Nothing Special   »   [go: up one dir, main page]

CFD Analysis For Cone Helically Coiled Tube Heat Exchanger by Varying Pitch Ijariie11095

Download as pdf or txt
Download as pdf or txt
You are on page 1of 8

Vol-5 Issue-6 2019 IJARIIE-ISSN(O)-2395-4396

CFD ANALYSIS FOR CONE HELICALLY


COILED TUBE HEAT EXCHANGER BY
VARYING PITCH
Prof. Pushparaj Singh1, Manish Tripathi2
1
Rewa Institute of Technology, Professor, REWA, MP, INDIA
2
Rewa Institute of Technology, M.Tech Scholar, REWA, MP, INDIA

ABSTRACT

Now-a-days heat exchangers have become indispensable in various fields of engineering such as in air
conditioning, power stations, chemical plants, automobiles, etc. It necessitates the compact size along with the
high performance of the heat exchangers. For the improvement in heat transfer performance of heat exchangers,
heat transfer coefficient has an important role to play. Generally modifications which are made to enhance heat
transfer coefficient leads to increase in pressure drop in heat exchangers. Hence the selection of most
appropriate configuration is an important consideration in design of a heat exchanger. Secondary flow pattern
formed in curved tubes plays an important role in mixing of fluid which leads to an increase in heat transfer
coefficient along with an increase in pressure drop also.

Helically coiled exchangers offer certain advantages. Compact size provides a distinct benefit. Higher film
coefficients—the rate at which heat is transferred through a wall from one fluid to another— and more effective
use of available pressure drop result in efficient and less-expensive designs. Heat transfer rate of helically coiled
heat exchangers is significantly larger because of the secondary flow pattern in planes normal to the main flow
than in straight pipes.

This work aims to study on passive technique of heat transfer enhancement by some variation in geometry of
helical coil tube heat exchanger. In this work the heat transfer and pressure drop analysis has been done for
conical coil with varying pitch. The pitch number taken for the study are 18mm, 20mm and 22mm. The
nanofluid of 0.5% volume concentration are supplied for cone helically coiled tube and hot water is supplied to
the shell side. The mass flow rate of shell side is maintained constant at 0.15 Kg/s.The inlet temperature of hot
fluid (shell) is 338 K whereas the inlet temperature of cold fluid (for cone helically coiled tube) is 305 K. The
flow rate of the cone tube which handled nanofluid is varies from 0.05-0.07 Kg/s. It is found that the maximum
overall heat transfer coefficient for pitch=22 mm is 32.23% higher than the pitch=18mm and maximum Nusselt
number for pitch=22 mm is 14.91% higher than the pitch=18mm.

Keywords: Cone coiled helical tube, Heat Exchanger, Nusselt number, Reynold’s number, Pressure drop,
Nano-fluids, CFD.

I. INTRODUCTION:

Heat exchangers are an essential part in an assortment of mechanical settings, for example, cooling frameworks,
force plants, refineries, and in this way ceaseless endeavour are made to expand their heat transfer efficiencies.

The design procedure of heat exchangers is quite complicated, as it needs exact analysis of heat transfer rate and
pressure drop estimations apart from issues such as long-term performance and the economic aspect of the
equipment. The major challenge in designing a heat exchanger is to make the equipment compact and achieve a
high heat transfer rate using minimum pumping power. Techniques for heat transfer augmentation are relevant
to several engineering applications. In recent years, the high cost of energy and material has resulted in an
increased effort aimed at producing more efficient heat exchange equipment. Furthermore, sometimes there is a
need for miniaturization of a heat exchanger in specific applications, such as space application, through an
augmentation of heat transfer. Heat transfer enhancement is one of the most promising methods to optimize heat

11095 www.ijariie.com 1006


Vol-5 Issue-6 2019 IJARIIE-ISSN(O)-2395-4396

transfer equipment and to increase heat recovery in industrial processes. Heat transfer enhancement techniques
have been extensively developed to improve the thermal performance of heat exchanger systems with a view to
reducing the size and cost of the systems. Swirl flow is the one of the enhancement techniques widely applied to
heating or cooling systems in many engineering applications.

Heat transfer enhancement techniques are classified as the - Passive Methods, Active Methods, and Compound
Methods. These methods are commonly used in areas such as process industries, heating and cooling in
evaporators, thermal power plants, air-conditioning equipment, refrigerators, radiators for space vehicles,
automobiles, etc. The rate of heat transfer can be increased passively by increasing the surface area, roughness,
and by changing the boundary conditions. The active method involves addition of nano sized, high thermal
conductivity, and metallic powder to the base fluid, to increase the heat transfer rate.

Passive techniques, where inserts are used in the flow passage to enhance the heat transfer rate, are best suited
compared to active techniques. Because the insert manufacturing process is simple and these techniques can be
easily applied in an existing application.

A. Active Technique
The active method involves external power input for the enhancement in heat transfer; for examples it includes
mechanical aids and the use of a magnetic field to disturb the light seeded particles in a flowing stream, etc.

B. Passive Technique
The Passive heat transfer methods does not need any external power input. In the convective heat transfer one of
the ways to enhance heat transfer rate is to increase the effective surface area and residence time of the heat
transfer fluids. By Using this technique causes the swirl in the bulk of the fluids and disturbs the actual
boundary layers which increase effective surface area, residence time and simultaneously heat transfer
coefficient increases in an existing system. Methods generally used are, extended surface, displaced
enhancements devices, rough surfaces surface tension devices, Inserts etc.

C. Compound method
A compound method is a hybrid method in which both active and passive methods are used in combination. The
compound method involves the complex designs and hence it has limited applications.

Helically coiled-tube heat exchangers


Helically coiled-tube heat exchangers are one of the most common equipment found in many industrial
applications ranging from solar energy applications, nuclear power production, chemical and food industries,
environmental engineering, and many other engineering applications. Heat transfer rate of helically coiled heat
exchangers is significantly larger because of the secondary flow pattern in planes normal to the main flow than
in straight pipes.

Figure 1. Helically coiled-tube heat exchanger.

Helically coiled exchangers offer certain advantages. Compact size provides a distinct benefit. Higher film
coefficients—the rate at which heat is transferred through a wall from one fluid to another— and more effective
use of available pressure drop result in efficient and less-expensive designs. True counter-current flow fully
utilizes available LMTD (logarithmic mean temperature difference). Helical geometry permits handling of high
temperatures and extreme temperature differentials without high induced stresses or costly expansion joints.
High-pressure capability and the ability to fully clean the service-fluid flow area add to the exchanger’s
advantages. Although various configurations are available, the basic and most common design consists of a

11095 www.ijariie.com 1007


Vol-5 Issue-6 2019 IJARIIE-ISSN(O)-2395-4396

series of stacked helically coiled tubes. The tube ends are connected to manifolds, which act as fluid entry and
exit locations.

1.6 Nanofluids

Nanofluids have some unique features which are quite different from dispersions of mm or μm sized particles.
Compared to conventional cooling liquids such as water, kerosene, ethylene glycol and micro fluids, nanofluids
have been shown to exhibit higher thermal conductivities. There are mainly two techniques of nanofluids
production, namely two-step technique and single-step technique. In the two-step technique, the first step is the
production of nanoparticles and the second step is the mixing of the nanoparticles in a conventional base fluid.

Figure 2. Nanofluid Preparation.

Computational Fluid Dynamics Analysis


This is a computer-based analysis by which we analyse the various things like fluid flow, pressure distribution,
heat transfer, and related to the phenomenon in the chemical reactions.

There are the three main elements for the processing of the CFD simulations discussed below;
1. Preliminaries processing: this is the first step where the geometry of the issues to be solved are analyzed A
pre-processor is defined to the geometry regarding the problem. They are fixed into the domain for the
computational analysis and then yields the mesh associated with geometry. Here also put the nomenclature like
inlet, outlet, wall, etc. Usually, the finer the mesh associated with geometry into the CFD analysis offers more
solution that is accurate. The choice of computer hardware and the time for calculations are dictated by the
fineness of the grid.

2. Solver: - The calculations are done by using the numerical solution methods in the solver processor. You will
find the countless numerical practices that are utilized for the computations for example:-the finite factor
method, finite amount technique, the finite huge difference technique additionally the spectral strategy. Most of
them in computer codes use the finite volume method into the following steps:
• Firstly the fluid movement equations are integrated on the control volumes (leading to the actual preservation
of appropriate properties for every finite amount),
•Then these key equations tend to be discretized (creating algebraic equations through converting of the
fundamental fluid movement mathematical expressions)
• Finally, mathematical relations and equations are fixed using the iterative method.
• Pressure based paired option method CFD rule is used for resolving the simulations in this task.

3. Post Processing: This is done to visualize the total link between the solutions. It includes the ability to display
the mesh and geometry also. As well as in this processor we could create the vectors, contours, and 2D and
surface that is 3D of the issue solutions. Right Here the model can also be manipulated. In this method, we could
also look at the cartoon of the problem.

II. LITERATURE REVIEW


It has been widely reported in literature that heat transfer rates in helical coils are higher as compared to a
straight tube. Due to the compact structure and high heat transfer coefficient, helical coil heat exchangers are
widely used. Striving to ensure high performance of the heat exchangers, HX, nowadays is a source of universal
trend both to the miniaturization of these devices for both industrial and domestic applications, while

11095 www.ijariie.com 1008


Vol-5 Issue-6 2019 IJARIIE-ISSN(O)-2395-4396

maintaining the highest possible size to thermal energy ratio. As is well known, in the case of Recuperators the
heat transfer coefficient has a decisive influence on their efficiency. Overall heat transfer coefficient, depends
mainly on the lower value of heat transfer value (HTC) from working media.

It is, therefore, most significant to improve the heat transfer with special attention on the side of the medium
with lower heat transfer coefficient. Helical coils are widely used in applications such as heat recovery systems,
chemical processing, food processing, nuclear reactors, and high temperature gas cooling reactors. Helical coils
have been widely studied both experimentally and numerically.

A considerable amount of experimental as well as analytical and computational research has been carried out on
the enhancement of heat transfer. In this chapter, a brief survey of the relevant literature is presented to indicate
the extent of work already reported in open literature pertaining to the enhancement of heat transfer by
introducing nano fluid and helical coil in the heat exchanger.

2.1 Previous work

G. Rahul Kharat et. al. [2009], carried out a comparative study between helical coil heat exchanger and
straight tube heat exchanger, and found that the effectiveness of heat exchanger is greatly affected by hot water
mass flow rate and cold water flow rate. When cold water mass flow rate is constant and hot water mass flow
rate increased the effectiveness decreases. Increase in cold water mass flow rate for constant hot water mass
flow rate resulted in increase in effectiveness. For both helical coil and straight tube heat exchangers with
parallel and counter flow configuration this result obtained. Helical coil counter flow is effective in all these
conditions than the straight tube parallel flow heat exchanger. Overall heat transfer coefficient on other hand
increases with increase in hot water mass flow rate and cold water mass flow rate. Use of a helical coil heat
exchanger was seen to increase the heat transfer coefficient compared to a similarly dimensioned straight tube
heat exchanger [3].

Ghadimi et al. [2011] suggested that the two-step method gives higher stability and low agglomeration with a
better nanostructure. The MWCNT water-based nanofluids have been synthesized at 0.1%, 0.3%, 0.5%, volume
concentration. The morphological characters of MWCNT in base fluid nanofluid are obtained by Transmission
Electron Microscopy (TEM). TEM Image clearly illustrates that the MWCNT core is hollow with multiple
layers almost parallel to the MWCNT axis [4].

E. Jung-Yang San et. al. [2012], Heat transfer characteristics of a helical heat exchanger”, found that the
impact of coil curvature is to suppress turbulent fluctuations arising within the flowing fluid and smoothing the
appearance of turbulence. Thus it will increase the value of the Reynolds number (Re) needed to attain a fully
turbulent flow, as compared to it of a straight pipe. The impact of turbulent fluctuations suppression enhances as
the curvature ratio of coil increases [5].

Wang et al. [2013] investigated the heat transfer and pressure drop of working fluids as water-based CNT
nanofluids in a circular tube as a horizontal position. They concluded that the enhancement of average
convective heat transfer increases with increase in volume concentration of nanoparticles at constant Reynolds
number [6].

Ellahi et al. [2016] carried out the particle shape effects on Marangoni convection boundary layer flow of a
nanofluids with the blend of numerical and analytical studies. They suggested that the interface velocity reduces
by increasing particle volume fraction and the spherical shape is better for heat transfer point view [11].

Bahiraei et al. [2018] applied a novel hybrid nanofluid containing graphene – platinum nanoparticles in twisted
geometry in a miniature devices. They proposed that the heat transfer and pumping power in the channel
increase by increasing pressure drop and Dean Number. The ratio of heat transfer to the power in the chaotic
channel is greater than 1.5 [17].

Bahiraei et al. [2019] numerically inverted the hydro thermal and energy efficiency of a hybrid nanofluids
(graphene – platinum nanofluid) in a tube connected by twisted tapes. They have taken the twisted angle, twin
co – twisted tape and counter twisted tape for co-swirling flows recommended to use the counter twisted tapes
with higher twisted ratio to enhance the heat transfer with reduced energy consumption [18].

K. Palanisamy et al. [2019] numerically investigated the heat transfer and the pressure drop of cone helically
coiled tube heat exchanger using (Multi wall carbon nano tube) MWCNT/water nanofluids. The tests was

11095 www.ijariie.com 1009


Vol-5 Issue-6 2019 IJARIIE-ISSN(O)-2395-4396

conducted under the turbulent flow in the Dean number range of 2200 < De < 4200. The experiments was
conducted with experimental Nusselt number is 28%, 52% and 68% higher than water for the nanofluids volume
concentration of 0.1%, 0.3% and 0.5% respectively. It was found that the pressure drop of 0.1%, 0.3% and 0.5%
nanofluids are found to be 16%, 30% and 42% respectively higher than water. It is also studied that there is no
immediate risk of handling MWCNT and studied that there is no significant erosion of coiled tube inner wall
surface even after several test runs. Therefore the MWCNT/water nanofluids are the alternate heat transfer
fluids for traditional fluids in the cone helically coiled tube heat exchanger to improve the heat transfer with
considerable pressure drop [21].

It is studied from the literature review that most of the experimental works on double helically coiled tube heat
exchanger have been done by using oxide nanofluids. Very little works have been done on cone helically coiled
tube heat exchanger by using MWCNT/water nanofluids with CFD software. Therefore this investigation deals
with the thermal and flow behaviour of cone helically coiled tube heat exchanger handling MWCNT/water
nanofluids at three different pitch number by varying pitch of helical coil.

III. RESEARCH OBJECTIVES


The objectives of this study are:
(i) Investigating the thermal and flow behaviours of MWCNT/water nanofluids with higher volume concentration
at different Dean number in cone helically coiled heat exchanger by varying pitch size.
(ii) To observe which configurations and parameters that gives the best results.
(iii) To study and modeling the heat transfer of cone helically coiled tube heat exchanger using CFD simulation.

IV. METHODOLOGY
Table 1. Dimensions of cone coil tube Figure 3 Cone helically coiled tube heat exchanger.

Cone coil angle (θ) 8 degree


Cone inner tube
0.08 cm
dimeter(di)
Cone outer tube diameter
0.1 cm
(do)
Diameter of the shell 11.4 cm
Effective length of the coil 470 cm
Pitch of the coil 1.8, 2.0, 2.2 cm
Calming section length 11 cm
Cone coil diameter 6.4 cm
Number of turns 16

The designed model of Cone helically coiled tube heat exchanger is meshed in ICEM Meshing.

Model Selection

The governing equations are discretized by finite volume method and solved in steady-state implicit format. The
SIMPLE algorithm is used to couple the velocity and pressure fields. The second order upwind scheme is
applied and standard k-ε turbulent model with standard wall function is selected.

Boundary Conditions

Flow is turbulent and counter flow conditions. The nanofluid of 0.5% volume concentration are supplied for
cone helically coiled tube and hot water is supplied to the shell side. The mass flow rate of shell side is
maintained constant at 0.15 Kg/s.The inlet temperature of hot fluid (shell) is 338 K whereas the inlet
temperature of cold fluid (for cone helically coiled tube) is 305 K. The flow rate of the cone tube which handled
nanofluid is varies from 0.05-0.07 Kg/s.After putting the boundary conditions, the solution is initialized and
then iteration is applied so that the values of all parameters can be seen in a curve or line graph. After the
iteration gets completed final result could be seen.

11095 www.ijariie.com 1010


Vol-5 Issue-6 2019 IJARIIE-ISSN(O)-2395-4396

V. RESULTS AND DICUSIONS

Here in this section nanofluid of 0.5% volume concentration for cone helically coiled tube flowing at Dean
Number 2200. While the mass flow rate of shell side is maintained constant at 0.15 Kg/s.

Figure 4. Contours of static temperature at Dean number 2200 for pitch= 20 mm.

Figure 5. Contours of static temperature at Dean number 2200 for pitch= 18mm.

Figure 6. Contours of static temperature at Dean number 2200 for pitch= 22mm.

11095 www.ijariie.com 1011


Vol-5 Issue-6 2019 IJARIIE-ISSN(O)-2395-4396

Table 2. Comparison of values of Nusselt no. at different Dean No. for different pitch number
Nusselt Number
Dean
S.No. Pitch=20 Pitch=20 Pitch=18mm Pitch=22
Number
mm(Experimental) mm(CFD) mm(CFD) mm(CFD)
1. 2200 74 74.84 72.67 85.36
2. 3025 97 97.9 94.47 98.85
3. 4200 119.5 126.99 114.57 131.88

Table 3. Comparison of values of Overall heat transfer coefficient at different Dean No. for different pitch
number
Overall heat transfer coefficient (W/m2-K)
Dean
S.No. Pitch=20 Pitch=20 Pitch=18mm Pitch=22
Number
mm(Experimental) mm(CFD) mm(CFD) mm(CFD)
1. 2200 860 872 860.87 885.54
2. 3025 970 983 969.32 1001.20
3. 4200 1140 1156 1141.56 1179.80

Table 4. Comparison of values of Pressure drop at different Dean No. for different pitch number
Pressure drop (Pascal)
Dean
S.No. Pitch=20 Pitch=20 Pitch=18mm Pitch=22
Number
mm(Experimental) mm(CFD) mm(CFD) mm(CFD)
1. 2200 10520 11180 12443 10120
2. 3025 14750 15717 16116 14320
3. 4200 16950 17469 18965 16732

VI. CONCLUSIONS

In recent years a lot of attention has been paid to improving the Thermal performance of heat exchanger. In this
work a heat exchanger of cone helical coil tube type was first designed in CFD. Helical coil heat exchangers of
three different coil pitches were investigated for counter flow configuration. The mass flow rate of the hot fluid
was kept stable at 0.15 kg/s and the values of the MWCNT/water fluid were altered between 0.05 kg/s up to
0.07 kg/s. From the outcomes of the present study, it is found that at higher mass flow rate of the
MWCNT/water fluid an increased heat transfer in the heat exchanger was achieved. It is also found that
maximum heat transfer characteristics are exhibited by coil of pitch 22mm as compared to other two coils of
pitch 18mm and 20mm.

REFERENCES

[1] Dravid, A. N., Smith., K. A., Merrill, E.A., and Brian, P.L.T., (1971).Effect of secondary fluid motion on
laminar flow heat transfer in helically coiled tubes AIChE Journal, Vol.17(5):1114-1122
[2] Patankar S.V., Pratap V.S., Spalding D.B.: Prediction of laminar flow and heat transfer in helically coiled
pipes. J. Fluid Mech. 62(1974), 539–551.
[3] Rahul Kharat, NitinBhardwaj, R.S. Jha, 2009, Development of heat transfer coefficient correlation for
concentric helical coil heat exchanger.
[4] Ghadimi, R. Saidur, H.S.C. Metselaar, A review of nanofluid stability properties and characterization in
stationary conditions, Int. J. Heat Mass Transf. 54 (2011) 4051–4068.
[5] Jung-Yang San, Chih-Hsiang Hsu and Shih-Hao Chen, “Heat transfer characteristics of a helical heat
exchanger”, Applied Thermal Engineering 39 (2012) 114e120, Jan 2012
[6] J. Wang, J. Zhang, X. Zhang, Y. Chen, Heat transfer and pressure drop of nanofluids containing carbon
nanotubes in laminar flows, Exp. Therm. Fluid Sci. 44 (2013) 716–721.

11095 www.ijariie.com 1012


Vol-5 Issue-6 2019 IJARIIE-ISSN(O)-2395-4396

[7] B. ChinnaAnkanna, B. Sidda Reddy, “Performance analysis of fabricated helical coil heat exchanger”,
International Journal of Engineering Research, ISSN:2319-6890), Volume No.3 Issue No: Special 1, pp: 33-39,
March 2014.
[8] C. A. Chaves, D. R. F. de Castro, W. Q. Lamas, J. R. Camargo and F. J. Grandinetti, “Computational Fluid
Dynamics (CFD) simulation to analyze the performance of tube-in-tube helically coiled of a heat exchanger”,
Academic Journals Article No. 06A188B43755, ISSN 1992-2248, 2014
[9] Jaivin A. Varghese ,Sreejith K., T.R. Sreesastha Ram, Sreejith K., Jaivin A. Varghese, Manoj Francis,
Mossas V.J., Nidhin M.J., Nithil E.S., Sushmitha S. Experimental Investigation of a Helical Coil Heat
Exchanger Vol.5, Issue 8(August 2015), PP -01-05
[10] Jian Wen, Huizhu Yang, Simin Wang, YulanXue and Xin Tong, “Experimental investigation on
performance comparison for shell-and-tube heat exchangers with different baffles”, 2015.
[11] R. Ellahi, A. Zeeshan Mohsan Hassan, Particle shape effects on Marangoni convection boundary layer
flow of a nanofluid, Int. J. Numer. Methods Heat Fluid Flow 26 (2016) 2160–2174.
[12] Aaqib Majeed, Ahmad Zeeshan, Sultan Z. Alamri, Rahmat Ellahi, Heat transfer analysis in ferromagnetic
viscoelastic fluid flow over a stretching sheet with suction, Neural Comput. Appl. 30 (2018) 1947–1955.
[13] Zeeshan Ahmed, Nouman Ijaz, Tehseen Abbas, Rahmat Ellahi, The sustainable characteristic of bio-Bi-
phase flow of peristaltic transport of MHD Jeffrey fluid in the human body, Sustain. MDPI 10 (2018) 1–17.
[14] Farooq Hussain, Rahmat Ellahi, Zeeshan Ahmad, Mathematical models of Electromagneto hydrodynamic
multiphase flows synthesis with nano-sized Hafnium particles, Appl. Sci. 8 (2018) 275.
[15] N. Shehzad, A. Zeeshan, R. Ellahi, Electroosmotic flow of MHD power law Al2O3- PVC nanofluid in a
horizontal channel: Couette-Poiseuille flow model, Commun. Theor. Phys. 69 (2018) 655–666.
[16] M. Hassan, M. Marin, AbdullahAlsharif, R. Ellahi, Convective heat transfer flow of nanofluid in a porous
medium over wavy surface, Phys. Lett. 382 (2018) 2749–2753.
[17] Mehdi Bahiraei, Nima Mazaheri, Application of a novel hybrid nanofluid containing grapheme -platinum
nanoparticles in a chaotic twisted geometry for utilization in miniature devices: thermal and energy efficiency
considerations, Int. J. Mech. Sci. 138–139 (2018) 337–349.
[18] Mehdi Bahiraei, Nima Mazaheri, Seyed Mohammadhossein Hassanzamani, Efficacy of a new grapheme -
platinum nanofluid in tubes fitted with single and twin twisted tapes regarding counter and co-swirling flows for
efficient use of energy, Int. J. Mech. Sci. 150 (2019) 290–303.
[19] Mehdi Bahiraei, Nima Mazaheri, Ali Rizehvandi, Application of a hybrid nanofluid containing graphene
nanoplatelet–platinum composite powder in a triple-tube heat exchanger equipped with inserted ribs, Appl.
Therm. Eng. 149 (2019) 588–601.
[20] Mehdi Bahiraei, Saeed Heshmatian, Mansour Keshavarzi, Multi-criterion optimization of thermohydraulic
performance of a mini pin fin heat sink operated with eco friendly graphene nanoplatelets nanofluid considering
geometrical characteristics, J. Mol. Liq. 276 (2019) 653–666.
[21] K. Palanisamy, P.C. Mukesh Kumar, Experimental investigation on convective heat transfer and pressure
drop of cone helically coiled tube heat exchanger using carbon nanotubes/ water nanofluids, Heliyon 5 (2019)
e01705.

11095 www.ijariie.com 1013

You might also like