The present invention relates to an air conditioner having a function to sense that refrigerant has an insufficient amount.
A conventionally known air conditioner has a function to sense that refrigerant has an insufficient amount. For example, Japanese Patent No. 5245576 (PTL1) discloses an air conditioner that determines whether an amount of refrigerant is appropriate within a range of environmental conditions under which a sensing error is maximally reduced. This air conditioner can reduce erroneous sensing of refrigerant in amount.
PTL1: Japanese Patent No. 5245576
In the air conditioner disclosed in Japanese Patent No. 5245576 (PTL 1), when a degree of subcooling of the refrigerant flowing out of a condenser is equal to or less than a reference value, it is determined that the refrigerant has an insufficient amount.
When the amount of refrigerant circulating through an air conditioner (an amount of refrigerant in circulation) has decreased and it becomes difficult to sufficiently cool the refrigerant by a condenser, the condenser discharges the refrigerant with a degree of subcooling smaller than 0, and an expansion valve receives the refrigerant in a gas-liquid two-phase state (or wet steam). Normally, the expansion valve has its degree of opening controlled on the assumption that the expansion valve receives refrigerant in the form of liquid (or liquid refrigerant). Therefore, when the expansion valve receives refrigerant in the form of wet steam, the air conditioner may be impaired in stability.
The present invention has been made to solve the above-described problem, and an object of the present invention is to improve an air conditioner in stability.
According to the present invention, an air conditioner circulates refrigerant. The air conditioner comprises: a compressor; a first heat exchanger; a first expansion valve; a second heat exchanger; and a controller. The controller changes a degree of opening of the first expansion valve by a first operation amount according to a temperature difference between a target temperature and the temperature of the refrigerant discharged by the compressor. The refrigerant circulates through the compressor, the first heat exchanger, the first expansion valve, and the second heat exchanger. A first ratio when a specific condition is satisfied is larger than a second ratio when the specific condition is not satisfied. The specific condition indicates that a degree of subcooling of the refrigerant flowing between the first heat exchanger and the first expansion valve is smaller than zero. The first and second ratios are each a ratio of the first operation amount to the temperature difference.
According to the present invention, an air conditioner can be improved in stability by making a first ratio when a specific condition indicating that refrigerant flowing between a first heat exchanger and a first expansion valve has a degree of subcooling smaller than zero is satisfied larger than a second ratio when the specific condition is not satisfied.
Hereinafter, embodiments of the present invention will specifically be described with reference to the drawings. In the figures, identical or corresponding components are identically denoted and will not be described redundantly in principle.
As shown in
In the cooling operation, the refrigerant circulates in the order of compressor 1, four-way valve 5, outdoor heat exchanger 2, first expansion valve 3 and indoor heat exchanger 4. Compressor 1 adiabatically compresses and discharges refrigerant in the form of gas (or gas refrigerant). The gas refrigerant discharged by compressor 1 is guided to outdoor heat exchanger 2 by four-way valve 5. Outdoor heat exchanger 2 functions as a condenser in the cooling operation. In outdoor heat exchanger 2, the refrigerant radiates heat of condensation to the surrounding external air to become a high-pressure liquid refrigerant. Outdoor heat exchanger 2 discharges the high-pressure liquid refrigerant, which in turn passes through first expansion valve 3, when the refrigerant is reduced in pressure and thus becomes low-pressure wet steam and flows into indoor heat exchanger 4. Indoor heat exchanger 4 functions as an evaporator in the cooling operation. In indoor heat exchanger 4, the refrigerant exchanges heat with indoor air blown by indoor fan 7. The refrigerant cools the indoor air by absorbing heat of evaporation from the indoor air and becomes a low-pressure gas refrigerant. Indoor heat exchanger 4 releases the gas refrigerant, which is in turn guided to compressor 1 by four-way valve 5.
Referring to
Controller 11 controls four-way valve 5 to switch a direction in which the refrigerant circulates. Controller 11 controls outdoor fan 6 and indoor fan 7 to blow air in an amount per unit time. Controller 11 controls a circulation flow rate Gr [kg/h] by changing a rotation speed Fz [rps] of compressor 1. When compressor 1 has a stroke volume Vst [cc] (i.e., an amount of refrigerant discharged by the compression mechanism of compressor 1 per rotation), sucks refrigerant having a density ρs [kg/m3], and has a volumetric efficiency ηv [dimensionless number] (i.e., a ratio of an amount of refrigerant discharged to the displacement of the compression mechanism of compressor 1) the circulation flow rate Gr is expressed by the following expression (1):
[expression 1]
Gr=V
st
·F
z·3600·10−6·ρs·ηv (1).
Controller 11 obtains a discharging temperature from a temperature sensor 8e. Controller 11 obtains from a temperature sensor 8a the temperature of the refrigerant moving through outdoor heat exchanger 2. Controller 11 obtains from a temperature sensor 8b the temperature of the refrigerant flowing between outdoor heat exchanger 2 and first expansion valve 3. Controller 11 obtains from a temperature sensor 8d the temperature of the refrigerant flowing between indoor heat exchanger 4 and first expansion valve 3. Controller 11 obtains from a temperature sensor 8c the temperature of the refrigerant moving through indoor heat exchanger 4. In the cooling operation, controller 11 uses each temperature obtained from temperature sensors 8a and 8b to calculate a degree of subcooling SC. In the heating operation, controller 11 uses each temperature obtained from sensors 8c and 8d to calculate a degree of subcooling SC.
Controller 11 uses each temperature obtained from temperature sensors 8a to 8e to control the degree of opening of first expansion valve 3 through feedback to bring a discharging temperature Td closer to a target discharging temperature Tdm. Temperature sensors 8a to 8e each include a thermistor for example.
Controller 11 detects a condensation temperature Tc [° C.] and an evaporation temperature Te [° C.] from the temperatures obtained from temperature sensors 8a and 8c. Controller 11 calculates the target discharging temperature Tdm [° C.] from the following expression (2) so as to maximize a COP (a coefficient of performance). In the expression (2), Pc [MPa] represents condensation pressure. Pe [MPa] represents evaporation pressure. Te [° C.] represents evaporation temperature. A1 represents a constant for ensuring a degree of superheating for the refrigerant sucked into compressor 1. Index n represents a polytropic index.
[expression 2]
Td
m=(Te+273.15+A1)·(Pc/Pe)(n−1)/n−273.15 (2).
The condensation pressure Pc and the evaporation pressure Pe can be calculated from the condensation temperature Tc and the evaporation temperature Te. For example, a value of 0 or more and 10 or less is used as the constant A1. For the polytropic index n, for example, a value of 1.2 or more and 1.4 or less is used with the efficiency of compressor 1 considered.
Whenever a sampling time arrives, controller 11 uses the expression (1) to calculate the target discharging temperature Tdm, and calculates a degree of opening LPt[Pulse] for first expansion valve 3 for the current time. When first expansion valve 3 immediately previously had a degree of opening represented as LPt−1 [Pulse] and a control constant is represented as Kp, the degree of opening LPt can be expressed by the following expression (3):
[expression 3]
LP
t
=LP
t−1
+K
p(Td−Td m) (3).
When an amount of operation (LPt−LPt−1) for a degree of opening LP is represented as ΔLPop and a temperature difference (Td−Tdm) is represented as ΔTa, the amount of operation ΔLPop is expressed by an expression (4):
[expression 4]
ΔLPop=Kp·ΔTa (4).
From the expression (4), the control constant Kp is expressed as a ratio of the amount of operation ΔLPop to the temperature difference ΔTa as indicated by an expression (5):
When the refrigerant flowing into first expansion valve 3 has a pressure P1 [MPa] and the refrigerant flowing out of first expansion valve 3 has a pressure P2 [MPa], and the refrigerant flowing into first expansion valve 3 has a density ρl [MPa] [kg/m3], air conditioner 100 is stabilized when the degree of opening LP, the circulation flow rate Gr, the pressures P1 and P2, and the density ρl have a relationship expressed by the following expression (6):
When the degree of opening LP is changed, the discharging temperature Td changes, and the state of the refrigerant sucked into compressor 1 also changes, and accordingly, the circulation flow rate Gr changes. When the discharging temperature Td has a variation ΔTd and first expansion valve 3 has a variation ΔLP in degree of opening, then, from the expression (6), variation ΔTd and variation ΔLP have a relationship represented by the following expression (7):
When refrigerant is circulated in an insufficient amount, first expansion valve 3 receives refrigerant in the form of wet steam, and accordingly, the density pl of the expression (6) decreases. Accordingly, in order to change the discharging temperature Td as in the case where refrigerant is circulated in a sufficient amount, the variation ΔLP in the degree of opening of first expansion valve 3 needs to be larger than when refrigerant is circulated in a sufficient amount.
When refrigerant is circulated in an insufficient amount, the discharging temperature Td starts to rise earlier than when the refrigerant is circulated in a sufficient amount, and accordingly, the temperature difference ΔTa between the discharging temperature Td and the target discharging temperature Tdm decreases earlier than when refrigerant is circulated in a sufficient amount. When the temperature difference ΔTa decreases, the amount of operation ΔLPop decreases according to the expression (4). As a result, the discharging temperature Td changes dully, and a time tm4 after the discharging temperature Td reaches the target discharging temperature Tdm before air conditioner 100 stabilizes is longer than a time tm2 shown in
Accordingly, in the first embodiment, whether refrigerant is circulated in an insufficient amount is determined based on the degree of subcooling SC of the refrigerant flowing into first expansion valve 3, and a control constant Kp2 applied when the degree of subcooling SC is not ensured is set to be larger than a control constant Kp1 applied when the degree of subcooling SC is ensured. By making the control constant Kp2 larger than Kp1, even when refrigerant is circulated in an insufficient amount, the amount of operation ΔLPop of the same extent as when the refrigerant is circulated in a sufficient amount can be ensured. As a result, a period of time before air conditioner 100 stabilizes can be reduced.
When the degree of subcooling SC is ensured and first expansion valve 3 receives refrigerant in the form of liquid, the refrigerant normally has a density ρl of about 860 to 1000 kg/m3. In contrast, when the degree of subcooling SC is not ensured and first expansion valve 3 receives refrigerant in the form of wet steam having a dryness of about 0.15, the refrigerant has a density ρl of about 300 kg/m3. A term in the expression (7) that includes the density ρl in the denominator varies about twice between when first expansion valve 3 receives refrigerant in the form of liquid (or when refrigerant is circulated in a sufficient amount) and when first expansion valve 3 receives refrigerant in the form of wet steam (or when refrigerant is circulated in an insufficient amount). When refrigerant is circulated in an insufficient amount, ensuring that the discharging temperature has a variation ΔTd of the same extent as when refrigerant is circulated in a sufficient amount requires first expansion valve 3 to have a degree of opening with a variation ΔLP about twice as large as when the refrigerant is circulated in a sufficient amount. By making the control constant Kp2 about twice as large as Kp1, the amount of operation ΔLPop can be approximately doubled. As a result, even when refrigerant is circulated in an insufficient amount, the variation ΔLP of the same extent as when refrigerant is circulated in a sufficient amount can be ensured.
The first embodiment does not require a configuration such as a receiver tank for reserving refrigerant in case that refrigerant is circulated in an insufficient amount. Further, it can also reduce an amount of refrigerant required for steadily operating the air conditioner. The air conditioner according to the embodiment can thus be manufactured at a reduced cost.
Controller 11 in S111 determines whether the degree of subcooling SC is 0 or less. When the degree of subcooling SC is 0 or less (YES in S111), controller 11 proceeds to S112 to set the control constant Kp to Kp2 and proceeds to S114. When the degree of subcooling SC is larger than 0 (NO in S111), controller 11 proceeds to S113 to set the control constant Kp to Kp1, and proceeds to S114.
In S114, controller 11 calculates a target discharging temperature Tdm, and proceeds to S115. In S115, controller 11 calculates a degree of opening LPt for the current time, and proceeds to S116. In S116, controller 11 substitutes the degree of opening LPt for the immediately previous degree of opening LPt−1 in preparation for the next sampling time, and ends the process.
Thus, the air conditioner according to the first embodiment can be enhanced in stability.
In the first embodiment has been described an example in which a degree of subcooling of refrigerant flowing into first expansion valve 3 is directly calculated. In a second embodiment will be described an example in which whether a degree of subcooling is ensured for the refrigerant flowing into the first expansion valve is estimated from the degree of opening of the first expansion valve.
As shown in
The reference degree of opening LPbase is a degree of opening of first expansion valve 3 that is required when it is assumed that the degree of subcooling is ensured for the refrigerant flowing into first expansion valve 3 (that is, the refrigerant is in the form of liquid). When the refrigerant flowing into first expansion valve 3 has density ρl_base [kg/m3] and pressure Ph_base [MPa], and the refrigerant released from first expansion valve 3 has pressure Pl_base [MPa], the reference degree of opening LPbase is represented by the following expression (8):
A constant A2 is a constant determined by a characteristic of first expansion valve 3. The density ρl_base is a numerical value of about 800 to 1000. The stroke volume Vst and the volumetric efficiency rev are values determined from the specification of compressor 1. The density ρs, the pressures P_base and the Pl_base are calculated from the temperatures obtained from temperature sensors 8a and 8c.
Thus, the air conditioner according to the second embodiment can be enhanced in stability.
In the first and second embodiments, a single-type air conditioner including one indoor unit has been described. An air conditioner according to an embodiment may be a multi-type air conditioner including a plurality of indoor units. In a multi-type air conditioner, liquid refrigerant stagnates in a plurality of indoor heat exchangers, and refrigerant is more likely circulated in an insufficient amount than in a single-type air conditioner. In a multi-type air conditioner, when refrigerant is circulated in an insufficient, it is more necessary to increase a control constant for the degree of opening of an expansion valve than in a single-type air conditioner. Accordingly, in a third embodiment, a multi-type air conditioner including two indoor units will be described.
As shown in
Controller 113 performs S120 to S115 to calculate a degree of opening LPt for the current time, as it does in the second embodiment, and subsequently, proceeds to S130. In S130, controller 113 sets the amount of operation ΔLPop multiplied by α as the amount of operation ΔLP1op and the amount of operation ΔLPop multiplied by β as the amount of operation ΔLP2op, and proceeds to S116. In S116, controller 113 substitutes the degree of opening LPt for the immediately previous degree of opening LPt−1, and ends the process.
The sum of α and β is 1. A ratio of the heat exchange capacity of indoor heat exchanger 43 to the heat exchange capacity of indoor heat exchanger 4 is α to β. As the heat exchange capacity, the heat exchanger's rated capacity [W/K] can be used for example.
S130 of
Thus, the air conditioner according to the third embodiment can be enhanced in stability.
The embodiments disclosed herein are also planned to be combined together as appropriate within a range without contradiction. It should be understood that the embodiments disclosed herein have been described for the purpose of illustration only and in a non-restrictive manner in any respect. The scope of the present invention is defined by the terms of the claims, rather than the description above, and is intended to include any modifications within the meaning and scope equivalent to the terms of the claims.
1 compressor, 2 outdoor heat exchanger, 3 first expansion valve, 4, 43 indoor heat exchanger, 5 four-way valve, 6 outdoor fan, 7, 73 indoor fan, 8a-8e temperature sensor, 9 outdoor unit, 10, 103 indoor unit, 11, 112, 113 controller, 33 second expansion valve, 100, 200, 300 air conditioner.
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/JP2017/041952 | 11/22/2017 | WO | 00 |