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 Authors : Bishal Bhandari , Madhav Rijal
 Paper ID : IJERTV7IS090088
 Volume & Issue : Volume 07, Issue 09 (September – 2018)
 Published (First Online): 05012019
 ISSN (Online) : 22780181
 Publisher Name : IJERT
 License: This work is licensed under a Creative Commons Attribution 4.0 International License
Evaluation of Convective Heat Transfer Coefficient of Air Flowing Through an Inclined Circular Duct
Evaluation of Convective Heat Transfer Coefficient of Air Flowing Through an Inclined Circular Duct
Bishal Bhandari[1] Madhav Rijal[2] [1] Mechanical Engineering Graduate [2] BE Mechanical Engineering Graduate Shri Pillappa College of Engineering, Bangalore Sambhram Institute of Technology, Bangalore
Abstract Circular duct has various applications pipelines, HVAC, and refrigeration as it can withstand more pressure drop than noncircular duct. Generally, fluids are forced through the pipes for various purposes. So, Pipes are generally required to be installed at various positions in order to minimize or maximize heat loss, regulate the flow and for the proper utilization of space to meet the design considerations. When fluids are forced through pipes, Heat transfer follows forced convection and the convective heat transfer coefficient plays pivotal role in the design considerations. Hence, it is must to understand the influence of factors such as inclination of pipe, velocity of fluid, and temperature gradient on convective heat transfer coefficient. Literature survey showed little research on effect of those factors in convective heat transfer coefficient. The main purpose of this work is to find out the nature of convective heat transfer coefficient when the air is forced through the copper pipe at different inclination and velocity at constant heat input. Different temperature at various points and the manometer reading were noted and were used to calculate Reynolds number, Prandtl number, and Nusselts number to find
Radiation is the process of heat transfer in which transfer of energy takes place in absence of medium. It occurs place in vacuum.
c) Convection:
The heat transfer by the energy exchange between the molecules of fluid due to the temperature difference is known as convection.
It can be classified as follows:
I ) Free Convection
Free convection occurs due to the buoyancy effect that is by the difference in density of fluid molecules. The heavy molecules travel down to the bottom surface and light molecules travels up there by exchange of heat occurs. The heat transfer coefficient varies with geometry of the system.
out convective heat transfer coefficient. The result obtained was II ) Forced Convection
plotted to observe the nature of heat transfer coefficient. The graph showed that heat transfer coefficient rises to its peak at 900 inclination of the duct for velocity of 12 m/s and falls to minimum value at 300 inclination of the duct for velocity of 8.38 m/s. It is also found that heat transfer coefficient is linearly dependent on velocity and is also influenced by inclination of the duct.
Keywords – Fluids, convection, Convective heat transfer coefficient, Reynolds number, Prandtl number, Nusselts number.

INTRODUCTION

Heat Transfer:
Heat transfer may be defined as the transmission of energy from one region to another as a result of temperature gradient and it takes place by three modes

Conduction

Radiation

Convection

Conduction:
Conduction is heat transfer phenomena from one part of the substance to same substance or from one part of substance to another without appreciable displacement of molecules forming the substance.

Radiation:
The convection process where the fluid motion in a pipe is
regulated by external media that is blower or pump is called forced convection. Here, the heat transfer takes place between the adjacent molecules. Forced convection augments the convection process.



Mechanism of Forced Convection:
Convection heat transfer occurs due to fluid motion and heat conduction there by it is a complicated phenomenon. When fluid is forced, the convection rate is augmented as compared to that of natural convection. The heat transfer process follows Newtons laws of cooling and can be expressed mathematically as follows:
QConv = hA(TSTa) Equation (1)
Where, Q= rate of heat transfer in watts
h= heat transfer coefficient in w/m2co TS= Surface Temperature in co.
Ta=ambient temperature in co.
The convection heat transfer coefficient depends on boundary crosssectional area of pipe through which fluid flows, the temperature difference across test specimen and fluid properties.
Fig. 1.1: Forced convection.
The velocity of fluid at the boundary of solid surface is nearly zero and is known as no slip condition whereas the velocity of fluid at the centre of the pipe is maximum. The heat transfer rate at the boundary surface of pipe is conduction as there is no motion of fluid molecules. Therefore,


EXPERIMENTAL WORK

Experimental Setup of Circular Duct
The experimental setup which comprises of test specimen is made up of copper having Circular cross section of dimensions 36x38x500mm, which is connected to a blower through a GI pipe and bellows. Mounting of the five thermocouples takes place on test section at equal distance. The equipment is mounted on 2ft X 3 ft rectangular board which is made up of mild stainless sheets. The panel board consists of voltmeter, ammeter, temperature indicator, and manometer. The difference in height is observed manually whereas other readings are digitally displayed. The Nichrome wire surrounds the test specimen through which specimen is heated. Also, insulation is provided by wool or rope so that heat is not dissipated to surrounding.

Experimental Setup of Circular Duct at 00
Fig. 2.2 Experimental Setup of Circular Duct at 00

Experimental Setup of Circular Duct at 300
Fig. 2.3 Experimental Setup of Circular Duct at 300

Experimental Setup of Circular Duct at 600
Fig. 2.4 Experimental Setup of Circular Duct at 600

Experimental Setup of Circular Duct at 900
Fig. 2.5 Experimental Setup of Circular Duct at 900

Experimental Setup of Circular Duct at 1200
Fig. 2.6 Experimental Setup of Circular Duct at 1200

Experimental Setup of Circular Duct at 1500
comparison to Type R & S over at a tenth of the cost, therefore prove to be popular alternatives.
TYPE R
Type R thermocouples have similar applications as Type S but provides improved stability and a marginal increase in range. Also, Type R tend to be used in preference to Type S.
TYPE S
Type S thermocouples have capability to continually withstand temperatures up to 1450Â°C while they can be used at the temperature up to 1650Â°C for short period of time. Emf generated gets reduced if they are not protected from high temperature atmosphere which ingress metallic vapor at the tip.
TYPE T
Type T thermocouples are highly used in the laboratory application and have very rare application in industrial sector.
TYPE B
This type of thermocouple gives negligible output up to 500C. It has low electrical output below 6000C, therefore not used below that temperature, and it can be used in the temperature range of 1600Â°C – 1800Â°C.
3.1. Layout of experimental set up
Fig. 2.7 Experimental Setup of Circular Duct at 1500


THERMOCOUPLES
Thermocouples measure the temperature of specimen at different positions. Different types of thermocouple available are listed below.
BL
TYPE E
Type E thermocouple is known as ChromelConstantan thermocouple. Havingmore stability in comparison to type K
T2
T3
T4
T1 T5
B Specimen
Fig.3.1 Layout of experiment setup
they are used where higher accuracy is needed.
TYPE J
In oxidizing atmosphere above 550Â°C, Type J thermocouple degrades very rapidly. Around 750oC they can be operated continuously while 1000Â°C is the maximum temperature they can withstand for short term. They are generally not used below ambient temperature due to condensation forming on the wires which leads to rusting of the iron when used below ambient temperature.
TYPE K
Due to their wide range and low cost, Type K is the most widely used thermocouples in the Oil & Gas, and refining industries. They are occasionally referred to as Chromel Alumel thermocouples. Above about 750Â°C oxidation leads to drift and the need for recalibration.
TYPE N
In the range of 300 to 500Â°C Type N thermocouples can handle higher temperatures than type K, and also offer better repeatability. They provides far more advantages in
Where BL = Blower
B = Bellows
T1 = Inlet temperature of air T5 = Outlet temperatue of air
T2, T3, T4 ,= Specimen surface temperature
The above figure shows the layout of experimental setup when the pipe is at 0 0. The angle of inclinations can be varied to different angle by adjusting the positionof the pipe and obseving at the angular protacter attached to panel board. The different angles varied for this work was 00, 300, 600, 900, 1200, 1500. Temperature at inlet and outlet of duct is measured by temperature sensor at T1 and T5 respectively. The surface temperature is measured by the different thermocouples provided at equal distances on testspecimen by T2 , T3, T4 respectively. Thermocouples used here is Ktype because of its easy availibilty and wide range of operating temperature. The heat input is varied by operating variac knob and the reading of voltmeter and ammeter can be digitally observed. Bellows used in this set up is for the purpose of facilitating the connecting between the blower and the copper duct. The blower valve positions can be varied at different valve position
to vary the velocity and the manometer reading can be noted as well from manometer tube atttached to the panel.

METHODOLOGY
The methodology consists of detailed operating procedure of experimental set up and procedure to take the various readings such as temperature, heads, voltmeter, and ammeter reading.

Description of the Apparatus
The apparatus consists of a blower for forced circulation. The air from the blower passes through a flow passage, heater and then to the test section. Air flow is measured by the height difference of water in manometer tube. A heater placed around the tube heats the air, heat input is controlled by a dimmer stat. Temperature of the air at inlet and at outlet are measured using thermocouples. The surface temperature of the tube is measured at different sections using thermocouples embedded on the Circular duct. Test section is enclosed with wool and rope, where the circulation of rope avoids the heat loss tosurrounding.

Operating Procedure

The valve position is kept at desired level then the blower is turned ON.

Switch ON the heater unit and set the voltage to required level by operating voltage knob and wait until the voltmeter shows stable reading of desired voltage value.

Note down all the temperatures from T1 to T5, voltmeter, ammeter, and manometer head readings.

Repeat the procedure for the different angle of inclination of pipes and for different valve positions.


Precautions to be taken
Dos:

The variac knob should be at zero positions before switching ON an apparatus..

Operate thermocouple selector switch gently.

Operate the experimental set up at least once in two weeks.

Increase the voltage very slowly by using variec knob. Donts:

Heating testspecimen above 200V is prohibited.

Do not perform operations when the line voltage is below 200V.



Specifications
Specimen : Copper Circular duct, 36 mm x 38 mm x 500 mm long.
Heater : Nichrome wire, Externally heated, Band Heater 500W.
Ammeter : Digital type,020amps, AC. Voltmeter : Digital type, 0300volts, AC.
Dimmer stat for heating Coil : 0230v, 2amps. Thermocouple Used : 5 no. ktype, range: 0 to 4000c. Centrifugal Blower : Single Phase 230v, 50 Hz, 13000rpm.
Outer duct : Aluminum.
Insulation : Wool rope

Procedure For Calculation

All the parameters like voltage, current, manometer head, inclination of duct and all temperatures should be noted down precisely and accurately.

Calculate the surface temperature, ambient temperatures and film temperature by using the following formulae
Ts = (T2+T3+T4)/3 Ta = (T1+T5)/2
Tfilm = ( Ts+Ta)/2

Find the properties of air like kinematic viscosity (), Prandtl number (Pr), thermal conductivity (K) at obtained film temperature.

Calculate the Reynolds number (Re) using formula. Re= (V Dh)/

Based on the on Reynolds number calculated above, find out Hilperts constants: C and m.

Use parameters like Pr, C, m, Re to calculate Nusselts number. Its formula is given by
Nu = C x Rem x pr0.333

Find out convective heat transfer coefficient by using the formula
Nu= ( hxDh) / K
Hence, h=( KxNu) / Dh

Repeat the calculation part for following different conditions.

Keeping the heat input as constant. Vary the velocities by adjusting the nozzle position at (1/4)th open, (1/2)th open, (3/4)th open, and full open, and for various angle of inclinations like 00, 300,600, 900 , 1200, and 1500.


9) Tabulate all the calculations for separate angle of inclinations.

RESULTS AND DISCUSSIONS
The readings are noted for constant heat input and the calculations were made. The following table shows the value of Reynolds number, Nusselts number and Heat transfer coefficient for different valve position and angle of inclinations. The following table presents only results.
Sl.
No.
deg
Open Valve Posn
Velocity (m/s)
Re
Nu
h
(kW/m
2 0k)
01
0
1/4th
11.097
21369
81.02
64.98
1/2
12.578
25132.5
89.6
70.92
3/4th
12.58
24736.01
88.77
70.04
Full
12.24
23966.08
86.19
68.24
02
30
1/4th
8.386
16052.12
68.05
54.53
1/2
12.58
24729.28
88.73
70.24
3/4th
12.58
24926.84
89.18
70.4
Full
11.86
23680.18
86.4
67.97
03
60
1/4th
9.375
17835.88
72.45
58.31
1/2
16.245
31869.22
81.99
3/4th
16.245
32268.65
104.6
82.49
Full
16.245
32191.64
104.5
82.45
04
90
1/4th
9.375
18026.91
72.92
120.9
1/2
20.54
40866.74
120.9
95.38
3/4th
22.966
46128.92
131
102.7
Full
23.72
47907.58
135.1
105.6
05
120
1/4th
13.26
25766.61
90.98
72.51
1/2
21.787
43276.04
124.9
98.48
3/4th
23.345
46297.83
131.1
103.6
Full
23.34
46990.67
132.9
104.3
06
150
1/4th
12.57
21042.95
81.36
70.12
1/2
19.66
39401.96
117.4
92.26
3/4th
24.08
48753.44
136.9
108.4
Full
23.34
46549.82
130.9
103.9
5.1 Graphs

Comparison between velocity and heat transfer co efficient for 00 inclination
Fig.5.1. heat transfer coefficient Vs velocity at 00
The above graph shows that the heat transfer coefficient, h, varies linearly with respect to the velocity. The maximum value of h observed is 70.92 (kW/m2 0k) at the velocity of
12.58 m/s and minimum value of h is 64.98 (kW/m2 0k) at the velocity of 11.09 m/s. The increases in velocity has overall resulted the increase in value of h for zerodegree inclination.

Comparison between velocity and heat transfer coefficient for 300 inclinations.
Fig.5.2. heat transfer coefficient Vs velocity at 300
The above graph shows that the heat transfer coefficient, h, varies linearly with respect to the velocity. The maximum value of h observed is 70.4 (kW/m2 0k) at the velocity of 12.58 m/s and minimum value of h is 54.53 (kW/m2 0k) at the velocity of
8.38 m/s. The increases in velocity has overall resulted the increase in value of h for thirtydegree inclination.

Comparison between velocity and heat transfer co efficient for 600 inclination
Fig.5.3. heat transfer coefficient Vs velocity at 600
The above graph shows that the heat transfer coefficient, h, varies linearly with respect to the velocity. The maximum value of h observed is 82.49 (kW/m2 0k) at the velocity of
16.25 m/s and minimum value of h is 58.31 (kW/m2 0k) at the velocity of 9.37 m/s. The increases in velocity has overall resulted the increase in value of h for zerodegree inclination.

Comparison between velocity and heat transfer co efficient for 900 inclinations.
Fig.5.4. heat transfer coefficient Vs velocity at 900
The graph shows that the value of heat transfer coefficient is maximum i.e. 105.6 (kW/m2 0k) at the velocity of 23.72 m/s. The minimum value of h is 57.17(kW/m2 0k) at the velocity of
9.375 m/s. This shows that the value of h varies linearly with respect to velocity for 90degree.

Comparison between velocity and heat transfer co efficient for 1200 inclination.
Fig 5.5. heat transfer coefficient Vs velocity at 1200
In the above plot it can be seen that the heat transfer coefficient increases linearly with respect to velocity. The minimum value of h is 72.51 (kW/m2 0k) at lowest velocity
13.26 m/s and starts increasing to the maximum value of 104.3(kW/m2 0k) at the velocity 23.34 m/s. This indicates the heat transfer coefficient varies linearly in this inclination.

Comparison between velocity and heat transfer co efficient for 1500 inclination.
i.
Fig.5.6. heat transfer coefficient Vs velocity at 1500
It is clear from the above graph that h is linearly dependent on velocity. The value of convective heat transfer coefficient increases as velocity increases. The highest value of h is 108.4(kW/m2 0k) at the velocity of 24.08 m/s whereas the minimum value is 70.12(kW/m2 0k) at the velocity of 12.57 m/s.

Comparison between Reynolds number and Nusselts number
Fig.5.7.Reynolds number v/s Nusselts number
The above graph shows the variation of Reynolds number Vs Nusselts number. It is evident that the increase in Reynolds number increases Nusselts number in each of the different openings. The lowest value of Reynolds number has resulted lowest value of Nusselts number for onefourth of opening of the valve. Similarly, highest value of Nusselts number is obtained at highest Reynolds number at threefourth opening of the valve.

Comparison between inclination of Circular duct and heat transfer co efficient for different angles and different valve positions.
Fig.5.1.Inclination v/s heat transfer coefficient for all velocities

When the valve is onefourth open, the heat transfer coefficient has decreased at 300 inclination compared to that of 00 inclination and increases at 600 then again it decreases at 900 then the value of convective heat transfer increases somewhat abruptly than previous degrees at 1200 and falls slightly at 1500 inclination of duct.

When the valve was half open, the heat transfer coefficient slightly decreased at 300 compared to 00 then increased at 600 , 900 , and 1200 respectively and again decreased at 1500 .

When the valve is threefourth open, the heat transfer coefficient slightly decreased at 300 compared to 00 then increased at 600 , 900 , and decreased slightly at 1200 and reaches maximum value at 1500 inclination of the pipe.

The heat transfer coefficient plot shows same nature for full opening of the valve at angles 300, 600, 900, 1200 as that of plot of threefourth opening at same angles respectively but shows nearly constant value for 1500 as that of 1200.

The variation of velocity is established by operating the valve. The higher value of heat transfer coefficient for zero degree inclination is recorded for half open. The near constant value was obtained for halfopen, three fourth open, and full open at 60 degree which was highest at that angle but the lowest value was observed for onefourth angle for the same angle of inclination of pipe. The value of heat transfer coefficient was decreasing in the order for full open, threefourth open, half open and onefourth open valve position respectively and was maximum for full opening and lowest for onefourth opening at 900 inclination of the duct. Highest value of heat transfer coefficient is obtained for full opening, same value for half and threefourth open but is slightly lesser than that of full open and then lowest value is recorded for onefourth opening at an angle of 1200. For 1500 inclination of duct the value of heat transfer coefficient was in the decreasing order for the threefourth, full, half, one fourth opening of the valve respectively.

The highest value of convective heat transfer coefficient is recorded for threefourth opening of the valve at 1500 inclination of the duct where as the lowest value is obtained for onefourth opening of the valve at 300 inclination of the duct.



CONCLUSIONS

This work has indicated that the use of correlations for horizontal pipe in correlations for inclined pipe produces erroneous result. Therefore, formulation of correlations for convective heat transfer coefficient for inclined duct is necessary.

It is also observed that angle of inclination of the duct influences heat transfer coefficient.

The heat transfer coefficient varies linearly with respect to the velocity.

From our work it can be concluded that the maximum value of heat transfer coefficient (h max = 108.4 kW/m2 0k) is obtained at the inclination of 1500 for threefourth opening of the valve.

The lowest value of heat transfer coefficient (h min =
54.53 kW/m2 0k) is obtained at the inclination of 300 for one fourth opening of the valve.
7. SCOPE FOR FUTURE WORK

This research work can be carried out for different fluids. Work can be done at various heat input values so that the natures for various parameters can be compared.

Work can be done for the different geometrical cross sections.

Heat transfer rate can also be determined by boundary layer analysis to compare with the values obtained experimentally.

The accurate measurement by computerized control can be done to increase the accuracy of the method.

Fins can be attached and its effect can be observed on convective heat transfer coefficients.
8. ACKNOWLEDGMENT
I would like to acknowledge Dr. Channabasavraj, Head of Department, Mechanical Engineering, Shri Pillappa college of Engineering, Bangalore for being a constant source of inspiration in my life.
I would like to thank Dr. H D Ramesh, Principal, Shri Pillappa College of Engineering, Bangalore for giving me permission to perform this research work at SPCE, Bangalore.
I take this opportunity to express my thanks to all the staff of the Department of Mechanical Engineering, SPCE,Bangalore and all my friends and my parents who are directly or indirectly responsible for the accomplishment of this project work.
9. REFERENCES
[1] R. Langebach, and Ch. Haberstroh, Natural convection in inclined pipes – A new correlation for heat transfer estimations Aip conference proceedings 1573,1404; https://doi.org/10.1063/1.4860885, 2014 [2] Prof. R. Telrandhe et al, Thermal Analysis of Circular Inclined Pipe Subjected To Natural Convection Using CFD. Int. Journal of Engineering Research and Applications Vol. 3, Issue 5, pp.19111913, SepOct 2013 [3] Yasuo, Mow,Wataru,Naka,yama, Study On Forced Convective Heat Transfer In Curved Pipes. International Journal Of Heat And Mass Transfer, vol 8, Issue 1, page 6782, Jan 1965. [4] J.B.Will N .P.Kruyt C.H.Venner, An experimental study of forced convective heat transfer from smooth, solid spheres. International Journal of Heat and Mass Transfer Volume 109, Pages 10591067 June 2017. [5] Zhang, Z.C. Zhang, S. Eckels, Study of heattransfer on the surface of a circular cylinder in flow using an immersed boundary method. Int. Journal of Heat Fluid Flow, vol 29 page 15581566, 2008. [6] S. Sanitjai, R.J. Goldstein , Forced convection heat transfer from a circular cylinder in cross flow to air and liquids Journal of Fluid Mechanics, Vol. 47, pp.4795 4805,2004. [7] R.P. Bharti, R.P. Chhabra, V. Eswaran ,A numerical study of the steady forced convection heat transfer from an unconfined circular cylinder Int.J. Heat Mass Transfer, Vol 43, pp. 639 648, 2007 [8] Akram W. Ezzat, Hassan W. Zghaer , Forced Convection Heat Transfer around Heated Inclined Cylinder International Journal of Computer Applications ,Volume 73 No.8, July 2013. [9] Petukhov, B.S., Heat transfer and friction in turbulent pipe flow with variable properties Advances in Heat Transfer, Vol.6,pp 504506,1970. [10] Sunil S, Basavaraj H.T , Evaluation of Convective Heat Transfer Coefficient of Air Flowing Through an Inclined Square Duct International Journal of Engineering Research & Technology ,Vol.4 issue 2, February2015
[11] Churchill, S. W. and M. Bernstein. A correlating Equation for Forced Convection from Gases and Liquids to a Circular Cylinder in Crossflow J. Heat Transfer, 99:300306. 1977. [12] Mohammed, Hussein & Salman, Yasin. Free and forced convection heat transfer in the thermal entry region for laminar flow inside a circular cylinder horizontally oriented Energy Conversion and Management. 48. 21852195. 10.1016/j.enconman.2006.12.016,2007