Technical Field
[0001] The invention relates to a system of an engine heat pump. Particularly, the invention
relates to a technology for reducing the total compression work of the engine heat
pump without increase of consumed electric power.
Background Art
[0002] There is a well-known conventional engine heat pump including a compressor driven
by an engine as disclosed in
Japanese Laid Open Gazette No. 2004-20153. A compression work of the engine heat pump is shared between a main compressor and
a sub compressor. An evaporation pressure set for one compressor (the sub compressor)
is kept higher than that for the other compressor (the main compressor) so as to reduce
the compression work by the one compressor, thereby reducing the total compression
work of the engine heat pump.
The reference document discloses an electromotive compressor serving as the compressor
(sub compressor) subjected to the higher evaporation pressure. Namely, the engine
heat pump is provided with an additional device (i.e., the electromotive compressor)
requiring electric power. As a result, although the compression work is reduced, the
consumed electric power is increased so as to reduce the essential merit of the engine
heat pump, that is, reduction of consumed electric power.
Brief Summary of the Invention
Object of the Invention
[0003] An object of the invention is to provide an engine heat pump whose compression work
is reduced without increase of consumed electric power, thereby improving its driving
efficiency (energy efficiency).
Way for Attaining the Object
[0004] An engine heat pump according to the invention comprises: an engine; a main compressor
driven by the engine; a sub compressor delivering a refrigerant to be joined to a
refrigerant delivered from the main compressor; an indoor heat exchanger; an outdoor
heat exchanger; an expansion valve for the indoor heat exchanger; an expansion valve
for the outdoor heat exchanger; and a supercooling heat exchanger disposed on a liquid
refrigerant passage of a connection passage between the indoor heat exchanger and
the outdoor heat exchanger. In the supercooling heat exchanger, a supercooling liquid
refrigerant branched into a branching passage supercools a liquid refrigerant before
being branched. The sub compressor is driven by the engine so as to compress the supercooling
liquid refrigerant. A ratio of a capacity of the sub compressor to a total capacity
of the main compressor and the sub compressor ranges between 20% and 29%.
In the engine heat pump according to the invention, an engine exhaust heat recovery
unit is disposed in parallel to the outdoor heat exchanger. The supercooling liquid
refrigerant is evaporated by the engine exhaust heat recovery unit and compressed
by the sub compressor.
Effect of the Invention
[0005] In the engine heat pump of the invention, the sub compressor is driven by the engine
so as to compress the supercooling refrigerant subjected to a higher evaporation pressure
(refrigerant suction pressure) than the evaporation pressure of refrigerant compressed
by the main compressor. Therefore, the engine heat pump requires no additional electric
power required for an electromotive sub compressor, so that the total compression
work in a refrigeration cycle is reduced while ensuring or improving the cooling capacity
by the supercooling performance of the supercooling heat exchanger.
[0006] Further, a capacity ratio of the sub compressor relative to a total capacity of the
main compressor and the sub compressor the sub compressor is set within a certain
range. Therefore, while the cooling efficiency for the cooling operation is ensured
or improved, the capacity of the supercooling heat exchanger for the heating operation
is ensured. That is, in the present invention, since the common engine drives the
main compressor and the sub compressor, sufficient driving efficiency (energy efficiency)
is ensured whether the engine heat pump is operated for cooling or for heating.
In the engine heat pump of the invention, since a capacity ratio of the sub compressor
to a total capacity of the main compressor and the sub compressor the sub compressor
is set within a certain range, while the total compression work for the cooling operation
is reduced, the total compression work for the heating operation is also reduced because
it requires no additional electric power.
[0007] When the engine heat pump is operated for heating, the liquid refrigerant is supercooled
so as to improve the capacity of refrigerant per unit mass and unit flow rate for
absorbing heat from an outdoor air, thereby reducing the total amount of refrigerant
flowing in the refrigeration cycle. As a result, the total compression work is reduced
so as to improve the driving efficiency (energy efficiency) of the engine heat pump.
Brief Description of the Drawings
[0008]
Fig. 1 is a diagram of a refrigerant circuit of an engine heat pump according to the
invention.
Fig. 2 is a block diagram of control units for the refrigerant circuit of the engine
heat pump.
Fig. 3 is a Moliere chart due to the refrigerant circuit.
Fig. 4 is a graph of COP relative to the capacity share of a sub compressor.
Fig. 4 is a graph of temperature of refrigerant in a supercooling exchanger relative
to the capacity share of a sub compressor.
Description of Notations
[0009]
- 2
- Main Compressor
- 3
- Sub compressor
- 4
- Engine
- 5
- Outdoor Heat Exchanger
- 6
- Engine Exhaust Heat Recovery Unit
- 8
- Indoor Heat Exchanger
- 15
- Supercooling Heat Exchanger
- 21
- Expansion Valve for Outdoor Heat Exchanger
- 22
- Expansion Valve for Supercooling Heat Exchanger
- 23
- Expansion Valve for Indoor Heat Exchanger
- 26
- Main Passage
- 27a
- Divisional Passage
- 27b
- Divisional Passage
Best Mode for Carrying out the Invention
[0010] A refrigerant circuit system and a refrigeration cycle of an engine heat pump according
to the invention will be described with reference to Figs. 1.
[0011] The engine heat pump of the invention comprises: an engine 4; a main compressor 2
driven by engine 4; a sub compressor 3 driven by engine 4; an indoor heat exchanger
8; an outdoor heat exchanger 5; an expansion valve 23 for the indoor heat exchanger
8; an expansion valve 21 for the outdoor heat exchanger; and a supercooling heat exchanger
15.
[0012] Supercooling heat exchanger 15 is disposed on a main passage 26 serving as a liquid
refrigerant passage of a connection passage between indoor heat exchanger 8 and outdoor
heat exchanger 5, so that, in supercooling heat exchanger 15, a supercooling liquid
refrigerant branched into a branching passage 27 (including passages 27a and 27b)
supercools a liquid refrigerant before being branched. The engine heat pump uses a
refrigeration cycle caused by these components. Supercooling heat exchanger 15 includes
connection points 15a and 15b to be connected to main passage 26, and connection points
15c and 15d to be connected to branching passage 27. A plurality of indoor heat exchangers
8 may be provided to the engine heat pump.
Main compressor 2, driven by engine 4, absorbs and compresses a vapor refrigerant
separated from a liquid refrigerant by an accumulator (not shown), and delivers vapor
refrigerant having a high temperature and a high pressure. A four-way valve 24 introduces
the vapor refrigerant delivered from main compressor 2 into a predetermined direction.
Four-way valve 24 also receives a vapor refrigerant to be supplied to main compressor
2. Therefore, a passage 32, serving as a suction line of main compressor 2, is interposed
between a refrigerant inlet of main compressor 2 and four-way valve 24, so as to introduce
the vapor refrigerant from four-way valve 24 into main compressor 2.
[0013] A supercooling liquid refrigerant is separated into branching passage 27 and passed
through supercooling heat exchanger 15. An accumulator (not shown) separates a vapor
refrigerant from the supercooling liquid refrigerant passed through supercooling heat
exchanger 15. Sub compressor 3, driven by engine 4, absorbs and compresses the vapor
refrigerant separated from the supercooling liquid refrigerant, and delivers a vapor
refrigerant having a high temperature and a high pressure.
An expansion valve 22 for the supercooling heat exchanger is provided on branching
passage 27, so as to cool a refrigerant as the supercooling liquid refrigerant supplied
to supercooling heat exchanger 15 for supercooling the liquid refrigerant before being
branched. Sub compressor 3 absorbs the supercooling liquid refrigerant whose heat
has been exchanged by supercooling heat exchanger 15. Therefore, a passage 33, serving
as a suction line of sub compressor 3, is interposed between supercooling heat exchanger
15 and a refrigerant inlet of sub compressor 3.
Branching passage 27 connected to main passage 26 includes branching passage 27a between
indoor heat exchanger 8 and supercooling heat exchanger 15. Branching passage 27 also
includes branching passage 27b between outdoor heat exchanger 5 and supercooling heat
exchanger 15. An on-off valve 28a is interposed between branching passage 27a and
expansion valve 22, and an on-off valve 28b is interposed between branching passage
27b and expansion valve 22. During either a cooling cycle or a heating cycle, on-off
valves 28a and 28b are selectively switched on or off for supercooling the liquid
refrigerant in main passage 26 before being branched
The refrigerant delivered from sub compressor 3 is joined to the refrigerant delivered
from main compressor 2 at a confluence point 65 before four-way valve 24. Four-way
valve 24 changes the flow direction of the joined refrigerant from confluence point
65, so as to perform either the cooling cycle or the heating cycle. An oil separator
(not shown) is interposed between confluence point 65 and four-way valve 24. The oil
separator separates a refrigerator oil from the high-temperature and high-pressurized
vapor refrigerant, and returns the refrigerator oil to suction sides of main compressor
2 and sub compressor 3, so as to smoothly lubricate compressors 2 and 3.
The above construction makes a refrigeration cycle, which is switched between the
cooling cycle and the heating cycle depending on the change of the flow direction
of refrigerant by four-way valve 24.
[0014] In the cooling cycle, the respective refrigerants compressed by main compressor 2
and sub compressor 3 join each other at confluence point 65, and the joined refrigerant
is sent to outdoor heat exchanger 5 through four-way valve 24. The refrigerant is
radiated and condensed by outdoor heat exchanger 5, and sent to supercooling heat
exchanger 15. The refrigerant flows into supercooling heat exchanger 15 through connection
point 15b, and flows out from supercooling heat exchanger 15 through connection point
15a. The liquid refrigerant supercooled by supercooling heat exchanger 15 is expanded
by expansion valve 23, and evaporated by the endothermic action of indoor heat exchanger
8. The vapor refrigerant is supplied to main compressor 2 through four-way valve 24,
and compressed by main compressor 2 to be delivered again.
A part of the liquid refrigerant flowing from outdoor heat exchanger 5 through main
passage 26 is branched into branching passage 27a so as to serve as the supercooling
liquid refrigerant. The branched refrigerant is expanded and cooled by expansion valve
22 so as to be changed into a wet low-temperature refrigerant. The wet low-temperature
refrigerant flows into supercooling heat exchanger 15 through connection point 15c,
supercools the refrigerant flowing in main passage 26, and flows out from supercooling
heat exchanger 15 through connection point 15d. In this cycle, on-off valve 28a is
opened and on-off valve 28b is closed, so that the refrigerant flowing in main passage
26 is not branched into branching passage 27b, but into branching passage 27a. The
supercooling refrigerant branched into branching passage 27a supercools the undivided
liquid refrigerant before being branched.
[0015] In this way, the liquid refrigerant flowing through main passage 26 is supercooled
so as to improve the efficiency of the refrigeration cycle. The supercooling liquid
refrigerant is supplied to sub compressor 3 so as to be compressed and delivered again.
On the other hand, in the heating cycle, the respective refrigerants compressed by
main compressor 2 and sub compressor 3 join each other at confluence point 65, and
the joined refrigerant is sent to indoor heat exchanger 8 through four-way valve 24.
The refrigerant is radiated and condensed (liquefied) by indoor heat exchanger 8,
and sent to supercooling heat exchanger 15. The refrigerant flows into supercooling
heat exchanger 15 through connection point 15a, and flows out from supercooling heat
exchanger 15 through connection point 15b. The liquid refrigerant supercooled by supercooling
heat exchanger 15 is expanded by expansion valve 21, and evaporated by the endothermic
action of outdoor heat exchanger 5. The vapor refrigerant is supplied to main compressor
2 through four-way valve 24, and compressed by main compressor 2 to be delivered again.
A part of the liquid refrigerant flowing from indoor heat exchanger 8 through main
passage 26 is branched into branching passage 27b so as to serve as the supercooling
liquid refrigerant. The branched refrigerant is expanded and cooled by expansion valve
22 so as to be changed into a wet low-temperature refrigerant. The wet low-temperature
refrigerant flows into supercooling heat exchanger 15 through connection point 15c,
supercools the refrigerant flowing in main passage 26, and flows out from super cooling
heat exchanger 15 through connection point 15d. In this cycle, on-off valve 28a is
closed and on-off valve 28b is opened, so that the refrigerant flowing in main passage
26 is not branched into branching passage 27a, but into branching passage 27b. The
supercooling refrigerant branched into branching passage 27b supercools the undivided
liquid refrigerant before being branched.
[0016] The liquid refrigerant flowing out from supercooling heat exchanger 15 is radiated
and evaporated by engine exhaust heat recovery unit 6, and supplied to sub compressor
3 so as to be compressed and delivered again.
A system for controlling the engine heat pump of the present invention will be described
with reference to Fig. 2.
[0017] A controller 25 serves as a control unit provided in the engine heat pump of the
present invention. Controller 25 is connected to expansion valve 21 for the outdoor
heat exchanger, expansion valve 22 for the supercooling heat exchanger, and expansion
valve 23 for the indoor heat exchanger, so as to control the respective expansion
valves.
Controller 25 is also connected to on-off valves 28a and 28b provided on respective
branching passages 27a and 27b. On-off valves 28a and 28b are controlled as follows:
On-off valve 28a is opened for supercooling the liquid refrigerant in the cooling
cycle, and closed in the other cases. On-off valve 28b is opened for supercooling
the liquid refrigerant in the heating cycle, and closed in the other cases. Due to
such a control of on-off valves 28a and 28b, whether it is the cooling cycle or the
heating cycle, the liquid refrigerant is branched at the downstream side of supercooling
heat exchanger 15, and the undivided whole liquid refrigerant before being branched
is supercooled by supercooling heat exchanger 15.
[0018] Controller 25 is connected to engine 4 (or a control circuit of engine 4), so as
to control the on-off operation of engine 4 for driving main compressor 2 and sub
compressor 3.
In this system, controller 25 controls the opening of expansion valve 22 so that the
wet refrigerant expanded by expansion valve 22 is overheated in passage 33 serving
as the suction line of sub compressor 3. As discussed later, sub compressor 3 is selected
(or configured) so that the refrigerant suction pressure of sub compressor 3 becomes
higher than the refrigerant suction pressure of main compressor 2, that is, as shown
in the Moliere chart of Fig. 3, a compression work ΔWs by sub compressor 3 becomes
smaller than a compression work ΔWm by main compressor 2, thereby reducing the total
compression work of the engine heat pump in comparison with only the compression work
ΔWm for the whole refrigerant.
The Moliere chart of the refrigeration cycle due to the above refrigerant circuit
system will be described with reference to the flow of refrigerant in the refrigerant
circuit system. The Moliere chart indicates a change of condition of refrigerant having
a unit mass and a unit flow rate. The axis of abscissas indicates a specific enthalpy
(kJ/kg), which is an energy of 1kg refrigerant. The axis of ordinate indicates a (absolute)
pressure (MPa abs).
A cooling cycle regarding to the refrigeration cycle indicated as the Moliere chart
will be described.
[0019] A point Am on the Moliere chart defines a condition of the refrigerant flowing in
passage 32 serving as the suction line of main compressor 2. At point Am, the refrigerant
is set to have a specific enthalpy h2 (kJ/kg) and a pressure p2 (MPa abs), and have
a flow rate Gm. A point As on the Moliere chart defines a condition of the refrigerant
flowing in passage 33 serving as the suction line of sub compressor 3. At point As,
the refrigerant is set to have a specific enthalpy h1 (kJ/kg) and a pressure p1 (MPa
abs), and have a flow rate Gs.
[0020] The refrigerants set to have the above conditions at the respective points are supplied
to respective compressors 2 and 3, so as to be compressed. Main compressor 2 performs
compression work ΔWm relative to the refrigerant having the unit mass and the unit
flow rate (a compression process AmB). Sub compressor 3 performs compression work
ΔWs relative to the refrigerant having the unit mass and the unit flow rate (a compression
process AsB).
The high-pressurized refrigerants (vapor refrigerants) compressed by respective compressors
2 and 3 join each other at confluence point 65. At confluence point 65, the joined
refrigerant has a total flow rate Go (=Gm+Gs). The joined high-pressurized vapor refrigerant
is sent to outdoor heat exchanger 5 so as to be condensed and radiated, i.e., cooled,
thereby being changed into the liquid refrigerant (a condensation process BC). In
this regard, a point B defines a condition of the refrigerant flowing in the passage
from confluence point 65 to outdoor heat exchanger 5. At point B, the refrigerant
is set to have a specific enthalpy h0(kJ/kg).
The liquid refrigerant discharged from outdoor heat exchanger 5 is supercooled by
the supercooling liquid refrigerant which has been branched into branching passage
27a at the downward side of supercooling heat exchanger 15 (a supercooling process
CD). In this process, isothermal lines T1, T2 and T3 are set at respective constant
temperatures t1(°C), t2(°C) and t3(°C) (t1>t2>t3). The chart indicates that supercooling
heat exchanger 15 supercools the liquid refrigerant flowing in main passage 26 so
as to reduce the temperature of the liquid refrigerant flowing in main passage 26
from t1(°C) to t2(°C). The supercooled liquid refrigerant has a pressure p0 (MPa abs)
at a point D.
A part of the supercooled liquid refrigerant flowing in main passage 26 is branched,
and the remaining supercooled liquid refrigerant is expanded by expansion valve 23
for the indoor heat exchanger, so as to be changed into a liquid refrigerant whose
temperature and pressure are lower than those of an indoor air to be cooled (an expansion
process DEm). The low-temperature and low-pressurized liquid refrigerant is set to
have a pressure p2 (MPa abs) at a point Em. The liquid refrigerant having gotten pressure
p2 at point Em is sent to indoor heat exchanger 8, and indoor heat exchanger 8 absorbs
heat from the indoor air so as to evaporate the refrigerant (an evaporation process
EmAm). The evaporated refrigerant flows through passage 32 serving as the suction
line of main compressor 2 so as to be supplied to main compressor 2. Namely, in evaporation
process EmAm, pressure p2 of the refrigerant is equaled to a refrigerant suction pressure
Pm of main compressor 2, and the flow rate of refrigerant absorbed into main compressor
2 becomes Gm.
On the other hand, the supercooling liquid refrigerant branched into the branching
passage is expanded so as to have the pressure and temperature which are lower than
those of the liquid refrigerant at point C (an evaporation process DEs). In this process,
the temperature of the supercooling refrigerant is reduced from t2(°C) to t3(°C).
A part of this supercooled liquid refrigerant by supercooling heat exchanger 15 is
branched into branching passage 27a so as to serve as the supercooling liquid refrigerant.
The liquid refrigerant branched into branching passage 27a is set to have flow rate
Gs.
[0021] In this process, the evaporation scale of the branched liquid refrigerant by expansion
valve 22 (evaporation process DEs) is smaller than that of the liquid refrigerant
by expansion valve 23 (evaporation process Dem) because of the following reason. The
only requirement for supercooling the liquid refrigerant flowing in main passage 26
by the supercooling refrigerant branched into branching passage 27a is that the temperature
of the supercooling refrigerant is lower than the liquid refrigerant (having the condition
at point C) before being supplied to expansion valve 22. That is, the supercooling
effect is ensured even when the pressure drop of the refrigerant having the condition
at point D is such a small degree between pressure p0 and pressure p1.
In supercooling heat exchanger 15, the supercooling refrigerant having the condition
at point Es absorbs heat from the liquid refrigerant flowing in main passage 26, so
as to supercool the liquid refrigerant flowing in main passage 26 (an evaporation
process EsAs). The supercooling refrigerant, having finished supercooling, flows through
passage 33 serving as the suction line of sub compressor 3 so as to be supplied to
sub compressor 3.
[0022] In this regard, since a part of the liquid refrigerant flowing in main passage 26
is branched to have flow rate Gs, flow rate Gm of the liquid refrigerant supplied
to indoor heat exchanger 8 is smaller than flow rate Go of the whole refrigerant.
However, since supercooling heat exchanger 15 supercools the undivided refrigerant
before being branched, the endoergic capacity (cooling capacity) of the liquid refrigerant
per unit mass and unit flow rate (kJ/kg) is increased so as to ensure or improve the
cooling effect of outdoor heat exchanger 8.
In this way, the evaporation scale of expansion valve 22 for expanding the liquid
refrigerant having flow rate Gs branched into branching passage 27a is smaller than
that of expansion valve 23 for expanding the remaining liquid refrigerant having flow
rate Gm remaining after being branched, so as to ensure a small pressure drop of the
supercooling liquid refrigerant from pressure p0 to pressure p1, thereby ensuring
a high evaporation pressure p1 in evaporation process EsAs. Namely, the evaporation
pressure of the branched supercooling liquid refrigerant having flow rate Gs is higher
than the evaporation pressure of the remaining refrigerant having flow rate Gm after
being branched, thereby greatly reducing compression work ΔWs required for compression
process AsB in comparison with compression work ΔWm required for compression process
AmB. As a result, the compression work by sub compressor 3 is very small relative
to the compression work by main compressor 2, thereby reducing the total compression
work of the engine heat pump.
The reduction of the compression work will be detailed. The basis of comparison is
the total compression work of the engine heat pump with the whole refrigerant having
flow rate Go under only compression work ΔWm. In other words, this is a total compression
work in a refrigerant circuit with no sub compressor, i.e., with only a single compressor
performing compression work ΔWm for the whole refrigerant having flow rate Go. This
compression work is equal to the total compression work when the pressure drop of
the supercooling liquid refrigerant having flow rate Gs branched into branching passage
27a in evaporation process DEs is set between pressure p0 and p2.
[0023] When the whole refrigerant having flow rate Go is compressed by only compression
work ΔWm, the total compression work (the basis of comparison) is calculated according
to a formula 1.

[0024] Due to the above-mentioned small pressure drop of the supercooling liquid refrigerant
having flow rate Gs branched into branching passage 27a from pressure p0 to pressure
p1, the total compression work of the engine heat pump of the invention is calculated
according to a formula 2.

[0025] As a result, the reduction of compression work due to the small pressure drop of
the supercooling liquid refrigerant having flow rate Gs branched into branching passage
27a from pressure p0 to pressure p1, i.e., due to the high evaporation pressure of
the refrigerant having flow rate Gs is calculated according to a formula 3.

In this way, sub compressor 3 is driven by engine 4 so as to compress the supercooling
refrigerant subjected to evaporation pressure (pressure of refrigerant to be supplied
to the compressor) which is higher than that for the refrigerant compressed by main
compressor 2. Therefore, the engine heat pump requires no additional electric power
that is required for a conventional engine heat pump with an electromotive sub compressor.
Therefore, the total compression work in the refrigeration cycle is reduced while
ensuring or improving the cooling capacity due to the supercooling performance of
supercooling heat exchanger 15.
A capacity ratio between main compressor 2 and sub compressor 3 in the engine heat
pump of the invention will now be described.
[0026] The capacity ratio between main compressor 2 and sub compressor 3 is referred to
as a ratio between a delivery capacity of main compressor 2 and a delivery capacity
of sub compressor 3. The delivery capacity of each of compressors 2 and 3 is determined
based on its volumetric capacity and rotary speed. The volumetric capacity is a volume
of refrigerant supplied to each of compressors 2 and 3 per cycle of a rotor of corresponding
compressor 2 or 3 (cc/cycle). Since main compressor 2 and sub compressor 3 are driven
by common engine 4, the rotary speed of each of compressors 2 and 3 is determined
by a pulley ratio (speed ratio) of corresponding compressor 2 or 3 relative to a pulley
of engine 4.
[0027] Accordingly, the delivery capacity of each of compressors 2 and 3 is produced by
multiplying the volumetric capacity and the pulley ratio. When main compressor 2 has
a volumetric capacity Vm and a pulley ratio Um, and sub compressor 3 has a volumetric
capacity Vs and a pulley ratio Us, the delivery capacity of main compressor 2 is produced
by Vm*Um, and the delivery capacity of sub compressor 3 is produced by Vs*Us. As a
result, the capacity ratio of sub compressor 3 to the total capacity of main compressor
2 and sub compressor 3 (hereinafter, referred to as a sub compressor capacity ratio
R) is calculated by the following formula.

[0028] According to the formula, when volumetric capacities Vm and Vs of respective compressors
2 and 3 are equal to each other, sub compressor capacity ratio R is determined according
to pulley ratios Um and Us of respective compressors 2 and 3 to engine 4. When pulley
ratios Um and Us are equal to each other, sub compressor capacity ratio R is determined
according to volumetric capacities Vm and Vs. In the present invention, the delivery
capacity of sub compressor 3 is smaller than that of main compressor 2.
[0029] Sub compressor capacity ratio R(%) ranges between 20% and 29%. Description will be
given of this range of sub compressor capacity ratio R.
In the refrigerant circuit of the engine heat pump, variation of sub compressor capacity
ratio R is reflected in variation of the ratio of flow rate Gs of the supercooling
liquid refrigerant branched from main passage 26 into branching passage 27a (in the
cooling cycle) or 27b (in the heating cycle) to flow rate Go of the whole liquid refrigerant.
As sub compressor capacity ratio R increases, the ratio of flow rate Gs to flow rate
Go increases. As sub compressor capacity ratio R decreases, the ratio of flow rate
Gs to flow rate Go decreases.
[0030] The determination of range of sub compressor capacity ratio R between 20% and 29%
according to the invention will be described. The following description is based on
that the supercooling liquid refrigerant (having flow rate Gs) branched from main
passage 26 into branching passage 27a or 27b is referred to as "branched liquid refrigerant",
and the remaining liquid refrigerant (having flow rate Gm) flowing in main passage
26 after being branched is referred to as "main liquid refrigerant".
The reason why the upper limit of the range of sub compressor capacity ratio R is
29% will be described.
[0031] The upper limit 29% is determined based on variation of driving efficiency (energy
efficiency) in the cooling cycle (for cooling). In this regard, when the engine heat
pump is operated for cooling, as sub compressor capacity ratio R increases, flow rate
Gs of the branched liquid refrigerant increases, i.e., the amount of the supercooling
liquid refrigerant for supercooling the undivided liquid refrigerant having flow rate
Go flowing in main passage 26 increases so as to enhance the cooling capacity of the
main liquid refrigerant per unit mass and unit flow rate. However, as flow rate Gs
of branched liquid refrigerant increases, flow rate Gm of the main liquid refrigerant
decreases so as to reduce the cooling capacity of indoor heat exchanger 8. This phenomenon
defines the variation of driving efficiency (energy efficiency) for defining the upper
limit of sub compressor capacity ratio R.
The upper limit 29% of sub compressor capacity ratio R is determined based on measurement
data indicated as graphs of Fig. 4.
[0032] The graphs of Fig. 4 are defined by the axis of abscissas indicating sub compressor
capacity ratio R and the axis of ordinate indicating coefficient of performance (COP)
in the refrigeration cycle. COP is obtained by dividing the cooling or heating capacity
by the quantity of consumed fuel. As COP increases, the driving efficiency (energy
efficiency) is enhanced. A dotted graph indicates COP of a refrigerant circuit system
with no sub compressor, i.e., with only a single compressor.
[0033] As noticed from the graph, under the cooing operation, when sub compressor capacity
ratio R is close to 10%, COP is larger than COP with the single compressor, and is
almost kept constant while sub compressor capacity R increases. After increasing sub
compressor capacity ratio R passes a value close to 15%, COP decreases according to
increase of sub compressor capacity ratio R. When increasing sub compressor capacity
ratio R reaches approximate 30%, COP under the cooling operation becomes smaller than
COP by the single compressor. Namely, this value (approximate 30%) of sub compressor
capacity ratio R is a critical value (upper limit) for the engine heat pump of the
present invention to ensure the improvement of driving efficiency (COP) with the reduction
of the total compression work under the cooling operation. That is, when sub compression
capacity ratio R is smaller than approximate 30%, COP under the cooling operation
is kept larger than COP by the conventional system. This is the reason why the upper
limit of sub compressor capacity ratio R is set to 29% according to the present invention.
Incidentally, COP under the heating operation is constantly larger than COP by the
conventional system regardless of sub compression capacity ratio R.
The reason why the lower limit of the range of sub compressor capacity ratio R is
20% will be described.
[0034] During the heating operation, connection point 15a serves as a refrigerant inlet
for introducing the refrigerant from main passage 26 to supercooling heat exchanger
15, and connection point 15b serves as a refrigerant outlet for discharging the refrigerant
from supercooling heat exchanger 15 to main passage 26. The lower limit 20% of sub
compressor capacity ratio R is determined based on the relation of the refrigerant
temperature at connection point 15a (hereinafter referred to as "inlet temperature")
to the refrigerant temperature at connection point 15b (hereinafter referred to as
"outlet temperature") during the heating operation. In this regard, when the engine
heat pump is operated for heating, as sub compressor capacity ratio R decreases, flow
rate Gs of the branched liquid refrigerant branched into branching passage 27b decreases,
i.e., the amount of the supercooling liquid refrigerant for supercooling the undivided
liquid refrigerant having flow rate Go flowing in main passage 26 decreases so as
to reduce the supercooling effect of supercooling heat exchanger 15. Accordingly,
the branched liquid refrigerant tends to be easily evaporated. However, as flow rate
Gs of branched liquid refrigerant decreases, flow rate Gm of the main liquid refrigerant
increases so that the undivided liquid refrigerant having flow rate Go is insufficiently
supercooled by supercooling heat exchanger 15. That is, in supercooling heat exchanger
15, the outlet temperature rises while the inlet temperature is kept constant. This
outlet temperature rising relative to the inlet temperature in supercooling heat exchanger
15 is obstacle to the sufficient supercooling action of supercooling heat exchanger
15. Consequently, to ensure a satisfactory performance of supercooling heat exchanger
15 under the heating operation, sub compressor 3 has to be selected (or configured)
in its capacity for ensuring the enough supercooling degree, i.e., a difference of
the inlet temperature of the supercooling refrigerant from the outlet temperature
of the supercooling refrigerant after supercooling has to be not lower than a certain
level (e.g., 5°C). The lower limit of sub compression capacity range R is set so as
to ensure the enough supercooling degree.
The lower limit 20% of sub compressor capacity ratio R is determined based on measurement
data indicated as graphs of Fig. 5.
[0035] The graphs of Fig. 5 are defined by the axis of abscissas indicating sub compressor
capacity ratio R and the axis of ordinate indicating the inlet or outlet temperature
(°C) of supercooling heat exchanger 15 under the heating operation.
[0036] As noticed from the graph, the inlet temperature of supercooling heat exchanger 15
is substantially kept constant (32-33°C) regardless of sub compressor capacity ratio
R. On the other hand, as sub compressor capacity ratio R decreases, the outlet temperature
of supercooling heat exchanger 15 increases from a value lower than the inlet temperature
to a value higher than the inlet temperature. To ensure the sufficient performance
of supercooling heat exchanger 15, the relation between the inlet temperature and
the outlet temperature is preferably set so that the outlet temperature is lower than
the inlet temperature by a temperature difference that is not less than approximate
5°C. A critic value (lower limit) of sub compressor capacity ratio R for reducing
the outlet temperature lower than the inlet temperature by the difference that is
not less than approximate 5°C is 20%. This is the
reason why the lower limit of sub compressor capacity ratio R is set to 20% according
to the present invention.
As mentioned above, in the engine heat pump of the present invention, the upper limit
of sub compressor capacity ratio R is determined in due consideration of the cooling
operation, and the lower limit of sub compressor capacity ratio R is determined in
due consideration of the heating operation, so that sub compressor capacity ratio
R ranges between 20% and 29%, thereby ensuring or improving the cooling capacity during
the cooling operation, and thereby ensure the performance of supercooling heat exchanger
15 during the heating operation. As a result, whether the engine heat pump is operated
for cooling or heating, the engine heat pump according to the present invention ensures
a good driving efficiency (energy efficiency) because common engine 4 drives main
compressor 2 and sub compressor 3, and because sub compressor capacity range R ranges
between 20% and 29%.
Incidentally, in the refrigerant circuit of the engine heat pump of the present invention,
a continuously variable transmission (CVT) can be adapted to transmit power from engine
4 to main compressor 2 and sub compressor 3.
[0037] In this case, the CVT is set so as to change a speed ratio between main compressor
2 and sub compressor 3 in due consideration of the critic values of sub compressor
capacity ratio R in the respective cases of cooling operation and heating operation.
In the engine heat pump of the invention, during the cooling operation, any sub compressor
ratio R is allowed only if it does not exceed the upper limit, and during the heating
operation, any sup compressor ratio R is allowed only if it is not smaller than the
lower limit. Therefore, the CVT is configured so as to change the speed ratio due
to whether the engine heat pump is operated for cooling or heating, so that sub compressor
capacity ratio R under the cooling operation is less than approximate 30%, and sub
compressor capacity ratio R under the heating operation is not less than 20%.
[0038] Due to the CVT having this configuration, the freedom degree in setting volumetric
capacity Vs and pulley ratio Us relative to volumetric capacity Vm and pulley ratio
Um can be enhanced. Each of optimal values of sub compressor capacity ratio R for
each of the cooling cycle and heating cycle is easily determined so as to improve
the driving efficiency (energy efficiency) in either of the cooling cycle and the
heating cycle, because only the upper limit has to be determined for the cooling cycle,
and only the lower limit has to be determined for the heating cycle.
The engine heat pump of the invention is provided with engine exhaust recovery unit
6 in parallel to outdoor heat exchanger 5. The supercooling liquid refrigerant branched
from
main passage 26 is evaporated by engine exhaust heat recovery unit 6, and compressed
by sub compressor 3.
Engine exhaust heat recovery unit 6 is adapted to evaporate the endothermic branched
liquid refrigerant having passed through supercooling heat exchanger 15 under the
heating operation. In engine exhaust heat recovery unit 6, the branched liquid refrigerant
exchanges heat with engine cooling water CW having a higher temperature than the branched
liquid refrigerant, i.e., absorbs heat from engine cooling water CW so as to be evaporated.
The refrigeration cycle in the heating cycle represented in the Moliere chart (Fig.
3) will be described. Description of the same parts as the above-mentioned parts in
the cooling cycle will be omitted.
[0039] The high-pressurized vapor refrigerants having been compressed by respective compressors
2 and 3 join each other at confluence point 65, and the joined refrigerant is sent
to indoor heat exchanger 8. Indoor heat exchanger 8 condenses the high-pressurized
vapor refrigerant so as to radiate heat from the refrigerant into the indoor space,
whereby the refrigerant is cooled and liquefied (a condensation process BC). In this
regard, point B defines the condition of refrigerant on the way from confluence point
65 to indoor heat exchanger 8.
The liquid refrigerant discharged from indoor heat exchanger 8 is supercooled in supercooling
heat exchanger 15 by the supercooling refrigerant branched into branching passage
27b at the downstream side of supercooling heat exchanger 15 (a supercooling process
CD).
A part of the supercooled liquid refrigerant flowing in main passage 26 is branched,
and the remaining supercooled liquid refrigerant is expanded by expansion valve 21
so as to be changed into a low-temperature and low-pressurized liquid refrigerant
(an expansion process DEm). The liquid refrigerant having the condition at point Em
is sent to outdoor heat exchanger 5. In outdoor heat exchanger 5, the refrigerant
absorbs heat from an outdoor air so as to be evaporated (an evaporation process EmAm).
The vapor refrigerant flows in passage 32 serving as the suction line of main compressor
2 so as to be sucked to main compressor 2 again.
On the other hand, the supercooling liquid refrigerant branched into branching passage
27b is expanded by expansion valve 22 so as to have pressure and temperature lower
than the pressure and temperature of the refrigerant at point C (an expansion process
DEs). In this way, a part of the liquid refrigerant supercooled by supercooling heat
exchanger 15 is
branched into branching passage 27b so as to serve as the supercooling refrigerant
having flow rate Gs.
In supercooling heat exchanger 15, the supercooling liquid refrigerant having the
condition at point Es absorbs heat from the liquid refrigerant flowing in main passage
26 so as to supercool the liquid refrigerant flowing in main passage 26. The supercooling
liquid refrigerant having passed through supercooling heat exchanger 15 is sent to
engine exhaust heat recovery unit 6. In engine exhaust heat recovery unit 6, the supercooling
liquid refrigerant exchanges heat with engine cooling water CW, i.e., absorbs heat
from engine cooling water CW so as to be evaporated (an evaporation process EsAs).
The evaporated refrigerant flows in passage 33 serving as the suction line of sub
compressor 3 so as to be sucked into sub compressor 3 again.
In this way, in the engine heat pump under the cooling operation, the supercooling
is performed so as to improve the driving efficiency (energy efficiency) by the following
action.
[0040] The undivided liquid refrigerant having the total flow rate Go flowing in main passage
26 is supercooled by supercooling heat exchanger 15. The supercooled liquid refrigerant
increases its endothermic reaction capacity per unit mass and unit flow rate (kJ/kg).
Therefore, when the supercooled liquid refrigerant reaches outdoor heat exchanger
5, the supercooled liquid refrigerant has an increased capacity per unit mass and
unit flow rate for absorbing heat from the outdoor air. That is, the supercooled refrigerant
can absorb heat as much as that absorbed by a non-supercooled refrigerant even if
the supercooled refrigerant is less than the non-supercooled refrigerant. Therefore,
flow rate Gm of the main liquid refrigerant sent into outdoor heat exchanger 5 under
the heating operation can be reduced so as to reduce total flow rate Go of the refrigerant
circulating in the refrigeration cycle. As a result, the total compression work in
the refrigeration cycle can be reduced so as to improve the driving efficiency (energy
efficiency).
Since the branched supercooling liquid refrigerant is evaporated by engine exhaust
heat recovery unit 6 provided in parallel to outdoor heat exchanger 5 and is compressed
by sub compressor 3, the total compression work during the heating operation is reduced
without requiring additional consumption of electric power while the total compression
work during the heating operation is reduced due to the above-mentioned range of sub
compressor capacity ratio R.
[0041] Further, due to the supercooling of liquid refrigerant during the heating operation,
the capacity of the refrigerant for absorbing heat from the outdoor air per unit mass
and unit flow rate so as to reduce the quantity of whole refrigerant flowing in the
refrigeration cycle.
As a result, the total compression work is reduced so as to enhance the driving efficiency
(energy efficiency).
In the above-mentioned engine heat pump, main compressor 2 and sub compressor 3, which
are driven by engine 4, may be operable individually. Due to this configuration, one
or both of main compressor 2 and sub compressor 3 is/are selectively driven in correspondence
to the rate of air-conditioning load, thereby improving the driving efficiency (energy
efficiency).
In this case, as shown in Fig. 1, a main compressor clutch 42 is interposed between
main compressor 2 and engine 4 so as to selectively drivingly connect or disconnect
main compressor 2 to and from engine 4, and a sub compressor clutch 43 is interposed
between sub compressor 3 and engine 4, so as to selectively drivingly connect or disconnect
sub compressor 3 to and from engine 4.
[0042] Passage 33 serving as the suction line of sub compressor 3 to passage 32 serving
as the suction of main compressor 2 through a connection passage 34 with an on-off
valve 35. On-off valve 35 on connection passage 34 is opened to connect passages 32
and 33 to each other, and closed to separate passages 32 and 33 from each other, thereby
forming a refrigerant circuit in correspondence to each of a low air-conditioning
load rate, a middle air-conditioning load rate and a high air-conditioning load rate.
[0043] In this regard, as shown in Fig. 2, controller 25 is connected to main compressor
clutch 42 and sub compressor clutch 43 so as to control the engagement and disengagement
operation of each of clutches 42 and 43, and is connected to on-off valve 35 so as
to control the opening and closing operation of on-off valve 35.
Due to this configuration, an example of the control of clutches 42 and 43 and valve
35 corresponding to load during either of the cooling operation and the heating operation
is performed as follows. During the cooling operation, when the air-conditioning load
rate is low, only sub compressor 3 is driven. When the air-conditioning load rate
is middling, only main compressor 2 is driven. When the air-conditioning load rate
is high, both compressors 2 and 3 are driven and supercooling heat exchanger 15 performs
the supercooling operation. On the other hand, during the heating operation, when
the air-conditioning load rate is low, only sub compressor 3 is driven. When the air-conditioning
load rate is middling, only main compressor 2 is driven and engine exhaust heat recovery
unit 6 performs the heat exchange. When the air-conditioning load rate is high, both
compressors 2 and 3 are driven, supercooling heat exchanger 15 performs the supercooling
operation, and engine exhaust heat recovery unit 6 performs the heat exchange.
[0044] With respect to the magnitude of air-conditioning load rate, the low air-conditioning
load rate ranges between 0% and 15%, the middle air-conditioning load rate ranges
between 15% and 60%, and the high air-conditioning load rate ranges between 60% and
100%. The engine heat pump is controlled for cooing as follows:
[0045] When the air-conditioning load rate is low, only sub compressor 3 is driven. In this
case, controller 25 disengages main compressor clutch 42, and opens on-off valve 35.
Therefore, the driving power of engine 4 is transmitted to only sub compressor 3,
and passage 32 serving as the suction line of main compressor 2 is connected to passage
33 serving as the suction line of sub compressor 3, so that sub compressor 3 compresses
the whole refrigerant having flow rate Go. Supercooling heat exchanger 15 is exercised
or not depending on the control of opening and closing operation of expansion valve
22 for the supercooling heat exchanger. To exercise supercooling heat exchanger 15
for the supercooling, the pressure relation at a confluence point 64 (see Fig. 1)
is considered to reduce the pressure loss. Controller 25 controls the opening degrees
of respective expansion valves 22 and 23 so as to substantially equalize the pressure
of refrigerant from passage 33 to the pressure of refrigerant from passage 32.
When the air-conditioning load rate is middling, only main compressor 2 is driven.
In this case, controller 25 disengages sub compressor clutch 43, so as to transmit
the driving power of engine 4 to only main compressor 2, so that main compressor 2
compresses the whole refrigerant having flow rate Go. To exercise supercooling heat
exchanger 15 for the supercooling, controller 25 opens on-off valve 35 and controls
the opening degrees of respective expansion valves 22 and 23, so that, at a confluence
point 63 (see Fig. 1), the pressure of refrigerant from passage 33 is substantially
equal to the pressure of refrigerant from passage 32.
When the air-conditioning load rate is high, both main and sub compressors 2 and 3
are driven, and supercooling heat exchanger 15 is exercised for the supercooling.
In this case, controller 25 engages main compressor clutch 42 and sub compressor clutch
43, and closes on-off valve 35. Therefore, the driving power of engine 4 is transmitted
to main and sub compressors 2 and 3, and simultaneously, passages 32 and 33 are separated
from each other, so that main compressor 2 compresses the refrigerant having flow
rate Gm, and sub compressor 3 compresses the supercooling refrigerant having flow
rate Gs.
The engine heat pump is controlled for heating as follows:
[0046] When the air-conditioning load rate is low, only sub compressor 3 is driven. In this
case, the control pattern with controller 25 is similar to the control during the
cooling operation under the low air-conditioning load rate.
When the air-conditioning load rate is middling, only main compressor 2 is driven
and engine exhaust heat recovery unit 6 performs the heat exchange. In this case,
controller 25 disengages sub compressor clutch 43 to transmit the driving power of
engine 4 to only main compressor 2, and opens on-off valve 35 to exercise engine exhaust
heat recovery unit 6 for the heat exchange, so that main compressor 2 compresses the
whole refrigerant having flow rate Go joined at confluence point 63. Further, when
supercooling heat exchanger 15 is exercised for the supercooling, controller 25 opens
on-off valve 35 and controls the opening degrees of respective expansion valves 22
and 23, so that, at confluence point 63, the pressure of refrigerant from passage
33 is substantially equal to the pressure of refrigerant from passage 32.
When the air-conditioning load rate is high, both main and sub compressors 2 and 3
are driven, supercooling heat exchanger 15 is exercised for the supercooling, and
engine exhaust heat recovery unit 6 is exercised for the heat exchange. In this case,
controller 25 engages main compressor clutch 42 and sub compressor clutch 43, and
closes on-off valve 35. Therefore, the driving power of engine 4 is transmitted to
main and sub compressors 2 and 3, and simultaneously, passages 32 and 33 are separated
from each other, so that main compressor 2 compresses the refrigerant having flow
rate Gm, and sub compressor 3 compresses the supercooling refrigerant having flow
rate Gs under the heat exchanging by engine exhaust heat recovery unit 6.
In this way, one or both of main and sub compressors 2 and 3 is/are selectively driven
in correspondence to the rate of required air-conditioning load, so as to reduce a
load part of the engine heat pump where the fuel efficiency of engine 4 is reduced,
thereby improving the driving efficiency (energy efficiency) of the engine heat pump.
Industrial Applicability
[0047] The present invention is broadly applicable to various engine heat pumps each of
which has an engine and a compressor driven by the engine, so as to reduce the compression
work of the engine heat pump without increase of consumed electric power, thereby
improving the driving efficiency (energy efficiency).