Comparative study of Different Geometry of Ribs for roughness on absorber plate of Solar Air Heater -A Review

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Comparative study of Different Geometry of Ribs for roughness on absorber plate of Solar Air Heater -A Review Gulshan Singh Baghel 1, Dr. A R Jaurker 2 1. Student, M.E. (Heat Power engineering), Jabalpur Engineering College, Jabalpur, India 2. Professor Jabalpur Engineering College Jabalpur, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - This paper includes study of Different Design of 2. NOMENCLATURE Solar Air Heater used for application in the field of agriculture and many other drying processes. In this paper a brief overview of various technique used for artificial roughness is taken into the consideration. Turbulent flow plays very important role in the field of heat because it increase heat and to generate this turbulent flow various types of artificial roughness such as ribs, grooves, dimple, metal mesh etc. is used by many researchers in previous research. A p A o C d C p area of absorber plate, m 2 cross Section area of orifice, coefficient of discharge of orifice Specific heat of air at constant pressure, J/kg K Key Words: Solar Air Heater, Artificial roughness, Solar Energy, Turbulent flow etc. 1.INTRODUCTION Increasing demand of energy and limited resources of conventional energy is biggest threat for human being in future because our generation life style is wholly depends on machinery and electronics which are operated by power (Electricity) and in present scenario the main fuel for production of electricity is fossils fuel which is in verge of ending after 50 years from today according to some surveys. This threat can be thrashed by development in the field of solar energy because this is known to everybody solar energy is a biggest form of energy and free of cost available to us for millions of year. Solar Energy is the most abundant Energy and freely available to us. It emits Energy at a rate of 3.8x10 23 kw but approximately 1.8x10 14 kw is intercepted by earth. Heat and Light are the form of solar Energy which are directly available to us in free of cost and conversion of these form to other form of Energy is required for various applications. For conversion of Solar Energy to Thermal Energy for heating application Solar collectors are used costs very efficient and easy to manufacture. 2016, IRJET Impact Factor value: 4.45 ISO 9001:2008 Certified Journal Page 2626 D G d/l v g/e h h m m Nu Q u T f T i T o T p W/w hydraulic diameter of duct, m Relative Gap Distance relative gap width convective heat coefficient, W/m 2 K average convective heat coefficient, W/m 2 K mass flow rate, kg/s Nusselt number of roughened duct difference of manometric fluid level in U-tube manometer, m difference of water column level in micro- manometer, m useful heat gain rate, W mean temperature of air, K inlet temperature of air, K outlet temperature of air, K average plate temperature, K relative roughness width ratio ratio of orifice diameter to pipe diameter

(e/d) relative roughness height 4. ARTIFICIAL ROUGHNESS ensity of air, kg/m 3 3. CLASSIFICATION OF SOLAR AIR HEATER ON THE BASIS OF ABSORBING SURFACE 3.1 Simple flat-plate collector: This is the simplest and most commonly used type of collector. In its simplest form it is composed of one or two glazings over a flat plate backed by insulation. The path of air flow may be either above or below or the absorber plate. 3.2 Finned-plate collector: This is a modified version of the type (3.1) collector, where the heat coefficient is increased by using fins on the flat plate absorber, and in certain design the is made directionally selective. The fins are usually located in the air-flow passage. 3.3 Corrugated- plate collector: This is another variation of the simple flat-plate design, in which the absorber is corrugated either in rounded troughs or V-troughs. This increases the heat area and may make the directionally selective. 3.4 Matrix type collector: In this design an absorbing matrix is plate, cotton gauze or loosely packed porous material. This type of collector offers a high heat to volume ratio; it may also offer low friction losses depending on the design. 3.5 Overlapped transparent plate type collector: This type of collector is composed of a staggered array of transparent plates which are partially blacked. The air flow paths are between the overlapped plates. 3.6 Transpiration collector: The transpiration or porous bed design is a variation of type (3.4), in which the The thermal efficiency of Solar Air Heater is poor due to low heat coefficient between absorber plate and air flowing over absorber plate because laminar sub layer is formed over absorber plate and Laminar layer is responsible for low heat so to break this Laminar sub layer various types of roughness is created on the absorber plate such as ribs, Rib-grooved, metal mesh, Dimple etc. Following are the dimensionless geometrical parameter used to characterized roughness. 4.1 Relative Roughness Pitch (p/e):- It is the ratio of Distance Between two consecutive ribs and height of ribs. 4.2 Relative Roughness Height (e/d):- It is the ratio of rib height to equivalent diameter of the air passage. 4.3 Angle of Attack (α):- It is inclination of rib with direction of air flow in the duct. 4.4 Aspect Ratio:- It is ratio of duct width to duct height. 5. LITERATURE REVIEW 5.1 1 Investigation By Anil Kumar et al.[5] for V Shaped rib with gap roughness the effect on heat and fluid flow encompassed Reynolds no range 2000 to 20000, relative width ratio (W/w) of 6, relative gap distance G d/l v of 0.24-0.80, relative gap width (g/e) 0f 0.5-1.5, relative roughness height (e/d) of 0.043, relative roughness pitch (P/e) of 10, angle of attack (α) of 60. In mentioned condition thermo-hydraulic parameter is found to be best for the relative gap distance of 0.69 and the relative gap width of 1.0. Equation used for calculation of heat coefficient h matrix material is closely packed and the backed and the back absorber-plate is eliminated. The air flow usually enters just under the innermost cover and flows downward through the porous bed and into the ; distribution ducting. )] 0.5 2016, IRJET Impact Factor value: 4.45 ISO 9001:2008 Certified Journal Page 2627

; 5.2 T.T.Wong et al.[7] experimentally and numerically investigated the force convection and flow friction of a turbulent flow friction of a turbulent airflow in a horizontal air-cooled rectangular duct, with square sectioned cross ribs mounted on its bottom. Dimensions of the cross ribs were 6.37mmx6.37mm. Reynolds number of the fully turbulent flow was maintained constant at 12380. Heat was supplied uniformly to the airflow via bottom only. Experiment done on effects of varying the angle formed by the cross ribs between 30 to 120 on the force convection and results was forced convection can be enhanced by mounting cross-ribs on the heated of a rectangular duct and average heat coefficient would be obtained at an angle between 60 and 70 and this range is optimum corresponding to the maximum force convection from the ribbed duct to the airflow. number difference for the two rib arrangements, especially just upstream of the ribs, which are due to significant difference in global and local primary and secondary flow characteristics. 5.4 A. R. Jaurker et al.[4] experimentally investigated heat can be more improved by introducing the groove between the ribs. Experimentally investigation encompassed the Reynolds number range from 2000 to 21000; relative roughness height 0.0363; relative roughness pitch 6 and relative groove position of 0.3 to 0.7. Result showed the heat coefficient for rib-grooved arrangement is higher than that for the transverse ribs, whereas the friction factor is slightly higher for rib-grooved arrangement as compared to that of rectangular transverse ribs of similar rib height and rib spacing. 5.5 Y. M. Zhang et al.[8] studied on the effects of compound turbulators on friction factors and heat coefficients in rectangular channel with 5.3 S.Y. Won et al[6] compared spatially resolved local flow structure, spatially averaged flow structure and Nusselt number for stationary channels with aspect ratio of 4 and rib turbulators inclined at 45. Two different rib arrangements with parallel and perpendicular orientation on two opposite are investigated at Reynolds number from 480 to 18300. Comparison showed important local Nusselt two opposite ribbed-groove walls, Reynolds number ranging from 10,000 to 50,000 in channel having width to height ratio 10. They measured fully developed heat coefficient and friction factors for spacings (p/e = 8, 10, 15, 20, 25 and 30). The result showed that the heat performance of the rib-groove roughened duct is much better than the rib roughened duct. The ribgroove roughened wall enhance the heat 3.4 times and pays 6 time the penalty, whereas the rib roughened wall with similar rib height and rib spacing, enhance the heat 2.4 times and pays about the same pressure drop penalty. 5.6 Firth and Meyer[1] investigated the heat and friction factor performance based on equal pumping power, of four different type of artificially roughened common namely. 2016, IRJET Impact Factor value: 4.45 ISO 9001:2008 Certified Journal Page 2628

Square transverse ribbed. Helically ribbed. Trapezoidal ribbed. Three dimensional ribs. The ribbed geometries of above cases are studied by them and found that: The square transverse ribbed has an overall performance, which compares well with the other s considered. The helically ribbed has a thermal performance, which compares as closely with squares transverse ribbed. The performance of trapezoidal ribbed is substantially poorer then the other entire. The best overall thermal performance is given by the three dimensional ribs, which shows an improvement of over 15% compared with the trapezoidal transverse ribbed. 5.7 Han et al.[3] investigated the effect of rib shape, angle of attack and pitch to height ratio on friction factor and heat coefficient. The main conclusions of the investigation are; At a given value of relative roughness height, e/d, the friction factor approaches a constant value as the Reynolds number increases, whereas the Stanton does reattach close to the next rib. For larger rib spacing the reattachment point is reached and a boundary layer begins to grow before the succeeding rib is encountered, reducing both the average shear stress and heat. The optimum thermo-hydraulic performance occurred at an angle of attack of about 45. 5.8 Han et al.[2] investigated the effect of rib angle of attack and channel aspect ratio on the heat and friction for developing flow in short rectangular channel (L/D=10 and 15) with a pair of opposite rib roughened walls for Reynolds number range of 10000 to 60000. The important conclusions drawn from the study are; The highest heat and accompanying highest pressure drop is obtained at an angle of attack of 60 in the Square channel while the highest heat and highest pressure drop occur at the angle of attack of 90 in the rectangular channel with an aspect ratio of 4. The best heat performance in the square channel with rib angle between range from 30 to 45 is about 30% higher than with the transverse ribs for a constant pumping power. The best heat performance in the rectangular channel (with W/H= 2 and 4) with angle of attack between 30 to 45 is only about 5% higher than with the transverse ribs on a constant pumping power basis. number continues to decreases with Reynolds number. The influence of rib shape on the Stanton number disappears at higher Reynolds number when the flow is in the completely rough region. For small value of relative roughness pitch ( 5), the flow which separates after each rib does not reattach before the succeeding rib while for a 5. CONCLUSION As mentioned above by studying various research paper it is clear that heat coefficient can be increased by using different types of artificial roughness and it can be further increased by using new types of roughness like new structure, geometry for roughness and conclusion is relative roughness pitch value of about 10, the flow 2016, IRJET Impact Factor value: 4.45 ISO 9001:2008 Certified Journal Page 2629

for heat is summarized according to various researchers in following table. Author Parameter Heat Friction Remark Kumar Anil et al[5] Re 2000 to 20000 W/w 6 G d /L v 0.24 to 0.80 g/e 0.5 to 1.5 p/e 10 and angle of attack is 60 Sufficient increase in Heat 6.32 times of smooth Wong T T et al.[7] Re 12380 e/d 0.12 Ɵ 30 to 120 Sufficient increase in Heat 2 11 % Highest heat at 60 and 70 Won S Y and Ligrani P M[6] Re 480 to 18300 p/e 10 AR 4 Sufficient increase in Heat Increased Zhang Y M et al.[8] Re 10000to 50000 p/e 8,10, 15,20,25 3.4 times of smooth 3.2 times of smooth at p/e =8 Highest heat and largest p drop e/d 0.028 Jaurker A R et al.[4] Re 2000 to 21000 e/d - 0.0363 2.75 times 3.48 times of smooth 2016, IRJET Impact Factor value: 4.45 ISO 9001:2008 Certified Journal Page 2630

p/e - 6 g/p 0.30 to 0.70 Han et al.[2] Re 10000 to 60000 L/D = 10 and 15 30% Heat increased Friction increased Highest at rib angle 30 to 45 AR 4 REFERENCES [1] Firth R.J. and Meyer, L., A comparison of the heat and friction factor performance of four different types of artificially roughened, Int. J. Heat and Mass Transfer, Vol.26, pp. 175-183, 1983. [2] Han J.C., Glicksman, L.R. and Rosenow, W.M., An investigation of heat and friction for rib-roughness, Int. Journal of heat and mass, Vol. 21, pp. 1143-1156, 1978. [3] Han J.C., Zhang Y.M. and Lee C.P., Augmented heat in square channels with parallel, crossed, and V shaped angled ribs, trans. ASME Journal of Heat Transfer, Vol. 113, pp. 590-596, 1991. [4] Jaurkar A. R., Saini J. S. and Gandhi B. K., Experimentally Investigation of heat Characteristics and thermohydraulic Performance of Rib-grooved Artificially Roughened Solar air Heater Ducts. [5] Kumar Anil, Saini R.P. and Saini J.S., Experimental investigation on heat and fluid flow characteristics of air flow in a rectangular duct with Multi V shaped rib with gap roughness on the heated plate. [6] Won S.Y. and Ligrani P.M., Comparisons of flow structure and local Nusselt numbers in channels with parallel and crossedrib turbulators. [7] Wong T.T., Leung C.W., Li Z. Y., Tao W.Q., Turbulent convection of air-cooled rectangular duct with -mounted cross ribs. [8] Zhang Y.M., Gu W.Z. and Han J. C., Heat and friction in rectangular channels with ribbed-grooved walls. 2016, IRJET Impact Factor value: 4.45 ISO 9001:2008 Certified Journal Page 2631