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Refrigeration and air
conditioning
Dr. Najam Ul Hassan Shah
Lecture # 8
Vapor Absorption
Refrigeration Systems
(Chapter 17)
Part - 2
2
Basic Absorption Refrigeration Unit
• The Basic Absorption Cycle - The condenser, expansion
valve and the evaporator are similar as in a standard vapor-
compression cycle. The compression operation is now
provided by the assembly in the left-half of the diagram.
COP of Ideal Absorption Cycle
( )
( )
r
a
s
a
s
r
Gen
evep
T
T
T
T
T
T
Q
Q
COP
−
−
=
=
It can be noted from
above equation (and
Figure) :
As Ts increases → COP
increases
As Tr increases → COP
increases
As Ta increases → COP
decreases
Also see Ex. 17.1 and
equations 17.2 – 17.4
Ts
Tr
Ta
Absorption Refrigeration System
S.# Refrigerant Absorber Absorber
State
1 Ammonia Water Liquid
2 Ammonia Sodiumthiocynate Solid
3 Ammonia Lithium nitrate Solid
4 Ammonia Calcium chloride Solid
5 Water Lithium bromide Solid
6 Water Lithium chloride Solid
7 Methylene
chloride
Dimethyl ether or tetra
ethylene glycol
Liquid
Refrigerant-absorber pairs
Temperature-Pressure-Concentration Properties
Lithium Bromide (LiBr) Water Absorption Cycle
LiBr is a solid salt crystal. When exposing it to water vapor (in
absorber tank) it will absorb the water vapor and become a liquid
solution
• If two vessels were connected as shown in the figure,
one vessel containing LiBr-water solution and the other
pure water, each liquid would exert a water-vapor
pressure that is a function of the solution temperature
and the concentration of the solution.
Temperature-Pressure-Concentration Properties
Lithium Bromide (LiBr) Water Absorption Cycle
• At equilibrium the water-vapor pressure exerted by the two
liquids would be equal , reaching a T-P-C point state
having Tw = 40 C, Tsolution = 80 C and concentration of
solution 59% LiBr.
• Many such combinations Tw = f ( Tsolution , LiBr %, Pvapor) are
possible for a given solution and can be plotted on graphs;
like Fig 17.5 let see it
Temperature-Pressure-Concentration Properties
Temperature-pressure concentration diagram:
LiBr-water solutions
• Concentration is the abscissa of the graph and water-
vapor pressure could be considered as the ordinate on
the vertical scale on the right
• The saturation temperature of pure water corresponding
to these vapor pressures is shown as the ordinate on the
left
• The chart applies to saturated conditions where the
solution is in equilibrium with water vapor
Temperature-Pressure-Concentration Properties
Temperature-pressure concentration diagram:
LiBr-water solutions
• If the temperature of pure water is 40 °C, the vapor
pressure the liquid exerts is 7.38 kPa, which can be
determined from the opposite side of vertical scale.
• A LiBr solution with a concentration of 59 % &
temperature of 80°C also develops a water-vapor
pressure of 7.38 kPa
• If the solution had a concentration of 54% & temperature
of 70°C the water-vapor pressure would again be 7.38
kPa
Temperature-Pressure-Concentration Properties
Ex.2 :Temperature-Pressure-Concentration Properties
The pressure in vessel A is 4.24 kPa and it is 1.22 kPa in
vessel B. The surrounding temp is 30C. If the valve between
vessels is opened. Initially due to pressure difference water
vapor will flow from vessel A to vessel B, and this vapor will
be absorbed by the solution in vessel B
Ex.2 :Temperature-Pressure-Concentration Properties
If the concentration and
temperature of vessel B
are maintained constant
at 50 % and 30oC,
respectively. Then at
equilibrium, the pressure
in the entire system
(vessels A and B) will be
1.22 kPa (equilibrium
pressure of 50 % LiBr
solution at 30oC).
And temperature of water
in vessel A will lower to
the saturation
temperature
corresponding to 1.22
kPa, which is equal to
about 10C, as shown in
the figure
Ex.2 :Temperature-Pressure-Concentration Properties
Since the temperature of A is lower than surroundings, cooling
effect will be produces ; Qc
Now for the above process to continue, there should always be
pure water in vessel A, and vessel B must be maintained
always at 50 percent concentration and 30oC
Ex.2 :Temperature-Pressure-Concentration Properties
• In the example discussed the system is a closed system with finite
sized reservoirs
• Thus, gradually the amount of water in A decreases and the solution in
B becomes diluted with water. As a result, the system pressure and
temperature of water in A increase with time
• Hence the refrigeration effect at A reduces gradually due to the
reduced temperature difference between the surroundings and water.
Thus, refrigeration produced by systems using only two vessels is
intermittent in nature.
ME - 437 : Refrigeration & Air
Conditioning
Ex.2 :Temperature-Pressure-Concentration Properties
• In these systems, after a period, the refrigeration process
has to be stopped and both the vessels A and B have to be
brought back to their original condition. This requires
removal of water absorbed in B and adding it back to vessel
A in liquid form, i.e., a process of regeneration as shown in
Fig. below
Calculation of Mass Flow Rate and Enthalpy
Example 17.2 : Compute the rate flow of refrigerant (water) through the
condenser and evaporator in the cycle shown in Figure below if the pump
delivers 0.6 kg/s and the following temperatures prevail: generator, 100C;
condenser, 40C; evaporator. 10C; and absorber, 30C.
Calculation of Mass Flow Rates
• The mass flow rate abortion unit can be determined by
knowing the concentrations of the LiBr in the solution
• Two different pressures exist in the system: a high pressure
prevails in the generator and condenser, while the low
pressure prevails in the absorber and evaporator
• Knowing that the pressure in condenser & generator must
be same and at condenser inlet (station 3), saturated pure
water enters from generator at the condensing temperature
(40 C) gives us High Pressure of cycle. i.e
• At 40°C → (from fig 17,5 ) , Pgen = 7.38 kPa
• Similarly, evaporator an absorber pressure are same and at
evaporator operating at 10 C gives (Fig 17.5) the value of
low pressure;
• At 10°C → (from fig 17,5 ) , Pabs = 1.23 Kpa
Calculation of Mass Flow Rates
• At 40°C → (from fig 17,5 ) , Pgen = 7.38 kPa
• At 10°C → (from fig 17,5 ) , Pabs = 1.23 Kpa
• Knowing Low and high pressures, the concentration of LiBr
in absorber (Station1) and generator ( Station 2) can be
established from Fig 17.5 , see extract of Fig 17.5 below
X1 = 0.5 or 50%
X2 = 0.664 or
66.4%
Knowing and applying mass balance across generator
give us following two equations
Total mass flow balance :
LiBr Solution Mass flow :
Calculation of Mass Flow Rates
s
Kg
m /
148
.
0
3 =
•
s
kg
m /
6
.
0
1 =
•
6
.
0
1
3
2 =
=
+
•
•
•
m
m
m
2
2
1
1 x
m
x
m
•
•
=
s
kg
m /
452
.
0
2 =
•
( ) ( )
664
.
0
50
.
0
6
.
0 2
•
=m
Solving these two equations,
you get the values of mass
flow rates
Enthalpy of LiBr Solutions
• For thermal calculations on the absorption cycle, enthalpy
data must be available for the working substances at all
crucial positions in the cycle
• Water in liquid and vapor forms flows in and out of the
condenser & evaporator, so enthalpies at these points can
be determined from a table of properties of water
• In the generator and absorber, LiBr-water solutions exist for
which enthalpy is a function of both - solution temperature
and concentration
Absorption Refrigeration System
Calculation of Enthalpy, Q and COP
Ex. 17.3 : For absorption system of previous example, compute qg, qc, qa,
qe & COP.
SOLUTION:
Data from Previous Example:
m1 = 0.6 Kg/s, m2 = 0.452 Kg/s, m3 = m4 = m5 = 0.148 Kg/s,
X1 =0.5 and X2 =0.664
Enthalpy of Solution from Fig. 17.8
at 30 °C and x1 of 50% → h1 = -168 kJ/kg
At 100 °C and x2 of 66.4% → h2 = -52 kJ/kg
Enthalpy of water are found from Table A.1 as:
h3 = hvapor @ 100 C = 2676 KJ/Kg
h4 = hliquid @ 40 C = 167.5 KJ/Kg
h5 = hvapor @ 10 C = 2520 KJ/Kg
Absorption Refrigeration System
Absorption Refrigeration System
Calculation of Enthalpy, Q and COP
KW
h
m
h
m
h
m
Q
g 3
473
1
1
2
2
3
3 .
=
−
+
=
•
•
•
KW
h
m
h
m
Q
c 2
.
371
4
4
3
3 =
−
=
•
•
KW
h
m
h
m
h
m
Q
a 3
.
450
1
1
5
5
2
2 =
−
+
=
•
•
•
KW
h
m
h
m
Q
e 2
.
384
4
4
5
5 =
−
=
•
•
Ex. 17.3 : For absorption system of previous example, compute qg, qc, qa,
qe & COP.
736
.
0
6
.
476
2
.
348 =
=
=
g
e
Q
Q
COP
Now from Energy Balance, heat transfer rates are established as:
Absorption cycle with heat exchanger
Absorption cycle with heat exchanger
• By addition of heat exchanger, the COP increases
• The heat-exchanger transfers heat between the two streams
of solutions
• It heats the cool solution from the absorber on its way to the
generator and cools the solution returning from the generator
to the absorber
Example 17.4
A water-LiBr absorption refrigeration system is shown (see
figure). The temperature at point 2 is 52 °C. The mass flow rate
delivered by the solution pump is 0.6 kg/s. What are the rates of
energy transfer at each of the components and the COP of this
cycle? Also, what is the temperature at state 4?
Example 17.4
Example 17.4
Example 17.4
Example 17.4
The solution of Ex. Show that Qa reduces while Qg reduces
slightly and increases COP to 0.783 (from 0.736)
Example 17.4
• Crystallization occurs when the solution state is on right side of
crystallization line on P-T-C diagram
• Dropping into this region formation of a slash or solidification of
Solution, which can block the flow in a pipe and stop the operation of
absorption unit
• Crystallization must be avoiding by proper designing
• See Example 17.5
Crystallization
Example 17.5
In the system shown in Fig. 17-9, the ambient wet bulb
temperature decreases so that the temperature of the cooling
water drops, which also reduce the condensing temperature to 34
°C. All other temperatures specified on Fig. 17-9 remain
unchanged. Is there a danger of crystallization?
Example 17.5
Example 17.5
Example 17.5
Example 17.5
Example 17.5
Capacity Control ; It reduces the reduction to a desired level. Without
capacity control a given system yields maximum refrigeration. The
control can be achieved by following three methods :
▪ Reducing flow rate delivered by pump at Staion1
▪ Reducing generator Temperature
▪ Increasing the condensing Temperature
Capacity Control
Example 17.6
Example 17.6
Many Other Systems including combination with other cycles and
different combination of refrigerant and absorber. Few commonly
used systems are listed here:
Other Systems
▪ Double Effect Units
▪ Combined absorption
and vapor
compression system
▪ Aqua Ammonia
System
Double-effect units
Combined absorption and vapor compression system
Example 17.7
Example 17.7
Example 17.7
Aqua-Ammonia System
• In aqua-ammonia absorption system, water is used as an
absorbent while ammonia is used as a refrigerant
• Dissolution of NH3 into water is exothermic and inversely
proportional to temperature.
• The system consists of all the components i.e., generator,
absorber, condenser, evaporator, and heat exchanger----
plus a rectifier & analyzer.
• The work input to the pump is usually very small, and the
COP of absorption refrigeration systems is defined as
gen
L
in
p
gen
L
abs
Q
Q
W
Q
Q
input
Work
effect
Cooling
COP

+
=
=
,
Aqua-Ammonia System
Aqua-Ammonia System
Aqua-Ammonia System
• Additional components as refrigerant vapors released at
generator contains water vapor as well
• Normally aqua-ammonia system operate at evaporating
temperature below 0 °C
• If large amounts of water vapors are present in the
evaporator, chance that they may get converted to ice &
block the lines
• So, to remove as much water vapor as possible, the vapors
driven off from the generator first flows through the
rectifier, which is a direct-cooled heat exchanger
• In the rectifier, the vapors from the generator first flow
counter-current to the incommoding strong solution from
the absorber
• Next the solution passes through the analyzer which is a
water-cooled heat exchanger, condensing some water rich
liquids which drains back to the rectifier
Solar heating based absorption chiller
• Ideally fits into the concept of Integrated Energy Systems
such as Cogeneration involving combined generation, heat,
refrigeration and power (CHRP Plants) on various fuels like
bio-mas, coal, Natural Gas, Heavy Oil, Solar, geothermal,
etc.
• Excellent for waste heat utilization
• Earns carbon credits, reduces taxes, promotes sustainable
development.
• Uses best eco-friendly refrigerant – ammonia
• Wide operational range + 5 C to – 55 C
• Low maintenance cost – no moving parts
• Can operate well for over 25 years
Advantages of ammonia systems
Comparison: Vapor compression and absorption
systems
Thanks
Any Questions…???

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R & AC-8 - Vapour Absorption - PART 2,3.pdf

  • 1. Refrigeration and air conditioning Dr. Najam Ul Hassan Shah Lecture # 8
  • 3. Basic Absorption Refrigeration Unit • The Basic Absorption Cycle - The condenser, expansion valve and the evaporator are similar as in a standard vapor- compression cycle. The compression operation is now provided by the assembly in the left-half of the diagram.
  • 4. COP of Ideal Absorption Cycle ( ) ( ) r a s a s r Gen evep T T T T T T Q Q COP − − = = It can be noted from above equation (and Figure) : As Ts increases → COP increases As Tr increases → COP increases As Ta increases → COP decreases Also see Ex. 17.1 and equations 17.2 – 17.4 Ts Tr Ta
  • 5. Absorption Refrigeration System S.# Refrigerant Absorber Absorber State 1 Ammonia Water Liquid 2 Ammonia Sodiumthiocynate Solid 3 Ammonia Lithium nitrate Solid 4 Ammonia Calcium chloride Solid 5 Water Lithium bromide Solid 6 Water Lithium chloride Solid 7 Methylene chloride Dimethyl ether or tetra ethylene glycol Liquid Refrigerant-absorber pairs
  • 6. Temperature-Pressure-Concentration Properties Lithium Bromide (LiBr) Water Absorption Cycle LiBr is a solid salt crystal. When exposing it to water vapor (in absorber tank) it will absorb the water vapor and become a liquid solution • If two vessels were connected as shown in the figure, one vessel containing LiBr-water solution and the other pure water, each liquid would exert a water-vapor pressure that is a function of the solution temperature and the concentration of the solution.
  • 7. Temperature-Pressure-Concentration Properties Lithium Bromide (LiBr) Water Absorption Cycle • At equilibrium the water-vapor pressure exerted by the two liquids would be equal , reaching a T-P-C point state having Tw = 40 C, Tsolution = 80 C and concentration of solution 59% LiBr. • Many such combinations Tw = f ( Tsolution , LiBr %, Pvapor) are possible for a given solution and can be plotted on graphs; like Fig 17.5 let see it
  • 9. Temperature-pressure concentration diagram: LiBr-water solutions • Concentration is the abscissa of the graph and water- vapor pressure could be considered as the ordinate on the vertical scale on the right • The saturation temperature of pure water corresponding to these vapor pressures is shown as the ordinate on the left • The chart applies to saturated conditions where the solution is in equilibrium with water vapor Temperature-Pressure-Concentration Properties
  • 10. Temperature-pressure concentration diagram: LiBr-water solutions • If the temperature of pure water is 40 °C, the vapor pressure the liquid exerts is 7.38 kPa, which can be determined from the opposite side of vertical scale. • A LiBr solution with a concentration of 59 % & temperature of 80°C also develops a water-vapor pressure of 7.38 kPa • If the solution had a concentration of 54% & temperature of 70°C the water-vapor pressure would again be 7.38 kPa Temperature-Pressure-Concentration Properties
  • 11. Ex.2 :Temperature-Pressure-Concentration Properties The pressure in vessel A is 4.24 kPa and it is 1.22 kPa in vessel B. The surrounding temp is 30C. If the valve between vessels is opened. Initially due to pressure difference water vapor will flow from vessel A to vessel B, and this vapor will be absorbed by the solution in vessel B
  • 12. Ex.2 :Temperature-Pressure-Concentration Properties If the concentration and temperature of vessel B are maintained constant at 50 % and 30oC, respectively. Then at equilibrium, the pressure in the entire system (vessels A and B) will be 1.22 kPa (equilibrium pressure of 50 % LiBr solution at 30oC). And temperature of water in vessel A will lower to the saturation temperature corresponding to 1.22 kPa, which is equal to about 10C, as shown in the figure
  • 13. Ex.2 :Temperature-Pressure-Concentration Properties Since the temperature of A is lower than surroundings, cooling effect will be produces ; Qc Now for the above process to continue, there should always be pure water in vessel A, and vessel B must be maintained always at 50 percent concentration and 30oC
  • 14. Ex.2 :Temperature-Pressure-Concentration Properties • In the example discussed the system is a closed system with finite sized reservoirs • Thus, gradually the amount of water in A decreases and the solution in B becomes diluted with water. As a result, the system pressure and temperature of water in A increase with time • Hence the refrigeration effect at A reduces gradually due to the reduced temperature difference between the surroundings and water. Thus, refrigeration produced by systems using only two vessels is intermittent in nature.
  • 15. ME - 437 : Refrigeration & Air Conditioning Ex.2 :Temperature-Pressure-Concentration Properties • In these systems, after a period, the refrigeration process has to be stopped and both the vessels A and B have to be brought back to their original condition. This requires removal of water absorbed in B and adding it back to vessel A in liquid form, i.e., a process of regeneration as shown in Fig. below
  • 16. Calculation of Mass Flow Rate and Enthalpy Example 17.2 : Compute the rate flow of refrigerant (water) through the condenser and evaporator in the cycle shown in Figure below if the pump delivers 0.6 kg/s and the following temperatures prevail: generator, 100C; condenser, 40C; evaporator. 10C; and absorber, 30C.
  • 17. Calculation of Mass Flow Rates • The mass flow rate abortion unit can be determined by knowing the concentrations of the LiBr in the solution • Two different pressures exist in the system: a high pressure prevails in the generator and condenser, while the low pressure prevails in the absorber and evaporator • Knowing that the pressure in condenser & generator must be same and at condenser inlet (station 3), saturated pure water enters from generator at the condensing temperature (40 C) gives us High Pressure of cycle. i.e • At 40°C → (from fig 17,5 ) , Pgen = 7.38 kPa • Similarly, evaporator an absorber pressure are same and at evaporator operating at 10 C gives (Fig 17.5) the value of low pressure; • At 10°C → (from fig 17,5 ) , Pabs = 1.23 Kpa
  • 18. Calculation of Mass Flow Rates • At 40°C → (from fig 17,5 ) , Pgen = 7.38 kPa • At 10°C → (from fig 17,5 ) , Pabs = 1.23 Kpa • Knowing Low and high pressures, the concentration of LiBr in absorber (Station1) and generator ( Station 2) can be established from Fig 17.5 , see extract of Fig 17.5 below X1 = 0.5 or 50% X2 = 0.664 or 66.4%
  • 19. Knowing and applying mass balance across generator give us following two equations Total mass flow balance : LiBr Solution Mass flow : Calculation of Mass Flow Rates s Kg m / 148 . 0 3 = • s kg m / 6 . 0 1 = • 6 . 0 1 3 2 = = + • • • m m m 2 2 1 1 x m x m • • = s kg m / 452 . 0 2 = • ( ) ( ) 664 . 0 50 . 0 6 . 0 2 • =m Solving these two equations, you get the values of mass flow rates
  • 20. Enthalpy of LiBr Solutions • For thermal calculations on the absorption cycle, enthalpy data must be available for the working substances at all crucial positions in the cycle • Water in liquid and vapor forms flows in and out of the condenser & evaporator, so enthalpies at these points can be determined from a table of properties of water • In the generator and absorber, LiBr-water solutions exist for which enthalpy is a function of both - solution temperature and concentration
  • 22. Calculation of Enthalpy, Q and COP Ex. 17.3 : For absorption system of previous example, compute qg, qc, qa, qe & COP. SOLUTION: Data from Previous Example: m1 = 0.6 Kg/s, m2 = 0.452 Kg/s, m3 = m4 = m5 = 0.148 Kg/s, X1 =0.5 and X2 =0.664 Enthalpy of Solution from Fig. 17.8 at 30 °C and x1 of 50% → h1 = -168 kJ/kg At 100 °C and x2 of 66.4% → h2 = -52 kJ/kg Enthalpy of water are found from Table A.1 as: h3 = hvapor @ 100 C = 2676 KJ/Kg h4 = hliquid @ 40 C = 167.5 KJ/Kg h5 = hvapor @ 10 C = 2520 KJ/Kg
  • 25. Calculation of Enthalpy, Q and COP KW h m h m h m Q g 3 473 1 1 2 2 3 3 . = − + = • • • KW h m h m Q c 2 . 371 4 4 3 3 = − = • • KW h m h m h m Q a 3 . 450 1 1 5 5 2 2 = − + = • • • KW h m h m Q e 2 . 384 4 4 5 5 = − = • • Ex. 17.3 : For absorption system of previous example, compute qg, qc, qa, qe & COP. 736 . 0 6 . 476 2 . 348 = = = g e Q Q COP Now from Energy Balance, heat transfer rates are established as:
  • 26. Absorption cycle with heat exchanger
  • 27. Absorption cycle with heat exchanger • By addition of heat exchanger, the COP increases • The heat-exchanger transfers heat between the two streams of solutions • It heats the cool solution from the absorber on its way to the generator and cools the solution returning from the generator to the absorber
  • 28. Example 17.4 A water-LiBr absorption refrigeration system is shown (see figure). The temperature at point 2 is 52 °C. The mass flow rate delivered by the solution pump is 0.6 kg/s. What are the rates of energy transfer at each of the components and the COP of this cycle? Also, what is the temperature at state 4?
  • 32. Example 17.4 The solution of Ex. Show that Qa reduces while Qg reduces slightly and increases COP to 0.783 (from 0.736)
  • 34. • Crystallization occurs when the solution state is on right side of crystallization line on P-T-C diagram • Dropping into this region formation of a slash or solidification of Solution, which can block the flow in a pipe and stop the operation of absorption unit • Crystallization must be avoiding by proper designing • See Example 17.5 Crystallization
  • 35. Example 17.5 In the system shown in Fig. 17-9, the ambient wet bulb temperature decreases so that the temperature of the cooling water drops, which also reduce the condensing temperature to 34 °C. All other temperatures specified on Fig. 17-9 remain unchanged. Is there a danger of crystallization?
  • 41. Capacity Control ; It reduces the reduction to a desired level. Without capacity control a given system yields maximum refrigeration. The control can be achieved by following three methods : ▪ Reducing flow rate delivered by pump at Staion1 ▪ Reducing generator Temperature ▪ Increasing the condensing Temperature Capacity Control
  • 44. Many Other Systems including combination with other cycles and different combination of refrigerant and absorber. Few commonly used systems are listed here: Other Systems ▪ Double Effect Units ▪ Combined absorption and vapor compression system ▪ Aqua Ammonia System
  • 46. Combined absorption and vapor compression system
  • 50. Aqua-Ammonia System • In aqua-ammonia absorption system, water is used as an absorbent while ammonia is used as a refrigerant • Dissolution of NH3 into water is exothermic and inversely proportional to temperature. • The system consists of all the components i.e., generator, absorber, condenser, evaporator, and heat exchanger---- plus a rectifier & analyzer. • The work input to the pump is usually very small, and the COP of absorption refrigeration systems is defined as gen L in p gen L abs Q Q W Q Q input Work effect Cooling COP  + = = ,
  • 53. Aqua-Ammonia System • Additional components as refrigerant vapors released at generator contains water vapor as well • Normally aqua-ammonia system operate at evaporating temperature below 0 °C • If large amounts of water vapors are present in the evaporator, chance that they may get converted to ice & block the lines • So, to remove as much water vapor as possible, the vapors driven off from the generator first flows through the rectifier, which is a direct-cooled heat exchanger • In the rectifier, the vapors from the generator first flow counter-current to the incommoding strong solution from the absorber • Next the solution passes through the analyzer which is a water-cooled heat exchanger, condensing some water rich liquids which drains back to the rectifier
  • 54. Solar heating based absorption chiller
  • 55. • Ideally fits into the concept of Integrated Energy Systems such as Cogeneration involving combined generation, heat, refrigeration and power (CHRP Plants) on various fuels like bio-mas, coal, Natural Gas, Heavy Oil, Solar, geothermal, etc. • Excellent for waste heat utilization • Earns carbon credits, reduces taxes, promotes sustainable development. • Uses best eco-friendly refrigerant – ammonia • Wide operational range + 5 C to – 55 C • Low maintenance cost – no moving parts • Can operate well for over 25 years Advantages of ammonia systems
  • 56. Comparison: Vapor compression and absorption systems