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CHAPTER 12
HEAT PUMPS, HEAT
RECOVERY, GAS COOLING,
AND COGENERATION SYSTEMS
12.1 BASICS OF HEAT PUMP AND HEAT
RECOVERY
12.1
Heat Pumps
12.1
Heat Pump Cycle
12.2
Classification of Heat Pumps
12.3
HVAC&R Heat Recovery Systems
12.3
Heat Balance and Building Load
Analysis
12.4
12.2 AIR-SOURCE HEAT PUMP
SYSTEMS
12.5
System Components
12.6
Suction Line Accumulator
12.8
Operating Modes
12.9
System Performance
12.9
Cycling Loss and Degradation Factor
12.11
Minimum Performance
12.12
Defrosting
12.12
Controls
12.13
Capacity and Selection
12.13
12.3 GROUNDWATER HEAT PUMP
SYSTEMS
12.13
Groundwater Systems
12.14
Groundwater Heat Pump System for a
Hospital
12.14
Groundwater Heat Pump Systems for
Residences
12.15
12.4 GROUND-COUPLED AND SURFACE
WATER HEAT PUMP SYSTEMS
12.17
12.5 AIR-TO-AIR HEAT RECOVERY
12.19
Types of Air-to-Air Heat Recovery
12.19
Effectiveness
12.19
Fixed-Plate Heat Exchangers
12.20
Runaround Coil Loops
12.21
Rotary Heat Exchangers
12.21
Heat Pipe Heat Exchangers
12.22
Comparison between Various Air-to-Air
Heat Exchangers
12.25
12.6 GAS COOLING AND
COGENERATION
12.25
Gas Cooling
12.25
Cogeneration
12.25
Gas-Engine Chiller
12.27
Gas Engines
12.27
Exhaust Gas Heat Recovery
12.28
Engine Jacket Heat Recovery
12.28
Cogeneration Using a Gas Turbine
12.29
REFERENCES
12.29
12.1 BASICS OF HEAT PUMP AND HEAT RECOVERY
Heat Pumps
A heat pump extracts heat from a heat source and rejects heat to air or water at a higher tempera-
ture. During summer, the heat extraction, or refrigeration effect, is the useful effect for cooling,
whereas in winter the rejected heat alone, or rejected heat plus the supplementary heating from a
heater, forms the useful effect for heating.
A heat pump is a packaged air conditioner or a packaged unit with a reversing valve or other
changeover setup. A heat pump has all the main components of an air conditioner or packaged unit:
fan, filters, compressor, evaporator, condenser, short capillary tube, and controls. The apparatus for
changing from cooling to heating or vice versa is often a reversing valve, in which the refrigerant
flow to the condenser is changed to the evaporator. Alternatively, air passage through the evaporator
may be changed over to passage through the condenser. A supplementary heater is often provided
when the heat pump capacity does not meet the required output during low outdoor temperatures.
12.1
12.2
CHAPTER TWELVE
A heat pump system consists of heat pumps and piping work; system components include heat
exchangers, heat source, heat sink, and controls to provide effective and energy-efficient heating
and cooling operations. HCFC-22, HFC-134a, and HFC-407C are the most widely used refrigerants
in new heat pumps. According to the data in the EIA’s Commercial Buildings Characteristics, for
the 57 billion ft
2
(5.3 m
2
) of air conditioned commercial building floor area in the United States in
1992, the use of heat pumps for heating and cooling was about 15 percent (by floor space).
Heat Pump Cycle
A heat pump cycle comprises the same processes and sequencing order as a refrigeration cycle ex-
cept that the refrigeration effect
q
1
4
or
q
rf
, and the heat pump effect
q
2
3
, both in Btu / lb (J / kg), are
the useful effects, as shown in Fig. 12.1. As defined in Eqs. (9.7) and (9.9), the coefficient of perfor-
mance of a refrigeration system COP
ref
is
COP
ref
h
1
h
4
W
q
1
4
W
in
(12.1)
where
h
4
,
h
1
enthalpy of refrigerant entering and leaving evaporator, respectively, Btu / lb (J / kg)
W
in
work input, Btu / lb (J / kg)
The coefficient of performance of the heating effect in a heat pump system COP
hp
is
COP
hp
q
2
3
W
in
(12.2)
and the useful heating effect
q
2
3
can be calculated as
q
2
3
h
2
h
3
h
1
h
4
h
2
h
1
(12.3)
FIGURE 12.1
Heat pump cycle: (
a
) schematic diagram; (
b
) cycle on
p
-
h
diagram.
HEAT PUMPS, HEAT RECOVERY, GAS COOLING, AND COGENERATION SYSTEMS
12.3
where
h
2
enthalpy of hot gas discharged from compressor, Btu / lb (J / kg)
h
3
enthalpy of subcooled liquid leaving condenser, Btu / lb (J / kg)
Here polytropic compression is a real and irreversible process. Both the subcooling of the liquid
refrigerant in the condenser and the superheating of the vapor refrigerant after the evaporator
increase the useful heating effect
q
2
3
. Excessive superheating, which must be avoided, leads to a
too-high hot-gas discharge temperature and to a lower refrigeration capacity in the evaporator.
Classification of Heat Pumps
According to the types of heat sources from which heat is absorbed by the refrigerant, currently
used heat pump systems can be mainly classified into two categories: air-source and water-source
heat pump systems. Water-source heat pumps can again be subdivided into water-source, ground-
water, ground-coupled, and surface water heat pump systems. Water-source heat pump systems are
discussed in Chap. 29.
Heat pump systems are often energy-efficient cooling / heating systems. Many new technologies
currently being developed, such as engine-driven heat pumps, may significantly increase the system
performance factor of the heat pump system. Ground-coupled heat pumps with direct-expansion
ground coils provide another opportunity to increase the COP of the heat pump system.
HVAC&R Heat Recovery Systems
An HVAC&R heat recovery system converts waste heat or cooling from any HVAC&R process to
useful heat or cooling. Here heat recovery is meant in a broad sense. It includes both waste heat and
cooling recovery. An HVAC&R heat recovery system includes the following:
The recovery of internal heat loads — such as heat energy from lights, occupants, appliances, and
equipment inside the buildings — by reclaiming the heat rejected at the condenser and absorber of
the refrigeration systems
The recovery of heat from the flue gas of the boiler
The recovery of heat from the exhaust gas and water jacket of the engine that drives the
HVAC&R equipment, especially engine-driven reciprocating vapor compression systems
The recovery of heat or cooling from the exhaust air from air conditioning systems
Although heat pump systems sometimes are used to recover waste heat and convert it into a
useful effect, a heat recovery system is different from a heat pump system in two ways:
In a heat pump system, there is only one useful effect at a time, such as the cooling effect in sum-
mer or the heating effect during winter. In a heat recovery system, both its cooling and heating
effects may be used simultaneously.
From Eq. (12.2), the coefficient of performance of the useful heating effect in a heat pump is
COP
hp
q
2
3
/
W
in
, whereas for a heat recovery system, the coefficient of performance COP
hr
is
always higher if both cooling and heating are simultaneously used and can be calculated as
COP
hr
q
1
4
q
2
3
W
in
(12.4)
A heat pump is an independent unit. It can operate on its own schedule, whereas a heat recovery
system in HVAC&R is usually subordinate to a refrigeration system or to some other system that
produces the waste heat or waste cooling.
12.4
CHAPTER TWELVE
Heating or cooling produced by a heat recovery system is a by-product. It depends on the opera-
tion of the primary system. A heat recovery system can use waste heat from condenser water for
winter heating only if the centrifugal chiller is operating.
A centrifugal chiller that extracts heat from a surface water source (e.g., a lake) through its evap-
orator and uses condensing heat for winter heating is a heat pump, not a heat recovery system. Heat
recovery systems that are subordinate to a centrifugal or absorption refrigeration system are dis-
cussed in Chaps. 13 and 14, respectively. Recovery of waste heat from industrial manufacturing
processes to provide heating shows great potential for saving energy. These heat recovery systems
must be closely related to the specific requirements of corresponding manufacturing processes and
are not discussed here.
Heat Balance and Building Load Analysis
The building load consists of transmission gain or loss, solar radiation, ventilation load and infil-
tration load, people, electric lights, appliances (or equipment), and heat gains from fans and
pumps. Building load is actually the load of the cooling or heating coil in an air-handling unit, or
DX coil in a packaged unit or air conditioner. On hot summer days, solar radiation and the latent
ventilation load must be included in the building load. However, both sunny and cloudy days may
occur in cold weather; therefore, building load is calculated and analyzed with and without solar
radiation in cold weather, especially for the control zones facing south in a building in northern
latitudes, or facing north in southern latitudes, where solar radiation is often a primary cooling
load on sunny days.
Figure 12.2 shows the building load analysis of a typical floor of a multistory building without
solar radiation in winter. In this figure, line
ABCDE
represents the building load curve at various
outdoor temperatures
T
o
, in °F (°C). Point
A
on this curve represents the summer design refrigera-
tion load
Q
rl
, in MBtu / h (kW). During summer design load, all the space cooling loads are offset
by the cold supply air, and the condensing heat of the refrigeration system is rejected to the cooling
tower.
When the outdoor temperature
T
o
drops below 75°F (23.9°C) on the left side of point
B
on the
building load curve, then the following things occur:
The perimeter zone may suffer a transmission loss.
Solar radiation is excluded.
The latent load of the outdoor ventilation air is no longer included in the building load because
the outdoor air is often drier than the space air.
T
F
, hot condenser water is supplied to the heating coils in the
perimeter zone to satisfy the heating load. Here
T
F
indicates the outdoor temperature at point
F
.
When the outdoor temperature drops to
T
D
, the heat recovered from the interior zone plus the
power input to the compressor is exactly equal to the heating load of the perimeter zone. No supple-
mentary heating is needed. Point
D
is called the break-even point of the building. When
T
o
T
D
,
supplementary heating is necessary to maintain a desirable space temperature.
As the outdoor temperature falls to
T
H
, the cooling coil load in the interior zone becomes
zero. The refrigeration compressors are turned off. No recovery of condensing heat is possible.
When
T
o
heating.
The area of triangle
FGH
indicates the heat energy recovered from the internal loads in the
interior zone, which is used to offset the heat losses in the perimeter zone by means of hot
condenser water. Similar building load curves with solar radiation for the entire building and for
the south-facing zones in the building should be calculated and analyzed in winter. For building
load with solar radiation, break-even point
D
will move to a lower
T
o
. Recovered heat will be
greater, and supplementary heating will be less. For south-facing zones in buildings in northern
T
H
, all the heat needed for the perimeter zone will be provided by the supplementary
If the outdoor temperature
T
o
HEAT PUMPS, HEAT RECOVERY, GAS COOLING, AND COGENERATION SYSTEMS
12.5
FIGURE 12.2
Building load analysis of a typical floor in a multistory building without solar radiation.
climates, cold supply air may be required during sunny days in the perimeter zone even in
winter.
12.2 AIR-SOURCE HEAT PUMP SYSTEMS
In an air-source heat pump system, outdoor air acts as a heat source from which heat is extracted
during heating, and as a heat sink to which heat is rejected during cooling. Since air is readily avail-
able everywhere, air-source heat pumps are the most widely used heat pumps in residential and
many commercial buildings. The cooling capacity of most air-source heat pumps is between 1 and
30 tons (3.5 and 105 kW).
Air-source heat pumps can be classified as individual room heat pumps and packaged heat
pumps. Individual room heat pumps serve only one room without ductwork. Packaged heat pumps
can be subdivided into rooftop heat pumps and split heat pumps.
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