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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume: 3 | Issue: 2 | Jan-Feb 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 - 6470
@ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 209
CFD Analysis of a Double Pipe Heat Exchanger
by using Fluid Based Nanomaterials
Golkonda Venkata Apparao, K. Srinivasa Rao
Department of Mechanical Engineering, Sri Vaishnavi College of Engineering,
Singupuram, Srikakulam, Andhra Pradesh, India
ABSTRACT
Double pipe heat exchanger design is a device which we using for heat transfer applications straightforward. This maintains
one heat exchanger pipe inside another. After determining the required heat exchanger surfacearea,foreithercounterflowor
parallel flow, the pipe sizes and number of bends for the double pipe heat exchanger can be selected.
In double pipe heat exchanger design, an important factor is the type of flow pattern in the heat exchanger. A double pipe heat
exchanger will typically be either counterblow or parallel flow. Cross flow just doesn't work for a double pipe heat exchanger.
The flow pattern and the required heat exchange duty allow calculation of the log mean temperature difference. Thattogether
with an estimated overall heat transfer coefficient allows calculationoftherequired heattransfer surfacearea.Thenpipesizes,
pipe lengths and number of bends can be determined.
The convective heat transfer, friction factor and effectivenessof differentvolumeconcentrations of Fe3O4Nanofluidflowinan
inner tube of double pipe heat exchanger with return bend has been estimated experimentally and turbulent flow conditions.
The test section used in this study is of double pipe type in which the innertubediameteris0.019m,the annulustubediameter
is 0.05m and the total length of inner tube is 5 m. At a distance of 2.2mfromthe inlet of the inner tube the return bend is
provided.
The hot Nanofluids flows through an inner tube, whereas the cold water flows through an annulus tube. The volume
concentrations of the nanoparticles used in this studyare 0.03%and 8lpm ,10lpmmassflowratewith Reynoldsnumberrange
from 9,000 to 30,000.in the process analyze the CFD analysis is performed in Ansys Fluent 15.0 workbench and its used
different nanofluids used, which nanofluids better heat transfer rate find base on the results.In this process choose different
nanofluids( Al2o3, Cuo ,Fe3o4) this nanofluids properties taken by different base papers.
KEYWORDS: Heat Exchanger, Nano Fluids, Thermo Physical Properties, Heat Transfer, CFD Analysis
I. INTRODUCTION
A heat exchanger is a device used to transfer heat between
one or more fluids. The fluids may be separated by a solid
wall to prevent mixing or they may be in directcontact.They
are widely used in space heating, refrigeration, air
conditioning, power stations,chemicalplants,petrochemical
plants, petroleum refineries, natural-gas processing, and
sewage treatment. The classicexampleofaheatexchangeris
found in an internal combustion engine in which a
circulating fluid known as engine coolant flows through
radiator coils and air flows past the coils, which cools the
coolant and heats the incoming air.
Double pipe heat exchangers are the simplest exchangers
used in industries. On one hand, these heat exchangers are
cheap for both design and maintenance, makingthemagood
choice for small industries. On the other hand, their low
efficiency coupled with the high space occupied in large
scales, has led modern industries to use more efficient heat
exchangers like shell and tube or plate.
However, since double pipe heatexchangers aresimple,they
are used to teach heat exchanger designbasicstostudentsas
the fundamental rules for all heat exchangers are the same.
To start the design of a double pipe heat exchanger, the first
step is to calculate the heat duty of the heat exchanger. It
must be noted that for easier design, it’sbetterto ignoreheat
loss to the environment for initial design.
Nano fluid is a new kind of heat transfer medium, containing
nanoparticles (1-100 nm) which are uniformly and stably
distributed in a base fluid. These distributed nanoparticles
generally metal or metal oxides greatly enhance the thermal
conductivity of the Nano fluid, increases conduction and
convection coefficients, allowing for more heat transfer.The
nanoparticle material includeschemicallystablemetals(e.g.,
gold, copper), metal oxides (e.g., alumina,silica, zirconia, and
titania), oxide ceramics (e.g., Al2O3, and CuO), metal
carbides (e.g., SiC), metal nitrides (e.g., AIN, SiN), carbon in
various forms (e.g., diamond, graphite, carbon nanotubes,
andfullerene) and other functionalized nanoparticles. The
Nano fluids have various applications as they provide an
efficient thermal energy transfer due to higher heat transfer
with a comparable pumping power required
II. REVIEW OF LITERATURE
N. T. Ravi kumar [1] in their paper discussed that the
convective heat transfer, friction factor and effectiveness of
different volume concentrations of Fe3O4 nanofluid flow in
an inner tube of double pipe heat exchanger with return
bend has been estimated experimentally and turbulent flow
conditions. The test section used in this study is of double
pipe type in which the inner tube diameter is 09 m, the
annulus tube diameter is 0.05m and the total length of inner
tube is 5 m. At a distance of 2.2mfromthe inlet of the inner
tube the return bend is provided. The hot Fe3O4 nanofluid
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 210
flows through an inner tube, where as the cold water flows
through an annulus tube. The volume concentrations of the
nanoparticles used in this study are 0.005%, 0%, 0.03% and
0.06% with Reynolds number range from 15,000 to 30,000.
Based on the results, the Nusselt number enhancement is
14.7% for 0.06% volume concentration of nanofluid flow in
an inner tube of heat exchanger at a Reynolds number of
30,000 when compared to base fluid data; the pumping
penalty of nanofluid is b10%. New correlations for Nusselt
number and friction factor have been developed based on
the experimental data.
Arjumand Adi[2] in his paper described that the Mini
channel flow of Nano fluids has been predicted considering
Nano fluid as a single phase homogeneous mixture. The
homogeneous mixture model for the Nano fluid holds good
to predict the average Nusselt number and friction factor in
case of laminarflow.Hence,thepresentcomputationalmodel
can be a good alternative approach to predict heat transfer
and pressure drop characteristics of minichannelflowusing
Nano fluids. Also, the error in prediction of Nusselt number
is less if we consider Brownian motion in our computational
model, which is within 4%.
M. Esfandiary[3] in their study discussed thattheproblemof
turbulent forced convection flow of water- alumina Nano
fluid in a uniformly heated pipe has been thoroughly
investigated. In numerical study, single and two-phase
models have been used. In single-phase modeling of Nano
fluid, thermal and flow properties of Nano fluid have been
considered to be dependent on temperature and volume
fraction. Effects of volume fraction and Reynolds number
(3000<Re<9000) on convective heattransfercoefficientand
pressure drop were investigated for various axial locations
of the tube.
III. MODELING OF DOUBLE PIPE HEAT EXCHANGER
The modeling of a double pipe heat exchanger is done in
CATIAV5R20 modeling software.
Select the file  click on model properties  assign the
material properties, system of units, accuracy click on ok.
IV. COMPUTATION ANALYSIS
Computational Fluid Dynamics (CFD) is the science of
predicting fluid flow, heat transfer, mass transfer, chemical
reaction (e.g., combustion), and related phenomena by
solving the mathematical equations that govern these
processes using a numerical algorithm on a computer. The
technique is very powerful and spans a wide range of
industrial and non-industrial application areas.
All the CFD codes contain three main elements. They are as
follows,
Preprocessor
Solver
Post processor
The geometry is created in ANSYS ICEM CFD asperthegiven
data for each of the model and a domain is created to
encompass the flow inside the domain to the walls of the
body. In order to study domain independence, three
cylindrical domains are considered intrialanderror method
taking the distances from nose and tail ends of the model
and taking the radius from the axis of the model. Three
dimensional hexahedral grids were generated to discretize
the body and the domain.
Three dimensional segregated implicit solvers is used in the
present analysis, the k-ω, k-є turbulence models in addition
to the continuity and momentum equations were used as
governing equations. Boundary conditions used in the
present analysis are inlet as velocity inlet, outlet as Pressure
Outlet, far field, and body as walls. All the three models are
computed in the solver Fluent. The solution was stopped
when changes in solution variables from one iteration tothe
next is negligible. Solution is iterated till the convergence is
observed. Then forces and moments results were extracted
from it. This data is saved as the data file in the solver itself.
Solve the momentum equations to find the velocity
components (Uo, Vo).
Solve the pressure-correction equation to find 'p' at each
grid point.
Replace the previous intermediate values of pressure and
velocity with the new corrected values and return to the
original step. Repeat the step until the step converges.
A. Geometry and Domain are created in ANSYS 15.0.
Blocking and Meshing is done.Checkingthemesh quality
and saving the file to solver Fluent. Export it into fluent
software. Computing and monitoring the solution in
Fluent.Examine and save the results.
B. pressure distribution
Fig1 0.034% volume concentration for 8 lpm pressure distribution Fe3o4
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 211
Fig2 0.034% volume concentration for 10 lpm pressure distribution cuo
Fig3 0.034% volume concentration for 10 lpm pressure distribution Al2o3
Fig4 0.034% volume concentration for 10 lpm pressure distribution Fe3o4
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 212
TABLE OF RESULTS:
Mass flow rate
ALUMINUM OXIDE
(Al2o3) Vol 0.034%
COPPER OXIDE
(Cuo) Vol 0.043%
FERROUS OXIDE
(Fe3O4) Vol 0.0034%
8 Lpm or 0.137 KG/Sec 2.667 e+03 2.527 e+03 3.417 e+03
10 Lpm or 0.171 KG/Sec 2.737 e+02 3.817 e+03 4.277 e+03
TABLE: MASS FLOW RATE AND VOLUME CONCENTRATIONS WITH DIFFERENT
Fig 5 PRESSURE DISTRIBUTAION GRAPH
In the above graph represent by pressure vary from point to point on y-axis, taken different Nano fluids but same volume
concentration(0.03%) and different mass flow rate(8lpm) litblue colour and (10 lpm) represent by red colour. Aluminium
oxide <copper oxide < ferrous oxide.
CONCLUSION
The convective heat transfer performance and flow
characterstics of Cuo ,Al2o3 ,Fe304 nanofluid flowing in a
double pipe heat exchanger has been experimentally
investigated. Experiments have been carried out under
turbulent conditions. Theeffectof particle concentrationand
the Reynolds number on the heat transfer performance and
flow behavior of the nanofluid has been determined.
Dispersion of the nano particles into the base fluid (water)
increases the average heat transfer coefficient with the
increase in the flow rate of fluid. Taken three nanofluids
objered by thermal physical properties(Cuo,Al2o3 ,Fe304).
CUO Heat transfer rate 8lpm heat transfer rate ,4797.793
(w),pressure2.52e+03(pa),temperature3.07e+02(k),velocity
distribution2.35e+01(m/s), Aluminium oxide Heat transfer
rate 8lpm heat transfer rate 9658.334 (w),pressure
2.66e+03(pa), temperature3.10e+02(k), velocity
distribution6. 17e+o1(m/s)ferrous oxide Heat transfer rate
8lpm heat transfer rate 12829.021 (w),pressure
3.41e+03(pa), temperature3.33e+02(k), velocity
distribution7.36e+01(m/s)CUO Heat transfer rate 10lpm
heat transfer rate 15047.63 (w)pressure 3.81e+03(pa),
temperature 3.20e+01(k), velocity distribution 2.47e+02
(m/s) Aluminium oxide Heat transfer rate 10lpm heat
transfer rate 17102.24 (w) pressure 2.73e+02(pa),
temperature3.00e+01(k), velocity distribution
6.22e+02(m/s) ferrous oxide Heat transfer rate 10lpm heat
transfer rate 24761.22 (w) pressure 4.27e+03(pa),
temperature 3.33e+04(k), velocity distribution
7.56e+02(m/s).(0.03%)volume concentration and 8lpm
mass flow rate copper oxide <Aluminium oxide < ferrous
oxide.(0.03%)volume concentration and 10lpm mass flow
rate, y-axis taken by heat transfer rate. copper oxide
<Aluminium oxide < ferrous oxide.fe3o4 is better nanofluid.
REFERENCES
[1] N.T. Ravi Kumar, P. Bhramara, BirhanuMulat Addis, L.
SyamSundarHeat transfer, friction factor and
effectiveness analysis of Fe3O4 /water nanofluid flow
in a double pipe heat exchanger with return bend,
International Communications in Heat and Mass
Transfer, volume 81 (2017) pages 155–163
[2] Byung-Hee Chun, Hyun Uk Kang, and Sung Hyun Kim
Effect of alumina nanoparticles in the fluid on heat
transfer in double-pipe heat exchanger system
Department of Chemical and Biological Engineering,
Applied Rheology Center, Korea University, Seoul 136-
701, Korea (Received 5 October 2007 • accepted 5
March 2008)
[3] KuruvaUmamahesh,K. Venugopal- DesignAnd Analysis
Of Double Pipe Heat Exchanger Using Computational
Method International Journal Of Professional
Engineering Studies Volume V /Issue 2 /JULY 2015
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 213
[4] ArjumandAdil , Sonam Gupta, and Pradyumna Ghosh,
“Numerical Prediction of Heat Transfer Characteristics
of Nano fluids in a Mini channel Flow”, Journal of
Energy Volume 2014, Article ID 307520, 7.
[5] M. Esfandiary 1, A. Habibzadeh 2, H. Sayehvand,
“Numerical Study of Single Phase/Two-Phase Models
for Nano fluid Forced Convection and Pressure Dropin
a Turbulence Pipe Flow”, Trans. Phenom. Nano Micro
Scales, 4(1):11-18, Winter - Spring 2016.
[6] Payam Rahim Mashaei, SeyedMostafaHosseinalipour,
and Mehdi Bahiraei, “Numerical Investigation of Nano
fluid Forced ConvectioninChannelswithDiscreteHeat
Sources”, Hindawi Publishing Corporation Journal of
Applied Mathematics Volume 2012.
[7] 4. HoomanYarmand, Samira Gharehkhani,
SalimNewazKazi, EmadSadeghinezhad, and
Mohammad Reza Safaei,“Numerical Investigation of
Heat Transfer Enhancement in a Rectangular Heated
Pipe for Turbulent Nano fluid”, Hindawi Publishing
Corporation, The Scientific World Journal, Volume
2014.
[8] Mohammad Nazififard, MohammadrezaNematollahi,
KhosrowJafarpur, and Kune Y. Suh, “Numerical
Simulation of Water-Based Alumina Nano fluid in Sub
channel Geometry”, Science and Technologyof Nuclear
Installations, Volume 2012.
[9] S. J. Palm, G. Roy, and C. T. Nguyen, “Heat transfer
enhancement with the use of Nano fluids in radial flow
cooling systems considering temperature-dependent
properties,” Applied Thermal Engineering, vol. 26, no.
17-18, pp. 2209–2218, 2006.
[10] J. A. Eastman, S. R. Phillpot, S. U. S. Choi, and P.
Keblinski, “Thermal transport in ,” Annual Review of
Materials Research, vol. 34, pp. 219–246, 2004.
[11] S. J. Kim, I. C. Bang, J. Buongiorno, and L.W.Hu, “Surface
wettability change during pool boiling of nanofluids
and its effect on critical heatflux,” InternationalJournal
of Heat and Mass Transfer, vol. 50, no.19-20,pp. 4105–
4116, 2007.
[12] J. Buongiorno and B. Truong, “Preliminary study of
water based nanofluid coolants for PWRs,”
Transactions of the American Nuclear Society, vol. 92,
pp. 383–384, 2005.

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CFD analysis of double pipe heat exchanger

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume: 3 | Issue: 2 | Jan-Feb 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 - 6470 @ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 209 CFD Analysis of a Double Pipe Heat Exchanger by using Fluid Based Nanomaterials Golkonda Venkata Apparao, K. Srinivasa Rao Department of Mechanical Engineering, Sri Vaishnavi College of Engineering, Singupuram, Srikakulam, Andhra Pradesh, India ABSTRACT Double pipe heat exchanger design is a device which we using for heat transfer applications straightforward. This maintains one heat exchanger pipe inside another. After determining the required heat exchanger surfacearea,foreithercounterflowor parallel flow, the pipe sizes and number of bends for the double pipe heat exchanger can be selected. In double pipe heat exchanger design, an important factor is the type of flow pattern in the heat exchanger. A double pipe heat exchanger will typically be either counterblow or parallel flow. Cross flow just doesn't work for a double pipe heat exchanger. The flow pattern and the required heat exchange duty allow calculation of the log mean temperature difference. Thattogether with an estimated overall heat transfer coefficient allows calculationoftherequired heattransfer surfacearea.Thenpipesizes, pipe lengths and number of bends can be determined. The convective heat transfer, friction factor and effectivenessof differentvolumeconcentrations of Fe3O4Nanofluidflowinan inner tube of double pipe heat exchanger with return bend has been estimated experimentally and turbulent flow conditions. The test section used in this study is of double pipe type in which the innertubediameteris0.019m,the annulustubediameter is 0.05m and the total length of inner tube is 5 m. At a distance of 2.2mfromthe inlet of the inner tube the return bend is provided. The hot Nanofluids flows through an inner tube, whereas the cold water flows through an annulus tube. The volume concentrations of the nanoparticles used in this studyare 0.03%and 8lpm ,10lpmmassflowratewith Reynoldsnumberrange from 9,000 to 30,000.in the process analyze the CFD analysis is performed in Ansys Fluent 15.0 workbench and its used different nanofluids used, which nanofluids better heat transfer rate find base on the results.In this process choose different nanofluids( Al2o3, Cuo ,Fe3o4) this nanofluids properties taken by different base papers. KEYWORDS: Heat Exchanger, Nano Fluids, Thermo Physical Properties, Heat Transfer, CFD Analysis I. INTRODUCTION A heat exchanger is a device used to transfer heat between one or more fluids. The fluids may be separated by a solid wall to prevent mixing or they may be in directcontact.They are widely used in space heating, refrigeration, air conditioning, power stations,chemicalplants,petrochemical plants, petroleum refineries, natural-gas processing, and sewage treatment. The classicexampleofaheatexchangeris found in an internal combustion engine in which a circulating fluid known as engine coolant flows through radiator coils and air flows past the coils, which cools the coolant and heats the incoming air. Double pipe heat exchangers are the simplest exchangers used in industries. On one hand, these heat exchangers are cheap for both design and maintenance, makingthemagood choice for small industries. On the other hand, their low efficiency coupled with the high space occupied in large scales, has led modern industries to use more efficient heat exchangers like shell and tube or plate. However, since double pipe heatexchangers aresimple,they are used to teach heat exchanger designbasicstostudentsas the fundamental rules for all heat exchangers are the same. To start the design of a double pipe heat exchanger, the first step is to calculate the heat duty of the heat exchanger. It must be noted that for easier design, it’sbetterto ignoreheat loss to the environment for initial design. Nano fluid is a new kind of heat transfer medium, containing nanoparticles (1-100 nm) which are uniformly and stably distributed in a base fluid. These distributed nanoparticles generally metal or metal oxides greatly enhance the thermal conductivity of the Nano fluid, increases conduction and convection coefficients, allowing for more heat transfer.The nanoparticle material includeschemicallystablemetals(e.g., gold, copper), metal oxides (e.g., alumina,silica, zirconia, and titania), oxide ceramics (e.g., Al2O3, and CuO), metal carbides (e.g., SiC), metal nitrides (e.g., AIN, SiN), carbon in various forms (e.g., diamond, graphite, carbon nanotubes, andfullerene) and other functionalized nanoparticles. The Nano fluids have various applications as they provide an efficient thermal energy transfer due to higher heat transfer with a comparable pumping power required II. REVIEW OF LITERATURE N. T. Ravi kumar [1] in their paper discussed that the convective heat transfer, friction factor and effectiveness of different volume concentrations of Fe3O4 nanofluid flow in an inner tube of double pipe heat exchanger with return bend has been estimated experimentally and turbulent flow conditions. The test section used in this study is of double pipe type in which the inner tube diameter is 09 m, the annulus tube diameter is 0.05m and the total length of inner tube is 5 m. At a distance of 2.2mfromthe inlet of the inner tube the return bend is provided. The hot Fe3O4 nanofluid
  • 2. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 210 flows through an inner tube, where as the cold water flows through an annulus tube. The volume concentrations of the nanoparticles used in this study are 0.005%, 0%, 0.03% and 0.06% with Reynolds number range from 15,000 to 30,000. Based on the results, the Nusselt number enhancement is 14.7% for 0.06% volume concentration of nanofluid flow in an inner tube of heat exchanger at a Reynolds number of 30,000 when compared to base fluid data; the pumping penalty of nanofluid is b10%. New correlations for Nusselt number and friction factor have been developed based on the experimental data. Arjumand Adi[2] in his paper described that the Mini channel flow of Nano fluids has been predicted considering Nano fluid as a single phase homogeneous mixture. The homogeneous mixture model for the Nano fluid holds good to predict the average Nusselt number and friction factor in case of laminarflow.Hence,thepresentcomputationalmodel can be a good alternative approach to predict heat transfer and pressure drop characteristics of minichannelflowusing Nano fluids. Also, the error in prediction of Nusselt number is less if we consider Brownian motion in our computational model, which is within 4%. M. Esfandiary[3] in their study discussed thattheproblemof turbulent forced convection flow of water- alumina Nano fluid in a uniformly heated pipe has been thoroughly investigated. In numerical study, single and two-phase models have been used. In single-phase modeling of Nano fluid, thermal and flow properties of Nano fluid have been considered to be dependent on temperature and volume fraction. Effects of volume fraction and Reynolds number (3000<Re<9000) on convective heattransfercoefficientand pressure drop were investigated for various axial locations of the tube. III. MODELING OF DOUBLE PIPE HEAT EXCHANGER The modeling of a double pipe heat exchanger is done in CATIAV5R20 modeling software. Select the file  click on model properties  assign the material properties, system of units, accuracy click on ok. IV. COMPUTATION ANALYSIS Computational Fluid Dynamics (CFD) is the science of predicting fluid flow, heat transfer, mass transfer, chemical reaction (e.g., combustion), and related phenomena by solving the mathematical equations that govern these processes using a numerical algorithm on a computer. The technique is very powerful and spans a wide range of industrial and non-industrial application areas. All the CFD codes contain three main elements. They are as follows, Preprocessor Solver Post processor The geometry is created in ANSYS ICEM CFD asperthegiven data for each of the model and a domain is created to encompass the flow inside the domain to the walls of the body. In order to study domain independence, three cylindrical domains are considered intrialanderror method taking the distances from nose and tail ends of the model and taking the radius from the axis of the model. Three dimensional hexahedral grids were generated to discretize the body and the domain. Three dimensional segregated implicit solvers is used in the present analysis, the k-ω, k-є turbulence models in addition to the continuity and momentum equations were used as governing equations. Boundary conditions used in the present analysis are inlet as velocity inlet, outlet as Pressure Outlet, far field, and body as walls. All the three models are computed in the solver Fluent. The solution was stopped when changes in solution variables from one iteration tothe next is negligible. Solution is iterated till the convergence is observed. Then forces and moments results were extracted from it. This data is saved as the data file in the solver itself. Solve the momentum equations to find the velocity components (Uo, Vo). Solve the pressure-correction equation to find 'p' at each grid point. Replace the previous intermediate values of pressure and velocity with the new corrected values and return to the original step. Repeat the step until the step converges. A. Geometry and Domain are created in ANSYS 15.0. Blocking and Meshing is done.Checkingthemesh quality and saving the file to solver Fluent. Export it into fluent software. Computing and monitoring the solution in Fluent.Examine and save the results. B. pressure distribution Fig1 0.034% volume concentration for 8 lpm pressure distribution Fe3o4
  • 3. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 211 Fig2 0.034% volume concentration for 10 lpm pressure distribution cuo Fig3 0.034% volume concentration for 10 lpm pressure distribution Al2o3 Fig4 0.034% volume concentration for 10 lpm pressure distribution Fe3o4
  • 4. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 212 TABLE OF RESULTS: Mass flow rate ALUMINUM OXIDE (Al2o3) Vol 0.034% COPPER OXIDE (Cuo) Vol 0.043% FERROUS OXIDE (Fe3O4) Vol 0.0034% 8 Lpm or 0.137 KG/Sec 2.667 e+03 2.527 e+03 3.417 e+03 10 Lpm or 0.171 KG/Sec 2.737 e+02 3.817 e+03 4.277 e+03 TABLE: MASS FLOW RATE AND VOLUME CONCENTRATIONS WITH DIFFERENT Fig 5 PRESSURE DISTRIBUTAION GRAPH In the above graph represent by pressure vary from point to point on y-axis, taken different Nano fluids but same volume concentration(0.03%) and different mass flow rate(8lpm) litblue colour and (10 lpm) represent by red colour. Aluminium oxide <copper oxide < ferrous oxide. CONCLUSION The convective heat transfer performance and flow characterstics of Cuo ,Al2o3 ,Fe304 nanofluid flowing in a double pipe heat exchanger has been experimentally investigated. Experiments have been carried out under turbulent conditions. Theeffectof particle concentrationand the Reynolds number on the heat transfer performance and flow behavior of the nanofluid has been determined. Dispersion of the nano particles into the base fluid (water) increases the average heat transfer coefficient with the increase in the flow rate of fluid. Taken three nanofluids objered by thermal physical properties(Cuo,Al2o3 ,Fe304). CUO Heat transfer rate 8lpm heat transfer rate ,4797.793 (w),pressure2.52e+03(pa),temperature3.07e+02(k),velocity distribution2.35e+01(m/s), Aluminium oxide Heat transfer rate 8lpm heat transfer rate 9658.334 (w),pressure 2.66e+03(pa), temperature3.10e+02(k), velocity distribution6. 17e+o1(m/s)ferrous oxide Heat transfer rate 8lpm heat transfer rate 12829.021 (w),pressure 3.41e+03(pa), temperature3.33e+02(k), velocity distribution7.36e+01(m/s)CUO Heat transfer rate 10lpm heat transfer rate 15047.63 (w)pressure 3.81e+03(pa), temperature 3.20e+01(k), velocity distribution 2.47e+02 (m/s) Aluminium oxide Heat transfer rate 10lpm heat transfer rate 17102.24 (w) pressure 2.73e+02(pa), temperature3.00e+01(k), velocity distribution 6.22e+02(m/s) ferrous oxide Heat transfer rate 10lpm heat transfer rate 24761.22 (w) pressure 4.27e+03(pa), temperature 3.33e+04(k), velocity distribution 7.56e+02(m/s).(0.03%)volume concentration and 8lpm mass flow rate copper oxide <Aluminium oxide < ferrous oxide.(0.03%)volume concentration and 10lpm mass flow rate, y-axis taken by heat transfer rate. copper oxide <Aluminium oxide < ferrous oxide.fe3o4 is better nanofluid. REFERENCES [1] N.T. Ravi Kumar, P. Bhramara, BirhanuMulat Addis, L. SyamSundarHeat transfer, friction factor and effectiveness analysis of Fe3O4 /water nanofluid flow in a double pipe heat exchanger with return bend, International Communications in Heat and Mass Transfer, volume 81 (2017) pages 155–163 [2] Byung-Hee Chun, Hyun Uk Kang, and Sung Hyun Kim Effect of alumina nanoparticles in the fluid on heat transfer in double-pipe heat exchanger system Department of Chemical and Biological Engineering, Applied Rheology Center, Korea University, Seoul 136- 701, Korea (Received 5 October 2007 • accepted 5 March 2008) [3] KuruvaUmamahesh,K. Venugopal- DesignAnd Analysis Of Double Pipe Heat Exchanger Using Computational Method International Journal Of Professional Engineering Studies Volume V /Issue 2 /JULY 2015
  • 5. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Reference Paper ID - IJTSRD20306 | Volume – 3 | Issue – 2 | Jan-Feb 2019 Page: 213 [4] ArjumandAdil , Sonam Gupta, and Pradyumna Ghosh, “Numerical Prediction of Heat Transfer Characteristics of Nano fluids in a Mini channel Flow”, Journal of Energy Volume 2014, Article ID 307520, 7. [5] M. Esfandiary 1, A. Habibzadeh 2, H. Sayehvand, “Numerical Study of Single Phase/Two-Phase Models for Nano fluid Forced Convection and Pressure Dropin a Turbulence Pipe Flow”, Trans. Phenom. Nano Micro Scales, 4(1):11-18, Winter - Spring 2016. [6] Payam Rahim Mashaei, SeyedMostafaHosseinalipour, and Mehdi Bahiraei, “Numerical Investigation of Nano fluid Forced ConvectioninChannelswithDiscreteHeat Sources”, Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2012. [7] 4. HoomanYarmand, Samira Gharehkhani, SalimNewazKazi, EmadSadeghinezhad, and Mohammad Reza Safaei,“Numerical Investigation of Heat Transfer Enhancement in a Rectangular Heated Pipe for Turbulent Nano fluid”, Hindawi Publishing Corporation, The Scientific World Journal, Volume 2014. [8] Mohammad Nazififard, MohammadrezaNematollahi, KhosrowJafarpur, and Kune Y. Suh, “Numerical Simulation of Water-Based Alumina Nano fluid in Sub channel Geometry”, Science and Technologyof Nuclear Installations, Volume 2012. [9] S. J. Palm, G. Roy, and C. T. Nguyen, “Heat transfer enhancement with the use of Nano fluids in radial flow cooling systems considering temperature-dependent properties,” Applied Thermal Engineering, vol. 26, no. 17-18, pp. 2209–2218, 2006. [10] J. A. Eastman, S. R. Phillpot, S. U. S. Choi, and P. Keblinski, “Thermal transport in ,” Annual Review of Materials Research, vol. 34, pp. 219–246, 2004. [11] S. J. Kim, I. C. Bang, J. Buongiorno, and L.W.Hu, “Surface wettability change during pool boiling of nanofluids and its effect on critical heatflux,” InternationalJournal of Heat and Mass Transfer, vol. 50, no.19-20,pp. 4105– 4116, 2007. [12] J. Buongiorno and B. Truong, “Preliminary study of water based nanofluid coolants for PWRs,” Transactions of the American Nuclear Society, vol. 92, pp. 383–384, 2005.