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International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
344 Vol. 10, Issue 3, pp. 344-353
STUDY ON THE BEHAVIOUR OF CUO NANO PARTICLES IN
RADIATOR HEAT EXCHANGER FOR AUTO MOBILES
V D M Bharathi Mahanti 1*, V Ravi Kumar2**
*1 PG Student, **2Assistant Professor, ASRCE, Tanuku, India
ABSTRACT
In this present study, the forced convective heat transfer performance of automobile radiator has been studied
experimentally by using Nano fluid (CuO-Water) as a coolant for an automobile radiator.. Experimental works
were conducted to investigate the effect of Copper-Oxide (CuO) nanoparticles volume concentration and the
operating temperatures on the rate of Nano fluids heat transfer in a radiator heat Exchanger. CuO nanoparticles
were mixed with the base fluid water and also Sodium Lauryl Sulphate (SLS) powder was added to enhance the
mixing process and stabilize the dispersion of the Nano fluids. Experimental runs were conducted at varying
operating temperatures which include that, CuO-water at different temperature such as 40℃, 50℃, 60℃, 70℃,
75℃, 78℃, 80℃, 83℃. Among the operating temperatures selected for study 80℃, gives the best performance in
heat transfer and the convection heat transfer coefficient. The results of the current work generally indicate that
Nano fluids have the potential to enhance the heat transfer of a compact heat exchanger. Results indicate that,
best overall heat transfer coefficient for the radiator is obtained at a hot fluid inlet temperature of 80℃, and at a
flow rate of 0.075kg/sec.
KEYWORDS- Nano fluids, CuO, Heat Exchangers, Radiator.
I. INTRODUCTION
Automobile Radiators are typical heat exchangers used to cool the engine jacket water. To cool down
the engine, a coolant is passed through the engine block, where it absorbs heat from the engine. The hot
coolant is then fed into the inlet tank of the radiator (located either on the top of the radiator, or along
one side), from which it is distributed across the radiator core through tubes to another tank on the
opposite end of the radiator. As the coolant passes through the radiator tubes on its way to the opposite
tank, it transfers much of its heat to the tubes which, in turn transfer the heat to the fins that are lodged
between each row of tubes. Fins are used to greatly increase the contact surface of the tubes to the air,
thus increasing the exchange efficiency. The cooled coolant is fed back to the engine, and the cycle
repeats. Normally, the radiator does not reduce the temperature of the coolant back to ambient air
temperature, but it is still sufficiently cooled to keep the engine from overheating.
Nano fluids are dilute liquid suspended Nano particles which have only one critical dimension smaller
than ~100nm. Much research work has been made in the past decade to this new type of material
because of its high rated properties and behavior associated with heat transfer. The thermal behavior of
Nano fluids could provide a basis for a huge innovation for heat transfer. Nano fluids are prepared by
dispersing and stably suspending Nano meter sized solid particles in conventional heat transfer fluids.
Nano fluids consist of nanoparticles and base fluids. Nanoparticles are Al2O3, Fe, CuO, etc. Base fluids
can be DI-water, Sodium Lauryl Sulphate, ethylene glycol, pump oil, transformer oil.
II. LITERATURE REVIEW
All internal combustion engines produce heat as a byproduct of combustion and friction. Pistons, valves
and cylinder heads must be cooled to reduce the risk of detonation. Cooling systems must be properly
designed, operated and maintained for proper engine operation and service life. Khot et al, [1]
International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
345 Vol. 10, Issue 3, pp. 344-353
determined various methods for radiator performance evaluation and testing of the radiator are
considered.
JP Yadav and Bharat Raj Singh stated that33% of the energy generated by the engine through
combustion is lost in heat. To minimize the stress on the engine as a result of heat generation, automotive
radiators must be redesigned to be more compact while still maintaining high levels of heat transfer
performance. In an automobile, If this excess heat is not removed, the engine temperature becomes too
high which results in overheating and viscosity breakdown of the lubricating oil, metal weakening of
the overheated engine parts, and stress between engine parts resulting in quicker wear.
Changhua Lin developed a theoretical model for the calculation of Specific Dissipation (SD) to predict
the effect of ambient and coolant radiator inlet temperatures. Results indicated that the effect of ambient
and coolant inlet temperature variation on SD is small (less than 2%) and a 1 % variation in coolant
flow rate will cause about ±0.6% SD variation. Therefore the coolant flow rate should be carefully
controlled. Mintsa [10] predicted overall effect of an increase in the effective thermal conductivity with
an increase in particle volume fraction by using Alumina and Copper Oxide.
K.Y. Leong et al found that the heat transfer rate is increased with increase in volume concentration of
nano particles (ranging from 0% to 2%). About 3.8% heat transfer enhancement was achieved with
addition of 2% copper particles at 6000 and 5000 Reynolds number for air and coolant respectively.
From the above literature, it can be concluded that the excess heat will harm the engine parts. This heat
has to be removed through the radiator in automobiles. This heat removal rate depends mostly on the
coolant flow rate. So, by adding the nanoparticles to the coolant the heat transfer rate will be increased.
Thus, for the present work, we considered the available nanoparticles CuO and a stabilizer as Sodium
Lauryl Sulfate to study the effect on the heat transfer rate in automobile engines, which has not done
before.
III. EXPERIMENTAL SETUP
The performance of an automobile radiator is tested by designing and fabricating a test setup. Different
components used in test setup are shown in below figure 1. One of the types of cross flow heat
exchanger, Maruti Suzuki Alto 800 radiator is used in this experiment. It contains 36 Aluminium pipes
of length and diameters are 31cm and 0.8cm respectively. A Radiator fan of 12V DC supply and requires
4 to 6 Amps of current is used in this project. It consists of 3 blades and frame for create blow. It is
placed in front of the radiator with the help of nut and bolt fittings. This fan draws fresh air through the
radiator i.e., pumping air at ambient temperature to decrease the temperature of coolant. A water pump
of capacity ¼ Hp is used for pumping and circulating the water throughout the system. It is most
desirable one, because it is less in weight and moderate in size. It consists of both suction and discharge
ports.An immersion heater is attached to the thermally insulated water tank and it heats the water, which
is initially filled in the tank. The capacity of this immersion heater is 198°C. A tank of 20 litres capacity
is thermally insulated by insulating material (thermocol), and having 3 ports of suction, delivery and
bypass ports respectively. It also consists of a fitting arrangement for heater. A Rota-meter is used for
measuring the mass flow rate of the hot fluid that is circulating in the radiator of a range 10-100lit/s.
International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
346 Vol. 10, Issue 3, pp. 344-353
Fig 1 Schematic experimental setup
IV. METHODOLOGY
During the experimentation, initially a sufficient amount of water taken into the insulated tank, fitted
with the heater. Then the mixture of CuO and SLS added in proper ratio of volume and stir manually
until it dissolve in water. Then the heater is turned on until the water gains the required hot fluid inlet
temperature (T1). Now switch on the pump to obtain constant coolant mass flow rate as well as the
fan attached to the radiator. Wait for few minutes until the apparatus get stabilized. Then, required
temperature readings are noted by varying the 5 way selector present on the digital logger. This process
is repeated for various temperature of T1. From this experiment, the optimum hot fluid temperature is
obtained. Overall heat transfer coefficient and heat transfer rates are calculated from the recorded values
of coolant inlet (T2), coolant outlet (T3), air inlet (T4), air outlet (T5) temperatures using the governing
equations. Then keeping this optimum operating temperature T1 as constant, the mass flow rate of
coolant is varied from 0.025kg/s to 0.1kg/s in 4 steps. From the above experiments, the optimum
conditions (optimum hot fluid inlet temperature and mass flow rates) of the radiator are calculated.
International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
347 Vol. 10, Issue 3, pp. 344-353
Fig 2 Experimental setup for testing the performance of radiator
V. RESULTS & DISCUSSION
The performance of an automobile radiator varies with different parameters, in our experiment we are
concentrating on hot fluid inlet temperature and mass flow rate depending on these two parameters we
are evaluating the performance of an automobile radiator. To know the optimum conditions i.e., the
temperature and the mass flow rate where the efficiency of the automobile radiator increases, firstly we
have to maintain either temperature or mass flow rate as a constant. Let us maintain the temperature as
a constant and get know at what temperature the overall heat transfer coefficient will be more to the
optimum temperature value the coolant is circulated through the radiator at different temperature such
as 40℃ , 50℃, 60℃, 70 ℃, 75℃, 78℃, 80°C, 83°C.
5.1 RESULTS
Temperature Reading Tables At Different Hot Fluid Inlet Temperatures
At first coolant pumped at temperature of (𝑇2) 40℃ and the value of coolant outlet temperature (𝑇3), air
inlet temperature (𝑇4), air outlet temperature (𝑇5) are noted with the help of digital indicator. By using
all these parameters rate of heat transfer and then overall heat transfer coefficient values are calculated.
The values that are obtained are tabulated in the following tables.
Table 1: Experimental results at various hot fluid Inlet Temperatures
SNo T1 T2 T3 T4 Heat Transfer Rate
Overall Heat Transfer
Coefficient
1 40 39 31 33 313.5 42.8
2 50 47 34 43 940.5 128.26
3 60 59 34 54 313.5 42.84
4 70 66 35 52 1254 167.72
5 75 68 35 55 627 89.76
6 78 73 35 59 1567.5 214.87
7 80 75 35 59 1567.5 234.47
8 83 80 35 62 1567.5 219.41
International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
348 Vol. 10, Issue 3, pp. 344-353
Graph 1. Effect of hot fluid inlet temperature on Heat transfer and Overall heat transfer coefficient
Graph 2. Variation of T2, T3 and T4 with Inlet radiator temperature
Optimum Hot Fluid Inlet Temperature
At 800
C the optimum overall heat transfer coefficient value is obtained, that is 234.47 W/m2o
C, at a rate
of heat transfer 1567.5 W.
From the table, we can see that the hot fluid inlet temperature is 800
C the overall heat transfer coefficient
value is 234.47 W/m2o
C and the further increase in the coolant inlet temperature the overall heat transfer
coefficient value is being decreased. As the overall heat transfer coefficient value is more at 80o
C we
can say that optimum temperature value is 800
C. Now maintaining the coolant inlet temperature
constant at 800
C we have to vary the mass flow rates to find out that what temperature and mass flow
rate the overall heat transfer coefficient will be more.
The coolant mass flow rate are varied such as 0.035kg/s, 0.05kg/s, 0.075kg/s, 0.1kg/s. the experiment
is carried out by maintaining coolant inlet temperature at 80 and varying the mass flow rate. The values
of coolant outlet temperature (𝑇3), air inlet temperature (𝑇4), air outlet temperature (𝑇5) are noted with
the help of digital indicator. By using all these parameters rate of heat transfer and then overall heat
transfer coefficient values are calculated. The values that are obtained are tabulated in the following
tables.
20
30
40
50
60
70
80
90
40 50 60 70 75 78 80 83
Temperaturesin°C
Inlet Radiator Temperature in °C
T2
T3
T4
25
75
125
175
225
275
0
300
600
900
1200
1500
1800
40 50 60 70 75 78 80 83
OveralllHeatTransferCoefficient
W/mK
HeatTransferRateW
Inlet Temperature of Radiator in °C
Heat Transfer Rate
Overall Heat Transfer Coefficient
International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
349 Vol. 10, Issue 3, pp. 344-353
Temperature Reading Tables of Different Mass Flow Rates at Constant Hot Fluid Inlet
Temperature
Optimum Hot Fluid Mass Flow Rate
The optimum over all heat transfer coefficient value is obtained at 0.075 kg/s of mass flow rate and
keep the hot fluid inlet temperature value as constant.
Table 2: Optimum mass flow rate
Flow rate
(kg/s)
Heat transfer rate(Q)
(W)
Overall heat transfer coefficient(U)
(w/m2 o
C)
0.025 585.2 98.98
0.050 836 143.56
0.075 1254 177.93
0.1 1254 172.98
From the above table, we can see that the overall heat transfer coefficient value is more when the coolant
mass flow rate is 0.075kg/s and the further increase in mass flow rate the overall heat transfer coefficient
value is being decreased. So we can say that 0.075kg/s is the optimum mass flow rate where maximum
overall heat transfer coefficient values will be more.
The overall heat transfer coefficient values at different coolant inlet temperature are summarized in the
table
Graph 3. Coolant Flow rate vs Heat transfer Rate
Coolant Flow rate vs Heat transfer Rate and Overall heat transfer coefficient
According to the values obtained a graph is plotted between coolant inlet temperature and overall heat
transfer coefficient. Graph is plotted between overall heat transfer coefficient and hot fluid inlet
temperature.
The values of coolant inlet temperature are taken on x-axis and the values of overall heat transfer
coefficient are taken on y-axis. From the graph 5.1 it is clear that the overall heat transfer coefficient
value is maximum at coolant inlet temperature 80℃ and the value is 234.47 W/m2o
C.Similarly, the
overall heat transfer coefficient values at different mass flow rate are summarized in the table.
In the above table represents the optimum flow rate of 0.075m/sec add obtained maximum Overall heat
transfer coefficient value is 177.78 W/m2o
C.it is best result for this experiment. According to the values
obtained a graph is plotted between mas flow rate and overall heat transfer coefficient.
90
110
130
150
170
190
0
200
400
600
800
1000
1200
1400
0.025 0.05 0.075 0.1
OverallHeatTransferCoefficient
HeatTransferRateinW
Coolant Flow Rate in Kg/s
Heat transfer rate(Q)
Overall heat transfer coefficient(U)
International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
350 Vol. 10, Issue 3, pp. 344-353
Table 3. Overall heat transfer coefficient values at different mass flow rates
SNo
Mass Flow
rate Kg/s
T2 °C T3 °C T4°C T5 °C
Heat Transfer
Rate Watts
Overall Heat
Transfer
Coefficient
W/m K
1 0.035 80 76 35 70 585.2 98.98
2 0.05 80 76 36 70 836 143.56
3 0.075 80 76 35 64 1254 177.93
4 0.1 80 77 35 64 1254 172.93
Graph 4. Variation of Temperatures with different coolant mass flow rates
Graph 5. Graph for overall heat transfer coefficient at different mas flow rates.
70
100
130
160
190
220
0
200
400
600
800
1000
1200
1400
0.035 0.05 0.075 0.1
OveralllHeatTransferCoefficient
HeatTransferRateW
Coolant Mass flow rate in Kg/s
Heat Transfer Rate
Overall Heat Transfer Coefficient
20
30
40
50
60
70
80
90
0.035 0.05 0.075 0.1
Temperaturesin°C
Coolant mass flow rate in Kg/s
T2 T3
T4 T5
International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
351 Vol. 10, Issue 3, pp. 344-353
The values of mass flow rate are taken on x-axis and overall heat transfer coefficient values on y-axis.
From the graph it is clear that the overall heat transfer coefficient value is maximum when the mass
flow rate is 0.075kg/s and the value is 177.93 W/m2o
C
Similarly, the overall heat transfer coefficient of CuO at optimum temperature and mass flow rate is
summarized in the following table
Table 4. Overall heat transfer coefficient at various sintering temperatures
S no
Sintering
Temperature °C
Hot Fluid inlet
Temperature °C
Mass Flow
rate Kg/s
Heat Transfer
Rate W
Avg Overall Heat
Transfer Coefficient
W/m K
1 Normal 80 0.075 214.97 98.98
2 150 80 0.075 222.02 143.56
3 250 80 0.075 247.06 177.93
According to the values obtained a graph is plotted between sintering condition and overall heat transfer
coefficient.
Graph 6. Graph plotted between overall heat transfer coefficient and sintering condition.
The values of sintering condition are taken on x-axis and values of overall heat transfer coefficient are
taken on y-axis. From the graph it is clear that the overall heat transfer coefficient value is maximum at
sintering condition at 250℃ and the value is 247.06 w/𝑚2
℃
5. 2 Discussion
 Experiments are conducted to find out optimum hot fluid temperature and mass flow rate.
 As per the results obtained from the graph plotted between overall heat transfer coefficient and
mass flow rate, the overall heat transfer value is 247.06W/𝑚2
℃.
 The maximum value of overall heat transfer coefficient and heat transfer rate are found to be
80℃ fluid inlet temperature and 0.075kg/sec mass flow rate.
 Addition of small amount of CuO nanoparticles into demineralized water as the base fluid
would increase the rate of heat transfer and convection heat transfer coefficient by at least
17.3% and 40% respectively.
 Nano fluids as the coolant for automotive radiator and various ranges of operating temperatures
and volume concentrations may need to be explored in order to better optimal conditions.
0
40
80
120
160
200
0
60
120
180
240
Normal 150 250 OveralllHeatTransferCoefficient
HeatTransferRateW
Sintering Temperature °C
Heat Transfer Rate
Avg Overall Heat Transfer
Coefficient
International Journal of Advances in Engineering & Technology, June, 2017.
©IJAET ISSN: 22311963
352 Vol. 10, Issue 3, pp. 344-353
VI. CONCLUSION
In this experimental study, the heat transfer performance of automobile radiator has been estimated by
using CuO Nano fluids at various coolant temperature ranges and mass flow rates.
 The optimum hot fluid temperature and mass flow rates are determined using its inlet
temperature based on the overall heat transfer coefficient and heat transfer rates.
 The Nano coolants found to enhance the thermal performance of the automobile radiator.
 With the increase in the coolant flow rate, the heat transfer performance increase for the various
coolants namely CuO-water.
 After several iterations the optimum overall heat transfer coefficient is find out to be 247.06
W/m² °C at the mass flow rate 0.075kg/sec and inlet temperature 80℃.
VII. FUTURE SCOPE
In the application of Nanofluids instead of water enhance thermal performance of the automobile
radiator system, some associated problems such as stability and sedimentation should also be studied
in detail.
The research work also drawn the attention of the many researchers to concentration on farm equipment
development for improved performance in their field. The thermal management of heavy vehicles such
as cars, tractor and earth moving equipment through Nano mechanism are essential areas for future
researchers. Nano fluids shows promising potential as the coolant for automotive radiator and more
ranges of operating temperature and volume concentrations may need to be explored in order to better
understand its full potential.
ACKNOWLEDGMENT
The Author would like to thank all the persons who helped in the completion of this experimental work.
Also thanks are extended to ASR College of Engineering, Tanuku, India for support throughout the
execution of the experimental work.
REFERENCES
[1] Prof. A. R. Khot, Prof. D. G. thom bare,prof.s.p. Gaikwad and Prof. A. S. “Adadande were reported
various methods for radiator performance evaluation and testing of the radiator” (IOSR-JMCE)
ISSN:2278-1684,PP:07-14.
[2] Eastmen, J. A. Choi, S. U. S., Li, S., Yu, W., and Thompson, LJ., 2001, “Anomalously Increased
Effective Thermal Conductivies of Ethylene Glycol- Based Nnofluids Containing Copper
Particles,”Appl. Phys. Lett., 78(6), pp.718-720
[3] Heris, S. Z., Esfahany, M. N., and Etemad, S.Gh., 2006, “Investigation of Convective Heat Transfer of
A𝑙2 𝑂3/Water Nanofluid in Circular Tube,” Int. J. Heat Fluid Flow, 28, pp. 203-210
[4] vajjah,R.S ,Das, D.K., and Namburu, P.K.,2010, “numerical study of fluid dynamics and heat transfer
performance of Al2 O3 and CuO Nano fluids in the Flat tubes of a radiator”,
Int. J. Heat fluid flow, 31,pp,613-621.
[5] Nariki, M., Peyghambarzadeh, S.M., hashemabadi, S.H., and vermahmoudi, Y., 2013,
“Parametric study of overall heat transfer coefficient of CuO/water nano fluids in a car radiator”, Int. J.
Them. Sci., 66,pp. 82-90.
[6] Leong, K. Y., R. Saidur, S. N. Kazi, and a. H. Mamun. 2010. “Performance Investigation of an
Automotive Car Radiator Operated with NanofluidBased Coolants (nanofluid as a Coolant in a
Radiator).” Applied Thermal Engineering 30 (17-18). Elsevier Ltd: 2685–92
doi:10.1016/j.applthermaleng.2010.07.019.
[7] Lomascolo, Mauro, Gianpiero Colangelo, Marco Milanese, and Arturo De Risi. 2015. “Review of Heat
Transfer in Nano Fl Uids : Conductive, Convective and Radiative Experimental Results.” Renewable
and Sustainable Energy Reviews 43. Elsevier: 1182
[8] Rahul A. Bhogare, B. S. Kothawale. “A Review on applications and challenges of Nano-fluids as coolant in
Automobile Radiator". International Journal of Scientific and Research Publications, Volume 3, Issue 8, August 2013
[9] P. sai sasank1, V.Govinda naik. Empirical Review on Car Radiator Using H2O and Al2O3. International Journal of
Innovative Research in Science, Engineering and Technology. Vol. 3, Issue 10, October2014
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[10] Mintsa HA, Roy G, Nguyen CT, Doucet D. New temperature dependent thermal conductivity data for water-based
nanofluids. Int J Therm Sci 2009;48(2):363–71.
[11] D.H. Kumar, H.E. Patel, V.R. Kumar, T. Sundararajan, T. Pradeep, S.K.vDas, Model for heat conduction in
nanofluids, Physical Review Letters 93 (14) (2004) 1–3.
[12] H. Xie, M. Fujii, X. Zhang, Effect of interfacial nanolayer on the effective thermal conductivity of nanoparticle-fluid
mixture, International Journal of Heat and Mass Transfer 48 (2005) 2926–2932.
[13] S.P. Jang, S.U.-S. Choi, Role of Brownian motion in the enhanced thermal conductivity of nanofluids, Applied
Physics Letters 84 (2004) 4316.
[14] C.H. Li, G.P. Peterson, Experimental investigation of temperature and volume fraction variations on the effective
thermal conductivity of nanoparticle suspensions (nanofluids), Journal of Applied Physics 99 (084314) (2006) 1–8.
[15] R. Prasher, P. Bhattacharya, P.E. Phelan, Thermal conductivity of nanoscale colloidal solutions nanofluids, Physical
Review Letters 94 (025901) (2005) 1–4.
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fluids, Thermochimica Acta 455 (2007) 66–69.
AUTHORS BIOGRAPHY
V D M Bharathi Mahanti was born in Tanuku, India, in Year 1989. She received the
Bachelor’s degree in Mechanical engineering from the Jawaharlal Nehru Technological
University, Kakinada, in Year 2011. She is currently pursuing the Master degree in
Thermal engineering from the Jawaharlal Nehru Technological University,
Kakinada. Her research interests includes Design of Heat exchangers, Nano fluids,
Thermal systems design, Renewable sources of energy
V. Ravi Kumar graduated in Mechanical engineering from JNTUK His research interests
includes Robotics, Nano technology, Thermal systems design, Renewable sources of
energy. Currently in working on the Artificial intelligence and Green energy systems.

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STUDY ON THE BEHAVIOUR OF CUO NANO PARTICLES IN RADIATOR HEAT EXCHANGER FOR AUTO MOBILES

  • 1. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 344 Vol. 10, Issue 3, pp. 344-353 STUDY ON THE BEHAVIOUR OF CUO NANO PARTICLES IN RADIATOR HEAT EXCHANGER FOR AUTO MOBILES V D M Bharathi Mahanti 1*, V Ravi Kumar2** *1 PG Student, **2Assistant Professor, ASRCE, Tanuku, India ABSTRACT In this present study, the forced convective heat transfer performance of automobile radiator has been studied experimentally by using Nano fluid (CuO-Water) as a coolant for an automobile radiator.. Experimental works were conducted to investigate the effect of Copper-Oxide (CuO) nanoparticles volume concentration and the operating temperatures on the rate of Nano fluids heat transfer in a radiator heat Exchanger. CuO nanoparticles were mixed with the base fluid water and also Sodium Lauryl Sulphate (SLS) powder was added to enhance the mixing process and stabilize the dispersion of the Nano fluids. Experimental runs were conducted at varying operating temperatures which include that, CuO-water at different temperature such as 40℃, 50℃, 60℃, 70℃, 75℃, 78℃, 80℃, 83℃. Among the operating temperatures selected for study 80℃, gives the best performance in heat transfer and the convection heat transfer coefficient. The results of the current work generally indicate that Nano fluids have the potential to enhance the heat transfer of a compact heat exchanger. Results indicate that, best overall heat transfer coefficient for the radiator is obtained at a hot fluid inlet temperature of 80℃, and at a flow rate of 0.075kg/sec. KEYWORDS- Nano fluids, CuO, Heat Exchangers, Radiator. I. INTRODUCTION Automobile Radiators are typical heat exchangers used to cool the engine jacket water. To cool down the engine, a coolant is passed through the engine block, where it absorbs heat from the engine. The hot coolant is then fed into the inlet tank of the radiator (located either on the top of the radiator, or along one side), from which it is distributed across the radiator core through tubes to another tank on the opposite end of the radiator. As the coolant passes through the radiator tubes on its way to the opposite tank, it transfers much of its heat to the tubes which, in turn transfer the heat to the fins that are lodged between each row of tubes. Fins are used to greatly increase the contact surface of the tubes to the air, thus increasing the exchange efficiency. The cooled coolant is fed back to the engine, and the cycle repeats. Normally, the radiator does not reduce the temperature of the coolant back to ambient air temperature, but it is still sufficiently cooled to keep the engine from overheating. Nano fluids are dilute liquid suspended Nano particles which have only one critical dimension smaller than ~100nm. Much research work has been made in the past decade to this new type of material because of its high rated properties and behavior associated with heat transfer. The thermal behavior of Nano fluids could provide a basis for a huge innovation for heat transfer. Nano fluids are prepared by dispersing and stably suspending Nano meter sized solid particles in conventional heat transfer fluids. Nano fluids consist of nanoparticles and base fluids. Nanoparticles are Al2O3, Fe, CuO, etc. Base fluids can be DI-water, Sodium Lauryl Sulphate, ethylene glycol, pump oil, transformer oil. II. LITERATURE REVIEW All internal combustion engines produce heat as a byproduct of combustion and friction. Pistons, valves and cylinder heads must be cooled to reduce the risk of detonation. Cooling systems must be properly designed, operated and maintained for proper engine operation and service life. Khot et al, [1]
  • 2. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 345 Vol. 10, Issue 3, pp. 344-353 determined various methods for radiator performance evaluation and testing of the radiator are considered. JP Yadav and Bharat Raj Singh stated that33% of the energy generated by the engine through combustion is lost in heat. To minimize the stress on the engine as a result of heat generation, automotive radiators must be redesigned to be more compact while still maintaining high levels of heat transfer performance. In an automobile, If this excess heat is not removed, the engine temperature becomes too high which results in overheating and viscosity breakdown of the lubricating oil, metal weakening of the overheated engine parts, and stress between engine parts resulting in quicker wear. Changhua Lin developed a theoretical model for the calculation of Specific Dissipation (SD) to predict the effect of ambient and coolant radiator inlet temperatures. Results indicated that the effect of ambient and coolant inlet temperature variation on SD is small (less than 2%) and a 1 % variation in coolant flow rate will cause about ±0.6% SD variation. Therefore the coolant flow rate should be carefully controlled. Mintsa [10] predicted overall effect of an increase in the effective thermal conductivity with an increase in particle volume fraction by using Alumina and Copper Oxide. K.Y. Leong et al found that the heat transfer rate is increased with increase in volume concentration of nano particles (ranging from 0% to 2%). About 3.8% heat transfer enhancement was achieved with addition of 2% copper particles at 6000 and 5000 Reynolds number for air and coolant respectively. From the above literature, it can be concluded that the excess heat will harm the engine parts. This heat has to be removed through the radiator in automobiles. This heat removal rate depends mostly on the coolant flow rate. So, by adding the nanoparticles to the coolant the heat transfer rate will be increased. Thus, for the present work, we considered the available nanoparticles CuO and a stabilizer as Sodium Lauryl Sulfate to study the effect on the heat transfer rate in automobile engines, which has not done before. III. EXPERIMENTAL SETUP The performance of an automobile radiator is tested by designing and fabricating a test setup. Different components used in test setup are shown in below figure 1. One of the types of cross flow heat exchanger, Maruti Suzuki Alto 800 radiator is used in this experiment. It contains 36 Aluminium pipes of length and diameters are 31cm and 0.8cm respectively. A Radiator fan of 12V DC supply and requires 4 to 6 Amps of current is used in this project. It consists of 3 blades and frame for create blow. It is placed in front of the radiator with the help of nut and bolt fittings. This fan draws fresh air through the radiator i.e., pumping air at ambient temperature to decrease the temperature of coolant. A water pump of capacity ¼ Hp is used for pumping and circulating the water throughout the system. It is most desirable one, because it is less in weight and moderate in size. It consists of both suction and discharge ports.An immersion heater is attached to the thermally insulated water tank and it heats the water, which is initially filled in the tank. The capacity of this immersion heater is 198°C. A tank of 20 litres capacity is thermally insulated by insulating material (thermocol), and having 3 ports of suction, delivery and bypass ports respectively. It also consists of a fitting arrangement for heater. A Rota-meter is used for measuring the mass flow rate of the hot fluid that is circulating in the radiator of a range 10-100lit/s.
  • 3. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 346 Vol. 10, Issue 3, pp. 344-353 Fig 1 Schematic experimental setup IV. METHODOLOGY During the experimentation, initially a sufficient amount of water taken into the insulated tank, fitted with the heater. Then the mixture of CuO and SLS added in proper ratio of volume and stir manually until it dissolve in water. Then the heater is turned on until the water gains the required hot fluid inlet temperature (T1). Now switch on the pump to obtain constant coolant mass flow rate as well as the fan attached to the radiator. Wait for few minutes until the apparatus get stabilized. Then, required temperature readings are noted by varying the 5 way selector present on the digital logger. This process is repeated for various temperature of T1. From this experiment, the optimum hot fluid temperature is obtained. Overall heat transfer coefficient and heat transfer rates are calculated from the recorded values of coolant inlet (T2), coolant outlet (T3), air inlet (T4), air outlet (T5) temperatures using the governing equations. Then keeping this optimum operating temperature T1 as constant, the mass flow rate of coolant is varied from 0.025kg/s to 0.1kg/s in 4 steps. From the above experiments, the optimum conditions (optimum hot fluid inlet temperature and mass flow rates) of the radiator are calculated.
  • 4. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 347 Vol. 10, Issue 3, pp. 344-353 Fig 2 Experimental setup for testing the performance of radiator V. RESULTS & DISCUSSION The performance of an automobile radiator varies with different parameters, in our experiment we are concentrating on hot fluid inlet temperature and mass flow rate depending on these two parameters we are evaluating the performance of an automobile radiator. To know the optimum conditions i.e., the temperature and the mass flow rate where the efficiency of the automobile radiator increases, firstly we have to maintain either temperature or mass flow rate as a constant. Let us maintain the temperature as a constant and get know at what temperature the overall heat transfer coefficient will be more to the optimum temperature value the coolant is circulated through the radiator at different temperature such as 40℃ , 50℃, 60℃, 70 ℃, 75℃, 78℃, 80°C, 83°C. 5.1 RESULTS Temperature Reading Tables At Different Hot Fluid Inlet Temperatures At first coolant pumped at temperature of (𝑇2) 40℃ and the value of coolant outlet temperature (𝑇3), air inlet temperature (𝑇4), air outlet temperature (𝑇5) are noted with the help of digital indicator. By using all these parameters rate of heat transfer and then overall heat transfer coefficient values are calculated. The values that are obtained are tabulated in the following tables. Table 1: Experimental results at various hot fluid Inlet Temperatures SNo T1 T2 T3 T4 Heat Transfer Rate Overall Heat Transfer Coefficient 1 40 39 31 33 313.5 42.8 2 50 47 34 43 940.5 128.26 3 60 59 34 54 313.5 42.84 4 70 66 35 52 1254 167.72 5 75 68 35 55 627 89.76 6 78 73 35 59 1567.5 214.87 7 80 75 35 59 1567.5 234.47 8 83 80 35 62 1567.5 219.41
  • 5. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 348 Vol. 10, Issue 3, pp. 344-353 Graph 1. Effect of hot fluid inlet temperature on Heat transfer and Overall heat transfer coefficient Graph 2. Variation of T2, T3 and T4 with Inlet radiator temperature Optimum Hot Fluid Inlet Temperature At 800 C the optimum overall heat transfer coefficient value is obtained, that is 234.47 W/m2o C, at a rate of heat transfer 1567.5 W. From the table, we can see that the hot fluid inlet temperature is 800 C the overall heat transfer coefficient value is 234.47 W/m2o C and the further increase in the coolant inlet temperature the overall heat transfer coefficient value is being decreased. As the overall heat transfer coefficient value is more at 80o C we can say that optimum temperature value is 800 C. Now maintaining the coolant inlet temperature constant at 800 C we have to vary the mass flow rates to find out that what temperature and mass flow rate the overall heat transfer coefficient will be more. The coolant mass flow rate are varied such as 0.035kg/s, 0.05kg/s, 0.075kg/s, 0.1kg/s. the experiment is carried out by maintaining coolant inlet temperature at 80 and varying the mass flow rate. The values of coolant outlet temperature (𝑇3), air inlet temperature (𝑇4), air outlet temperature (𝑇5) are noted with the help of digital indicator. By using all these parameters rate of heat transfer and then overall heat transfer coefficient values are calculated. The values that are obtained are tabulated in the following tables. 20 30 40 50 60 70 80 90 40 50 60 70 75 78 80 83 Temperaturesin°C Inlet Radiator Temperature in °C T2 T3 T4 25 75 125 175 225 275 0 300 600 900 1200 1500 1800 40 50 60 70 75 78 80 83 OveralllHeatTransferCoefficient W/mK HeatTransferRateW Inlet Temperature of Radiator in °C Heat Transfer Rate Overall Heat Transfer Coefficient
  • 6. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 349 Vol. 10, Issue 3, pp. 344-353 Temperature Reading Tables of Different Mass Flow Rates at Constant Hot Fluid Inlet Temperature Optimum Hot Fluid Mass Flow Rate The optimum over all heat transfer coefficient value is obtained at 0.075 kg/s of mass flow rate and keep the hot fluid inlet temperature value as constant. Table 2: Optimum mass flow rate Flow rate (kg/s) Heat transfer rate(Q) (W) Overall heat transfer coefficient(U) (w/m2 o C) 0.025 585.2 98.98 0.050 836 143.56 0.075 1254 177.93 0.1 1254 172.98 From the above table, we can see that the overall heat transfer coefficient value is more when the coolant mass flow rate is 0.075kg/s and the further increase in mass flow rate the overall heat transfer coefficient value is being decreased. So we can say that 0.075kg/s is the optimum mass flow rate where maximum overall heat transfer coefficient values will be more. The overall heat transfer coefficient values at different coolant inlet temperature are summarized in the table Graph 3. Coolant Flow rate vs Heat transfer Rate Coolant Flow rate vs Heat transfer Rate and Overall heat transfer coefficient According to the values obtained a graph is plotted between coolant inlet temperature and overall heat transfer coefficient. Graph is plotted between overall heat transfer coefficient and hot fluid inlet temperature. The values of coolant inlet temperature are taken on x-axis and the values of overall heat transfer coefficient are taken on y-axis. From the graph 5.1 it is clear that the overall heat transfer coefficient value is maximum at coolant inlet temperature 80℃ and the value is 234.47 W/m2o C.Similarly, the overall heat transfer coefficient values at different mass flow rate are summarized in the table. In the above table represents the optimum flow rate of 0.075m/sec add obtained maximum Overall heat transfer coefficient value is 177.78 W/m2o C.it is best result for this experiment. According to the values obtained a graph is plotted between mas flow rate and overall heat transfer coefficient. 90 110 130 150 170 190 0 200 400 600 800 1000 1200 1400 0.025 0.05 0.075 0.1 OverallHeatTransferCoefficient HeatTransferRateinW Coolant Flow Rate in Kg/s Heat transfer rate(Q) Overall heat transfer coefficient(U)
  • 7. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 350 Vol. 10, Issue 3, pp. 344-353 Table 3. Overall heat transfer coefficient values at different mass flow rates SNo Mass Flow rate Kg/s T2 °C T3 °C T4°C T5 °C Heat Transfer Rate Watts Overall Heat Transfer Coefficient W/m K 1 0.035 80 76 35 70 585.2 98.98 2 0.05 80 76 36 70 836 143.56 3 0.075 80 76 35 64 1254 177.93 4 0.1 80 77 35 64 1254 172.93 Graph 4. Variation of Temperatures with different coolant mass flow rates Graph 5. Graph for overall heat transfer coefficient at different mas flow rates. 70 100 130 160 190 220 0 200 400 600 800 1000 1200 1400 0.035 0.05 0.075 0.1 OveralllHeatTransferCoefficient HeatTransferRateW Coolant Mass flow rate in Kg/s Heat Transfer Rate Overall Heat Transfer Coefficient 20 30 40 50 60 70 80 90 0.035 0.05 0.075 0.1 Temperaturesin°C Coolant mass flow rate in Kg/s T2 T3 T4 T5
  • 8. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 351 Vol. 10, Issue 3, pp. 344-353 The values of mass flow rate are taken on x-axis and overall heat transfer coefficient values on y-axis. From the graph it is clear that the overall heat transfer coefficient value is maximum when the mass flow rate is 0.075kg/s and the value is 177.93 W/m2o C Similarly, the overall heat transfer coefficient of CuO at optimum temperature and mass flow rate is summarized in the following table Table 4. Overall heat transfer coefficient at various sintering temperatures S no Sintering Temperature °C Hot Fluid inlet Temperature °C Mass Flow rate Kg/s Heat Transfer Rate W Avg Overall Heat Transfer Coefficient W/m K 1 Normal 80 0.075 214.97 98.98 2 150 80 0.075 222.02 143.56 3 250 80 0.075 247.06 177.93 According to the values obtained a graph is plotted between sintering condition and overall heat transfer coefficient. Graph 6. Graph plotted between overall heat transfer coefficient and sintering condition. The values of sintering condition are taken on x-axis and values of overall heat transfer coefficient are taken on y-axis. From the graph it is clear that the overall heat transfer coefficient value is maximum at sintering condition at 250℃ and the value is 247.06 w/𝑚2 ℃ 5. 2 Discussion  Experiments are conducted to find out optimum hot fluid temperature and mass flow rate.  As per the results obtained from the graph plotted between overall heat transfer coefficient and mass flow rate, the overall heat transfer value is 247.06W/𝑚2 ℃.  The maximum value of overall heat transfer coefficient and heat transfer rate are found to be 80℃ fluid inlet temperature and 0.075kg/sec mass flow rate.  Addition of small amount of CuO nanoparticles into demineralized water as the base fluid would increase the rate of heat transfer and convection heat transfer coefficient by at least 17.3% and 40% respectively.  Nano fluids as the coolant for automotive radiator and various ranges of operating temperatures and volume concentrations may need to be explored in order to better optimal conditions. 0 40 80 120 160 200 0 60 120 180 240 Normal 150 250 OveralllHeatTransferCoefficient HeatTransferRateW Sintering Temperature °C Heat Transfer Rate Avg Overall Heat Transfer Coefficient
  • 9. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 352 Vol. 10, Issue 3, pp. 344-353 VI. CONCLUSION In this experimental study, the heat transfer performance of automobile radiator has been estimated by using CuO Nano fluids at various coolant temperature ranges and mass flow rates.  The optimum hot fluid temperature and mass flow rates are determined using its inlet temperature based on the overall heat transfer coefficient and heat transfer rates.  The Nano coolants found to enhance the thermal performance of the automobile radiator.  With the increase in the coolant flow rate, the heat transfer performance increase for the various coolants namely CuO-water.  After several iterations the optimum overall heat transfer coefficient is find out to be 247.06 W/m² °C at the mass flow rate 0.075kg/sec and inlet temperature 80℃. VII. FUTURE SCOPE In the application of Nanofluids instead of water enhance thermal performance of the automobile radiator system, some associated problems such as stability and sedimentation should also be studied in detail. The research work also drawn the attention of the many researchers to concentration on farm equipment development for improved performance in their field. The thermal management of heavy vehicles such as cars, tractor and earth moving equipment through Nano mechanism are essential areas for future researchers. Nano fluids shows promising potential as the coolant for automotive radiator and more ranges of operating temperature and volume concentrations may need to be explored in order to better understand its full potential. ACKNOWLEDGMENT The Author would like to thank all the persons who helped in the completion of this experimental work. Also thanks are extended to ASR College of Engineering, Tanuku, India for support throughout the execution of the experimental work. REFERENCES [1] Prof. A. R. Khot, Prof. D. G. thom bare,prof.s.p. Gaikwad and Prof. A. S. “Adadande were reported various methods for radiator performance evaluation and testing of the radiator” (IOSR-JMCE) ISSN:2278-1684,PP:07-14. [2] Eastmen, J. A. Choi, S. U. S., Li, S., Yu, W., and Thompson, LJ., 2001, “Anomalously Increased Effective Thermal Conductivies of Ethylene Glycol- Based Nnofluids Containing Copper Particles,”Appl. Phys. Lett., 78(6), pp.718-720 [3] Heris, S. Z., Esfahany, M. N., and Etemad, S.Gh., 2006, “Investigation of Convective Heat Transfer of A𝑙2 𝑂3/Water Nanofluid in Circular Tube,” Int. J. Heat Fluid Flow, 28, pp. 203-210 [4] vajjah,R.S ,Das, D.K., and Namburu, P.K.,2010, “numerical study of fluid dynamics and heat transfer performance of Al2 O3 and CuO Nano fluids in the Flat tubes of a radiator”, Int. J. Heat fluid flow, 31,pp,613-621. [5] Nariki, M., Peyghambarzadeh, S.M., hashemabadi, S.H., and vermahmoudi, Y., 2013, “Parametric study of overall heat transfer coefficient of CuO/water nano fluids in a car radiator”, Int. J. Them. Sci., 66,pp. 82-90. [6] Leong, K. Y., R. Saidur, S. N. Kazi, and a. H. Mamun. 2010. “Performance Investigation of an Automotive Car Radiator Operated with NanofluidBased Coolants (nanofluid as a Coolant in a Radiator).” Applied Thermal Engineering 30 (17-18). Elsevier Ltd: 2685–92 doi:10.1016/j.applthermaleng.2010.07.019. [7] Lomascolo, Mauro, Gianpiero Colangelo, Marco Milanese, and Arturo De Risi. 2015. “Review of Heat Transfer in Nano Fl Uids : Conductive, Convective and Radiative Experimental Results.” Renewable and Sustainable Energy Reviews 43. Elsevier: 1182 [8] Rahul A. Bhogare, B. S. Kothawale. “A Review on applications and challenges of Nano-fluids as coolant in Automobile Radiator". International Journal of Scientific and Research Publications, Volume 3, Issue 8, August 2013 [9] P. sai sasank1, V.Govinda naik. Empirical Review on Car Radiator Using H2O and Al2O3. International Journal of Innovative Research in Science, Engineering and Technology. Vol. 3, Issue 10, October2014
  • 10. International Journal of Advances in Engineering & Technology, June, 2017. ©IJAET ISSN: 22311963 353 Vol. 10, Issue 3, pp. 344-353 [10] Mintsa HA, Roy G, Nguyen CT, Doucet D. New temperature dependent thermal conductivity data for water-based nanofluids. Int J Therm Sci 2009;48(2):363–71. [11] D.H. Kumar, H.E. Patel, V.R. Kumar, T. Sundararajan, T. Pradeep, S.K.vDas, Model for heat conduction in nanofluids, Physical Review Letters 93 (14) (2004) 1–3. [12] H. Xie, M. Fujii, X. Zhang, Effect of interfacial nanolayer on the effective thermal conductivity of nanoparticle-fluid mixture, International Journal of Heat and Mass Transfer 48 (2005) 2926–2932. [13] S.P. Jang, S.U.-S. Choi, Role of Brownian motion in the enhanced thermal conductivity of nanofluids, Applied Physics Letters 84 (2004) 4316. [14] C.H. Li, G.P. Peterson, Experimental investigation of temperature and volume fraction variations on the effective thermal conductivity of nanoparticle suspensions (nanofluids), Journal of Applied Physics 99 (084314) (2006) 1–8. [15] R. Prasher, P. Bhattacharya, P.E. Phelan, Thermal conductivity of nanoscale colloidal solutions nanofluids, Physical Review Letters 94 (025901) (2005) 1–4. [16] G. Roy, C.T. Nguyen, D. Doucet, S. Suiro, T. Maré, Temperature dependent thermal conductivity of alumina based nanofluids, in: G. de Vahl Davis, E. Leonardi (Eds.), Proceedings of the 13th International Heat Transfer Conference, Begell House Inc., 2006. [17] D.-H. Yoo, K. Hong, Y. Ho-Soon, Study of thermal conductivity of Nanofluids for the application of heat transfer fluids, Thermochimica Acta 455 (2007) 66–69. AUTHORS BIOGRAPHY V D M Bharathi Mahanti was born in Tanuku, India, in Year 1989. She received the Bachelor’s degree in Mechanical engineering from the Jawaharlal Nehru Technological University, Kakinada, in Year 2011. She is currently pursuing the Master degree in Thermal engineering from the Jawaharlal Nehru Technological University, Kakinada. Her research interests includes Design of Heat exchangers, Nano fluids, Thermal systems design, Renewable sources of energy V. Ravi Kumar graduated in Mechanical engineering from JNTUK His research interests includes Robotics, Nano technology, Thermal systems design, Renewable sources of energy. Currently in working on the Artificial intelligence and Green energy systems.