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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 
__________________________________________________________________________________________ 
Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 704 
EFFECT OF APPROCHING TEMPERATURE ON THE PERFORMANCE AND SIZE OF LiBr-WATER VAPOUR ABSORPTION REFRIGERATION IN THE ABSENCE OF SOLUTION HEAT EXCHANGER Sunil.B.S1, Manu S2, C.V.Mahesh3, T.K.Chandrashekar4 1 M.Tech, 4th sem Mechanical Engineering, SSIT, Tumkur. 2Assistant Professor, Department of Mechanical Engineering, SSIT, Tumkur 3Professor, Department of Mechanical Engineering, SSIT, Tumkur 4Professor, Department of Mechanical Engineering, MIT, Moodabidri Abstract In this study, a detailed thermodynamic analysis of the water/lithium bromide absorption refrigeration cycle is performed. The influences of approaching temperatures, conductance and coefficients of performance are investigated. Plots of coefficients of performance and conductance are shown against approaching temperatures of the system. It is concluded that the performance and conductance decreases with increase in approaching temperature of all the components. Keywords: Refrigeration, Absorption, Water/Lithium bromide. 
----------------------------------------------------------------------***------------------------------------------------------------------------ 1. INTRODUCTION During the recent years research has attempted to develop new technologies that can reduces energy consumption and cost without decreasing the level of comforts. By this reason absorption refrigeration technologies has greater advantages compared to conventional refrigeration systems because the system utilises waste heat and it is friendly with environment. Among different combination of refrigerant and absorbent, Lithium Bromide –Water (LiBr-H2O) showed the promising solution for effective ultisation of waste heat and zero determental effect on the atmospher since it uses water has refrigerant and Lithium-Bromide solution as absorbent 
Number of research has been carried out to enhance the performance of the system and reduce the size of the system. A.Kececiler et al. [1] conducted experiments in laboratory on LiBr H2O system which uses low temperature geothermal energy as a powering source. The result showed that, low-heat geothermal sources cannot be used efficiently in electricity generation and effective for the storing range at 4-10ºC. Da- Wen Sun [2] performed simulation on LiBr H2O absorption refrigeration systems. The simulation provides the detailed thermodynamic design data and optimum design map and also for new absorbent/refrigeration pairs. O. Kaynakli et al. [3] investigated the effect of operating temperature on the performance of single effect LiBr H2O absorption refrigeration cycle. The result showed that as the generator and evaporator temperature increases there is a drastic increase of COP (Coefficient of Performance) but decreases with rise of condenser and absorber temperatures. M. Izquierdo et al. [4] performed trials to investigate the performance of a commercial 4.5 kW air cooled, single effect LiBr H2O absorption chillier which is used for residential. The result showed as the cooling power tends to decreases with increase of outdoor dry bulb temperature and for the temperature ranges of 35 to 41.3ºC but the chilled water outlet temperature of evaporator peaks to 15ºC. Mostafavi and Agnew [5] investigated the effect of ambient temperature on the surface area of the component of an air-cooled absorption machine. The objective of the study to investigate the effect of approaching temperature on the performance of single stage water cooled LiBr–water absorption machine. The theoretical simulation is performed using MAT lab Software for the capacity of 0.5kW. 1.1 Approaching Temperature The approaching temperature refers to the maximum heat transfer for hot body to the cold body. If the approaching temperature is less then greater is the heat transfer. This approaching temperature play key role on the performance of the system because the system is cooled by the water and refrigeration effect is aborbed by the chilled water. There are mainly four approaching temperatures comes in the system and they are as follows:-Approaching absorber temperature (DTa). It is the temperature difference between T12 and T15, Approaching evaporator temperature (DTe), It is the temperature difference between T16and T1, Approaching generator temperature (DTg), It is the temperature difference between T10 and T7.Approaching Condenser temperature (DTc), It is the temperature difference between T14 and T13.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 
__________________________________________________________________________________________ 
Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 705 
1.2 Circulation Ratio 
The circulation ratio (CR) can be defined as the ratio of the 
mass flow rate of the solution coming from the generator to 
the absorber to the mass flow rate of the working fluid. 
CR = 
m s 
mH 2o 
2. VAPOUR ABSORPTION REFRIGERATION 
(VAR) SYSTEM 
. 
Fig-1: Schematic diagram of LiBr-H2O vapour absorption 
refrigeration cycle 
The refrigerant is vaporized in the evaporator after taking heat 
from the water. It is then sent to the absorber where the 
refrigerant vapours get condensed. During the process, latent 
heat liberated during condensation of refrigerant vapours is 
taken by the cooling water in absorber. The weak solution 
coming from absorber and rich in refrigerant concentration is 
pressurized through pump upto generator pressure where it is 
heated to give off refrigerant vapour, forming strong 
concentration refrigerant solution. This strong concentration 
refrigerant solution then returns to absorber and mixes with 
refrigerant vapours coming from evaporator, forming a strong 
concentration refrigerant solution which is then re-circulated 
in the circuit. The refrigerant vapours are condensed in the 
condenser liberating heat of condensation. Throttle valve and 
expansion valve are used to reduce the pressure of poor 
concentration refrigerant solution and refrigerant coming out 
from condenser to absorber and evaporator pressure 
respectively. The heat is supplied to the generator by hot 
water. The heat rejected in the condenser is passed to the 
circulating cold water. 
3. RESULTS AND DISCUSSION 
3.1 Effect of Approaching Condenser Temperature 
Fig-2(a) and (b) shows the variation of condenser approaching 
temperature on the performance of the system and the 
conductance. The simulation was performed by varying 
condenser approaching temperatures for 
DTa=DTg=DTe=5°C. The Fig 2(a), (b) shows an approaching 
temperature of condenser increases there is a decrease in the 
performance and conductance of the condenser. This is due to 
decrease in the heat transfer rate to the cooling water resulting 
in decrease in the condensate rate this reduces the performance 
of the system. Decreasing in the conductance of the condenser 
is due increase in the condenser temperature. 
0 1 2 3 4 5 
0.46 
0.48 
0.50 
0.52 
0.54 
0.56 
0.58 
0.60 
0.62 
0.64 
0.66 
Performance 
Approach Condenser Temperature (DTc) ( 
O 
C) 
COP 
Fig-2(a): Condenser approaching temperature 
Vs. Variation of performance 
0 1 2 3 4 5 
0.2 
0.4 
0.6 
0.8 
1.0 
1.2 
1.4 
1.6 
1.8 
Conductance (W K 
-1 
) 
Approach Condenser Temperature (DTc) ( 
O 
C) 
UAa 
UAc 
UAe 
UAg 
Fig- 2(b): Condenser approaching 
temperature Vs. Conductance
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 
__________________________________________________________________________________________ 
Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 706 
3.2 Effect of Approaching Evaporator Temperature 
Fig-3(a) and (b) shows the variation of evaporator 
approaching temperature on the performance of the system 
and the conductance. The simulation was performed by 
varying evaporator approaching temperatures for 
DTa=DTg=DTc=5°C.The Fig-3(a) and (b) shows an 
approaching temperature of evaporator increases there is a 
decrease in the performance and conductance of the 
evaporator. This is due to decrease in the heat transfer rate to 
the water resulting in decrease in the evaporation rate of 
refrigerant resulted in reduction in the performance of the 
system. Decreasing in the conductance of the evaporator is 
due increase in the evaporator temperature. 
3.3 Effect of Approaching Generator Temperature 
Fig-4(a) and (b) shows the variation of generator approaching 
temperature on the performance of the system and the 
conductance. The simulation was performed by varying 
generator approaching temperatures for DTa=DTe=DTc=5°C. 
The Fig 4(a) and (b) shows an approaching temperature of 
generator increases there is a decrease in the performance and 
conductance of the generator. This is due to decrease in the 
heat transfer rate to the cooling water resulting in decrease in 
the generation rate of refrigerant this reduces the performance 
of the system. There is a drastic decreasing in the conductance 
of the generator is due increase in the generator temperature. 
3.4 Effect of Approaching Absorber Temperature 
Fig-4(a) and (b) shows the variation of absorber approaching 
temperature on the performance of the system and the 
conductance. The simulation was performed by varying 
absorber approaching temperatures for DTe=DTg=DTc=5°C. 
The Fig 4(a) and (b) shows an approaching temperature of 
absorber increases there is a decrease in the performance and 
conductance of the absorber. This is due to decrease in the 
heat transfer rate to the cooling water resulting in decrease in 
the circulation rate this reduces the performance of the system. 
Fig-4(a): Generator approaching temperature Vs. 
Variation of performance 
0 1 2 3 4 5 
0.778 
0.780 
0.782 
0.784 
0.786 
Perforrmance 
Approach Generator Temperature (DTg) ( 
O 
C) 
COP 
0 1 2 3 4 5 
0.65 
0.70 
0.75 
0.80 
0.85 
Perforrmance 
Approach Evaporator Temperature (DTe) ( 
O 
C) 
COP 
Fig-3(a): Evaporator approaching temperature 
Vs. Variation of performance 
0 1 2 3 4 5 
0.2 
0.4 
0.6 
0.8 
1.0 
1.2 
Conductance (W K 
-1 
) 
Approach Evaporator Temperature (DTe) ( 
O 
C) 
UAa 
UAc 
UAe 
UAg 
Fig- 3(b): Evaporator approaching temperature 
Vs. Conductance 
Fig- 4(b): Generator approaching temperature 
Vs. Conductance 
0 1 2 3 4 5 
0 
1 
2 
3 
4 
5 
6 
Conductance (W K 
-1 
) 
Approach Generator Temperature (DTg) ( 
O 
C) 
UAa 
UAc 
UAe 
UAg
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 
__________________________________________________________________________________________ 
Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 707 
There is a low decreasing in the conductance of the absorber is 
due increase in the absorber temperature. 
4. CONCLUSIONS 
The theoretical simulation was performed on single effect 
water cooled vapour absorption refrigeration. The simulation 
is carried on MAT Lab software by varying approaching 
temperature. The paper concludes that as approaching 
temperature increases in condenser, evaporator, absorber, 
generator there is a decrease in the performance and 
conductance. 
REFERENCES 
[1] Kececiler, A., H.I. Acar, and A. Dogan, 
Thermodynamic analysis of the absorption refrigeration 
system with geothermal energy: an experimental study. 
Energy Conversion and Management, 41(1): p. 37-48, 
2000. 
[2] Sun, D.-W., Thermodynamic design data and optimum 
design maps for absorption refrigeration systems. 
Applied Thermal Engineering, 17(3): p. 211-221, 1997. 
[3] Kaynakli, O. and M. Kilic, Theoretical study on the 
effect of operating conditions on performance of 
absorption refrigeration system. Energy Conversion 
and Management, 48(2): p. 599-607, 2007. 
[4] Izquierdo, M., et al., Air conditioning using an air-cooled 
single effect lithium bromide absorption chiller: 
Results of a trial conducted in Madrid in August 2005. 
Applied Thermal Engineering, 28(8-9): p. 1074-1081, 
2008. 
[5] T Mostafavi, M. and B. Agnew, The impact of 
ambient temperature on lithium-bromide/water 
absorption machine performance. Applied Thermal 
Engineering, 16(6): p. 515-522, 1996. 
0 1 2 3 4 5 
0.15 
0.20 
0.25 
0.30 
0.35 
0.40 
0.45 
0.50 
0.55 
0.60 
Conductance (W K 
-1 
) 
Approach Absorber Temperature (DTa) ( 
O 
C) 
UAa 
UAc 
UAe 
UAg 
Fig- 5 (b): Absorber approaching temperature Vs. 
Conductance 
0 1 2 3 4 5 
0.775 
0.780 
0.785 
0.790 
0.795 
0.800 
0.805 
0.810 
0.815 
Performance 
Approach Absorber Temperature (DTa) ( 
O 
C) 
COP 
Fig-5(a): Absorber approaching temperature Vs. 
Variation of performance 
(DTg=DTe=DTc=5°C)

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Effect of approching temperature on the performance and size of li br water vapour absorption refrigeration in the absence of solution heat exchanger

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 704 EFFECT OF APPROCHING TEMPERATURE ON THE PERFORMANCE AND SIZE OF LiBr-WATER VAPOUR ABSORPTION REFRIGERATION IN THE ABSENCE OF SOLUTION HEAT EXCHANGER Sunil.B.S1, Manu S2, C.V.Mahesh3, T.K.Chandrashekar4 1 M.Tech, 4th sem Mechanical Engineering, SSIT, Tumkur. 2Assistant Professor, Department of Mechanical Engineering, SSIT, Tumkur 3Professor, Department of Mechanical Engineering, SSIT, Tumkur 4Professor, Department of Mechanical Engineering, MIT, Moodabidri Abstract In this study, a detailed thermodynamic analysis of the water/lithium bromide absorption refrigeration cycle is performed. The influences of approaching temperatures, conductance and coefficients of performance are investigated. Plots of coefficients of performance and conductance are shown against approaching temperatures of the system. It is concluded that the performance and conductance decreases with increase in approaching temperature of all the components. Keywords: Refrigeration, Absorption, Water/Lithium bromide. ----------------------------------------------------------------------***------------------------------------------------------------------------ 1. INTRODUCTION During the recent years research has attempted to develop new technologies that can reduces energy consumption and cost without decreasing the level of comforts. By this reason absorption refrigeration technologies has greater advantages compared to conventional refrigeration systems because the system utilises waste heat and it is friendly with environment. Among different combination of refrigerant and absorbent, Lithium Bromide –Water (LiBr-H2O) showed the promising solution for effective ultisation of waste heat and zero determental effect on the atmospher since it uses water has refrigerant and Lithium-Bromide solution as absorbent Number of research has been carried out to enhance the performance of the system and reduce the size of the system. A.Kececiler et al. [1] conducted experiments in laboratory on LiBr H2O system which uses low temperature geothermal energy as a powering source. The result showed that, low-heat geothermal sources cannot be used efficiently in electricity generation and effective for the storing range at 4-10ºC. Da- Wen Sun [2] performed simulation on LiBr H2O absorption refrigeration systems. The simulation provides the detailed thermodynamic design data and optimum design map and also for new absorbent/refrigeration pairs. O. Kaynakli et al. [3] investigated the effect of operating temperature on the performance of single effect LiBr H2O absorption refrigeration cycle. The result showed that as the generator and evaporator temperature increases there is a drastic increase of COP (Coefficient of Performance) but decreases with rise of condenser and absorber temperatures. M. Izquierdo et al. [4] performed trials to investigate the performance of a commercial 4.5 kW air cooled, single effect LiBr H2O absorption chillier which is used for residential. The result showed as the cooling power tends to decreases with increase of outdoor dry bulb temperature and for the temperature ranges of 35 to 41.3ºC but the chilled water outlet temperature of evaporator peaks to 15ºC. Mostafavi and Agnew [5] investigated the effect of ambient temperature on the surface area of the component of an air-cooled absorption machine. The objective of the study to investigate the effect of approaching temperature on the performance of single stage water cooled LiBr–water absorption machine. The theoretical simulation is performed using MAT lab Software for the capacity of 0.5kW. 1.1 Approaching Temperature The approaching temperature refers to the maximum heat transfer for hot body to the cold body. If the approaching temperature is less then greater is the heat transfer. This approaching temperature play key role on the performance of the system because the system is cooled by the water and refrigeration effect is aborbed by the chilled water. There are mainly four approaching temperatures comes in the system and they are as follows:-Approaching absorber temperature (DTa). It is the temperature difference between T12 and T15, Approaching evaporator temperature (DTe), It is the temperature difference between T16and T1, Approaching generator temperature (DTg), It is the temperature difference between T10 and T7.Approaching Condenser temperature (DTc), It is the temperature difference between T14 and T13.
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 705 1.2 Circulation Ratio The circulation ratio (CR) can be defined as the ratio of the mass flow rate of the solution coming from the generator to the absorber to the mass flow rate of the working fluid. CR = m s mH 2o 2. VAPOUR ABSORPTION REFRIGERATION (VAR) SYSTEM . Fig-1: Schematic diagram of LiBr-H2O vapour absorption refrigeration cycle The refrigerant is vaporized in the evaporator after taking heat from the water. It is then sent to the absorber where the refrigerant vapours get condensed. During the process, latent heat liberated during condensation of refrigerant vapours is taken by the cooling water in absorber. The weak solution coming from absorber and rich in refrigerant concentration is pressurized through pump upto generator pressure where it is heated to give off refrigerant vapour, forming strong concentration refrigerant solution. This strong concentration refrigerant solution then returns to absorber and mixes with refrigerant vapours coming from evaporator, forming a strong concentration refrigerant solution which is then re-circulated in the circuit. The refrigerant vapours are condensed in the condenser liberating heat of condensation. Throttle valve and expansion valve are used to reduce the pressure of poor concentration refrigerant solution and refrigerant coming out from condenser to absorber and evaporator pressure respectively. The heat is supplied to the generator by hot water. The heat rejected in the condenser is passed to the circulating cold water. 3. RESULTS AND DISCUSSION 3.1 Effect of Approaching Condenser Temperature Fig-2(a) and (b) shows the variation of condenser approaching temperature on the performance of the system and the conductance. The simulation was performed by varying condenser approaching temperatures for DTa=DTg=DTe=5°C. The Fig 2(a), (b) shows an approaching temperature of condenser increases there is a decrease in the performance and conductance of the condenser. This is due to decrease in the heat transfer rate to the cooling water resulting in decrease in the condensate rate this reduces the performance of the system. Decreasing in the conductance of the condenser is due increase in the condenser temperature. 0 1 2 3 4 5 0.46 0.48 0.50 0.52 0.54 0.56 0.58 0.60 0.62 0.64 0.66 Performance Approach Condenser Temperature (DTc) ( O C) COP Fig-2(a): Condenser approaching temperature Vs. Variation of performance 0 1 2 3 4 5 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 Conductance (W K -1 ) Approach Condenser Temperature (DTc) ( O C) UAa UAc UAe UAg Fig- 2(b): Condenser approaching temperature Vs. Conductance
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 706 3.2 Effect of Approaching Evaporator Temperature Fig-3(a) and (b) shows the variation of evaporator approaching temperature on the performance of the system and the conductance. The simulation was performed by varying evaporator approaching temperatures for DTa=DTg=DTc=5°C.The Fig-3(a) and (b) shows an approaching temperature of evaporator increases there is a decrease in the performance and conductance of the evaporator. This is due to decrease in the heat transfer rate to the water resulting in decrease in the evaporation rate of refrigerant resulted in reduction in the performance of the system. Decreasing in the conductance of the evaporator is due increase in the evaporator temperature. 3.3 Effect of Approaching Generator Temperature Fig-4(a) and (b) shows the variation of generator approaching temperature on the performance of the system and the conductance. The simulation was performed by varying generator approaching temperatures for DTa=DTe=DTc=5°C. The Fig 4(a) and (b) shows an approaching temperature of generator increases there is a decrease in the performance and conductance of the generator. This is due to decrease in the heat transfer rate to the cooling water resulting in decrease in the generation rate of refrigerant this reduces the performance of the system. There is a drastic decreasing in the conductance of the generator is due increase in the generator temperature. 3.4 Effect of Approaching Absorber Temperature Fig-4(a) and (b) shows the variation of absorber approaching temperature on the performance of the system and the conductance. The simulation was performed by varying absorber approaching temperatures for DTe=DTg=DTc=5°C. The Fig 4(a) and (b) shows an approaching temperature of absorber increases there is a decrease in the performance and conductance of the absorber. This is due to decrease in the heat transfer rate to the cooling water resulting in decrease in the circulation rate this reduces the performance of the system. Fig-4(a): Generator approaching temperature Vs. Variation of performance 0 1 2 3 4 5 0.778 0.780 0.782 0.784 0.786 Perforrmance Approach Generator Temperature (DTg) ( O C) COP 0 1 2 3 4 5 0.65 0.70 0.75 0.80 0.85 Perforrmance Approach Evaporator Temperature (DTe) ( O C) COP Fig-3(a): Evaporator approaching temperature Vs. Variation of performance 0 1 2 3 4 5 0.2 0.4 0.6 0.8 1.0 1.2 Conductance (W K -1 ) Approach Evaporator Temperature (DTe) ( O C) UAa UAc UAe UAg Fig- 3(b): Evaporator approaching temperature Vs. Conductance Fig- 4(b): Generator approaching temperature Vs. Conductance 0 1 2 3 4 5 0 1 2 3 4 5 6 Conductance (W K -1 ) Approach Generator Temperature (DTg) ( O C) UAa UAc UAe UAg
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 707 There is a low decreasing in the conductance of the absorber is due increase in the absorber temperature. 4. CONCLUSIONS The theoretical simulation was performed on single effect water cooled vapour absorption refrigeration. The simulation is carried on MAT Lab software by varying approaching temperature. The paper concludes that as approaching temperature increases in condenser, evaporator, absorber, generator there is a decrease in the performance and conductance. REFERENCES [1] Kececiler, A., H.I. Acar, and A. Dogan, Thermodynamic analysis of the absorption refrigeration system with geothermal energy: an experimental study. Energy Conversion and Management, 41(1): p. 37-48, 2000. [2] Sun, D.-W., Thermodynamic design data and optimum design maps for absorption refrigeration systems. Applied Thermal Engineering, 17(3): p. 211-221, 1997. [3] Kaynakli, O. and M. Kilic, Theoretical study on the effect of operating conditions on performance of absorption refrigeration system. Energy Conversion and Management, 48(2): p. 599-607, 2007. [4] Izquierdo, M., et al., Air conditioning using an air-cooled single effect lithium bromide absorption chiller: Results of a trial conducted in Madrid in August 2005. Applied Thermal Engineering, 28(8-9): p. 1074-1081, 2008. [5] T Mostafavi, M. and B. Agnew, The impact of ambient temperature on lithium-bromide/water absorption machine performance. Applied Thermal Engineering, 16(6): p. 515-522, 1996. 0 1 2 3 4 5 0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.50 0.55 0.60 Conductance (W K -1 ) Approach Absorber Temperature (DTa) ( O C) UAa UAc UAe UAg Fig- 5 (b): Absorber approaching temperature Vs. Conductance 0 1 2 3 4 5 0.775 0.780 0.785 0.790 0.795 0.800 0.805 0.810 0.815 Performance Approach Absorber Temperature (DTa) ( O C) COP Fig-5(a): Absorber approaching temperature Vs. Variation of performance (DTg=DTe=DTc=5°C)