Imperial Journal of Interdisciplinary Research (IJIR) Vol-2, Issue-9, 2016 ISSN: 2454-1362, http://www.onlinejournal.in Experimental Investigation on C and V Shaped Inline and Staggered Fins Array Using Forced Convective Heat Transfer Sujan T N1, Mr. Krishnamurthy K N2 & Mr. Akash Deep B N3 1 M Tech. Student, Department of Thermal Power Engineering, PG Studies-VTU-Mysuru, Karnataka, India 2 Assistant Prof, Department of Thermal Power Engineering, Centre for Post-Graduate Studies VTU, Mysuru, Karnataka, India 3 Assistant Prof, Department of Mechanical Engineering, KSSEM, Bengaluru, Karnataka, India Abstract-In orders to facilitate better heat transfer, various types of fins are studied extensively and various modifications are made in the design till date. Geometry of fin arrays plays an important role in heat transfer characteristics. This research was conducted in order to study C and V shaped fins with inline and staggered arrangement and makes comparisons on the basis of heat transfer and pressure drop characteristics. The result shows C shaped staggered arrangement is better in terms of heat transfer and pressure drop performance as compared to V shaped fins. The heat transfer coefficient for C shaped staggered fins are in the range of 51 – 80 W/m2K while for V shaped staggered arrangement, it is found to be in the range of 41 – 71 W/m2K for a Reynolds number in the range of 10000 – 35000. The pressure drop for C shaped staggered fins was found to be lower than corresponding to V shaped fins and is obtained in the range of 10 – 45 N/m2 while for V shaped fins, in the range of 23 – 93 N/m2. Overall analysis shows C shaped fins are more attractive than V shaped fins in terms of energy saving as well as heat transfer characteristics. Key words: V-shaped Pin fins, C-shaped pin fins, Inline Arrangement, Staggered Arrangement, Heat Transfer Enhancement, Pressure Drop. 1. Introduction The thermal energy present in any matter when comes in thermal contact with another matter having different thermal energy causes the phenomenon of heat transfer. The driving force in order to occur heat transfer is the temperature difference. No matter how much thermal energy is present in two bodies, if there is no temperature difference, heat transfer does not occur. Heat transfer is energy in transit and it is also known as Imperial Journal of Interdisciplinary Research (IJIR) boundary phenomenon. All the heat transfer processes that occur in nature obey the law of conservation of energy which is also known as first law of thermodynamics. With the demand of the new technology, many products in the industries are focused to make compact in size, economical and energy efficient. Various electronic devices are strictly focused to make them very small so as to provide sufficient flexibility in portable and aesthetic aspects. Equal efforts are also concentrated on compact engines and many other mechanical products. These all systems dissipate heat and have to be removed efficiently for smooth operation of the system. Heat transfer enhancement (HTE) techniques were studied with the help of the V shaped ribs. They conducted experiment in order to determine heat transfer factors, pressure drop parameters and thermal performance factors with Reynolds number in the range 1000 – 30000 and took rib height to hydraulic diameter ratio to be 0.06 and angle of attack of 600 for backward and forward flows. It is also found that the thermal performance factor is decreased with increasing in Reynolds number. The fanning friction factor and pressure drop were calculated using isothermal condition. They found that the V ribs which point downstream have largest heat transfer enhancement and also friction factors. [1,2]. Experiment was repeated for ribs for enhancing convective heat transfer by increasing turbulence on heat transfer surfaces. They created the roughness by repeated ribs techniques and heat flux was taken uniform. The angle of attack was chosen to be 450 or 600 relative to flow direction [3]. Conducted experiment on natural convection heat transfer over vertical V- shaped partition plates with bottom spacing of 20 mm and without bottom spacing. They found that the vertical V shaped fins are far better for heat transfer enhancement as compared to smooth vertical Page 405 Imperial Journal of Interdisciplinary Research (IJIR) Vol-2, Issue-9, 2016 ISSN: 2454-1362, http://www.onlinejournal.in surface, as they create turbulence in the flow [4]. Entropy generation analysis for laminar flow through a circular duct with three different shaped longitudinal fins was performed. After that they concluded that increasing the Reynolds number the entropy generation decreases and pumping power of heat transfer increases [5]. For high thermal efficiency in a gas turbine, they did two- pass rotating rectangular channels with five different orientations of 450 V-shaped rib turbulators. By this rotation effects shows an increase in the Nusselt number ratio in the first pass trailing surface and second pass leading surface [6,7]. Experimental set – up was designed and fabricated for inline and staggered arrangement. A uniform heat generation and equal weight of fins are maintained for the comparison. Different types of fin configurations viz., solid, hollow, solid pin fin with a single perforation solid pin fin with four perforations and solid fin with knurling, having equal weight are considered for the study [8,9]. Experimentshows that the use of the cylindrical perforated pin fins leads to heat transfer enhancement than the solid cylindrical fins. Enhancement efficiencies mainly depend on the clearance ratio and inter-fin spacing ratio. Small clearance ratio and small inter-fin spacing ratio and comparatively with smaller Reynolds numbers are suggested for higher thermal performance [10]. From the above literature V-shaped ribs are used to enhance heat transfer rate has done. But C-shaped fins are not used; also long fins are not used. As a result of this an experiment study of inline Cshaped fins, inline V-shaped fins and staggered Cshaped fins, staggered V-shaped fins are designed to determine heat transfer characteristics. To achieve the higher transfer rate, by considering the friction factor and pressure drop. Also in order to obtain the computational results of the experiment, CFD analysis is carried out. Symbols Abbreviations Kinematic viscosity µ Dynamic viscosity K Kelvin ρ Density k Thermal conductivity h Heat transfer co-efficient Vmean Free stream velocity of air Re Reynolds number Nu Nusselt number To Average temperature Tin inlet temperature Imperial Journal of Interdisciplinary Research (IJIR) Tout outlet temperature f Fanning friction factor Aw Wetted area dh Hydraulic diameter B Breadth of duct H Height of duct L Length of duct n Number of fins ƞ Enhancement of efficiency Atotal Total Area AS Surface area of fins Tbase Base plate temperature 2.0 Experimental Set-up The heat transfer equipment includes fallowing major components in the system as shown in fig 3. 1. Tunnel 2. Heater unit 3. Base plate 4. Control Panel 2.1 Tunnel The wind tunnel consists of a heating unit at the bottom, inlet section and outlet section, had an internal cross-section of 150 mm width and 150 mm of breadth and length 600 mm. The fin model is fixed to the base plate which is placed in the wind tunnel, it is made up of mild steel sheet of small thickness of 8 mm and sides are insulated by paint and Fiberglass reinforced plastic, the inlet section is made in such a way that the blower outlet is connected to the that by the application of pipe. The air coming out from the blower is directly entered into the inlet section and passed around the fins and exited through the outlet. The outlet is also designed in such a way that there is no obstruction to the flow of air, it is providing smooth flow of air movement. 2.2 Heating unit In this equipment 250 W mica heater is used which is having a cross-section of 250 mm length and 125 mm width. The power supply to the heating unit was connected through the controlling knob. Two layers of the insulating material such as asbestos and glass wool each having 5mm thickness was used at the bottom surface to avoid temperature distribution at the bottom side and to maintain unidirectional heat transfer. At the top Page 406 Imperial Journal of Interdisciplinary Research (IJIR) Vol-2, Issue-9, 2016 ISSN: 2454-1362, http://www.onlinejournal.in surface of the heating plate, copper plate of same dimension was fixed to get efficient heat transfer to the model. 2.3 Base Plate It consists of rectangular plate at base having the dimension 250 mm x 125 mm, thickness is 6 mm. Pin fins & base plate are made of same material of Aluminium 6061. Base plate is placed on the heater setup firmly with the help of two steel bars and bolts. Base plate and fins are fixed by permanent gas welding process. are installed in the setup. Two thermocouples are installed to measure inlet and outlet temperature of air at inlet section and outlet section respectively. One thermocouple is fixed at the bottom plate to measure base plate temperature and remaining 18 thermocouples are fixed at the fin surfaces. Digital portable anemometer is used to measure the velocity of air which is coming from blower. Figure 2: Photographic View of base Plates Figure 1: 3D model of C & V shaped fins inline arrangement and staggered arrangement Inline arrangement contains nine fins each having height of 80 mm, longitudinal distance between each fins are 60 mm and transverse distance between each fins is 30 mm. Staggered arrangement contains eight fins each having height of 80 mm, longitudinal distance between each fins are 60 mm and transverse distance between each fins is 15 mm, thickness of fin is 3 mm for both arrangement as shown in fig 1 &2. For taking the temperature distribution in the fins two M5 hole was made to fix the thermocouples at a distance of 20 mm from top and bottom for each fin. Figure 3: Experimental setup 3. Mathematical Relationship Governing Equation: The convective heat transfer rate Q convection from electrically heated test surface is calculated by using equ. (2,4) Qconv.= Qelect. - Qcond.-Qrad. (1) Where: Q indicates the heat transfer rate in which subscripts conv., elect., cond. and rad. denotes convection, electrical, conduction and radiation, respectively. The electrical heat input is calculated from the electrical potential and current supplied to the surface. 2.4 Control Panel Qelect.= I It consists of mainly heat input control and various indicating devices which indicate the reading taken by the various components like Digital voltmeter, Digital ammeter, Rheostat electric heater controller, Temperature selector. The main switch is used to supply and to cut off the power source and fuse is also adopted to avoid breakdown of the system in case of power fluctuation. For measuring the temperature distribution in the model 21 K-type thermocouples Imperial Journal of Interdisciplinary Research (IJIR) V (2) Where: I is current flowing through the heater and V is voltage. The total area is equal to the sum of the projected area and surface area contribution from the pin fins. These two areas can be related to each other by [4] Page 407 Imperial Journal of Interdisciplinary Research (IJIR) Vol-2, Issue-9, 2016 ISSN: 2454-1362, http://www.onlinejournal.in ATotal= (number of fins Wetted area of plate surface area of fins) + Wetted area of plate (Aw) = [Cross sectional area of Cross sectional area of plate – (number of fins fins)] ATotal = (n As ) + Aw (3) The heat transfer from the test section by convection can be expressed as Q conv. = h W (4) Hence, the average convective heat transfer coefficient can be calculated viaequ. (5) W/m2-K h= (5) Reynolds number [1], [3] (6) Hydraulic diameter m (7) = Volume of duct- (n Volume of fins) = B H L- (n Volume of fins) (8) = Wetted surface = 2 (B + H) L + [n (2 Area of fins)] (Surface Area) – (9) The dimensionless groups are calculated as fallows [1], [3] (10) The experimental pressure drops over the test section in the finned duct will be measured under the heated flow conditions. Fanning friction factor [1] f = 17.098 Re-0.449 (11) Pa (12) Darcy-Weisbach equation ΔP = Enhancement of Efficiency The effectiveness of the heat transfer for a constant pumping powerwas useful to determine the enhancement of a heat transfer. The enhancement efficiency is the ratio of heat transfer coefficient with Fins to without Fins.[4] Imperial Journal of Interdisciplinary Research (IJIR) Ƞ = 51.09 (1+ )0.1028 ( ) 0.0812 (13) 4. Results and Discussion In the present analysis forced convection experiment was carried out for Reynolds number ranging from 10000 to 35000 i.e. under turbulent conditions. Using centrifugal blower forced air was supplied over C- shaped and V-shaped fins through the duct with different velocity such as 2m/s, 3.5m/s, and 5m/s. Constant heat rate was maintained of 69.84 W to the base plate and all heat losses was measured to obtained actual heat dissipated from fin array by convection. The temperature of base plate gradually increase with respect to time and reaches steady state such that temperature of the base plate becomes constant, and fin surface temperature was noted as average temperature and further calculations has carried out. These temperatures are used to determine all the heat transfer performance parameters for all conditions and smooth curves are drawn with respect to variations in Reynolds number. 4.1. Nusselt number The forced convection is carried by supplying constant heat input of 69.84 W and varying the velocities like 2 m/s, 3.5 m/s and 5 m/s respectively for the V-shaped fins and C-shaped fins for inline and staggered arrangement. Fig.4 shows the comparative relation between Reynolds number and Nusselt number for V-shaped fins and C-shaped fins using inline and staggered arrangement. The Nusselt number for C-shaped fins and V-shaped fins, for inline arrangement were lies in the range of 159 to 291 and 128 to 260 respectively. For staggered arrangement Nusselt number were lies in the range of 195 to 308 and 161 to 281 respectively. The dimensionless Nusselt number was dependent on the thermal properties of air flowing over it and Reynolds number. When the Reynolds number increases the dimensionless Nusselt number increases, this is due to the developed turbulent flow of air through the fins. From the above fig. 4 the Nusselt number increases for fin with C-shaped for staggered compared to inline Vshaped fins, inline C-shaped fins, staggered Vshaped fins with increase in Reynolds number. Because V-shaped fins, early flow separation and wide wake formation takes place at the edge of the fin body. But in C-shaped fins, the flow separation will delay as compare to V-shaped fins and narrow wake formation takes place. Page 408 Imperial Journal of Interdisciplinary Research (IJIR) Vol-2, Issue-9, 2016 ISSN: 2454-1362, http://www.onlinejournal.in Fig 4: Comparison between the V-shaped fins and C-shaped fins in inline & staggered arrangement. 4.2. Heat transfer co-efficient From the experimental data a comparative relations of heat transfer coefficient and Nusselt number for different fin shapes corresponding to different Reynolds number are shown in Fig 5 The heat transfer co-efficient will increase with increase in Reynolds number. The heat transfer can be increased by increase in the area exposed to the flowing fluid. For the heat input 69.84 W and Reynolds number in the range of 11000 to 32000, The heat transfer co-efficient (h) for C-shaped fins and V-shaped fins, for inline arrangement was lies in the range of 43 W/m2-K to 77 W/m2-K and 34 W/m2-K to 68 W/m2-K respectively. For staggered arrangement was a lie in the range of 51 W/m2-K to 80 W/m2-K and 41 W/m2-K to 71 W/m2-K respectively. From the experimental data a comparative relations of heat transfer coefficient and Nusselt number for different fin shape and arrangement corresponding to different Reynolds number are shown in Fig 5. It can observe that heat transfer co-efficient (h) with respect to Reynolds number for C-shape fins with both inline and staggered arrangement was comparatively higher than the V-shape fins with both inline and staggered arrangement. The probable reason behind that was the C-shaped fins provides greater heat transfer surface between the plate and the fluid and hence it has higher heat transfer coefficient. It also worth mentioning that as using staggered arrangement fins, weight of heat sink decreases, which place an important role for the applications in which weight was considered has an important matter. Imperial Journal of Interdisciplinary Research (IJIR) Fig 5: Variation of heat transfer co-efficient (h) Vs Reynolds number (Re) 4.3 Pressure drop calculations 4.3.1 Effects of fanning frictionfactor Fig 6: Variation of friction factor (f) Vs Reynolds number (Re) for inline arrangement Fig 7: Variation of friction factor (f) Vs Reynolds number (Re) for staggered arrangement Figure 6 & 7 shows the relationship between Reynolds number and friction factor. The graph shows as the Reynolds number is increased, the friction factor was decreased. The reason is, as the fluid flow increases, the inertia force dominates the shear force caused by the surface of the plate and leads to decrement in friction factor. As it can be seen in the graph, the friction factor is obtained (0.1072 to 0.1642) & (0.1052 to 0.16076). If the Page 409 Imperial Journal of Interdisciplinary Research (IJIR) Vol-2, Issue-9, 2016 ISSN: 2454-1362, http://www.onlinejournal.in nature of the data is to be interpreted; the friction factor for the V-shaped fins was higher than that of the corresponding C-shaped fins. The smooth section of the C-shaped fins provides less resistance to the flow and hence it leads to lower pressure drop. 4.3.3 Enhancement of Efficiency 4.3.2 Effects of pressure drop Fig. 10 Effect of Reynolds number on enhancement of efficiency Fig 8: Variation of Pressure drop (ΔP) Vs Reynolds number for inline arrangement Fig.10 shows the comparative results of Vshaped fins and C-shape fins for inline & staggered arrangement. The effectiveness of V-shaped fins and C-shape fins in inline & staggered arrangement was 1.37 to 1.93, 1.37 to 1.94, 1.35 to 1.89, and 1.39 to 1.98 for the range of Reynolds number 11000 to 32000 respectively. The results show that the effectiveness of C-shaped fins with staggered arrangement higher when compared to other fin shapes and arrangement. Since C-shaped fins with staggered arrangement has more heat transfer area and lowerobstruction compare to other fins. Because C-shaped staggered fins has more area exposed to the heat transfer and it will dissipate more amount of heat to the surrounding compare to other fin patterns. 5. Conclusion Fig 9: Variation of Pressure drop (ΔP) Vs Reynolds number for inline arrangement Figure 8 & 9 illuminates the relationship between Reynolds number and pressure drop for heat input 69.84 W. The graph shows as the Reynolds number is increased, the pressure drop is increased. For inline arrangement, C-shaped fins pressure drop is 11.18 to 45.93 Pa but V-shaped fins lies 23.50 to 97.64 Pa. For staggered arrangement, C-shaped fins pressure drop lays in 10.66 to 44.15 Pa but V-shaped fins lie 22.47 to 92.78 Pa. Almost 50% of pressure drop is decreases for C-shaped fins with respect to Vshaped fins. From the nature of graph it can be observed that pressure drop for C-shaped fins provides less resistance to the flow compare to Vshaped fins in both inline and staggered arrangement. Imperial Journal of Interdisciplinary Research (IJIR) The experimental research was conducted in order to investigate on the heat transfer performance of C-shaped and V-shaped fins. The inline and the staggered arrangement of the fins were studied. The thermal performance and effectiveness are compared with varying Reynolds number and for constant heat input of 69.84 W for forced convection. The pressure drop across the fins was determined. Some of the conclusions was derived from experimental research are discussed below. In the wider picture, heat transfer and pressure drop performance for C-shaped fins was better than V-shaped fins. The C-shaped fins with staggered arrangement performed better than corresponding V-shaped fins. The Nusselt number for C-shaped staggered arranged fins for Q = 69.84 W was obtained to be in the range, 195 to 308 and is higher than the corresponding V-shaped fins which is in the range 161 to 281 for Reynolds number 11000 to Page 410 Imperial Journal of Interdisciplinary Research (IJIR) Vol-2, Issue-9, 2016 ISSN: 2454-1362, http://www.onlinejournal.in 32000. The higher Nusselt number for C-shaped fins showed better heat transfer performance. The convective heat transfer coefficient (h) for C-shaped staggered arranged fins showed attractive results in the range of 51 to 80W/m2-K than corresponding V- shaped fins with h in the range of 41 to 71 W/m2-K for given range of Reynolds number. The results showed less friction factor for Cshaped fins than V-shaped fins. The smooth surface of C-shaped fins gave better results. The friction factor for C-shaped fins was obtained in the range 0.1073 – 0.1642 which was lesser than corresponding V-shaped fins with values in the range 0.13452 – 0.2075. The pressure drop for C-shaped fins was lesser compared to V-shaped. This suggests, the blower with lower capacity can be used if C shaped fins are used as compared to V-shaped ones. So Cshaped fins are energy efficient than corresponding V-shaped fins. It also importance to mention that as change in arrangement from inline to stagger the weight of heat sink decreases, which place an important role for the applications in which weight, was considered as an essential matter. [2] [3] [4] [5] [6] 6. Acknowledgement I wish to express my sincere and heart full thanks to our guide Mr. Krishnamurthy K N, Assistant Professor, Department of Thermal Power Engineering, Centre for Post-Graduate studies VTU, Mysuru for his valuable guidance, patience, inspiration and continuous supervision during the entire course of this project work and successful completion of the same on time. [7] [8] [9] 7. References [1] Elshafei, “Natural convection heat transfer from a heat sink with hollow/perforated circular pin fins”. Elsevier Ltd., Energy 35(2010), pp. 28702877. Siddiqui. M. Abdullah and Dr. A. T. Autee, “Experimental Analysis of Heat Transfer from Square Perforated Fins in Staggered Arrangement”. International Journal of Engineering Research and Applications, Vol. 5(2015), ISSN: 2248-9622, pp.16-23 Amol B. Dhumne and Hemant S. Farkade, “Heat Transfer Analysis ofCylindrical Perforated Fins in Staggered Arrangement”. International Journal of Innovative Technology and Exploring Engineering (2013), Volume-2, ISSN: 2278-3075, pp.225-230. SiddiquiMohd Abdullah, and Prof. A.V.Gadeka, “A Review on Augmentation of Heat Transfer from Square Perforated fins in Staggered Arrangement”. International Journal of Innovative Science, Engineering & Technology (2015), Vol. 2 Issue 3, pp.863-867. M.J. Sable, oS.J. Jagtap , P.S. Patil, S.B. Barve, Enhancement of Natural convectionoheat transfer on vertical heatedoplate by multiple V-fin array, IJRRAS(2) November 2010. Dr. S B Prakash and Teja V, “Convective Heat Transfer Comparison between Solid and Perforated Pin Fins”. International Journal of Advanced Engineering Research and Science (IJAERS), Vol-2, Issue-12(2015), ISSN: 23496495, pp. 41-43. G. Ganesh kumar, “conjugate mixed convection through perforated extended surfaces”. International journal of engineering sciences & research technology (2015), issn: 2277-9655, pp. 306-311. GiovannioTanda, Heatotransfer in rectangular channels with transverse and V-shaped broken ribs, Jounaloof Heat and Mass transfer 47 (2004) 229-243. M.Bahrami, forced convection heatotransfer ENSC(F09) Page number 1-12. S.W.Chang, T-M. Liou, K.F. Chiang, Heatotransfer and pressureodrop in rectangularochannel with compoundoroughness of V-shaped ribs and depend scales, Journaloof heat andomass transfer 51 (2008) 457-468.E.A.M. Imperial Journal of Interdisciplinary Research (IJIR) Page 411