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JPH0776643B2 - Two room air conditioner - Google Patents
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JPH0776643B2 - Two room air conditioner - Google Patents

Two room air conditioner

Info

Publication number
JPH0776643B2
JPH0776643B2 JP1091064A JP9106489A JPH0776643B2 JP H0776643 B2 JPH0776643 B2 JP H0776643B2 JP 1091064 A JP1091064 A JP 1091064A JP 9106489 A JP9106489 A JP 9106489A JP H0776643 B2 JPH0776643 B2 JP H0776643B2
Authority
JP
Japan
Prior art keywords
compressor
indoor
load
indoor unit
equation
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP1091064A
Other languages
Japanese (ja)
Other versions
JPH02272250A (en
Inventor
雅昭 増田
勝広 若原
修一 阪田
正則 小谷
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.)
Sharp Corp
Original Assignee
Sharp Corp
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 Sharp Corp filed Critical Sharp Corp
Priority to JP1091064A priority Critical patent/JPH0776643B2/en
Priority to US07/367,141 priority patent/US4926653A/en
Publication of JPH02272250A publication Critical patent/JPH02272250A/en
Publication of JPH0776643B2 publication Critical patent/JPH0776643B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Compression-Type Refrigeration Machines With Reversible Cycles (AREA)
  • Air Conditioning Control Device (AREA)
  • Control Of Temperature (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、インバータ圧縮機により駆動される冷凍サイ
クル中に電動膨張弁を有し、該電動膨張弁によって冷媒
流量制御が行われる冷暖房装置に係り、特に1台と室外
機に2台の室内機が接続されたものに関する。
Description: TECHNICAL FIELD The present invention relates to a cooling and heating apparatus that has an electric expansion valve in a refrigeration cycle driven by an inverter compressor, and a refrigerant flow rate is controlled by the electric expansion valve. In particular, the present invention relates to one indoor unit and two outdoor units connected to an outdoor unit.

(従来の技術) 従来、2台の室内機を有する多室型冷暖房装置は、それ
ぞれの室内機に対応する膨張弁を有し、該膨張弁制御
は、冷凍サイクルの安定のため圧縮機の出力にのみ応じ
て行っていた。そこで、本発明者らは、冷凍サイクルの
安定を計るとともに、各室内機の負荷に応じて膨張弁制
御を行うために、各室内機への冷媒分流試験を行い、そ
の結果から得られる冷媒流量の理想特性図(第6図およ
び第8図参照)および制御特性図(第7図および第9図
参照)によって圧縮機の周波数と膨張弁の開閉度を関係
づけた二室型冷暖房装置を提案した。
(Prior Art) Conventionally, a multi-room type air conditioner having two indoor units has an expansion valve corresponding to each indoor unit, and the expansion valve control controls the output of the compressor to stabilize the refrigeration cycle. I was only going to go. Therefore, the present inventors measure the stability of the refrigeration cycle, and to perform expansion valve control according to the load of each indoor unit, perform a refrigerant shunt test to each indoor unit, and the refrigerant flow rate obtained from the result. A two-chamber cooling and heating system in which the frequency of the compressor and the opening / closing degree of the expansion valve are related by the ideal characteristic diagrams (see Figs. 6 and 8) and the control characteristic diagrams (see Figs. 7 and 9) of did.

第1図は、二室冷暖房装置の全体構成の概略を示す図で
ある。同図において、点線矢印は冷房運転時の冷媒の流
れを、実線矢印は暖房運転時の冷媒の流れを示す。つま
り、冷房の場合、圧縮機1で圧縮された冷媒蒸気は、四
方弁2を介して室外熱交換器3にて凝縮液化し、レシー
バータンク4a,4bに貯えられる。この後、冷媒液はそれ
ぞれの室内機A,Bに対応する電動膨張弁6a,6bにて減圧さ
れ、室内熱交換機7,8において、低圧蒸気となり、分岐
管18にて合流した後、再び四方弁2を介して圧縮機1に
戻る。この時、冷凍サイクルの安定を計るとともに、各
室内機A,Bの負荷に応じて電動膨張弁6a,6bの開閉度の制
御を行うための、圧縮機1の周波数Fおよび各電動膨張
弁6a,6bの開閉度Va,Vbの割合は、次のようにして決定さ
れる。
FIG. 1 is a diagram showing an outline of the overall configuration of a two-room cooling and heating device. In the figure, dotted arrows indicate the flow of the refrigerant during the cooling operation, and solid arrows indicate the flow of the refrigerant during the heating operation. That is, in the case of cooling, the refrigerant vapor compressed by the compressor 1 is condensed and liquefied by the outdoor heat exchanger 3 via the four-way valve 2 and stored in the receiver tanks 4a, 4b. After this, the refrigerant liquid is decompressed by the electric expansion valves 6a, 6b corresponding to the respective indoor units A, B, becomes low-pressure steam in the indoor heat exchangers 7, 8, merges in the branch pipe 18, and then again in four directions. Return to compressor 1 via valve 2. At this time, the frequency F of the compressor 1 and the electric expansion valves 6a for controlling the opening / closing degree of the electric expansion valves 6a, 6b according to the load of the indoor units A, B while stabilizing the refrigeration cycle are measured. The ratio of the switching degrees V a and V b of 6b is determined as follows.

すなわち、マイコン制御部13の構成要素である圧縮機周
波数制御部14(第2図参照)では、表2に示されるよう
な関係に基づいて、各室温設定器12a,12bでの設定温度
と各室内の実測室温との差(TRa−TIa),(TRb−TIb)
を各室内の負荷としてとらえ、その範囲を負荷係数a,b
に置換える。そして、表3に示すように、各負荷係数の
合計から圧縮機1の周波数Fを決定する。
That is, in the compressor frequency control unit 14 (see FIG. 2), which is a component of the microcomputer control unit 13, based on the relationship shown in Table 2, the set temperature in each room temperature setting device 12a, 12b and Difference from actual room temperature in room (TRa-TIa), (TRb-TIb)
Is regarded as the load in each room, and its range is defined by the load factors a, b.
Replace with. Then, as shown in Table 3, the frequency F of the compressor 1 is determined from the sum of the load coefficients.

一方、膨張弁開閉制御部15では、圧縮機周波数制御部14
で得られた各室内機A,Bの負荷係数a,bの信号を受け、各
電動膨張弁6a,6bの開閉度Va,Vbの割合を決定する。この
各電動膨張弁6a,6bの開閉度Va,Vbの割合を決定するに当
たっては、第6図に示すように、各膨張弁6a,6bの出口
温度(TA),(TB)の平均温度(TA+TB)/2と圧縮機1
の吸込温度(TS)との差から得られる過熱度を一定値に
保つ冷媒流量の理想特性図を予め求めておく。そして、
この理想特性図に基づいて上記負荷係数a,bと膨張弁開
閉度Va,Vbとの関係を求め、この関係に基づいて決定し
た第7図に示す制御特性図によって決定する。なお、第
7図は第6図に示す理想特性図に基づいて作成した制御
特性図である。
On the other hand, in the expansion valve opening / closing control unit 15, the compressor frequency control unit 14
The signals of the load coefficients a and b of the indoor units A and B obtained in step 1 are received, and the ratio of the opening / closing degrees V a and V b of the electric expansion valves 6a and 6b is determined. In determining the ratio of the opening / closing degrees V a , V b of the electric expansion valves 6a, 6b, as shown in FIG. 6, the average of the outlet temperatures (TA), (TB) of the expansion valves 6a, 6b is determined. Temperature (TA + TB) / 2 and compressor 1
The ideal characteristic diagram of the refrigerant flow rate that keeps the degree of superheat obtained from the difference between the suction temperature (TS) and the constant temperature is obtained in advance. And
The relationship between the load coefficients a and b and the expansion valve opening / closing degrees V a and V b is determined based on this ideal characteristic diagram, and is determined based on the control characteristic diagram shown in FIG. 7 determined based on this relationship. 7. FIG. 7 is a control characteristic diagram created based on the ideal characteristic diagram shown in FIG.

また、暖房の場合、圧縮機1で圧縮された冷媒蒸気は、
四方弁2を介して分岐管18で分岐した後、各室内機A,B
の室内熱交換器7,8にて凝縮液化し、レシーバータンク4
a,4bに貯えられる。この後、冷媒液はそれぞれの室内機
A,Bに対応する電動膨張弁6a,6bにて減圧され、室外熱交
換器3において蒸発し、再び四方弁2を介して圧縮機1
に戻る。この時、圧縮機1の周波数Fおよび各電動膨張
弁6a,6bの開閉度c,dの割合は、冷房の場合と同様にして
決定されるが、冷媒の流れが逆方向であるため、冷媒流
量の理想特性図は第8図となり、制御特性図は第9図と
なる。
In the case of heating, the refrigerant vapor compressed by the compressor 1 is
After branching through the branch pipe 18 via the four-way valve 2, each indoor unit A, B
It is condensed and liquefied in the indoor heat exchangers 7 and 8 of the receiver tank 4
Stored in a, 4b. After this, the refrigerant liquid is transferred to each indoor unit.
The pressure is reduced by the electric expansion valves 6a and 6b corresponding to A and B, evaporated in the outdoor heat exchanger 3, and again compressed through the four-way valve 2 into the compressor 1
Return to. At this time, the frequency F of the compressor 1 and the ratio of the opening / closing degrees c and d of the electric expansion valves 6a and 6b are determined in the same manner as in the case of cooling, but the refrigerant flow is in the opposite direction, so the refrigerant The ideal characteristic diagram of the flow rate is shown in FIG. 8 and the control characteristic diagram is shown in FIG.

このように、従来サイクルでは、冷媒分流試験によって
理想特性図を作成しておき、この理想特性図を基にした
制御特性図によって圧縮機の周波数と膨張弁の開閉度を
関係づけるようにしていた。
As described above, in the conventional cycle, the ideal characteristic diagram is created by the refrigerant diversion test, and the frequency of the compressor and the opening / closing degree of the expansion valve are related by the control characteristic diagram based on this ideal characteristic diagram. .

(発明が解決しようとする課題) しかし、この従来の膨張弁制御方法では、室内機の大き
さ(定格能力)が変わるごとに、理想特性図作成のため
の冷媒分流試験を実施する必要があり、また、この理想
特性図を基にした制御特性図は、マイコン容量の制約か
ら、冷媒分流ポイント数や設定圧縮機周波数に限界が生
じるため、階段状の雑な曲線がプロットされ、特に冷媒
分流ポイント数を多く必要とする低圧縮機周波数域では
冷媒分流ポイントが少なく制御が雑であった。
(Problems to be Solved by the Invention) However, in this conventional expansion valve control method, it is necessary to carry out a refrigerant diversion test for creating an ideal characteristic diagram every time the size (rated capacity) of the indoor unit changes. Also, the control characteristic diagram based on this ideal characteristic diagram has a limit on the number of refrigerant diversion points and the set compressor frequency due to the restriction of the microcomputer capacity, so a staircase-shaped rough curve is plotted, especially the refrigerant diversion In the low compressor frequency range, which requires a large number of points, there were few refrigerant diversion points and control was poor.

本発明は、係る実情に鑑みてなされたもので、上記制御
特性図に示される各室内機の負荷の関係を理想特性図に
近似した数式とすることで、圧縮機周波数の決定を容易
にし、各室内機への冷媒分流ポイントが自由に設定で
き、パラメータの変更によって異能力室内機の接続を可
能とした二室冷暖房装置を提供することを目的とする。
The present invention has been made in view of the actual situation, and facilitates determination of the compressor frequency by using a mathematical expression that approximates the load relationship of each indoor unit shown in the control characteristic diagram to an ideal characteristic diagram, It is an object of the present invention to provide a two-room cooling / heating device in which a refrigerant distribution point to each indoor unit can be freely set and a different capacity indoor unit can be connected by changing parameters.

(課題を解決するための手段) 本発明の二室冷暖房装置は、1台の室内機に2台の室内
機が各々電動膨張弁を介して接続され、周波数可変型の
圧縮機により圧縮され冷媒を各室内熱交換器もしくは室
外熱交換器で凝縮させ、さらに上記冷媒を各電動膨張弁
で膨張、減圧させた後、上記室外熱交換器もしくは各室
内熱交換器で蒸発させて各室内の暖房もしくは冷房を行
うようにした冷暖房装置をおいて、上記圧縮機の周波数
Fは、各室内機に設置された室温設定器の設定温度と実
際の室内温度との差から得られる各室内負荷に基づく負
荷係数をa,bとし、負荷係数aの室内機容量に対する負
荷係数bの室内機容量の比をMとして、冷房運転時には
(1)式から、暖房運転時には(2)式から算出される
とともに、 b=−{M2/(f・F)}a2+f・F …(1) b=−M・a+f・F …(2) ただし、fは比例定数 上記各電動膨張弁の開閉度の比Vb/Vaは、上記各負荷係
数a,bの比b/aによって決定されるものである。
(Means for Solving the Problem) In the two-room cooling and heating apparatus of the present invention, one indoor unit is connected to two indoor units via electric expansion valves, and the refrigerant is compressed by a variable frequency compressor. Is condensed in each indoor heat exchanger or outdoor heat exchanger, the refrigerant is expanded and decompressed by each electric expansion valve, and then evaporated in the outdoor heat exchanger or each indoor heat exchanger to heat each room. Alternatively, in a cooling and heating device that performs cooling, the frequency F of the compressor is based on each indoor load obtained from the difference between the set temperature of the room temperature setting device installed in each indoor unit and the actual indoor temperature. The load coefficients are a and b, and the ratio of the indoor unit capacity of the load coefficient b to the indoor unit capacity of the load coefficient a is M, which is calculated from Equation (1) during cooling operation and from Equation (2) during heating operation. , b = - {M 2 / (f · F)} a 2 + · F ... (1) b = -M · a + f · F ... (2) where, f is the ratio V b / V a of the opening and closing of the proportionality constant above the electric expansion valve, each load factor a, b ratio It is determined by b / a.

(作用) 第1図に点線矢印で示すように、2台の室内機A,Bを同
時に冷房運転する場合、圧縮機1で圧縮された冷媒蒸気
は、四方弁2を介して室外熱交換器3にて凝縮液化す
る。こうして得られた冷媒液は、2台のレシーバータン
ク4a,4bに貯えられる。この後、冷媒液は、それぞれの
室内機A,Bに対応する電動膨張弁6a,6bにて減圧し、室内
熱交換器7,8において低圧蒸気となり、再び四方弁2を
介して圧縮機1に戻る。
(Operation) As shown by a dotted arrow in FIG. 1, when the two indoor units A and B are simultaneously operated for cooling, the refrigerant vapor compressed by the compressor 1 passes through the four-way valve 2 and the outdoor heat exchanger. Condensate and liquefy at 3. The refrigerant liquid thus obtained is stored in the two receiver tanks 4a and 4b. After this, the refrigerant liquid is decompressed by the electric expansion valves 6a, 6b corresponding to the indoor units A, B, becomes low-pressure steam in the indoor heat exchangers 7, 8, and again passes through the four-way valve 2 to the compressor 1 Return to.

この際、第2図に示すように、マイコン制御部13の圧縮
機周波数制御部14には、室内機Aの設定温度(TIa)と
その室内の実測室温(TRa)、室内機Bの設定温度(TI
b)とその室内の実測室温(TRb)とが入力される。一
方、膨張弁開閉制御部15には、電動膨張弁6a,6bの出口
パイプに取付けた温度センサ16a,16bから得られる温度
(TA),(TB)と圧縮機1の吸込パイプに取付けた温度
センサ9から得られる温度(TS)とが入力される。この
うち、圧縮機周波数制御部14では、室内機Aの室内負荷
(TRa−TIa)と室内機Bの室内負荷(TRb−TIb)とから
得られる負荷係数a,bを(1)式に代入し、これによっ
て圧縮機の周波数を算出して圧縮機1の出力を制御する
とともに、前記負荷係数a,bを膨張弁開閉制御部15に出
力する。一方、膨張弁開閉制御部15では、各電動膨張弁
6a,6bの出口温度(TA),(TB)の平均値(TA+TB)/2
と圧縮機1の吸込温度(TS)との差から得られる過熱度
が一定となるように冷凍バランスを保ちつつ、各負荷係
数a,bの負荷比b/aと同一となるように各電動膨張弁6a,6
bの開閉度の比Vb/Vaを制御し、これによって冷房運転が
行われる。次に、暖房運転の場合、第1図に実線矢印で
示すように、冷媒蒸気の流れは、冷房運転の場合と逆方
向になり、室内熱交換器7,8で凝縮液化し、室外熱交換
器3で低圧蒸気となる。その他各部の働きは、圧縮機の
周波数を決定する数式が(2)式となる以外は上記冷房
運転の場合と同様である。
At this time, as shown in FIG. 2, the compressor frequency control unit 14 of the microcomputer control unit 13 causes the set temperature (TIa) of the indoor unit A, the actually measured room temperature (TRa) of the room, and the set temperature of the indoor unit B to be set. (TI
b) and the measured room temperature (TRb) in the room are input. On the other hand, in the expansion valve opening / closing control unit 15, the temperatures (TA) and (TB) obtained from the temperature sensors 16a and 16b attached to the outlet pipes of the electric expansion valves 6a and 6b and the temperature attached to the suction pipe of the compressor 1 are obtained. The temperature (TS) obtained from the sensor 9 is input. Among these, in the compressor frequency control unit 14, the load coefficients a and b obtained from the indoor load (TRa-TIa) of the indoor unit A and the indoor load (TRb-TIb) of the indoor unit B are substituted into the equation (1). Then, the frequency of the compressor is calculated by this, the output of the compressor 1 is controlled, and the load coefficients a and b are output to the expansion valve opening / closing control unit 15. On the other hand, the expansion valve opening / closing control unit 15
Average of outlet temperature (TA) and (TB) of 6a and 6b (TA + TB) / 2
And the suction temperature (TS) of the compressor 1 keeps the refrigeration balance so that the degree of superheat obtained is constant, and each load coefficient a, b is equal to the load ratio b / a Expansion valve 6a, 6
and controlling the ratio V b / V a of the opening and closing degree of b, this cooling operation by is performed. Next, in the heating operation, as shown by the solid arrow in FIG. 1, the flow of the refrigerant vapor is in the opposite direction to that in the cooling operation, and the indoor heat exchangers 7 and 8 condense and liquefy, and the outdoor heat exchange. It becomes low-pressure steam in vessel 3. The functions of the other parts are the same as in the case of the cooling operation, except that the formula for determining the frequency of the compressor is formula (2).

(実施例) 以下、本発明の一実施例を図面を参照して説明する。Embodiment An embodiment of the present invention will be described below with reference to the drawings.

第6図は、室内機Aおよび室内機Bの冷媒分流試験によ
って得られた冷房時における冷媒流量の理想制御特性図
を示し、第8図は、同暖房時における冷媒流量の理想制
御特性図を示している。この理想制御特性図は、冷媒流
量と負荷係数a,bとの間に一定の関係を仮定すると、室
内機Aおよび室内機Bの各負荷係数a,bと圧縮機周波数
Fをパラメーターとした数式で近似することができる。
FIG. 6 shows an ideal control characteristic diagram of the refrigerant flow rate during cooling, which is obtained by a refrigerant distribution test of the indoor units A and B, and FIG. 8 shows an ideal control characteristic diagram of the refrigerant flow rate during the heating. Shows. This ideal control characteristic diagram is a mathematical expression in which the load coefficients a and b of the indoor unit A and the indoor unit B and the compressor frequency F are parameters, assuming a constant relationship between the refrigerant flow rate and the load coefficients a and b. Can be approximated by

すなわち、近似式として(3)式に示す二次式を用いれ
ば、 b=−la2−ma+n …(3) ただし、l,m,nは定数 冷房の場合は第6図を参照して(3)式にm=0を代入
して近似することができる((4)式)。
That is, if the quadratic equation shown in the equation (3) is used as an approximate equation, b = −la 2 −ma + n (3) However, l, m, n are constants. In the case of cooling, refer to FIG. It can be approximated by substituting m = 0 into the equation (3) (the equation (4)).

b=−la2+n …(4) また、暖房の場合は第8図を参照にして(3)式にl=
0を代入して近似することができる〔(5)式〕。
b = −la 2 + n (4) Further, in the case of heating, referring to FIG.
It can be approximated by substituting 0 [Equation (5)].

b=−ma+n …(5) この近似式(4)式および(5)式で表される曲線は第
3図に示すような曲線となる。ここで、(4)式および
(5)式が第3図のY軸およびX軸と交わる座標(a,
0)(0,b)の点aおよび点bの値は、同一周波数におけ
る室内機Aと室内機Bとの容量比(定格時の能力比)M
として近似することができる〔(6)式〕。
b = -ma + n (5) The curves represented by the approximate expressions (4) and (5) are curves as shown in FIG. Here, equations (4) and (5) are the coordinates (a,
0) The values of points a and b of (0, b) are the capacity ratio (capacity ratio at the time of rating) M between the indoor unit A and the indoor unit B at the same frequency.
Can be approximated as [Equation (6)].

M=b/a …(6) この点aおよび点bは、冷房時の近似式である(4)式
に、それぞれ(a,0)(0,b)を代入することによって、
(7a)式および(7b)式で表すことができる。そして、
この(7a)式および(7b)式を(6)式に代入してlの
式に置き換えると(8)式となる。
M = b / a (6) These points a and b are obtained by substituting (a, 0) (0, b) into the equation (4), which is an approximate equation during cooling,
It can be expressed by equations (7a) and (7b). And
By substituting the equations (7a) and (7b) into the equation (6) and replacing it with the equation l, the equation (8) is obtained.

また、暖房時の近似式である(5)式に、それぞれ(a,
0)(0,b)を代入することによって、点aおよび点b
は、(9a)式および(9b)式で表すことができる。そし
て、この(9a)式および(9b)式を(6)式に代入して
mの式に置き換えると(10)式となる。
In addition, in equation (5), which is an approximate equation for heating,
0) by substituting (0, b) for points a and b
Can be expressed by equations (9a) and (9b). Then, by substituting the expressions (9a) and (9b) into the expression (6) and replacing it with the expression m, the expression (10) is obtained.

a=n/m …(9a) b=n …(9b) m=M …(10) さらに、第3図における(4)式および(5)式の切片
(nに相当する)は、第6図および第8図に示すよう
に、圧縮機の周波数Fをパラメーターとして変化し、こ
の関係は(11)式として表すことができる。ただし、f
は比例定数を示す。
a = n / m (9a) b = n (9b) m = M (10) Further, the intercepts (corresponding to n) of the equations (4) and (5) in FIG. As shown in the figure and FIG. 8, the frequency F of the compressor is changed as a parameter, and this relationship can be expressed as the equation (11). However, f
Indicates a constant of proportionality.

n=f・F …(11) そして、上記(8)式および(11)式を(4)式に代入
することによって、負荷係数a,bおよび圧縮機周波数F
をパラメーターとした冷房時の数式〔(1)式〕とする
ことができる。
n = f · F (11) Then, by substituting the equations (8) and (11) into the equation (4), the load coefficients a and b and the compressor frequency F
Can be used as a mathematical expression [equation (1)] during cooling.

b=−{M2/(f・F)}a2+f・F …(1) この(1)式を曲線化すると第4図のような理想制御特
性図が得られ、第6図の理想特性図に略近似しているこ
とがわかる。
b = − {M 2 / (f · F)} a 2 + f · F (1) When this equation (1) is made into a curve, the ideal control characteristic diagram as shown in FIG. 4 is obtained, and the ideal control characteristic diagram of FIG. 6 is obtained. It can be seen that the characteristics are close to each other.

また、上記(10)式および(11)式を(5)式に代入す
ることによって、負荷係数a,bおよび圧縮機周波数Fを
パラメーターとした暖房時の数式〔(2)式〕とするこ
とができる。
Further, by substituting the equations (10) and (11) into the equation (5), the equation [(2)] for heating with the load factors a and b and the compressor frequency F as parameters is obtained. You can

b=−M・a+f・F …(2) この(2)式を曲線化すると第5図のような理想制御特
性図が得られ、第8図の理想特性図に略近似しているこ
とがわかる。
b = −M · a + f · F (2) When the equation (2) is made into a curve, an ideal control characteristic diagram as shown in FIG. 5 is obtained, and it may be approximated to the ideal characteristic diagram of FIG. Recognize.

次に、この上記冷房時の数式〔(1)式〕および暖房時
の数式〔(2)式〕を用いた冷暖房制御について述べ
る。
Next, cooling / heating control using the mathematical expression [equation (1)] at the time of cooling and the mathematical expression [equation (2) at the time of heating will be described.

第1図は、二室冷暖房装置の全体構成の概略を示す回路
図である。
FIG. 1 is a circuit diagram showing an outline of the overall configuration of a two-room cooling and heating device.

同図において点線矢印で示すように、冷房運転の場合、
圧縮機1により圧縮された冷媒蒸気は、四方弁2を介し
て室外熱交換器3にて凝縮液化し、レシーバータンク4
a,4bに導かれる。その後、冷媒は、それぞれ電動膨張弁
6a,6bにて減圧され、各室内機A,Bの室内熱交換器7,8に
て蒸発し、分岐管18にて合流した後、再び四方弁2を介
して圧縮機1に戻る。
As shown by the dotted arrow in the figure, in the case of cooling operation,
The refrigerant vapor compressed by the compressor 1 is condensed and liquefied by the outdoor heat exchanger 3 via the four-way valve 2, and the receiver tank 4
Guided by a and 4b. After that, the refrigerant is the electric expansion valve
After being decompressed by 6a, 6b, evaporated by the indoor heat exchangers 7, 8 of the indoor units A, B, and joined by the branch pipe 18, they return to the compressor 1 via the four-way valve 2 again.

この際、圧縮機1の周波数及び電動膨張弁6a,6bの開閉
度Va,Vbは、次のようにして決定される。
At this time, the frequency of the compressor 1 and the opening / closing degrees V a and V b of the electric expansion valves 6a and 6b are determined as follows.

すなわち、第1図および第2図に示すように、マイコン
制御部13の圧縮機周波数制御部14に、各室温設定器12a,
12bでの設定温度(TIa),(TIb)と、各室内温度セン
サ11a,11bから得られる実測室温(TRa),(TRb)とが
入力され、膨張弁開閉制御部15に、各膨張弁6a,6bの出
口パイプに取付けられた温度センサ16a,16bから得られ
る温度(TA),(TB)と、圧縮機1の吸込パイプに取付
けられた温度センサ9から得られる温度(TS)とが入力
される。
That is, as shown in FIGS. 1 and 2, each of the room temperature setting devices 12a, 12a,
The set temperatures (TIa) and (TIb) at 12b and the actually measured room temperatures (TRa) and (TRb) obtained from the indoor temperature sensors 11a and 11b are input, and the expansion valve opening / closing control unit 15 inputs the expansion valves 6a to the expansion valves 6a. Temperature (TA) and (TB) obtained from temperature sensors 16a and 16b attached to the outlet pipes of 6 and 6b, and temperature (TS) obtained from temperature sensor 9 attached to the suction pipe of compressor 1 are input. To be done.

このうち、圧縮機周波数制御部14では、表1に示される
ような関係に基づいて、各室温設定器12a,12bでの設定
温度と各室内の実測室温との差(TRa−TIa),(TRb−T
Ib)を各室内の負荷としてとらえ、その範囲を負荷係数
a,bに置換え、膨張弁開閉制御部15へ出力すると同時
に、この負荷係数を(1)式に代入して圧縮機1の周波
数Fを決定する。
Among these, in the compressor frequency control unit 14, based on the relationship as shown in Table 1, the difference (TRa-TIa) between the set temperature in each room temperature setting device 12a, 12b and the actually measured room temperature in each room (TRa-TIa), ( TRb-T
Ib) is regarded as the load in each room, and the range is taken as the load factor.
At the same time as substituting a and b for output to the expansion valve opening / closing control unit 15, this load coefficient is substituted into the equation (1) to determine the frequency F of the compressor 1.

一方、膨張弁開閉制御部15では、圧縮機周波数制御部14
で得られた各室内機A,Bの負荷係数a,bの信号を受け、こ
の負荷係数a,bの数値によって各電動膨張弁6a,6bの開閉
度Va,Vbを制御する。すなわち、この各電動膨張弁6a,6b
の開閉度Va,Vbは、各膨張弁6a,6bの出口温度(TA),
(TB)の平均温度(TA+TB)/2と圧縮機1の吸込温度
(TS)との差から得られる過熱度を一定値に保ちつつ、
各電動膨張弁6a,6bの開閉度の比Vb/Vaと各負荷係数a,b
の比b/aとが同一となるように制御し、かつ、最初に仮
定した冷媒流量と負荷係数a,bとの間の一定の関係を考
慮して制御する。
On the other hand, in the expansion valve opening / closing control unit 15, the compressor frequency control unit 14
Load factor of each of the indoor units A, B obtained in a, receives a signal b, the electric expansion valve 6a by the load factor a, b figures, 6b of the opening and closing of V a, and controls the V b. That is, each of these electric expansion valves 6a, 6b
The open / close degrees V a , V b of the expansion valves 6a, 6b are the outlet temperatures (TA),
While keeping the superheat degree obtained from the difference between the average temperature (TA + TB) / 2 of (TB) and the suction temperature (TS) of the compressor 1 at a constant value,
Open / close ratio V b / V a of each electric expansion valve 6a, 6b and each load coefficient a, b
The ratio b / a is controlled to be the same, and the control is performed in consideration of a certain relationship between the initially assumed refrigerant flow rate and the load coefficients a and b.

次に、暖房運転の場合、第1図に実線矢印で示すよう
に、圧縮機1により圧縮された冷媒蒸気は、四方弁2を
介して分岐管18で分岐した後、各室内機A,Bの室内熱交
換器7,8にて凝縮液化し、レシーバータンク4a,4bに導か
れる。その後、冷媒は、それぞれの電動膨張弁6a,6bに
て減圧され、室外熱交換器3にて蒸発し、再び四方弁2
を介して圧縮機1に戻る。
Next, in the heating operation, as shown by a solid arrow in FIG. 1, the refrigerant vapor compressed by the compressor 1 is branched by the branch pipe 18 via the four-way valve 2 and then the indoor units A, B Are condensed and liquefied in the indoor heat exchangers 7 and 8 and guided to the receiver tanks 4a and 4b. After that, the refrigerant is decompressed by the electric expansion valves 6a and 6b, evaporated in the outdoor heat exchanger 3, and again the four-way valve 2
Return to compressor 1 via.

この際、圧縮機1の周波数及び電動膨張弁6a,6bの開閉
度の比Vb/Vaは冷房運転時と同様にして決定される。
At this time, the ratio V b / V a of the frequency of the compressor 1 and the opening / closing degrees of the electric expansion valves 6a, 6b is determined in the same manner as during the cooling operation.

ただし、冷媒の流れが逆方向であるため、負荷係数a,b
を代入する数式は(2)式となる。
However, since the refrigerant flow is in the opposite direction, the load factors a, b
The mathematical expression for substituting is (2).

次に、上記実施例と同一特性の第4図および第5図に示
すような理想制御特性図を示す数式を用いた二室冷暖房
装置の制御について、その具体例を説明する。
Next, a specific example of the control of the two-room cooling / heating apparatus using the mathematical formulas showing the ideal control characteristic diagrams as shown in FIGS. 4 and 5 having the same characteristics as those of the above-described embodiment will be described.

〔第1具体例〕 第4図に示すように、冷房時、圧縮機周波数F=80Hzで
a=14,b=14であるから、n=14,M=1となる。また、
(11)式よりf=0.175となり、(1)式は(1a)式の
ようになる。
[First Specific Example] As shown in FIG. 4, when cooling, a = 14 and b = 14 at a compressor frequency F = 80 Hz, so n = 14 and M = 1. Also,
From equation (11), f = 0.175, and equation (1) becomes equation (1a).

b=−{(1/(0.175・F)}a2+0.175・F …(1a) 例えば、冷房時において、室内機Aの設定温度がTIa=2
7℃,実測室温がTRa=30℃であり、室内機Bの設定温度
がTIb=27℃,実測室温がTRb=32℃であったとすると、
室内機Aの負荷が(TRa−TIa)=3、室内機Bの負荷が
(TRb−TIB)=5となり、それぞれの負荷係数a,bは表
1より室内機Aがa=5、室内機Bがb=7となる。こ
の負荷係数a,bを(1a)式に代入すると、 となり、圧縮機周波数F=55Hzが得られる。
b = − {(1 / (0.175 · F)} a 2 + 0.175 · F (1a) For example, during cooling, the set temperature of the indoor unit A is TIa = 2.
7 ° C, the measured room temperature is TRa = 30 ° C, the set temperature of the indoor unit B is TIb = 27 ° C, and the measured room temperature is TRb = 32 ° C.
The load of the indoor unit A is (TRa-TIa) = 3, the load of the indoor unit B is (TRb-TIB) = 5, and the respective load coefficients a and b are shown in Table 1 as a = 5 for the indoor unit A and the indoor unit. B becomes b = 7. Substituting these load factors a and b into equation (1a), And the compressor frequency F = 55 Hz is obtained.

一方、各電動膨張弁6a,6bの開閉度Va,Vbは、Vb/Va=7/5
の割合で決定する。
On the other hand, the opening / closing degrees V a and V b of the electric expansion valves 6a and 6b are V b / V a = 7/5
It is decided by the ratio of.

〔第2具体例〕 第5図に示すように、暖房時、圧縮機周波数F=80Hzで
a=14,b=14であるから、n=14,M=1となる。また、
(11)式よりf=0.175となり、(2)式は(2a)式の
ようになる。
[Second Specific Example] As shown in FIG. 5, since a = 14 and b = 14 at the compressor frequency F = 80 Hz during heating, n = 14 and M = 1. Also,
From equation (11), f = 0.175, and equation (2) becomes equation (2a).

b=−a+0.175・F …(2a) 例えば、暖房時において、室内機Aの設定温度がTIa=2
1℃,実測室温がTRa=18℃であり、室内機Bの設定温度
がTIb=21℃,実測室温がTRb=16℃であったとすると、
室内機Aの負荷が(TRa−TIa)=3、室内機Bの負荷が
(TRb−TIb)=5となり、それぞれの負荷係数a,bは表
1より室内機Aがa=5、室内機Bがb=7となる。こ
の負荷係数a,bを(2a)式に代入すると、 7=−5+0.175・F 12=0.175・F F≒69 となり、圧縮機周波数F=69Hzが得られる。
b = −a + 0.175 · F (2a) For example, during heating, the set temperature of the indoor unit A is TIa = 2
Assuming that the measured temperature is 1 ° C, the measured room temperature is TRa = 18 ° C, the set temperature of the indoor unit B is TIb = 21 ° C, and the measured room temperature is TRb = 16 ° C.
The load of the indoor unit A is (TRa-TIa) = 3, the load of the indoor unit B is (TRb-TIb) = 5, and the respective load coefficients a and b are shown in Table 1 for the indoor unit A as a = 5, the indoor unit B becomes b = 7. By substituting the load coefficients a and b into the equation (2a), 7 = -5 + 0.175 · F 12 = 0.175 · F F ≈69, and the compressor frequency F = 69 Hz is obtained.

一方、各電動膨張弁6a,6bが開閉度Va,Vbは、Vb/Va=7/5
の割合で決定する。
On the other hand, the opening / closing degrees V a and V b of the electric expansion valves 6a and 6b are V b / V a = 7/5
It is decided by the ratio of.

(発明の効果) 以上述べたように、本発明によれば、圧縮機周波数の決
定に、室内機の負荷係数に応じた数式を用いることによ
り、マイコンプログラム内にメモリーマップ等を必要と
することなく、負荷係数に応じた圧縮機周波数をきめ細
かく設定できる。また、異能力室内機と接続が数式の変
数を変えるだけで容易に行え、快適な冷暖房を行うこと
ができる。
(Effects of the Invention) As described above, according to the present invention, a memory map or the like is required in a microcomputer program by using a mathematical formula according to the load coefficient of the indoor unit in determining the compressor frequency. Instead, the compressor frequency can be finely set according to the load coefficient. In addition, connection with the indoor unit of different capacity can be easily performed by changing the variables of the mathematical expression, and comfortable cooling and heating can be performed.

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

第1図ないし第5図は本発明の図面を示し、第1図は二
室冷暖房装置の全体構成の概略を示す図、第2図はマイ
コン制御部の概略ブロック図、第3図は数式化した室内
機Aの負荷係数aと室内機Bの負荷係数bとの関係を示
す曲線図、第4図は第6図を基にして数式化した室内機
Aの負荷係数aと室内機Bの負荷係数bと圧縮機周波数
Fとの関係を示す曲線図、第5図は第8図を基にして数
式化した室内機Aの負荷係数aと室内機Bの負荷係数b
と圧縮機周波数Fとの関係を示す曲線図、第6図は従来
の制御で用いた冷房運転時の圧縮機の周波数における各
室内機への冷媒流量の理想値及びそれに対応する各室の
膨張弁開閉度の関係を示す曲線図、第7図は第6図を基
にして作成された各室内機の膨張弁開閉度及びそれに対
応する負荷係数の関係を示す曲線図、第8図は従来の制
御で用いた冷房運転時の圧縮機の周波数における各室内
機への冷媒流量の理想値及びそれに対応する各室の膨張
弁開閉度の関係を示す曲線図、第9図は第8図を基にし
て作成された各室内機の膨張弁開閉度及びそれに対応す
る負荷係数の関係を示す曲線図である。 1……圧縮機 3……室外熱交換器 4a,4b……レシーバータンク 5……暖房用膨張弁 6……電動膨張弁 7,8……室内熱交換器 9……圧縮機吸込パイプ表面温度センサ 11a,11b……室内温度センサ 12a,12b……室内温度設定器 13……マイコン制御部 14……圧縮機周波数制御部 15……膨張弁開閉制御部 16a,16b……膨張弁出口パイプ表面温度センサ
1 to 5 show the drawings of the present invention, FIG. 1 is a diagram showing the outline of the overall configuration of a two-room cooling and heating apparatus, FIG. 2 is a schematic block diagram of a microcomputer control unit, and FIG. FIG. 4 is a curve diagram showing the relationship between the load coefficient a of the indoor unit A and the load coefficient b of the indoor unit B, and FIG. 4 is a mathematical expression based on FIG. FIG. 5 is a curve diagram showing the relationship between the load coefficient b and the compressor frequency F, and FIG. 5 is a load coefficient a of the indoor unit A and a load coefficient b of the indoor unit B that are mathematically expressed based on FIG.
FIG. 6 is a curve diagram showing the relationship between the compressor frequency F and the compressor frequency F, and FIG. 6 is an ideal value of the refrigerant flow rate to each indoor unit at the frequency of the compressor during the cooling operation used in the conventional control and the expansion of each chamber corresponding thereto. FIG. 7 is a curve diagram showing the relationship between the valve opening / closing degrees, FIG. 7 is a curve view showing the relationship between the expansion valve opening / closing degree of each indoor unit created based on FIG. 6 and the corresponding load coefficient, and FIG. FIG. 9 is a curve diagram showing the relationship between the ideal value of the refrigerant flow rate to each indoor unit at the frequency of the compressor during the cooling operation used in the control of FIG. It is a curve figure which shows the relationship of the expansion valve opening / closing degree of each indoor unit produced based on it, and the load coefficient corresponding to it. 1 …… Compressor 3 …… Outdoor heat exchanger 4a, 4b …… Receiver tank 5 …… Heating expansion valve 6 …… Electric expansion valve 7,8 …… Indoor heat exchanger 9 …… Compressor suction pipe surface temperature Sensor 11a, 11b …… Indoor temperature sensor 12a, 12b …… Indoor temperature setter 13 …… Microcomputer control unit 14 …… Compressor frequency control unit 15 …… Expansion valve opening / closing control unit 16a, 16b …… Expansion valve outlet pipe surface Temperature sensor

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】1台の室外機に2台の室内機が各々電動膨
張弁を介して接続され、周波数可変型の圧縮機により圧
縮された冷媒を各室内熱交換器もしくは室外熱交換器で
凝縮させ、さらに上記冷媒を各電動膨張弁で膨張、減圧
させた後、上記室外熱交換器もしくは各室内熱交換器で
蒸発させて各室内の暖房もしくは冷房を行うようにした
冷暖房装置において、 上記圧縮機の周波数Fは、各室内機に設置された室温設
定器の設定温度と実際の室内温度との差から得られる各
室内負荷に基づく負荷係数をa,bとし、負荷係数bの室
内機容量に対する負荷係数aの室内機容量の比をMとし
て、冷房運転時には(1)式から、暖房運転時には
(2)式から算出されるとともに、 b=−{M2/(f・F)}a2+f・F …(1) b=−M・a+f・F …(2) ただし、fは比例定数 上記各電動膨張弁の開閉度の比Vb/Vaは、上記各負荷係
数a,bの比b/aによって決定されることを特徴とする二室
冷暖房装置。
1. An outdoor unit is connected to two outdoor units via electric expansion valves, and a refrigerant compressed by a frequency variable compressor is used in each indoor heat exchanger or outdoor heat exchanger. In a cooling and heating device configured to condense, further expand and depressurize the refrigerant by each electric expansion valve, and then evaporate by the outdoor heat exchanger or each indoor heat exchanger to heat or cool each room, The frequency F of the compressor is a load coefficient based on each indoor load obtained from the difference between the set temperature of the room temperature setting device installed in each indoor unit and the actual indoor temperature, and the indoor unit of the load coefficient b Letting M be the ratio of the indoor unit capacity of the load coefficient a to the capacity, it is calculated from equation (1) during cooling operation and from equation (2) during heating operation, and b = − {M 2 / (f · F)} a 2 + f · F ... ( 1) b = -M · a + f · F ... ( ) Where, f is the ratio V b / V a of the opening and closing of the proportionality constant above the electric expansion valve, each load coefficients a, b of the ratio b / a two-chamber air conditioner characterized in that it is determined by.
JP1091064A 1988-06-17 1989-04-10 Two room air conditioner Expired - Fee Related JPH0776643B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP1091064A JPH0776643B2 (en) 1989-04-10 1989-04-10 Two room air conditioner
US07/367,141 US4926653A (en) 1988-06-17 1989-06-16 Multi-room type air-conditioning equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1091064A JPH0776643B2 (en) 1989-04-10 1989-04-10 Two room air conditioner

Publications (2)

Publication Number Publication Date
JPH02272250A JPH02272250A (en) 1990-11-07
JPH0776643B2 true JPH0776643B2 (en) 1995-08-16

Family

ID=14016074

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1091064A Expired - Fee Related JPH0776643B2 (en) 1988-06-17 1989-04-10 Two room air conditioner

Country Status (1)

Country Link
JP (1) JPH0776643B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104110774B (en) * 2013-08-27 2016-12-28 广东美的制冷设备有限公司 A kind of operation of air conditioner control method and device

Also Published As

Publication number Publication date
JPH02272250A (en) 1990-11-07

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