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International Journal of Research in Engineering and Innovation (IJREI) Vol-1, Issue-2, (2017), 49-53
____________________________________________________________________________________________________________________________
International Journal of Research in Engineering and Innovation
(IJREI)
journal home page: http://www.ijrei.com
ISSN (Online): 2456-6934
___________________________________________________________________________________
Corresponding author: Kaushalendra Kumar Dubey1
Email Address: dubey.kaushalendra@gmail.com 49
Thermodynamic study of R134a in Vapour Compression Refrigeration
System in Summer Climate
Kaushalendra Kumar Dubey1
R.S Mishra2
Department of Mechanical Engineering, Delhi Technological University, Delhi-110042
Email id.: professor_rsmishra@yahoo.co.in, dubey.kaushalendra@gmail.com
__________________________________________________________________________________
Abstract
Thermodynamic analysis of an ideal vapour compression refrigeration system is done using refrigerants R134a.This Energy-
Exergy analysis is carried out by developed mathematical model. Various parameters are numerically computed are first
law efficiency in terms of coefficient of performance (COP) of the system both ideal case and actual experimental and
exergetic efficiency and exergy destruction ratio have been computed . The eco-friendly R134a refrigerant gives lower COP
than R22. Comparing with R22, R134a takes more compressor power and second law efficiency (exergetic efficiency) of
VCRS is also lower than using R22. Due to higher GWP and ODP of R22, R134a can be used for domestic / commercial
and industrial applications. © 2017 ijrei.com. All rights reserved
Keywords: Hydrofluorocarbon refrigerants, ozone-friendly, performance characteristics, ODP, GWP,
___________________________________________________________________________________________________
1. Introduction
Refrigerant is a substance which is used as a working
substance in refrigeration system to move heat from lower
temperature to higher temperature to get cooling effect.
Midgley discovered halogenated hydrocarbon refrigerants
having favourable thermodynamic properties. But these
halogenated hydrocarbon refrigerants attack the
atmospheric stratosphere and destroy ozone layer. With the
discovery of ozone hole in stratosphere as stated by Molina
and Rowland et al [1] and the Montreal protocols (Paul, et
al [2]), the CFC and HCFC refrigerants are to be phased
out due to their higher global worming potential (GWP)
and higher ozone depletion potential (ODP). For these
reasons, recently ODP and GWP plays a vital role in the
development of new environment friendly alternative
refrigerants other than CFC and HCFC refrigerants for
their higher ODP and GWP. So, develop countries stopped
production of CFC and HCFC refrigerants and looking for
alternative environment friendly refrigerants. So, HC and
HFC refrigerants with zero ODP and low GWP are
considered for long term purpose. Although the ODP of
some HFCs is zero, their GWP related to the greenhouse
effect is large. On the other hand, HC refrigerants have a
flammability issue, which restricts the usage in existing
systems. However this flammability issue can be avoided
by blending HC refrigerants with HFC refrigerants. It is
also found that an HC/HFC mixture makes a very good
solution with mineral oil and contribution to global
warming of HC/HFC mixture is very low due to very
lowGWP (about one third of HFC) and hence R134a is
found to be most suitable alternative refrigerant for R12.
Refrigerant R134a has very similar thermodynamic
properties such as molecular weight, critical temperature,
boiling point as R12, with zero ODP and less GWP as
compared to CFC12 are shown in table 1 (Calm and
Hourahan, et al [3]). This gave confidence to the
researchers to consider R134a as a suitable replacement to
R12 for short term basis. Hammad and Alsaad et al [4]
investigated on domestic refrigerator using LPG (24.4%
propane, 56.4% butane and 17.2 % iso-butane) as
refrigerant. They concluded that this is the environment
friendly refrigerant mixture and that can replace R12 in
domestic refrigerator. Jung et al. (Jung, et al, 1996)
investigated on domestic refrigerator using propane and
iso-butane as a refrigerant mixture and found that mass
fraction range of 0.2 to 0.6 of propane increase the COP up
to 2.3% compared to R12. Mani and Selladurai (Mani and
Kaushalendra Kumar et al/ International journal of research in engineering and innovation (IJREI), vol 1, issue 2 (2017), 49-53
50
Selladurai, 2008) experimented on vapour compression
refrigeration system using new refrigerant mixture of
propane and iso-butane for substitution of R12 and R134a.
They found that this mixture had a refrigeration capacity
19.9% to 50.1 % higher than R12 and 28.6% to 87.2%
higher than R134a and COP improved by 3.9% to 25.1%
than R12 at lower evaporator temperature and 11.8% to
17.6% at higher temperature. Chen and Prasad (Chen and
Prasad, 1999) theoretically analysed vapour compression
refrigeration system using R134a and R12 as refrigerants
and reported that the COP for R134a is slightly (3%) lower
than the R12.Richardson and Butterworth (Richardson and
Butterworth, 1995) experimentally investigated the
performance of hydrocarbon refrigerants in a hermetic
vapour compression refrigeration system and came to the
conclusion that propane and propane/isobutene mixtures
can be used in an unmodified R12 system and can achieved
better COPs than R12 under the same operating conditions.
They found that around 50% propane and 50% isobutene
mixture not only just give the similar saturation
characteristics but also gives a better COP when proportion
of propane is increased. They also mentioned that
hydrocarbon refrigerants have a flammability issue, they
can be safely used in hermetic vapour compression
refrigeration
The aim of this study is to investigate the performance of
vapour compression refrigeration systems using R12,
R125, R134a, R143a and R152a as refrigerants based on
energy and exergy concept. Various parameters like COP,
refrigerating capacity, compressor work, cycle efficiency,
exergy efficiency are computed and compared in this work.
Figure 1 (a) A basic Vapor Compression refrigeration Cycle. (b) T-S diagram (c) its P-H diagram. [1]
Vapor compression refrigeration cycle on p-h diagram.
The p-h diagram is frequently used in the analysis of vapor
compression refrigeration cycle and usually consists of the
four processes.
Process 1-2 is the compression.
Process 2-3 is the Condensation.
Process 3-4 is the expansion.
Process 4-1 is the evaporation.
T1 and T2 are the suction and discharge temperatures.
Pe and Pc are the evaporating and condensing pressures.
The different enthalpies involved in the cycle are,
h1: enthalpy of suction pipe or end of evaporation.
h2: end of suction pipe or end of compressor.
h3: inlet of throttling valve or end on heat exchanger.
h4: inlet of evaporation or end of expansion.
1.1 Thermal Analysis of Vapour Compression
Refrigeration System
Figure 1 shows the p-h diagram of a complete ideal vapour
compression refrigeration system. Various calculations are
done based on this system using different refrigerants. COP
of vapour compression refrigeration system is a very
important criterion for performance analysis. It represents
the refrigeration effect per unit compressor work.
COPVCRS = Refrigeration Effect/ Compressor Work= RE/W
Where RE is the refrigeration effect and W is the
compressor work.
The refrigerating effect, RE can be expressed as
RE= ṁ (h1– h4)
The compressor work, W can be expressed as
W = ṁ (h2– h1)
Where (h2– h1) is the difference of enthalpy which includes
the effect of compressor efficiency and ṁis the mass flow
rate of the refrigerants which can be expressed as
Kaushalendra Kumar et al/ International journal of research in engineering and innovation (IJREI), vol 1, issue 2 (2017), 49-53
51
ṁ = RE/ (h1– h4)
Where (h1–h4 ) is the difference of enthalpy in the cycle.
The exergetic efficiency, ɳII is computed in terms of second
law efficiency , which is a the ratio of COP of VCRS to
the COP of Carnot cycle, then
ɳII= COPVCRS/ COPCarnot =
𝑅 𝐸
𝑊
𝑇 𝑒
𝑇 𝑐− 𝑇 𝑒
and COPCarnot=
𝑇𝑒
𝑇𝑐− 𝑇𝑒
Where Te is evaporator temperature and Tc is condenser
temperature
(The COP of Carnot refrigeration cycle is a function of
evaporator and condenser temperatures only and is
independent of the nature of the working substance. The
Carnot COP sets an upper limit for refrigeration systems
operating between two constant temperature thermal
reservoirs (heat source and sink). From Carnot’s theorems,
for the same heat source and sink temperatures, no
irreversible cycle can have COP higher than that of Carnot
COP.)
The cycle efficiency (also called as second law efficiency)
is a good indication of the deviation of the standard VCRS
cycle from Carnot cycle. Unlike Carnot COP, the cycle
efficiency depends very much on the shape of T s diagram,
which in turn depends on the nature of the working fluid.
Exergy or availability of a system is the maximum
obtainable work output from the system. So exergy loss is
the very important criterion to evaluate the thermodynamic
performance of the vapour compression refrigeration
system. System performance improved if exergy loss is
less. For that reason it is our aim to minimize the exergy
loss to improve the system thermodynamically. The exergy
can be expressed following Chen and Prasad (Chen and
Prasad, 1999) as
e = (h-h0) –(s-s0)
where kinetic and potential energy are excluded.
The exergy loss can be calculated by calculating exergy
loss in each component of the system. Exergy loss in
compressor can be expressed as
Δew=(h1-h2)+T0(s2-s1)+W
Exergy loss in condenser can be expressed as
Δec= (h2-h3)+T0(s3-s2)
Exergy loss in expansion valve can be expressed as
Δev= (h3-h4)+T0(s4-s3)
Exergy loss in evaporator can be expressed as
Δew= (h4-h1)(T0/Tr)+T0(s1-s4)
And the total exergy loss can be expressed as
ΔE = ṁ(Δew +Δec+Δev+Δew)
Exergetic efficiency can be expressed as
ɳx=
W
Tr
To
RE 





1
1.2 Properties and Environmental Impacts of Selected
Alternative Refrigerants
The vapour compression refrigeration system operates on
refrigerant R12 which is most important CFC refrigerant
identified for phase out in the country by HFC refrigerant.
The institute has been one of the few institutes selected for
funding for research work under World Bank project
TEQIP. A research work was undertaken for finding the
most suitable ozone-friendly Hydrofluorocarbon
refrigerant for replacing ozone depleting refrigerant R12.
Then most suitable refrigerant has been selected for
replacing harmful refrigerant. Four non-ozone depleting
HFC refrigerants (R125, R134a, R143a and R152a) were
selected from methane and ethane derivatives and their
performances in vapour compression refrigeration system
were investigated. Properties and environmental impacts of
selected zero ozone-depleting refrigerants used as
substitutes in the refrigeration systems are listed in the
Table (1a) to Table-1(c) [3-6] respectively.
Table-1(a) : Some properties and environmental impacts of
selected alternative refrigerants.[3][5][6]
Table-1(b) : Some properties and environmental impacts of
selected alternative refrigerants.[3][5][6]
Refrigerants Chemical
formula
Molecular
mass
Freezing
point
(°C)
R12 CF2CL2 121 -157.5
R125 C2 HF5 120 -102.99
R134a C2H2F4 102 -96.67
R143a C2H3F4 84 -111
Refrigerants
Chemical
formula
Boiling
point
(ºC)
Critical
point
(°C)
R12 CF2CL2 -29.8 112
R125 C2 HF5 -48.1 66.18
R134a C2H2F4 -26.1 101.06
R143a C2H3F4 -47.2 72.89
R152a C2H4F2 -24.0 113.26
Kaushalendra Kumar et al/ International journal of research in engineering and innovation (IJREI), vol 1, issue 2 (2017), 49-53
52
Table-1(c): Some environmental properties of selected
alternative refrigerants [3][5][6.
2. Results and Discussions
Experiment was conducted in the laboratory for obtaining
thermal performance using eco-friendly R134a,
refrigerant. The following data have been recorded.
Atmospheric pressure: 1 bar
Atmospheric temperature: T0 =30°C =303 K
Condenser pressure: 135psi
Evaporator pressure: 8psi
Compressor delivery temperature: 61.9°C
Compressor suction temperature: -12.7°C
Ref. leaving condenser temperature: 29.6°C
Evaporator inlet temperature:-16.7°C
Mass flow rate: 5 kg/min
Evaporator volts: Ve/V = 196
Evaporator AMPS: Ie/n =2.24
Motor volts: Vm/V =198
Motor amps Im/A =2.892
Motor compressor speed: 2800rpm
The Enthalpy and Entropy have been computed on above
state temperature data as shown in the table-2.
Table-2 Enthalpy and Entropy of various components of
VCRS
States Tempe
rature
in 0
C
Enthalpy
in KJ/Kg
Entropy
in
KJ/Kg-K
Outlet of
evaporator-1
-12.7 391 1.7355
Compressor
outlet-2
61.9 427 1.7011
Condenser
outlet-3
29.6 240 1.1437
Evaporator
Inlet-4
-16.7 178.6 0.9179
 Coefficient of performance
COP ideal cycle = (h1-h4)/((h2-h1)/0.8) = 4.719
(Assuming 80% volumetric efficiency of compressor)
COP Actual =Qe/Power =V×I/Power= V×I/(Motor volts
×Motor amps×Cos⌀) =0.983
ɳIItheoritical = (COP Actual / COP ideal cycle) = 0.2083
 Exergy loss in each component of the system
Exergy loss in compressor
Δew= (h1-h2) +T0 (s2-s1) +W
Δew=133.5768 KJ/KG
Exergy loss in condenser
Δec= (h2-h3)+T0(s3-s2)
Δec= 18.1078 KJ/KG
Exergy loss in expansion valve
Δev= (h3-h4)+T0(s4-s3)
Δev=-7.0274KJ/KG
Exergy loss in evaporator
Δew= (h4-h1)(T0/T2)+T0(s1-s4)
Δew=-3.3565KJ/KG
And the total exergy loss
ΔE = ṁ(Δew + Δec+ Δev+ Δew)
ΔE = 706.5035 KJ/KG
 Exergectic Efficiency (ɳx)
ɳx=
W
T
To
RE 






2
1
ɳ_II_exp=0.1791= 17.91%
3. Conclusion
The experimental work presented in this paper on vapour
compression refrigeration system, the following
conclusions were made.
1. The eco-friendly R134a refrigerant gives lower COP
than R22.
2. Comparing with R22, R134a takes more compressor
power.
3. Second law efficiency (Exergetic efficiency of VCRS
is also lower than using R22.
4. Due to higher GWP and ODP of R22, R134a can be
used for domestic / commercial and industrial
applications.
Acknowledgement
Authors) thanks to my respected teachera Prof (Dr.) Vijay
Gupta, Vice-Chancellor, Sharda University, Greater Noida
and Prof. N K Bansal, Ex-VC of MVDU katra for
guidance.
References
[1] M.J.Molina, FS.Rowland, (1974) Stratospheric sink for
chlorofluoromethane: chlorine atom catalyzed destruction of
ozone, Nature, 249,810–812.
Refrigerants
Ozone Depletion
Potential
(ODP)
Global Warming
Potential (GWP)
R12 1 8100
R125 0 2800
R134a 0 1300
R143a 0 3800
R152a 0 140
Kaushalendra Kumar et al/ International journal of research in engineering and innovation (IJREI), vol 1, issue 2 (2017), 49-53
53
[2] S.Paul, A.Sarkar, B.K.Mandal, (2013) Environmental
impacts of halogenated refrigerants and their alternatives:
recent developments, International Journal of Emerging
Technology and Advanced Engineering, 3: Special Issue 3:
ICERTSD 2013:400-409.
[3] J.M.Calm, G.C.Hourahan, (2001) Refrigerant data
summery, Engineering Systems, 18,74–88.
[4] M.A.Hammad, M.A.Alsaad, (1999) The use of hydrocarbon
mixtures as refrigerants in domestic refrigerators, Applied
Thermal Engineering, 19,1181–1189.
[5] Bhatti, M.S. (1999). A historical look of
chlorofluorocarbonrefrigerants. ASHRAE Transactions,
part 1, 1999.pp.1186- 1206
[6] Cavallini A, Working fluids for mechanical refrigeration.
International Journal of Refrigeration 19 (1996) 485-496.
[7] McMullan JT, Refrigeration and the environment issues and
strategies for the future, International Journal of
Refrigeration 25 (2002) 89-99.

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IJREI_Thermodynamic study of R134a in Vapour Compression Refrigeration System in Summer Climate

  • 1. International Journal of Research in Engineering and Innovation (IJREI) Vol-1, Issue-2, (2017), 49-53 ____________________________________________________________________________________________________________________________ International Journal of Research in Engineering and Innovation (IJREI) journal home page: http://www.ijrei.com ISSN (Online): 2456-6934 ___________________________________________________________________________________ Corresponding author: Kaushalendra Kumar Dubey1 Email Address: dubey.kaushalendra@gmail.com 49 Thermodynamic study of R134a in Vapour Compression Refrigeration System in Summer Climate Kaushalendra Kumar Dubey1 R.S Mishra2 Department of Mechanical Engineering, Delhi Technological University, Delhi-110042 Email id.: professor_rsmishra@yahoo.co.in, dubey.kaushalendra@gmail.com __________________________________________________________________________________ Abstract Thermodynamic analysis of an ideal vapour compression refrigeration system is done using refrigerants R134a.This Energy- Exergy analysis is carried out by developed mathematical model. Various parameters are numerically computed are first law efficiency in terms of coefficient of performance (COP) of the system both ideal case and actual experimental and exergetic efficiency and exergy destruction ratio have been computed . The eco-friendly R134a refrigerant gives lower COP than R22. Comparing with R22, R134a takes more compressor power and second law efficiency (exergetic efficiency) of VCRS is also lower than using R22. Due to higher GWP and ODP of R22, R134a can be used for domestic / commercial and industrial applications. © 2017 ijrei.com. All rights reserved Keywords: Hydrofluorocarbon refrigerants, ozone-friendly, performance characteristics, ODP, GWP, ___________________________________________________________________________________________________ 1. Introduction Refrigerant is a substance which is used as a working substance in refrigeration system to move heat from lower temperature to higher temperature to get cooling effect. Midgley discovered halogenated hydrocarbon refrigerants having favourable thermodynamic properties. But these halogenated hydrocarbon refrigerants attack the atmospheric stratosphere and destroy ozone layer. With the discovery of ozone hole in stratosphere as stated by Molina and Rowland et al [1] and the Montreal protocols (Paul, et al [2]), the CFC and HCFC refrigerants are to be phased out due to their higher global worming potential (GWP) and higher ozone depletion potential (ODP). For these reasons, recently ODP and GWP plays a vital role in the development of new environment friendly alternative refrigerants other than CFC and HCFC refrigerants for their higher ODP and GWP. So, develop countries stopped production of CFC and HCFC refrigerants and looking for alternative environment friendly refrigerants. So, HC and HFC refrigerants with zero ODP and low GWP are considered for long term purpose. Although the ODP of some HFCs is zero, their GWP related to the greenhouse effect is large. On the other hand, HC refrigerants have a flammability issue, which restricts the usage in existing systems. However this flammability issue can be avoided by blending HC refrigerants with HFC refrigerants. It is also found that an HC/HFC mixture makes a very good solution with mineral oil and contribution to global warming of HC/HFC mixture is very low due to very lowGWP (about one third of HFC) and hence R134a is found to be most suitable alternative refrigerant for R12. Refrigerant R134a has very similar thermodynamic properties such as molecular weight, critical temperature, boiling point as R12, with zero ODP and less GWP as compared to CFC12 are shown in table 1 (Calm and Hourahan, et al [3]). This gave confidence to the researchers to consider R134a as a suitable replacement to R12 for short term basis. Hammad and Alsaad et al [4] investigated on domestic refrigerator using LPG (24.4% propane, 56.4% butane and 17.2 % iso-butane) as refrigerant. They concluded that this is the environment friendly refrigerant mixture and that can replace R12 in domestic refrigerator. Jung et al. (Jung, et al, 1996) investigated on domestic refrigerator using propane and iso-butane as a refrigerant mixture and found that mass fraction range of 0.2 to 0.6 of propane increase the COP up to 2.3% compared to R12. Mani and Selladurai (Mani and
  • 2. Kaushalendra Kumar et al/ International journal of research in engineering and innovation (IJREI), vol 1, issue 2 (2017), 49-53 50 Selladurai, 2008) experimented on vapour compression refrigeration system using new refrigerant mixture of propane and iso-butane for substitution of R12 and R134a. They found that this mixture had a refrigeration capacity 19.9% to 50.1 % higher than R12 and 28.6% to 87.2% higher than R134a and COP improved by 3.9% to 25.1% than R12 at lower evaporator temperature and 11.8% to 17.6% at higher temperature. Chen and Prasad (Chen and Prasad, 1999) theoretically analysed vapour compression refrigeration system using R134a and R12 as refrigerants and reported that the COP for R134a is slightly (3%) lower than the R12.Richardson and Butterworth (Richardson and Butterworth, 1995) experimentally investigated the performance of hydrocarbon refrigerants in a hermetic vapour compression refrigeration system and came to the conclusion that propane and propane/isobutene mixtures can be used in an unmodified R12 system and can achieved better COPs than R12 under the same operating conditions. They found that around 50% propane and 50% isobutene mixture not only just give the similar saturation characteristics but also gives a better COP when proportion of propane is increased. They also mentioned that hydrocarbon refrigerants have a flammability issue, they can be safely used in hermetic vapour compression refrigeration The aim of this study is to investigate the performance of vapour compression refrigeration systems using R12, R125, R134a, R143a and R152a as refrigerants based on energy and exergy concept. Various parameters like COP, refrigerating capacity, compressor work, cycle efficiency, exergy efficiency are computed and compared in this work. Figure 1 (a) A basic Vapor Compression refrigeration Cycle. (b) T-S diagram (c) its P-H diagram. [1] Vapor compression refrigeration cycle on p-h diagram. The p-h diagram is frequently used in the analysis of vapor compression refrigeration cycle and usually consists of the four processes. Process 1-2 is the compression. Process 2-3 is the Condensation. Process 3-4 is the expansion. Process 4-1 is the evaporation. T1 and T2 are the suction and discharge temperatures. Pe and Pc are the evaporating and condensing pressures. The different enthalpies involved in the cycle are, h1: enthalpy of suction pipe or end of evaporation. h2: end of suction pipe or end of compressor. h3: inlet of throttling valve or end on heat exchanger. h4: inlet of evaporation or end of expansion. 1.1 Thermal Analysis of Vapour Compression Refrigeration System Figure 1 shows the p-h diagram of a complete ideal vapour compression refrigeration system. Various calculations are done based on this system using different refrigerants. COP of vapour compression refrigeration system is a very important criterion for performance analysis. It represents the refrigeration effect per unit compressor work. COPVCRS = Refrigeration Effect/ Compressor Work= RE/W Where RE is the refrigeration effect and W is the compressor work. The refrigerating effect, RE can be expressed as RE= ṁ (h1– h4) The compressor work, W can be expressed as W = ṁ (h2– h1) Where (h2– h1) is the difference of enthalpy which includes the effect of compressor efficiency and ṁis the mass flow rate of the refrigerants which can be expressed as
  • 3. Kaushalendra Kumar et al/ International journal of research in engineering and innovation (IJREI), vol 1, issue 2 (2017), 49-53 51 ṁ = RE/ (h1– h4) Where (h1–h4 ) is the difference of enthalpy in the cycle. The exergetic efficiency, ɳII is computed in terms of second law efficiency , which is a the ratio of COP of VCRS to the COP of Carnot cycle, then ɳII= COPVCRS/ COPCarnot = 𝑅 𝐸 𝑊 𝑇 𝑒 𝑇 𝑐− 𝑇 𝑒 and COPCarnot= 𝑇𝑒 𝑇𝑐− 𝑇𝑒 Where Te is evaporator temperature and Tc is condenser temperature (The COP of Carnot refrigeration cycle is a function of evaporator and condenser temperatures only and is independent of the nature of the working substance. The Carnot COP sets an upper limit for refrigeration systems operating between two constant temperature thermal reservoirs (heat source and sink). From Carnot’s theorems, for the same heat source and sink temperatures, no irreversible cycle can have COP higher than that of Carnot COP.) The cycle efficiency (also called as second law efficiency) is a good indication of the deviation of the standard VCRS cycle from Carnot cycle. Unlike Carnot COP, the cycle efficiency depends very much on the shape of T s diagram, which in turn depends on the nature of the working fluid. Exergy or availability of a system is the maximum obtainable work output from the system. So exergy loss is the very important criterion to evaluate the thermodynamic performance of the vapour compression refrigeration system. System performance improved if exergy loss is less. For that reason it is our aim to minimize the exergy loss to improve the system thermodynamically. The exergy can be expressed following Chen and Prasad (Chen and Prasad, 1999) as e = (h-h0) –(s-s0) where kinetic and potential energy are excluded. The exergy loss can be calculated by calculating exergy loss in each component of the system. Exergy loss in compressor can be expressed as Δew=(h1-h2)+T0(s2-s1)+W Exergy loss in condenser can be expressed as Δec= (h2-h3)+T0(s3-s2) Exergy loss in expansion valve can be expressed as Δev= (h3-h4)+T0(s4-s3) Exergy loss in evaporator can be expressed as Δew= (h4-h1)(T0/Tr)+T0(s1-s4) And the total exergy loss can be expressed as ΔE = ṁ(Δew +Δec+Δev+Δew) Exergetic efficiency can be expressed as ɳx= W Tr To RE       1 1.2 Properties and Environmental Impacts of Selected Alternative Refrigerants The vapour compression refrigeration system operates on refrigerant R12 which is most important CFC refrigerant identified for phase out in the country by HFC refrigerant. The institute has been one of the few institutes selected for funding for research work under World Bank project TEQIP. A research work was undertaken for finding the most suitable ozone-friendly Hydrofluorocarbon refrigerant for replacing ozone depleting refrigerant R12. Then most suitable refrigerant has been selected for replacing harmful refrigerant. Four non-ozone depleting HFC refrigerants (R125, R134a, R143a and R152a) were selected from methane and ethane derivatives and their performances in vapour compression refrigeration system were investigated. Properties and environmental impacts of selected zero ozone-depleting refrigerants used as substitutes in the refrigeration systems are listed in the Table (1a) to Table-1(c) [3-6] respectively. Table-1(a) : Some properties and environmental impacts of selected alternative refrigerants.[3][5][6] Table-1(b) : Some properties and environmental impacts of selected alternative refrigerants.[3][5][6] Refrigerants Chemical formula Molecular mass Freezing point (°C) R12 CF2CL2 121 -157.5 R125 C2 HF5 120 -102.99 R134a C2H2F4 102 -96.67 R143a C2H3F4 84 -111 Refrigerants Chemical formula Boiling point (ºC) Critical point (°C) R12 CF2CL2 -29.8 112 R125 C2 HF5 -48.1 66.18 R134a C2H2F4 -26.1 101.06 R143a C2H3F4 -47.2 72.89 R152a C2H4F2 -24.0 113.26
  • 4. Kaushalendra Kumar et al/ International journal of research in engineering and innovation (IJREI), vol 1, issue 2 (2017), 49-53 52 Table-1(c): Some environmental properties of selected alternative refrigerants [3][5][6. 2. Results and Discussions Experiment was conducted in the laboratory for obtaining thermal performance using eco-friendly R134a, refrigerant. The following data have been recorded. Atmospheric pressure: 1 bar Atmospheric temperature: T0 =30°C =303 K Condenser pressure: 135psi Evaporator pressure: 8psi Compressor delivery temperature: 61.9°C Compressor suction temperature: -12.7°C Ref. leaving condenser temperature: 29.6°C Evaporator inlet temperature:-16.7°C Mass flow rate: 5 kg/min Evaporator volts: Ve/V = 196 Evaporator AMPS: Ie/n =2.24 Motor volts: Vm/V =198 Motor amps Im/A =2.892 Motor compressor speed: 2800rpm The Enthalpy and Entropy have been computed on above state temperature data as shown in the table-2. Table-2 Enthalpy and Entropy of various components of VCRS States Tempe rature in 0 C Enthalpy in KJ/Kg Entropy in KJ/Kg-K Outlet of evaporator-1 -12.7 391 1.7355 Compressor outlet-2 61.9 427 1.7011 Condenser outlet-3 29.6 240 1.1437 Evaporator Inlet-4 -16.7 178.6 0.9179  Coefficient of performance COP ideal cycle = (h1-h4)/((h2-h1)/0.8) = 4.719 (Assuming 80% volumetric efficiency of compressor) COP Actual =Qe/Power =V×I/Power= V×I/(Motor volts ×Motor amps×Cos⌀) =0.983 ɳIItheoritical = (COP Actual / COP ideal cycle) = 0.2083  Exergy loss in each component of the system Exergy loss in compressor Δew= (h1-h2) +T0 (s2-s1) +W Δew=133.5768 KJ/KG Exergy loss in condenser Δec= (h2-h3)+T0(s3-s2) Δec= 18.1078 KJ/KG Exergy loss in expansion valve Δev= (h3-h4)+T0(s4-s3) Δev=-7.0274KJ/KG Exergy loss in evaporator Δew= (h4-h1)(T0/T2)+T0(s1-s4) Δew=-3.3565KJ/KG And the total exergy loss ΔE = ṁ(Δew + Δec+ Δev+ Δew) ΔE = 706.5035 KJ/KG  Exergectic Efficiency (ɳx) ɳx= W T To RE        2 1 ɳ_II_exp=0.1791= 17.91% 3. Conclusion The experimental work presented in this paper on vapour compression refrigeration system, the following conclusions were made. 1. The eco-friendly R134a refrigerant gives lower COP than R22. 2. Comparing with R22, R134a takes more compressor power. 3. Second law efficiency (Exergetic efficiency of VCRS is also lower than using R22. 4. Due to higher GWP and ODP of R22, R134a can be used for domestic / commercial and industrial applications. Acknowledgement Authors) thanks to my respected teachera Prof (Dr.) Vijay Gupta, Vice-Chancellor, Sharda University, Greater Noida and Prof. N K Bansal, Ex-VC of MVDU katra for guidance. References [1] M.J.Molina, FS.Rowland, (1974) Stratospheric sink for chlorofluoromethane: chlorine atom catalyzed destruction of ozone, Nature, 249,810–812. Refrigerants Ozone Depletion Potential (ODP) Global Warming Potential (GWP) R12 1 8100 R125 0 2800 R134a 0 1300 R143a 0 3800 R152a 0 140
  • 5. Kaushalendra Kumar et al/ International journal of research in engineering and innovation (IJREI), vol 1, issue 2 (2017), 49-53 53 [2] S.Paul, A.Sarkar, B.K.Mandal, (2013) Environmental impacts of halogenated refrigerants and their alternatives: recent developments, International Journal of Emerging Technology and Advanced Engineering, 3: Special Issue 3: ICERTSD 2013:400-409. [3] J.M.Calm, G.C.Hourahan, (2001) Refrigerant data summery, Engineering Systems, 18,74–88. [4] M.A.Hammad, M.A.Alsaad, (1999) The use of hydrocarbon mixtures as refrigerants in domestic refrigerators, Applied Thermal Engineering, 19,1181–1189. [5] Bhatti, M.S. (1999). A historical look of chlorofluorocarbonrefrigerants. ASHRAE Transactions, part 1, 1999.pp.1186- 1206 [6] Cavallini A, Working fluids for mechanical refrigeration. International Journal of Refrigeration 19 (1996) 485-496. [7] McMullan JT, Refrigeration and the environment issues and strategies for the future, International Journal of Refrigeration 25 (2002) 89-99.