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K. Nagalakshmi et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643

RESEARCH ARTICLE

www.ijera.com

OPEN ACCESS

The Design and Performance Analysis of Refrigeration System
Using R12 & R134a Refrigerants
K. Nagalakshmi1, G. Marurhiprasad Yadav2
1

. Mechanical engineer at St.Jhons College of Engg &Technology, Yemmiganur-518360, A. P, India.
. Associate professor, Department of Mechanical engineering, St.Jhons College of Engg &Technology,
Yemmiganur-518360, A. P, India.
2

ABSTRACT
The design and performance analysis of refrigeration system using R12 & R134a refrigerants are presented in
this report. The design calculations of the suitable and necessary refrigerator equipment and their results are also
reported here. CFC-12 is the most widely used refrigerant. It serves both in residential and commercial
applications, from small window units to large water chillers, and everything in between. Its particular
combination of efficiency, capacity and pressure has made it a popular choice for equipment designers.
Nevertheless, it does have some ODP, so international law set forth in the Montreal Protocol has put CFC-12 on
a phase out schedule.HFC-134a has been established as a drop-in alternative for CFC-12 in the industry due to
their zero Ozone Depletion Potential (ODP) and similarities in thermodynamic properties and performance.
However, when a system is charged with a HFC-134a compressor oil has to be changed.Not enough research
has been done to cover all aspects of alternative refrigerants applications in the systems. This project intended to
explore behavior of this alternative refrigerants compare to CFC-12 and challenges the industry is facing in
design, operation services and maintenance of these equipments.The purpose of this project is to investigate
behavior of R134a refrigerant. This includes performance and efficiency variations when it replaces R12 in an
existing system as well as changes involved in maintaining the system charged with R134a. This project is
intended to address challenges faced in the real world and some practical issues. Theoretical and experimental
approaches used as a methodology in this work.
Keywords - alternate refrigirents, evaporator, HCFCs, ODP, GWP.
I. INTRODUCTION
Refrigeration is concerned with the
absorption of heat from where it is objectionable plus
its transfer to and rejection at a place where it is
unobjectionable. Regardless of means by which is
heat transfer is accomplished; the problem is one of
applied thermodynamics. In some methods of
refrigeration the working medium that approaches
perfect gases may be applied.A refrigerant is a
compound used in a heat cycle that undergoes a
phase change from a gas to a liquid and back. The
two
main
uses
of
refrigerants
are
refrigerators/freezers and air conditioners. In
broadest sense the word refrigerant is also applied to
such secondary cooling medium as brine solutions,
cooled water. The refrigerants include only those
working mediums, which pass through the cycle or
evaporation, recovery, compression and liquefaction.
ANALYSIS OF VAPOUR COMPRESSION
CYCLE DIAGRAM
The flow diagram T-Ǿ and P-H diagrams of a vapour
compression refrigerating system given below.

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fIg.1
1-2 ISENTROPIC COMPRESSION
Refrigerant
vapour
received
evaporator is compressed isentropically
compressor by external source of energy

from
in a

fig.2
(work in out), pressure and temperature increase.
638 | P a g e
K. Nagalakshmi et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643
2-3 CONDENSATION
Compressor discharges vapour into the
condenser where it condensed completely i.e. turns
in to liquid. Heat is rejected from the refrigerant to
cooling medium, usually air or water.
3-4 EXPANSION
From condenser liquid refrigerant passes
through the expansion valve where it is throttled
resulting in a drop of temperature and pressure.
However, enthalpy remains constant (throttling
expansion)
4-1 EVAPORATION
Liquid refrigerant at a low temperature
passes into evaporator where it extract heat from the
product to be cooled. Due to absorption of extract
heat liquid refrigerant turns into vapour, and enters in
to the compressor.
COEFFICIENT OF PERFORMANCE
Work input W=H2-H1
Refrigerating effect N=H1-H4
Since, during the process 3-4, enthalpy is constant.
Therefore enthalpy at 4(H4) is equal to enthalpy at
3(H3)
Refrigerating effect N=H1-H3
C.O.P=REF EFFECT /WORK INPUT=H1-H3/H2H1

II. DETAILS OF DESIGN AND
CONSTRUCTION
SELECTION OF COMPRESSOR
Compressor specifications
Motor H.P=1 H.P.
Speed= 640 r.p.m
Cylinder specifications
No of cylinders = 1
Bore diameter = 63.5 mm
Stroke length = 762 mm, Displacement = 4825
cm³
DETAILS OF DESIGN EVAPORATOR
The selected evaporator for the design is
natural convection bare tube, Dry Expansion, Shell
and tube Evaporators.
Heat reaches the Evaporator by all three
methods of heat transfer and conduction and
radiation.

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Inlet temperature of the evaporator coil (T 1) = -1.6°C
Outlet temperature of evaporator coil (T 2) = 3.4°C
Temperature difference between inside and outside
of the evaporator = (3.4)+(1.6) = 5
The overall heat transfer, co-efficient “U” factor
from data tables for copper = 400kcal/m2-hr-°C
Load taken by the evaporator = AU ∆T
i.e. Refrigerating capacity = AU ∆T
Refrigerating capacity = load taken by Evaporator =
1555 = AU ∆T
A = 1555/ U ∆T = 1555/ (400 x 5) = 0.77 m2
Diameter of the coil (D) = 5mm
Then
A = пDL
Length of the coil (L) = A/пD = 0.77/(п x 0.005) =
49.5m2
Length of coil in one turn = 2(40+20)
= 180 cm
Number of turns in the tank = 4950/180
= 27.4 turns, say 28 turns
Provide 10 cm gap between each turn of the coil. The
evaporator coil should be arranged the side of the
tank that will be easy for periodic cleaning.
SELECTION OF CONDENSER
The condenser load can be calculated by the
following equation:
Heat transfer Q=m Cpl (T3-T2)
Load on the condenser = m Cpl (T 3-T4)
Q = heat absorbed in evaporator + heat of
compressor.
Heat absorbed in evaporator = 1555 k cal/h
Heat of compressor = v x 1
= 220 x 3
=640w
= 640 x 0.86
= 550.4 kcal.
Q = 1555 + 550.4 = 2105.4 k cal
Q = UA ∆T
A = 2105.4/ 400 x 22
= 0.239
A = Пdl
d = 5mm
Length of coil (L) = 0.239 / 0.005
= 15.23m
LENGTH IN ONE TURN = (40 + 40) = 80cm
Number of turns required = 15.23 / 0.80
= 19.0389
= 20

DESIGN OF EVAPOURATOR

fig.4
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639 | P a g e
K. Nagalakshmi et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643

www.ijera.com

IV. RESULTS & DISCUSSIONS:
Graphs are drawn from the above tabulated
results.
 Coefficient of Performance with Evaporator
Temperature at a constant Condenser
Temperature.
 Compressor exit Temperature with Evaporator
Temperature at a constant Condenser
Temperature.
 Specific Volume at inlet to Compressor with
Evaporator Temperature.
Variation of Coefficient of performance with
evoparator temperature at condensor
temperature of 30 oc







Replace the compressor.
Flush the entire system clean with alcohol and
let it be free for few hours.
Then rinse it with alcohol again and then blew it
clean with DRY AIR (if you don't have a good
air dryer for your compressor (or have no
compressor), get a good compressed air).
Replace all seals on the spring clamp and screwtogether.
Put the required amount of lubricating oil in the
compressor.
Charge with the new R134A refrigerant

CALCULATIONS
Evaporator Temperature (T 1) = -30ºC
Condenser Temperature (T2¹) = 30ºC
From charts,
At -30ºC, Enthalpy (h1) = 338.143 kJ/kg
Entropy (s1) = 1.57507 kJ/ (kg.K)
At 30ºC, Enthalpy (h2¹) = 363.566 kJ/kg
Entropy (s2¹) = 1.54334 kJ/ (kg.K)
Enthalpy (h3) = 228.540 kJ/kg
From the graph,
s1 = s2 and h3 = h4
We know that,
h2 = h2¹ + Cр (T2 – T2¹)
Equation – A
s2 = s2¹ + Cр ln (T2/T2¹)
1.57507 = 1.54334 + 0.7253 * ln (T2/303)
On simplification we get, T2 = 316.5 K
Substituting in Equation – A we have,
h2 = 363.566 + 0.7253 * (316.5 – 303)
= 373.35 kJ/kg
(1)Refrigerating Effect = h1 – h4
= 109.603 kJ/kg
(2)Coefficient
of
Performance
(C.O.P)
=
Refrigerating Effect / Work done by the Compressor
= (h1 – h4)/ (h2 – h1)
= 3.11
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6
5
4
3
2
1
0

R-12
R-134a

-35 -30 -25 -20 -15 -10 -5 0
Temperature in oC
fig.6 Variation of C.O.P with evaporator temp.at
condenser temperature of 30oc
From the Fig.6 It is observed that the
coefficient of performance of the refrigeration
system is increasing almost linearly as the
Evaporator Temperature is increased when the
refrigerant used was R-12. the shape of the graph is
almost similar when the results were plotted using R134a as the refrigerant however it is observed that
the values of coefficient of performance are slightly
higher in case of refrigerants R-12 . But refrigerant
are R-134a may be preferred because of the zero
value of the ozone depletion potential.
Variation of Coefficient of performance
with evoparator temperature at condensor
temperature of 40 oc
6
5
4
3
2
1
0
C.O.P




III. STEPS FOR CONVERTING R-12
TO R-134A REFRIGERATOR

C.O.P

fig 5.Experimental Set-up

-35 -30 -25 -20 -15 -10 -5
Temperature in oC

R-12
R-134a

0

fig.7 Variation of C.O.P with evaporator temp.at
condenser temperature of 40oc
From the fig.7 It is observed that the
coefficient of performance of the refrigeration
system is increasing almost linearly as the
Evaporator Temperature is increased when the
refrigerant used was R-12. The shape of the graph is
almost similar when the results were plotted using R134a as the refrigerant however it is observed that
640 | P a g e
K. Nagalakshmi et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643

www.ijera.com

the values of coefficient of performance are slightly
higher in case of refrigerants R-12. But refrigerant
are R-134a may be preferred because of the zero
value of the ozone depletion potential
Variation of Coefficient of performance with
evoparator temperature at condensor
temperature of 50 oc

-35 -30 -25 -20 -15 -10 -5
Temperature in

R-12
R-134a

0

oC

fig.8 Variation of C.O.P with evaporator temp.at
condenser temperature of 50oc
From fig8 It is observed that the coefficient
of performance of the refrigeration system is
increasing almost linearly as the Evaporator
Temperature is increased when the refrigerant used
was R-12. The shape of the graph is almost similar
when the results were plotted using R-134a as the
refrigerant however it is observed that the values of
coefficient of performance are slightly higher in case
of refrigerants R-12. But refrigerant are R-134a may
be preferred because of the zero value of the ozone
depletion potential

fig.9 Variation of Compressor Exit Temperature with
evaporator temp.at condenser temperature of 30oc
From fig.9 it is observed that the
compressor exit Temperatures keeping the
Condenser Temperature constant at 30ºC the
Evaporator Temperature is varied from -30ºC to 10ºC at intervals of 10ºC it is absorbed that from the
graph the compressor Temperature as the Evaporator
Temperature is increased from -10ºC to -30 ºC . In
case of R-134a the shape of the graph is similar in
case R-12.

fig.10 Variation of Compressor Exit Temperature
with evaporator temp.at condenser temperature of
40oc
From fig.10 it is observed that the
compressor exit Temperatures keeping the
Condenser Temperature constant at 40ºC the
Evaporator Temperature is varied from -30ºC to 10ºC at intervals of -10ºC it is absorbed that from the
graph the difference in the Compressor exit
temperature between R-12 & R-134a is more at an
Evaporator Temperature of -30 and is relatively less
when the Evaporator Temperature is -10ºC .

fig.11 Variation of Compressor Exit Temperature
with evaporator temp.at condenser temperature of
30oc
From fig.11 it is observed that the
compressor exit Temperatures keeping the
Condenser Temperature constant at 50ºC the
Evaporator Temperature is varied from -30ºC to 10ºC at intervals of -10ºC it is absorbed that from the
graph the difference in the Compressor exit
temperature between R-12 & R-134a is more at an
Evaporator Temperature of -30ºC and is relatively
less when the Evaporator Temperature is -10ºC

Specific volume

C.O.P

6
5
4
3
2
1
0

0.25
0.2
0.15
0.1
0.05
0
-40

-30

-20

-10

Evaporator temperature

R-12
R-134a

0

fig.12 Variation of specific volume with evaporator
temperature
www.ijera.com

641 | P a g e
K. Nagalakshmi et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643
According to the graph fig.12 the specific
volume is plotted against Evaporator Temperature it
is observed that the difference in specific volume
between R-12 & R-134a is less at an evaporator
Temperature of -30ºC and is relatively less when the
Evaporator Temperature is -10ºC .
From the graphs, we know that Coefficient
of Performance for R-12 refrigerant is slightly
greater than that of R-134a refrigerant. Even though
the C.O.P for R-12 refrigerant is slightly greater than
that of R-134a refrigerant, we prefer to use R-134a
refrigerant because its Ozone Depletion Potential
value is zero. Also, the replacement of CFCs with
HFCs provides more efficient refrigeration and does
not act as greenhouse gas and the less electricity is
needed for refrigeration.

V. CONCLUSION
It has been observed that the refrigerator
test rig is very much suitable for educational
purposes. In order to know working of VCR system
practically and also for knowing the pressure and
temperatures at various points of the cycle. These
results will help for modifications and for new
designs. It has been seen from the results and graphs
that COP of R12 is little greater than COP of R134a.
Even though COP of R12 is grater than R134a it
must be replaced withR134a because of following
reasons.
 R134a refrigerant is non-toxic and does not flare
up within the whole range of operational
temperatures.
 Ozone depletion potential ODP=0, global
warming potential GWP=0.25 and Estimated
Atmospheric life EAL=16.
 In Middle temperature refrigeration facilities
and air conditioning systems, refrigerating factor
of R134a is equal to the factor for R12 or higher
than that.
 In high temperature refrigeration facilities,
specific cold-productivity when operating on
R134a is also a bit higher than that of R12.
 Increasing of dehumidifying ability of filter
dehydrators due to high hygroscopic property of
R134a system-synthetic oil.
 Improvement of widely used all over the world
as a main substitute of R12 for refrigeration
equipment operating within middle-temperature
range. It is used in automobile air-conditioners,
domestic refrigerators, commercial refrigeration
middle-temperature
equipment,
industrial
facilities, air-conditioning systems in building
and industrial areas, as well as on refrigeration
transport.
 As R134a molecule has smaller size than R12
molecule which makes danger of leakage, this
can be avoided by using suitable materials, in
particular, with pads, made of such materials as
www.ijera.com

www.ijera.com

“Buna-N”, “Khailaon”, “Neopren”, “Nordel
which are more compatible with R134a.

REFERENCES
[1]

[2]

[3]
[4]

[5]

[6]

[7]

[8]

[9]

[10]

[11]

S.B. Riffat (2007), “ Comparision of R134a
and R12 refrigerants in a vapour
compression system”, proceedings of the
International Journal of Energy Research,
University of Nottingham, Nottingham,
U.K, vol .17, pages 439-442.
N.J.Shanland (1989), “ Thermo physical
properties of 1,1,1,2 – tetra fluoro ethane
(R134a)”, proceedings of the International
Journal of Thermophysics, Netherlands, vol
.10, No.3, PP 591-603.
C.Aprea (2001), Department of Mechanical
Engineering, University of Salerno, Italy.
Molina M.J and Rowlands (1974), “
Stratospheric
sink
for
chlorofluoro
methanes,
chlorine
atom
catalysed
destruction of ozone”, vol.249, PP 808-812.
Parmer .A.S (1995), “ Performance fo
hydrocarbon refrigerants in motor car airconditioning”, B.E.thesis, School of
Mechanical
and
Manufacturing
Engineering, The University of New South
Wales, Sydney.
K.Mani and V. Selladura (2008),“
Experimental analysis of a new refrigerant
mixture
as
drop-in
replacement”.
Proceedings of the International Journal of
Thermal Sciences, vol.47, pages 1490-1495.
M.Mohanraj, S.Jayraj & C.Muraleetharan
(2008),“Environmental friendly alternatives
to halogenated refrigerants”.The review of
the International Journal of Greenhouse Gas
Control.
A.Anderson and I.Potts (2003), “A
comparision of the operating performance
of alternative refrigerants”. The review of
Applied Thermal Engineering, vol .23,
pages 1441-1451.
M.Fatouh, M.EI Kafaty (2006),“Assessment
of propane/commercial butane mixture as
possible alternatives to R134a in domestic
refrigerators”. The review of the energy
conversion and management, vol .47, pages
2644-2658.
Gallagher,
J.
Huber
(1993),
“
Thermodynamic properties of refrigerants
and refrigerants mixtures Database (ref
prop)”, version 4.0 user’s guide, NIST
standard reference database 23, NIST,
Gaithersburg MD.
S.C. Arora and S.Domakundwar, a course
in Refrigeration and Air Conditioning,
Dhanpat Rai and sons, 1996.

642 | P a g e
K. Nagalakshmi et al Int. Journal of Engineering Research and Applications
ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643
[12]
[13]

[14]
[15]
[16]
[17]

www.ijera.com

Dossat R.J., Principles of refrigeration, John
Wiley, S.I. Version (1989).
W.F.Stoecker, Refrigeration and Air
Conditioning,
McGraw-Hill
Book
Company, 1989.
Jordon and Priester, Refrigeration and Air
Conditioning, 1985.
V.K.Jain,
Refrigetration
and
Air
Conditioning – S.Chand Company, 1996.
http://www.brazeway.com/refrigeration
http://progdev.sait.ab.ca/pwen220/119.refcom.htm

www.ijera.com

643 | P a g e

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Cu4201638643

  • 1. K. Nagalakshmi et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643 RESEARCH ARTICLE www.ijera.com OPEN ACCESS The Design and Performance Analysis of Refrigeration System Using R12 & R134a Refrigerants K. Nagalakshmi1, G. Marurhiprasad Yadav2 1 . Mechanical engineer at St.Jhons College of Engg &Technology, Yemmiganur-518360, A. P, India. . Associate professor, Department of Mechanical engineering, St.Jhons College of Engg &Technology, Yemmiganur-518360, A. P, India. 2 ABSTRACT The design and performance analysis of refrigeration system using R12 & R134a refrigerants are presented in this report. The design calculations of the suitable and necessary refrigerator equipment and their results are also reported here. CFC-12 is the most widely used refrigerant. It serves both in residential and commercial applications, from small window units to large water chillers, and everything in between. Its particular combination of efficiency, capacity and pressure has made it a popular choice for equipment designers. Nevertheless, it does have some ODP, so international law set forth in the Montreal Protocol has put CFC-12 on a phase out schedule.HFC-134a has been established as a drop-in alternative for CFC-12 in the industry due to their zero Ozone Depletion Potential (ODP) and similarities in thermodynamic properties and performance. However, when a system is charged with a HFC-134a compressor oil has to be changed.Not enough research has been done to cover all aspects of alternative refrigerants applications in the systems. This project intended to explore behavior of this alternative refrigerants compare to CFC-12 and challenges the industry is facing in design, operation services and maintenance of these equipments.The purpose of this project is to investigate behavior of R134a refrigerant. This includes performance and efficiency variations when it replaces R12 in an existing system as well as changes involved in maintaining the system charged with R134a. This project is intended to address challenges faced in the real world and some practical issues. Theoretical and experimental approaches used as a methodology in this work. Keywords - alternate refrigirents, evaporator, HCFCs, ODP, GWP. I. INTRODUCTION Refrigeration is concerned with the absorption of heat from where it is objectionable plus its transfer to and rejection at a place where it is unobjectionable. Regardless of means by which is heat transfer is accomplished; the problem is one of applied thermodynamics. In some methods of refrigeration the working medium that approaches perfect gases may be applied.A refrigerant is a compound used in a heat cycle that undergoes a phase change from a gas to a liquid and back. The two main uses of refrigerants are refrigerators/freezers and air conditioners. In broadest sense the word refrigerant is also applied to such secondary cooling medium as brine solutions, cooled water. The refrigerants include only those working mediums, which pass through the cycle or evaporation, recovery, compression and liquefaction. ANALYSIS OF VAPOUR COMPRESSION CYCLE DIAGRAM The flow diagram T-Ǿ and P-H diagrams of a vapour compression refrigerating system given below. www.ijera.com fIg.1 1-2 ISENTROPIC COMPRESSION Refrigerant vapour received evaporator is compressed isentropically compressor by external source of energy from in a fig.2 (work in out), pressure and temperature increase. 638 | P a g e
  • 2. K. Nagalakshmi et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643 2-3 CONDENSATION Compressor discharges vapour into the condenser where it condensed completely i.e. turns in to liquid. Heat is rejected from the refrigerant to cooling medium, usually air or water. 3-4 EXPANSION From condenser liquid refrigerant passes through the expansion valve where it is throttled resulting in a drop of temperature and pressure. However, enthalpy remains constant (throttling expansion) 4-1 EVAPORATION Liquid refrigerant at a low temperature passes into evaporator where it extract heat from the product to be cooled. Due to absorption of extract heat liquid refrigerant turns into vapour, and enters in to the compressor. COEFFICIENT OF PERFORMANCE Work input W=H2-H1 Refrigerating effect N=H1-H4 Since, during the process 3-4, enthalpy is constant. Therefore enthalpy at 4(H4) is equal to enthalpy at 3(H3) Refrigerating effect N=H1-H3 C.O.P=REF EFFECT /WORK INPUT=H1-H3/H2H1 II. DETAILS OF DESIGN AND CONSTRUCTION SELECTION OF COMPRESSOR Compressor specifications Motor H.P=1 H.P. Speed= 640 r.p.m Cylinder specifications No of cylinders = 1 Bore diameter = 63.5 mm Stroke length = 762 mm, Displacement = 4825 cm³ DETAILS OF DESIGN EVAPORATOR The selected evaporator for the design is natural convection bare tube, Dry Expansion, Shell and tube Evaporators. Heat reaches the Evaporator by all three methods of heat transfer and conduction and radiation. www.ijera.com Inlet temperature of the evaporator coil (T 1) = -1.6°C Outlet temperature of evaporator coil (T 2) = 3.4°C Temperature difference between inside and outside of the evaporator = (3.4)+(1.6) = 5 The overall heat transfer, co-efficient “U” factor from data tables for copper = 400kcal/m2-hr-°C Load taken by the evaporator = AU ∆T i.e. Refrigerating capacity = AU ∆T Refrigerating capacity = load taken by Evaporator = 1555 = AU ∆T A = 1555/ U ∆T = 1555/ (400 x 5) = 0.77 m2 Diameter of the coil (D) = 5mm Then A = пDL Length of the coil (L) = A/пD = 0.77/(п x 0.005) = 49.5m2 Length of coil in one turn = 2(40+20) = 180 cm Number of turns in the tank = 4950/180 = 27.4 turns, say 28 turns Provide 10 cm gap between each turn of the coil. The evaporator coil should be arranged the side of the tank that will be easy for periodic cleaning. SELECTION OF CONDENSER The condenser load can be calculated by the following equation: Heat transfer Q=m Cpl (T3-T2) Load on the condenser = m Cpl (T 3-T4) Q = heat absorbed in evaporator + heat of compressor. Heat absorbed in evaporator = 1555 k cal/h Heat of compressor = v x 1 = 220 x 3 =640w = 640 x 0.86 = 550.4 kcal. Q = 1555 + 550.4 = 2105.4 k cal Q = UA ∆T A = 2105.4/ 400 x 22 = 0.239 A = Пdl d = 5mm Length of coil (L) = 0.239 / 0.005 = 15.23m LENGTH IN ONE TURN = (40 + 40) = 80cm Number of turns required = 15.23 / 0.80 = 19.0389 = 20 DESIGN OF EVAPOURATOR fig.4 www.ijera.com 639 | P a g e
  • 3. K. Nagalakshmi et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643 www.ijera.com IV. RESULTS & DISCUSSIONS: Graphs are drawn from the above tabulated results.  Coefficient of Performance with Evaporator Temperature at a constant Condenser Temperature.  Compressor exit Temperature with Evaporator Temperature at a constant Condenser Temperature.  Specific Volume at inlet to Compressor with Evaporator Temperature. Variation of Coefficient of performance with evoparator temperature at condensor temperature of 30 oc     Replace the compressor. Flush the entire system clean with alcohol and let it be free for few hours. Then rinse it with alcohol again and then blew it clean with DRY AIR (if you don't have a good air dryer for your compressor (or have no compressor), get a good compressed air). Replace all seals on the spring clamp and screwtogether. Put the required amount of lubricating oil in the compressor. Charge with the new R134A refrigerant CALCULATIONS Evaporator Temperature (T 1) = -30ºC Condenser Temperature (T2¹) = 30ºC From charts, At -30ºC, Enthalpy (h1) = 338.143 kJ/kg Entropy (s1) = 1.57507 kJ/ (kg.K) At 30ºC, Enthalpy (h2¹) = 363.566 kJ/kg Entropy (s2¹) = 1.54334 kJ/ (kg.K) Enthalpy (h3) = 228.540 kJ/kg From the graph, s1 = s2 and h3 = h4 We know that, h2 = h2¹ + Cр (T2 – T2¹) Equation – A s2 = s2¹ + Cр ln (T2/T2¹) 1.57507 = 1.54334 + 0.7253 * ln (T2/303) On simplification we get, T2 = 316.5 K Substituting in Equation – A we have, h2 = 363.566 + 0.7253 * (316.5 – 303) = 373.35 kJ/kg (1)Refrigerating Effect = h1 – h4 = 109.603 kJ/kg (2)Coefficient of Performance (C.O.P) = Refrigerating Effect / Work done by the Compressor = (h1 – h4)/ (h2 – h1) = 3.11 www.ijera.com 6 5 4 3 2 1 0 R-12 R-134a -35 -30 -25 -20 -15 -10 -5 0 Temperature in oC fig.6 Variation of C.O.P with evaporator temp.at condenser temperature of 30oc From the Fig.6 It is observed that the coefficient of performance of the refrigeration system is increasing almost linearly as the Evaporator Temperature is increased when the refrigerant used was R-12. the shape of the graph is almost similar when the results were plotted using R134a as the refrigerant however it is observed that the values of coefficient of performance are slightly higher in case of refrigerants R-12 . But refrigerant are R-134a may be preferred because of the zero value of the ozone depletion potential. Variation of Coefficient of performance with evoparator temperature at condensor temperature of 40 oc 6 5 4 3 2 1 0 C.O.P   III. STEPS FOR CONVERTING R-12 TO R-134A REFRIGERATOR C.O.P fig 5.Experimental Set-up -35 -30 -25 -20 -15 -10 -5 Temperature in oC R-12 R-134a 0 fig.7 Variation of C.O.P with evaporator temp.at condenser temperature of 40oc From the fig.7 It is observed that the coefficient of performance of the refrigeration system is increasing almost linearly as the Evaporator Temperature is increased when the refrigerant used was R-12. The shape of the graph is almost similar when the results were plotted using R134a as the refrigerant however it is observed that 640 | P a g e
  • 4. K. Nagalakshmi et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643 www.ijera.com the values of coefficient of performance are slightly higher in case of refrigerants R-12. But refrigerant are R-134a may be preferred because of the zero value of the ozone depletion potential Variation of Coefficient of performance with evoparator temperature at condensor temperature of 50 oc -35 -30 -25 -20 -15 -10 -5 Temperature in R-12 R-134a 0 oC fig.8 Variation of C.O.P with evaporator temp.at condenser temperature of 50oc From fig8 It is observed that the coefficient of performance of the refrigeration system is increasing almost linearly as the Evaporator Temperature is increased when the refrigerant used was R-12. The shape of the graph is almost similar when the results were plotted using R-134a as the refrigerant however it is observed that the values of coefficient of performance are slightly higher in case of refrigerants R-12. But refrigerant are R-134a may be preferred because of the zero value of the ozone depletion potential fig.9 Variation of Compressor Exit Temperature with evaporator temp.at condenser temperature of 30oc From fig.9 it is observed that the compressor exit Temperatures keeping the Condenser Temperature constant at 30ºC the Evaporator Temperature is varied from -30ºC to 10ºC at intervals of 10ºC it is absorbed that from the graph the compressor Temperature as the Evaporator Temperature is increased from -10ºC to -30 ºC . In case of R-134a the shape of the graph is similar in case R-12. fig.10 Variation of Compressor Exit Temperature with evaporator temp.at condenser temperature of 40oc From fig.10 it is observed that the compressor exit Temperatures keeping the Condenser Temperature constant at 40ºC the Evaporator Temperature is varied from -30ºC to 10ºC at intervals of -10ºC it is absorbed that from the graph the difference in the Compressor exit temperature between R-12 & R-134a is more at an Evaporator Temperature of -30 and is relatively less when the Evaporator Temperature is -10ºC . fig.11 Variation of Compressor Exit Temperature with evaporator temp.at condenser temperature of 30oc From fig.11 it is observed that the compressor exit Temperatures keeping the Condenser Temperature constant at 50ºC the Evaporator Temperature is varied from -30ºC to 10ºC at intervals of -10ºC it is absorbed that from the graph the difference in the Compressor exit temperature between R-12 & R-134a is more at an Evaporator Temperature of -30ºC and is relatively less when the Evaporator Temperature is -10ºC Specific volume C.O.P 6 5 4 3 2 1 0 0.25 0.2 0.15 0.1 0.05 0 -40 -30 -20 -10 Evaporator temperature R-12 R-134a 0 fig.12 Variation of specific volume with evaporator temperature www.ijera.com 641 | P a g e
  • 5. K. Nagalakshmi et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643 According to the graph fig.12 the specific volume is plotted against Evaporator Temperature it is observed that the difference in specific volume between R-12 & R-134a is less at an evaporator Temperature of -30ºC and is relatively less when the Evaporator Temperature is -10ºC . From the graphs, we know that Coefficient of Performance for R-12 refrigerant is slightly greater than that of R-134a refrigerant. Even though the C.O.P for R-12 refrigerant is slightly greater than that of R-134a refrigerant, we prefer to use R-134a refrigerant because its Ozone Depletion Potential value is zero. Also, the replacement of CFCs with HFCs provides more efficient refrigeration and does not act as greenhouse gas and the less electricity is needed for refrigeration. V. CONCLUSION It has been observed that the refrigerator test rig is very much suitable for educational purposes. In order to know working of VCR system practically and also for knowing the pressure and temperatures at various points of the cycle. These results will help for modifications and for new designs. It has been seen from the results and graphs that COP of R12 is little greater than COP of R134a. Even though COP of R12 is grater than R134a it must be replaced withR134a because of following reasons.  R134a refrigerant is non-toxic and does not flare up within the whole range of operational temperatures.  Ozone depletion potential ODP=0, global warming potential GWP=0.25 and Estimated Atmospheric life EAL=16.  In Middle temperature refrigeration facilities and air conditioning systems, refrigerating factor of R134a is equal to the factor for R12 or higher than that.  In high temperature refrigeration facilities, specific cold-productivity when operating on R134a is also a bit higher than that of R12.  Increasing of dehumidifying ability of filter dehydrators due to high hygroscopic property of R134a system-synthetic oil.  Improvement of widely used all over the world as a main substitute of R12 for refrigeration equipment operating within middle-temperature range. It is used in automobile air-conditioners, domestic refrigerators, commercial refrigeration middle-temperature equipment, industrial facilities, air-conditioning systems in building and industrial areas, as well as on refrigeration transport.  As R134a molecule has smaller size than R12 molecule which makes danger of leakage, this can be avoided by using suitable materials, in particular, with pads, made of such materials as www.ijera.com www.ijera.com “Buna-N”, “Khailaon”, “Neopren”, “Nordel which are more compatible with R134a. REFERENCES [1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] S.B. Riffat (2007), “ Comparision of R134a and R12 refrigerants in a vapour compression system”, proceedings of the International Journal of Energy Research, University of Nottingham, Nottingham, U.K, vol .17, pages 439-442. N.J.Shanland (1989), “ Thermo physical properties of 1,1,1,2 – tetra fluoro ethane (R134a)”, proceedings of the International Journal of Thermophysics, Netherlands, vol .10, No.3, PP 591-603. C.Aprea (2001), Department of Mechanical Engineering, University of Salerno, Italy. Molina M.J and Rowlands (1974), “ Stratospheric sink for chlorofluoro methanes, chlorine atom catalysed destruction of ozone”, vol.249, PP 808-812. Parmer .A.S (1995), “ Performance fo hydrocarbon refrigerants in motor car airconditioning”, B.E.thesis, School of Mechanical and Manufacturing Engineering, The University of New South Wales, Sydney. K.Mani and V. Selladura (2008),“ Experimental analysis of a new refrigerant mixture as drop-in replacement”. Proceedings of the International Journal of Thermal Sciences, vol.47, pages 1490-1495. M.Mohanraj, S.Jayraj & C.Muraleetharan (2008),“Environmental friendly alternatives to halogenated refrigerants”.The review of the International Journal of Greenhouse Gas Control. A.Anderson and I.Potts (2003), “A comparision of the operating performance of alternative refrigerants”. The review of Applied Thermal Engineering, vol .23, pages 1441-1451. M.Fatouh, M.EI Kafaty (2006),“Assessment of propane/commercial butane mixture as possible alternatives to R134a in domestic refrigerators”. The review of the energy conversion and management, vol .47, pages 2644-2658. Gallagher, J. Huber (1993), “ Thermodynamic properties of refrigerants and refrigerants mixtures Database (ref prop)”, version 4.0 user’s guide, NIST standard reference database 23, NIST, Gaithersburg MD. S.C. Arora and S.Domakundwar, a course in Refrigeration and Air Conditioning, Dhanpat Rai and sons, 1996. 642 | P a g e
  • 6. K. Nagalakshmi et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 4, Issue 2( Version 1), February 2014, pp.638-643 [12] [13] [14] [15] [16] [17] www.ijera.com Dossat R.J., Principles of refrigeration, John Wiley, S.I. Version (1989). W.F.Stoecker, Refrigeration and Air Conditioning, McGraw-Hill Book Company, 1989. Jordon and Priester, Refrigeration and Air Conditioning, 1985. V.K.Jain, Refrigetration and Air Conditioning – S.Chand Company, 1996. http://www.brazeway.com/refrigeration http://progdev.sait.ab.ca/pwen220/119.refcom.htm www.ijera.com 643 | P a g e