温度差ecとの違いが少し
のとき逆転駆動、上記目標値と上記温度差ecが大きけ
れば、その大きさに応じて1ステップ以上の操作量とす
る。In this embodiment, the example in which the operation amount is calculated by the PID control parameter has been described, but the present invention is not limited to this, and a method of inferring the operation amount by fuzzy inference may be used. In this fuzzy inference, the temperature detection signal d1
And the difference between the temperature difference of the temperature detection signal d2 and the target value ec and the amount of change in the difference are input to the fuzzy inference to deduce the operation amount of the expansion valve 4. For example, when there is almost no temperature difference between the target value and the temperature detection signal d1 and the temperature detection signal d2, the manipulated variable is 0.
When the difference between the target value and the temperature difference ec is small, reverse driving is performed. If the target value and the temperature difference ec are large, the operation amount is one step or more depending on the size.
【0052】[0052]
【発明の効果】以上説明したように請求項1の発明によ
れば、類推された冷媒配管の長さに対応した最適な制御
パラメータが設定されるから、設置場所の如何にかかわ
らず蒸気圧縮式冷凍装置の内部状態を安定して制御がで
きる。As described above, according to the invention of claim 1, the optimum control parameter corresponding to the estimated length of the refrigerant pipe is set. Therefore, the vapor compression type is set regardless of the installation place. The internal state of the refrigeration system can be controlled stably.
【0053】請求項2の発明では、単位操作量を出力す
ると逆に不安定となるようなわずかな内部状態の変化の
ときに対応した制御がされ、安定した内部状態が得られ
る。According to the second aspect of the present invention, when the unit operation amount is output, conversely, control is performed corresponding to a slight change in the internal state that is unstable, and a stable internal state is obtained.
【図1】本発明の第1実施例を示す蒸気圧縮式冷凍装置
の膨張弁制御方法の説明図。FIG. 1 is an explanatory diagram of an expansion valve control method for a vapor compression refrigeration system showing a first embodiment of the present invention.
【図2】蒸気圧縮式冷凍装置の蒸発器内部温度の応答
図。FIG. 2 is a response diagram of an evaporator internal temperature of a vapor compression refrigeration system.
【図3】配管長をファジィ推論により類推する手法の開
閉度変化量の前件部メンバシップ関数の一例を示す図。FIG. 3 is a diagram showing an example of a membership function of an antecedent part of an opening / closing degree change amount in a method of analogizing a pipe length by fuzzy inference.
【図4】配管長をファジィ推論により類推する手法の温
度検出信号d1の変化量の前件部メンバシップ関数の一
例を示す図。FIG. 4 is a diagram showing an example of an antecedent part membership function of a variation amount of a temperature detection signal d1 in a method of analogizing a pipe length by fuzzy inference.
【図5】配管長をファジィ推論により推論する手法の配
管長の後件部メンバシップ関数の一例を示す図。FIG. 5 is a diagram showing an example of a consequent part membership function of a pipe length in a method of inferring the pipe length by fuzzy inference.
【図6】ファジィ推論の手法により配管長を類推する第
1の例を示す説明図。FIG. 6 is an explanatory diagram showing a first example of inferring a pipe length by a fuzzy inference method.
【図7】ファジィ推論の手法により配管長を類推する第
2の例を示す説明図。FIG. 7 is an explanatory diagram showing a second example of inferring a pipe length by a fuzzy inference method.
【図8】配管長をニューラルネットワークの手法により
類推する一例を示す説明図。FIG. 8 is an explanatory diagram showing an example of analogizing a pipe length by a neural network method.
【図9】本発明の第2実施例を示す蒸気圧縮式冷凍装置
の膨張弁制御方法の説明図。FIG. 9 is an explanatory diagram of an expansion valve control method for a vapor compression refrigeration system showing a second embodiment of the present invention.
【図10】図9の制御方法の手順を示すフローチャー
ト。10 is a flowchart showing the procedure of the control method of FIG.
【図11】図9の作用を示す説明図。FIG. 11 is an explanatory view showing the operation of FIG.
【図12】蒸気圧縮式冷凍装置の冷媒回路の概念図。FIG. 12 is a conceptual diagram of a refrigerant circuit of a vapor compression refrigeration system.
【図13】従来の蒸気圧縮式冷凍機の内部冷媒温度の応
答図。FIG. 13 is a response diagram of the internal refrigerant temperature of the conventional vapor compression refrigerator.
1 蒸発器 2 凝縮器 3 コンプレッサ 4 膨張弁 7 冷媒配管 8 配管 9 温度検出器 10 温度検出器 11 制御部 12 駆動パルス発生部 13 推論部 14 制御部 15 制御タイミング発生部 16 制御指令部 17 駆動パルス発生部 18 逆転タイミング発生部 1 Evaporator 2 Condenser 3 Compressor 4 Expansion valve 7 Refrigerant piping 8 Piping 9 Temperature detector 10 Temperature detector 11 Control part 12 Drive pulse generation part 13 Inference part 14 Control part 15 Control timing generation part 16 Control command part 17 Drive pulse Generator 18 Reverse rotation timing generator
─────────────────────────────────────────────────────
─────────────────────────────────────────────────── ───
【手続補正書】[Procedure amendment]
【提出日】平成4年11月30日[Submission date] November 30, 1992
【手続補正1】[Procedure Amendment 1]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】請求項2[Name of item to be corrected] Claim 2
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【手続補正2】[Procedure Amendment 2]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0002[Name of item to be corrected] 0002
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0002】[0002]
【従来の技術】一般に、室内空調に利用する蒸気圧縮式
冷凍機では、室内温度が設定温度となるように一定に制
御され、その際、冷凍機自身が所有する冷房能力を最大
限に活用し、かつ、冷凍機内部の冷媒状態を安定に保つ
ために、冷媒流量の制御を行う。例えば、冷房の場合で
は冷凍機が室内から熱を蒸発器の内部の冷媒に吸収し、
凝縮器から室外に放出されており、室内温度が設定温度
より高いとき冷凍機を最大限に運転し、室内温度が設定
温度より低くなったときコンプレッサの運転を停止して
室内外の熱交換を停止している。この場合、冷凍機の内
部冷媒状態を安定に保たなければ室内外の熱交換が安定
に行われず、冷凍機の内部状態を安定に保つことで、結
果として室内温度が安定に保たれる。2. Description of the Related Art Generally, in a vapor compression refrigerator used for indoor air conditioning, the indoor temperature is constantly controlled so as to reach a set temperature, and at that time, the cooling capacity of the refrigerator itself is utilized to the maximum extent. In addition, in order to keep the refrigerant state inside the refrigerator stable, the refrigerant flow rate is controlled. For example, in the case of cooling, the refrigerator absorbs heat from the room into the refrigerant inside the evaporator,
Condenser being discharged to the outdoor from drive to maximize the refrigerator when the room temperature is higher than the set temperature, the heat exchange chamber out to stop the operation of the compressor when the indoor temperature is lower than the set temperature It has stopped. In this case, unless the internal refrigerant state of the refrigerator is kept stable, indoor and outdoor heat exchange is not performed stably, and by keeping the internal state of the refrigerator stable, the indoor temperature is consequently kept stable.
【手続補正3】[Procedure 3]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0004[Correction target item name] 0004
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0004】図12に、蒸気圧縮式冷凍機の冷媒回路の
概念図を示す。図において、1は蒸発器、2は凝縮器、
3はコンプレッサ、4は膨張弁で、この図は室内冷房機
の場合に適合しており、5は室外機、6は室内機を示し
ている。室外機5と室内機6の内部の実線7は、冷媒が
内部を移動する冷媒配管を示しており、点線8は、その
冷媒配管7の内で特に室外機5と室内機6とを接続する
ための配管を示している。ここで、冷媒は配管の中を図
示矢印の方向に流れる。図12では、コンプレッサ3は
室外機側にあるが、室内機側にあってもよい。FIG. 12 shows a conceptual diagram of a refrigerant circuit of a vapor compression refrigerator. In the figure, 1 is an evaporator, 2 is a condenser,
3 is a compressor, 4 is an expansion valve, and this figure is suitable for an indoor air conditioner, 5 is an outdoor unit, and 6 is an indoor unit. A solid line 7 inside the outdoor unit 5 and the indoor unit 6 indicates a refrigerant pipe through which the refrigerant moves, and a dotted line 8 connects the outdoor unit 5 and the indoor unit 6 in the refrigerant pipe 7 in particular. Shows the piping for. Here, the refrigerant flows through the pipe in the direction of the arrow in the figure. Although the compressor 3 is on the outdoor unit side in FIG. 12, it may be on the indoor unit side.
【手続補正4】[Procedure amendment 4]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0005[Name of item to be corrected] 0005
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0005】また、冷凍機を室内冷暖房機として使用す
る場合には、コンプレッサ3の出口に四方弁を設けて、
冷媒の流れる向きを切替えることで行われる。図12が
暖房機として動作する場合には、蒸発器1と凝縮器2の
役割は逆転する。蒸発器1と凝縮器2の内部では冷媒配
管7がジグザグに交差しているため、外気に触れる配管
表面積が大きくなり、空気と冷媒との熱交換率が良くな
っている。ここでは、図12を室内冷房機として、SH
制御では、蒸発器内部の冷媒温度、例えば、出口位置a
にある配管内部の冷媒温度と中間位置bにある配管内部
の冷媒温度を測定し、その温度差が一定値ecになるよ
うに制御する。これにより、冷凍機全体の内部状態を安
定にし、かつ高い冷凍能力を引き出す。SH制御では、
蒸発器単体での情報のみで制御を行えるため、凝縮器2
やコンプレッサ3等の状態を計測することが物理的に困
難、あるいはコスト的に困難な場合に有効な制御手段で
ある。When the refrigerator is used as an indoor air conditioner, a four-way valve is provided at the outlet of the compressor 3,
This is done by switching the direction in which the refrigerant flows. When FIG. 12 operates as a heater, the roles of the evaporator 1 and the condenser 2 are reversed. Since the refrigerant pipes 7 intersect in a zigzag manner inside the evaporator 1 and the condenser 2, the surface area of the pipes exposed to the outside air is increased and the heat exchange rate between air and the refrigerant is improved. Here, as shown in FIG. 12 as an indoor air conditioner, the SH
In the control, the temperature of the refrigerant inside the evaporator, for example, the outlet position a
The temperature of the refrigerant inside the pipe located at the point b and the temperature of the refrigerant inside the pipe located at the intermediate position b are measured, and the temperature difference is controlled to be a constant value ec. As a result, the internal state of the entire refrigerator is stabilized and high refrigerating capacity is brought out. In SH control,
Since it can be controlled only by the information of the evaporator itself, the condenser 2
This is an effective control means when it is physically difficult or costly to measure the state of the compressor or the compressor 3.
【手続補正5】[Procedure Amendment 5]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0011[Correction target item name] 0011
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0011】従来、上記問題のため、ある範囲で安定が
得られる場合には、できるだけ膨張弁4を開閉度の変化
をさせないようにして安定を保つようにしているが、従
来の方法では、変化を抑えるため膨張弁4を制御しても
変化に対する対応がおそいため、結果的に精度の良い安
定な制御が得られない。この場合、膨張弁4の1ステッ
プ(単位操作量)を小さくすることも考えられるが、コ
ストが大幅に増加することになると言う問題がある。Conventionally, due to the above problems, when stability is obtained within a certain range, the expansion valve 4 is kept as stable as possible by keeping the opening / closing degree unchanged. To control the expansion valve 4 to suppress
Since it is difficult to respond to changes , accurate and stable control cannot be obtained as a result. In this case, it is conceivable to reduce one step (unit operation amount) of the expansion valve 4, but there is a problem that the cost will increase significantly.
【手続補正6】[Procedure correction 6]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0014[Correction target item name] 0014
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0014】請求項2の発明は、コンプレッサと凝縮器
と膨張弁と蒸発器とを冷媒配管で循環接続すると共に、
冷凍機内部の冷媒温度の状態に基づき制御演算して操作
量を求め、求めた操作量に応じて前記膨張弁の開閉度を
制御する蒸気圧縮式冷凍装置の膨張弁制御方法におい
て、操作量に基づいて膨張弁の開閉度を単位ステップ量
変えると冷媒温度の安定状態からの変化が大きく、逆に
冷媒温度が不安定状態となる場合に、その不安定状態を
抑制するために膨張弁の開閉度を単位ステップ変えた
後、所定時間経過後に膨張弁の開閉度を変えた方向と逆
方向へ膨張弁の開閉度を単位ステップ変えるようにした
ものである。According to a second aspect of the present invention, the compressor, the condenser, the expansion valve and the evaporator are circulated and connected by a refrigerant pipe, and
In the expansion valve control method of the vapor compression refrigeration system for controlling the opening / closing degree of the expansion valve according to the calculated operation amount, the operation amount is calculated by control calculation based on the state of the refrigerant temperature inside the refrigerator. If the opening / closing degree of the expansion valve is changed by a unit step amount based on this, when the refrigerant temperature changes greatly from the stable state and conversely the refrigerant temperature becomes unstable, the opening / closing of the expansion valve is controlled to suppress the unstable state. The degree of opening and closing of the expansion valve is changed by a unit step in a direction opposite to the direction in which the degree of opening and closing of the expansion valve is changed after a predetermined time has elapsed after the degree of opening and closing is changed by a unit step.
【手続補正7】[Procedure Amendment 7]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】0035[Correction target item name] 0035
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【0035】具体的に図8の場合について説明すると、
最初に冷凍機での運転実験より、ある配管長、ある室内
温度、ある膨張弁開閉度、ある膨張弁開閉変化量の際の
温度検出信号d1と温度検出信号d2の変化量(つまり
傾き)を測定する。そして、この各々のパラメータをい
くつか変えて、また、測定する。この測定を各パラメー
タの代表的な値について行う。例えば、配管長について
は、5m,10m,15mなど、室内温度については2
0℃,25℃,30℃などについて、温度検出信号d1
と温度検出信号d2の変化量を測定する。こうして得ら
れた入出力のデータを教師としてNNに学習を行わせ
る。ただし、学習後のNNでは配管長などから温度検出
信号d1と温度検出信号d2の変化量を求めるのではな
く、温度検出信号d1と温度検出信号d2の変化量など
から配管長を求める。この場合、NNは、単に入出力変
数の組合せがどのようになっているかを学習するだけで
あるから、このようなことが可能となる。次に、学習後
はNNに学習させない場合の値、例えば、室内温度が2
2℃等を入力しても、その場合の全ての入力の組合せか
ら適切な配管長を推定出力する。このようにNNに学習
させることにより、入出力のすべての組合せを実験しな
くても、いくつかの代表的な実験を行えば、必要な配管
長の推定がされる。なお、図8では冷房の場合を述べて
いるから室内温度となっているが、暖房の場合には、室
外温度となる。The case of FIG. 8 will be specifically described.
First, from an operation experiment in a refrigerator, a change amount (that is, a slope) of the temperature detection signal d1 and the temperature detection signal d2 at a certain pipe length, a certain room temperature, a certain expansion valve opening / closing degree, and a certain expansion valve opening / closing change amount is determined. taking measurement. Then, some of these parameters are changed and measured again. This measurement is performed for typical values of each parameter. For example, the pipe length is 5 m, 10 m, 15 m, etc., and the room temperature is 2
Temperature detection signal d1 for 0 ° C, 25 ° C, 30 ° C, etc.
And the amount of change in the temperature detection signal d2 is measured. The NN is made to learn by using the input / output data thus obtained as a teacher. However, in the NN after learning, the amount of change in the temperature detection signal d1 and the temperature detection signal d2 is not obtained from the pipe length, but the pipe length is obtained from the amount of change in the temperature detection signal d1 and the temperature detection signal d2. In this case, the NN simply learns what the combination of the input / output variables is, so that such a thing is possible. Next, after learning, the value when the NN is not allowed to learn, for example, the room temperature is 2
Even if 2 ° C or the like is input, an appropriate pipe length is estimated and output from all combinations of inputs in that case. By making the NN learn in this way, the required pipe length can be estimated by conducting some representative experiments without experimenting with all combinations of input and output. In addition, in FIG. 8, the case of cooling is described.
Since it is indoor temperature, it is outdoor temperature in case of heating.
【手続補正8】[Procedure Amendment 8]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】符号の説明[Correction target item name] Explanation of code
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【符号の説明】 1 蒸発器 2 凝縮器 3 コンプレッサ 4 膨張弁 7 冷媒配管 8 配管 9 温度検出器 10 温度検出器 11 制御部 13 推輪部 14 制御部 15 制御タイミング発生部 16 制御指令部 17 駆動パルス発生部 18 逆転タイミング発生部[Explanation of Codes] 1 Evaporator 2 Condenser 3 Compressor 4 Expansion valve 7 Refrigerant pipe 8 Pipe 9 Temperature detector 10 Temperature detector 11 Control unit 13 Thrusting unit 14 Control unit 15 Control timing generation unit 16 Control command unit 17 Drive Pulse generator 18 Reverse rotation timing generator
Claims (2)
とを冷媒配管で循環接続すると共に、冷凍機内部の冷媒
温度の状態に基づき制御演算して操作量を求め、求めた
操作量に応じて前記膨張弁の開閉度を制御する蒸気圧縮
式冷凍装置の膨張弁制御方法において、 前記冷凍機内部の冷媒温度の状態の変化から前記冷媒配
管の長さを類推し、類推した冷媒配管の長さに対応した
最適な制御演算パラメータを設定して前記膨張弁を制御
することを特徴とする蒸気圧縮式冷凍装置の膨張弁制御
方法。1. A compressor, a condenser, an expansion valve, and an evaporator are circulatively connected by a refrigerant pipe, and a control operation is calculated based on a refrigerant temperature state inside a refrigerator to obtain an operation amount, and the operation amount is determined according to the operation amount thus obtained. In the expansion valve control method of the vapor compression refrigerating apparatus for controlling the opening / closing degree of the expansion valve, the length of the refrigerant pipe is inferred from the change in the state of the refrigerant temperature inside the refrigerator, and the length of the inferred refrigerant pipe is inferred. An expansion valve control method for a vapor compression refrigeration system, characterized in that the expansion valve is controlled by setting an optimum control calculation parameter corresponding to the height.
とを冷媒配管で循環接続すると共に、冷凍機内部の冷媒
温度の状態に基づき制御演算して操作量を求め、求めた
操作量に応じて前記膨張弁の開閉度を単位ステップ量ず
つ変えることにより制御する蒸気圧縮式冷凍装置の膨張
弁制御方法において、 前記操作量に基づいて前記膨張弁の開閉度を単位ステッ
プ量変えると前記冷媒温度の安定状態からの変化が大き
く、逆に前記冷媒温度が不安定状態となる場合に、その
不安定状態を抑制するために前記膨張弁の開閉度を単位
ステップ量変えた後、所定時間経過後に前記膨張弁の開
閉度を変えた方向と逆方向へ前記膨張弁の開閉度を単位
ステップ量変えることを特徴とする蒸気圧縮式冷凍装置
の膨張弁制御方法。2. A compressor, a condenser, an expansion valve, and an evaporator are circulated and connected by a refrigerant pipe, and a control calculation is performed based on the state of the refrigerant temperature inside the refrigerator to obtain an operation amount, and the operation amount is determined according to the operation amount thus obtained. In the expansion valve control method for a vapor compression refrigeration system, which controls the opening / closing degree of the expansion valve by changing the opening / closing degree of the expansion valve by a unit step amount, the refrigerant temperature is changed by changing the opening / closing degree of the expansion valve by a unit step amount based on the operation amount. The change from the stable state is large, and conversely, when the refrigerant temperature becomes unstable, after changing the opening / closing degree of the expansion valve by a unit step amount to suppress the unstable state, after a predetermined time elapses. An expansion valve control method for a vapor compression refrigeration system, wherein the opening / closing degree of the expansion valve is changed by a unit step amount in a direction opposite to the direction in which the opening / closing degree of the expansion valve is changed.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4243989A JPH0674573A (en) | 1992-08-21 | 1992-08-21 | Method for controlling expansion valve in vapor-compression refrigerating apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4243989A JPH0674573A (en) | 1992-08-21 | 1992-08-21 | Method for controlling expansion valve in vapor-compression refrigerating apparatus |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0674573A true JPH0674573A (en) | 1994-03-15 |
Family
ID=17112060
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4243989A Pending JPH0674573A (en) | 1992-08-21 | 1992-08-21 | Method for controlling expansion valve in vapor-compression refrigerating apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0674573A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100315784B1 (en) * | 1999-09-03 | 2001-12-12 | 구자홍 | Control unit with delay compensation for air conditioner and the same method |
| WO2007125959A1 (en) * | 2006-04-27 | 2007-11-08 | Daikin Industries, Ltd. | Air conditioner |
| JPWO2022185443A1 (en) * | 2021-03-03 | 2022-09-09 |
-
1992
- 1992-08-21 JP JP4243989A patent/JPH0674573A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100315784B1 (en) * | 1999-09-03 | 2001-12-12 | 구자홍 | Control unit with delay compensation for air conditioner and the same method |
| WO2007125959A1 (en) * | 2006-04-27 | 2007-11-08 | Daikin Industries, Ltd. | Air conditioner |
| JPWO2022185443A1 (en) * | 2021-03-03 | 2022-09-09 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5372015A (en) | Air conditioner controller | |
| US9182154B2 (en) | Adaptive control of vapor compression system | |
| US5442926A (en) | Control system for air-conditioner | |
| US6581847B2 (en) | Variable-air-volume diffuser, actuator assembly and method | |
| EP0380615B1 (en) | A method for the optimal comfort and efficiency control of variable speed heat pumps and air conditioners | |
| US8793003B2 (en) | Controlling operations of vapor compression system | |
| US10174957B2 (en) | System and method for controlling multi-zone vapor compression systems | |
| US5004149A (en) | Central air conditioning system having compensating control function for total heat load in a plurality of rooms | |
| JP2021103083A5 (en) | ||
| JP4022202B2 (en) | Self-regulated pull-down fuzzy logic temperature control for cooling system | |
| Li et al. | A new method for controlling refrigerant flow in automobile air conditioning | |
| Abdo-Allah et al. | Modeling, analysis, and design of a fuzzy logic controller for an AHU in the SJ Carew Building at Memorial University | |
| Li et al. | Cascade fuzzy control for gas engine driven heat pump | |
| Seem et al. | A new sequencing control strategy for air-handling units | |
| JPH1194327A (en) | Control device for air conditioner | |
| US20230332801A1 (en) | Hot water supply system | |
| JP2624171B2 (en) | Air conditioner operation control method | |
| JPH06281266A (en) | Air conditioner | |
| JPH0510568A (en) | Air conditioner | |
| JP2576349B2 (en) | Control method of hot water valve for air conditioner | |
| JP3388305B2 (en) | Multi-room air conditioner | |
| JP2611657B2 (en) | Air conditioner operation control method | |
| Zhang et al. | Adaptive fan-coil outlet wind temperature control with correction module of thermistor for the ASHPAC system | |
| EP0419214A2 (en) | System and method for fan speed control | |
| JPH0225090Y2 (en) |