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Scientific Journal Impact Factor (SJIF): 1.711
International Journal of Modern Trends in Engineering
and Research
www.ijmter.com
@IJMTER-2014, All rights Reserved 7
e-ISSN: 2349-9745
p-ISSN: 2393-8161
EFFECT OF CONCENTRATION OF LITHIUM BROMIDE
MIXTURE ON COP FOR SINGLE EFFECT LiBr-H2O
ABSORPTION REFRIGERATION SYSTEM
A.P.KORINGA1
, Dr. N.S.MEHTA2
1
PG Scholar, Mechanical Department, LDRP-ITR
2
Professor, Mechanical Department, LDRP-ITR
Abstract— In this paper effect of concentration of lithium bromide mixture on Co-efficient of
performance (COP) for single effect LiBr-H2O absorption chillers is calculated. Then find out how
the cop varies with the concentration of lithium bromide. For finding cop temperature of condenser
varies and the other parameter (temperature of generator, temperature of absorber, capacity of
evaporator, temperature of evaporator temperature of absorber) remains constant. Optimal value of
COP obtained 0.65 varying temperature of condenser.
Keywords- Absorption System; Lithium Bromide; COP; Concentration of lithium bromide;
condenser
I. INTRODUCTION
In recent years, special attention has been paid to absorption refrigeration systems (ARSs)
because of their low cost and environmentally friendly operation. In comparison to conventional
mechanical vapor compression refrigeration systems, ARSs require lower energy level, therefore
renewable energy sources or heat wasted by industrial processes can be used to operate such systems.
Different methodologies have been developed for improving ARSs. Generally single effect
chillers are the most common type on market. Single effect absorption refrigeration system have
been studied by number of others (Gomri, Kaushik and arora), they analyzed cycles both
energetically and exergetically. The condensation temperatures used in their simulation for
calculating enthalpy and entropy.
II. SYSTEM DESCRIPTION
Fig shows the schematic diagram of a single effect VARs, which uses water as refrigerant
and lithium bromide as absorbent. For this purpose of analysis following assumption are made:
 Refrigerant water at condenser and evaporator exit is in saturated states.
 Lithium bromide solutions in the generator and absorber are assumed to be in equilibrium
conditions at their respective temperature and pressure.
 Strong solution of refrigerant leaving the absorber and weak solution of refrigerant leaving
the generator are saturated.
 The reference environmental state for the system is water at an ambient temperature (T0) of
250
C.
 Pressure drop in pipes and other components are negligible.
 All components are externally adiabatic.
International Journal of Modern Trends in Engineering and Research (IJMTER)
Volume 02, Issue 01, [January - 2015] e-ISSN: 2349-9745, p-ISSN: 2393-8161
@IJMTER-2014, All rights Reserved 8
2.1 Desirable Properties of Refrigerant-Absorbent mixtures:
Refrigerant-absorbent mixtures for Vapour Absorption Cooling System should possess some
desirable properties like the refrigerant should be more volatile than the absorbent in other words the
boiling point of refrigerant should be much lower than the absorbent. There must be large difference
in the boiling points of refrigerant and absorbent (greater than 2000 0C), so that the solution in the
Generator need only to be heated to the temperature required to boil off only the refrigerant. This
ensures that only pure refrigerant circulates through refrigerant circuit (condenser-expansion valve-
evaporator). The refrigerant should exhibit high solubility with solution in the absorber. The
absorbent should have strong affinity for the refrigerant. This will minimize the amount of
refrigerant to be circulated. Operating pressures should be preferably low, so that the walls of the
shells and connecting pipes need not to be thick. It should not undergo crystallization or
solidification inside the system. Because crystallization will block the free flow of solution in the
line. The mixture should be safe, chemically stable, noncorrosive, inexpensive and should be
available easily. The refrigerant should have high heat of vaporization.
III. THERMODYNAMIC ANALYSIS OF THE SYSTEM
Form fig-1 schematic diagram of single effect LiBr-H2O system following equations are
used.
Let M= mass of refrigerant, kg/s
Mss= mass flow rate of strong solution, kg/s
Mws= mass flow rate of weak solution, kg/s
International Journal of Modern Trends in Engineering and Research (IJMTER)
Volume 02, Issue 01, [January - 2015] e-ISSN: 2349-9745, p-ISSN: 2393-8161
@IJMTER-2014, All rights Reserved 9
3.1 Mass (m) and Heat transfer (Q) balance for each component:
Condenser:
M1=M2=M
QC= M*(h1-h2)
Expansion Valve:
M2=M3=M
h2=h3
Evaporator:
M3 =M4=M
Qe=M*(h3-h4)
Absorber:
From total mass balance
M+Mss=Mws
Circulation Ratio:
λ=Mss/M
Mws= (1+λ)*M
λ=Ƹws/(Ƹss-Ƹws)
Qa=M*h4+Mss*h10-Mws*h5
Solution Pump:
M5=M6=Mws
Solution Heat Exchanger:
M6=M7=Mws
M8=M9=Mss
Mws*(h7-h6)=Mss*(h8-h9)
Generator:
Qg=M*h1+Mss*h8-Mws*h7
COP=Qe/Qg
IV. RESULTS
The parameter chosen as reference to optimize VAR system operation and maximize COP
varies with the solution concentration ΔX.
Where ΔX=Ƹss-Ƹws is most suitable choice as the reference variable for optimizing COP.
 Temperature of Evaporator TE=5o
C
 Capacity of Evaporator QE=7.5 Kw
 Temperature of Absorber TA=20o
C
 Temperature of Generator TG= 64o
C
 Temperature of condenser TC= 25o
C , 30o
C respectively
International Journal of Modern Trends in Engineering and Research (IJMTER)
Volume 02, Issue 01, [January - 2015] e-ISSN: 2349-9745, p-ISSN: 2393-8161
@IJMTER-2014, All rights Reserved 10
IV.CONCLUSION
In this method effect of condensation and desorption temperatures on COP and particularly effect of
the variation in solution concentration Δx were studied. The method proposed for maximize COP for
single effect LiBr-H2O absorption system is correct. In single effect LiBr-H2O the maximum COP
for TC of 25o
C, 30o
C and35o
C is reached when Δx is 6.5% and 7% respectively within the
crystallization effect.
REFERENCES
[1] Anand, D.K.., Kumar,B.,1987.Absorption machine irreversibility using new entropy calculation. Sol. Energy
39(3), 243-256.
[2] Kaushik, S.C., Arora, A., 2009 Energy and exergy analysis of single effect and series flow double effect water-
lithium bromide absorption refrigeration systems. Int. J. Refrig. 32,1247-1258.
[3] Kaynakli, O., Kilic, M., 2007.Theoretical study on the effect of operating conditions on performance of
absorption refrigeration system. Energy Convers. Manage. 48, 599-607.
[4] Kim, D.S., Infante Ferreira, C.A., 2008.Analytic modeling of steady state single-effect absorption cycles. Int. J.
Refrig. 31 (6), 1012-1020.
[5] Arun, M.B.,Maiya, M.P.,Murthy, S.S., 2000. Equilibrium low pressure generator temperatures for double effect
series flow absorption nrefrigeration systems. Appl. Therm. Eng. 20, 227-242.
[6] Felli, M., 1983.Absorption refrigeration thermodynamics. ASHRAE Trans. 89, 189-204.
[7] Gommed, K., Grossman, G., 1990. Performance analysis of staged absorption heat pumps: water-lithium bromide
systems. ASHRAE Trans. 30 (6), 1590-1598.
[8] Gomri, R., 2009. Second law comparison of single effect and double effect vapour absorption refrigeration
systems. Energy Convers. Manage. 50, 1279-1287.
[9] Hellmann, H.M., Ziegler, F., 1999. Simple absorption heat pump modules for system simulation programs.
ASHRAE Trans. 105,780-787.
[10] Henning, H., 2007. Solar assisted air conditioning of buildings- an overview. Appl. Therm. Eng. 27, 1734-1749.
[11] Herold, K.H., Radermacher, R., Klein, S.A., 1996. Absorption Chillers and Heat Pumps. CRC Press.
[12] Izquierdo, M., Martı´n, E., Palacios, E., 2009. Absorber and absorbere evaporator assembly for absorption
machines, PCT 09162208.4-2301. Priority Country: Spain. Countries to which protection has been extended:
European Union and others. Priority date: July 30, 2009.
[13] Izquierdo, M., Venegas, M., Rodrı´guez, P., Lecuona, A., 2004. Crystallization as a limit to develop solar air-
cooled LiBr-H2O absorption systems using low-grade heat. Sol. Energy Mater. Sol. Cells 81, 205-216
International Journal of Modern Trends in Engineering and Research (IJMTER)
Volume 02, Issue 01, [January - 2015] e-ISSN: 2349-9745, p-ISSN: 2393-8161
@IJMTER-2014, All rights Reserved 11
[14] Syed, A., Izquierdo, M., Rodrı´guez, P., Maidment, G., Missenden, J., Lecuona, A., Tozer, R., 2005.A novel
experimental investigation of a solar cooling system in Madrid. Int. J. Refrig. 28 (6), 859-871.
[15] Tozer, R., 2002. Sorption thermodynamics. ASHRAE Trans. 108 (1),781-791.
[16] Tozer, R., James, R.W., 1997.Fundamental thermodynamics of ideal absorption cycles. Int. J. of Refrig 20, 120-
135.
[17] Tufano, V.1998. Simplified criteria for the development of new absorption working pairs. Appl. Therm. Eng
18,171-177.
[18] Xu, G.P., Dai, Y.Q., 1997. Theoretical analysis and optimization of a double-effect parallel flow type absorption
chiller. Appl.Therm. Eng. 17 (2), 157-170.
EFFECT OF CONCENTRATION OF LITHIUM BROMIDE MIXTURE ON COP FOR SINGLE EFFECT LiBr-H2O ABSORPTION REFRIGERATION SYSTEM
EFFECT OF CONCENTRATION OF LITHIUM BROMIDE MIXTURE ON COP FOR SINGLE EFFECT LiBr-H2O ABSORPTION REFRIGERATION SYSTEM

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EFFECT OF CONCENTRATION OF LITHIUM BROMIDE MIXTURE ON COP FOR SINGLE EFFECT LiBr-H2O ABSORPTION REFRIGERATION SYSTEM

  • 1. Scientific Journal Impact Factor (SJIF): 1.711 International Journal of Modern Trends in Engineering and Research www.ijmter.com @IJMTER-2014, All rights Reserved 7 e-ISSN: 2349-9745 p-ISSN: 2393-8161 EFFECT OF CONCENTRATION OF LITHIUM BROMIDE MIXTURE ON COP FOR SINGLE EFFECT LiBr-H2O ABSORPTION REFRIGERATION SYSTEM A.P.KORINGA1 , Dr. N.S.MEHTA2 1 PG Scholar, Mechanical Department, LDRP-ITR 2 Professor, Mechanical Department, LDRP-ITR Abstract— In this paper effect of concentration of lithium bromide mixture on Co-efficient of performance (COP) for single effect LiBr-H2O absorption chillers is calculated. Then find out how the cop varies with the concentration of lithium bromide. For finding cop temperature of condenser varies and the other parameter (temperature of generator, temperature of absorber, capacity of evaporator, temperature of evaporator temperature of absorber) remains constant. Optimal value of COP obtained 0.65 varying temperature of condenser. Keywords- Absorption System; Lithium Bromide; COP; Concentration of lithium bromide; condenser I. INTRODUCTION In recent years, special attention has been paid to absorption refrigeration systems (ARSs) because of their low cost and environmentally friendly operation. In comparison to conventional mechanical vapor compression refrigeration systems, ARSs require lower energy level, therefore renewable energy sources or heat wasted by industrial processes can be used to operate such systems. Different methodologies have been developed for improving ARSs. Generally single effect chillers are the most common type on market. Single effect absorption refrigeration system have been studied by number of others (Gomri, Kaushik and arora), they analyzed cycles both energetically and exergetically. The condensation temperatures used in their simulation for calculating enthalpy and entropy. II. SYSTEM DESCRIPTION Fig shows the schematic diagram of a single effect VARs, which uses water as refrigerant and lithium bromide as absorbent. For this purpose of analysis following assumption are made:  Refrigerant water at condenser and evaporator exit is in saturated states.  Lithium bromide solutions in the generator and absorber are assumed to be in equilibrium conditions at their respective temperature and pressure.  Strong solution of refrigerant leaving the absorber and weak solution of refrigerant leaving the generator are saturated.  The reference environmental state for the system is water at an ambient temperature (T0) of 250 C.  Pressure drop in pipes and other components are negligible.  All components are externally adiabatic.
  • 2. International Journal of Modern Trends in Engineering and Research (IJMTER) Volume 02, Issue 01, [January - 2015] e-ISSN: 2349-9745, p-ISSN: 2393-8161 @IJMTER-2014, All rights Reserved 8 2.1 Desirable Properties of Refrigerant-Absorbent mixtures: Refrigerant-absorbent mixtures for Vapour Absorption Cooling System should possess some desirable properties like the refrigerant should be more volatile than the absorbent in other words the boiling point of refrigerant should be much lower than the absorbent. There must be large difference in the boiling points of refrigerant and absorbent (greater than 2000 0C), so that the solution in the Generator need only to be heated to the temperature required to boil off only the refrigerant. This ensures that only pure refrigerant circulates through refrigerant circuit (condenser-expansion valve- evaporator). The refrigerant should exhibit high solubility with solution in the absorber. The absorbent should have strong affinity for the refrigerant. This will minimize the amount of refrigerant to be circulated. Operating pressures should be preferably low, so that the walls of the shells and connecting pipes need not to be thick. It should not undergo crystallization or solidification inside the system. Because crystallization will block the free flow of solution in the line. The mixture should be safe, chemically stable, noncorrosive, inexpensive and should be available easily. The refrigerant should have high heat of vaporization. III. THERMODYNAMIC ANALYSIS OF THE SYSTEM Form fig-1 schematic diagram of single effect LiBr-H2O system following equations are used. Let M= mass of refrigerant, kg/s Mss= mass flow rate of strong solution, kg/s Mws= mass flow rate of weak solution, kg/s
  • 3. International Journal of Modern Trends in Engineering and Research (IJMTER) Volume 02, Issue 01, [January - 2015] e-ISSN: 2349-9745, p-ISSN: 2393-8161 @IJMTER-2014, All rights Reserved 9 3.1 Mass (m) and Heat transfer (Q) balance for each component: Condenser: M1=M2=M QC= M*(h1-h2) Expansion Valve: M2=M3=M h2=h3 Evaporator: M3 =M4=M Qe=M*(h3-h4) Absorber: From total mass balance M+Mss=Mws Circulation Ratio: λ=Mss/M Mws= (1+λ)*M λ=Ƹws/(Ƹss-Ƹws) Qa=M*h4+Mss*h10-Mws*h5 Solution Pump: M5=M6=Mws Solution Heat Exchanger: M6=M7=Mws M8=M9=Mss Mws*(h7-h6)=Mss*(h8-h9) Generator: Qg=M*h1+Mss*h8-Mws*h7 COP=Qe/Qg IV. RESULTS The parameter chosen as reference to optimize VAR system operation and maximize COP varies with the solution concentration ΔX. Where ΔX=Ƹss-Ƹws is most suitable choice as the reference variable for optimizing COP.  Temperature of Evaporator TE=5o C  Capacity of Evaporator QE=7.5 Kw  Temperature of Absorber TA=20o C  Temperature of Generator TG= 64o C  Temperature of condenser TC= 25o C , 30o C respectively
  • 4. International Journal of Modern Trends in Engineering and Research (IJMTER) Volume 02, Issue 01, [January - 2015] e-ISSN: 2349-9745, p-ISSN: 2393-8161 @IJMTER-2014, All rights Reserved 10 IV.CONCLUSION In this method effect of condensation and desorption temperatures on COP and particularly effect of the variation in solution concentration Δx were studied. The method proposed for maximize COP for single effect LiBr-H2O absorption system is correct. In single effect LiBr-H2O the maximum COP for TC of 25o C, 30o C and35o C is reached when Δx is 6.5% and 7% respectively within the crystallization effect. REFERENCES [1] Anand, D.K.., Kumar,B.,1987.Absorption machine irreversibility using new entropy calculation. Sol. Energy 39(3), 243-256. [2] Kaushik, S.C., Arora, A., 2009 Energy and exergy analysis of single effect and series flow double effect water- lithium bromide absorption refrigeration systems. Int. J. Refrig. 32,1247-1258. [3] Kaynakli, O., Kilic, M., 2007.Theoretical study on the effect of operating conditions on performance of absorption refrigeration system. Energy Convers. Manage. 48, 599-607. [4] Kim, D.S., Infante Ferreira, C.A., 2008.Analytic modeling of steady state single-effect absorption cycles. Int. J. Refrig. 31 (6), 1012-1020. [5] Arun, M.B.,Maiya, M.P.,Murthy, S.S., 2000. Equilibrium low pressure generator temperatures for double effect series flow absorption nrefrigeration systems. Appl. Therm. Eng. 20, 227-242. [6] Felli, M., 1983.Absorption refrigeration thermodynamics. ASHRAE Trans. 89, 189-204. [7] Gommed, K., Grossman, G., 1990. Performance analysis of staged absorption heat pumps: water-lithium bromide systems. ASHRAE Trans. 30 (6), 1590-1598. [8] Gomri, R., 2009. Second law comparison of single effect and double effect vapour absorption refrigeration systems. Energy Convers. Manage. 50, 1279-1287. [9] Hellmann, H.M., Ziegler, F., 1999. Simple absorption heat pump modules for system simulation programs. ASHRAE Trans. 105,780-787. [10] Henning, H., 2007. Solar assisted air conditioning of buildings- an overview. Appl. Therm. Eng. 27, 1734-1749. [11] Herold, K.H., Radermacher, R., Klein, S.A., 1996. Absorption Chillers and Heat Pumps. CRC Press. [12] Izquierdo, M., Martı´n, E., Palacios, E., 2009. Absorber and absorbere evaporator assembly for absorption machines, PCT 09162208.4-2301. Priority Country: Spain. Countries to which protection has been extended: European Union and others. Priority date: July 30, 2009. [13] Izquierdo, M., Venegas, M., Rodrı´guez, P., Lecuona, A., 2004. Crystallization as a limit to develop solar air- cooled LiBr-H2O absorption systems using low-grade heat. Sol. Energy Mater. Sol. Cells 81, 205-216
  • 5. International Journal of Modern Trends in Engineering and Research (IJMTER) Volume 02, Issue 01, [January - 2015] e-ISSN: 2349-9745, p-ISSN: 2393-8161 @IJMTER-2014, All rights Reserved 11 [14] Syed, A., Izquierdo, M., Rodrı´guez, P., Maidment, G., Missenden, J., Lecuona, A., Tozer, R., 2005.A novel experimental investigation of a solar cooling system in Madrid. Int. J. Refrig. 28 (6), 859-871. [15] Tozer, R., 2002. Sorption thermodynamics. ASHRAE Trans. 108 (1),781-791. [16] Tozer, R., James, R.W., 1997.Fundamental thermodynamics of ideal absorption cycles. Int. J. of Refrig 20, 120- 135. [17] Tufano, V.1998. Simplified criteria for the development of new absorption working pairs. Appl. Therm. Eng 18,171-177. [18] Xu, G.P., Dai, Y.Q., 1997. Theoretical analysis and optimization of a double-effect parallel flow type absorption chiller. Appl.Therm. Eng. 17 (2), 157-170.