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International Journal of Modern Engineering Research (IJMER)
www.ijmer.com Vol. 3, Issue. 3, May.-June. 2013 pp-1467-1469 ISSN: 2249-6645
www.ijmer.com 1467 | Page
Mahendra Agrawal, ¹ Gaurav Saxena²
1
Department of mechanical engineering, Assistant professor, SRCEM banmore, RGPV University, India
2
Department of mechanical engineering SRCEM banmore, RGPV University, India
Abstract: The purpose of this paper is to analysis the basic aerodynamic theory of wings and the provide an introduction to
wind tunnel testing. This is followed by the result from the wind tunnel testing of a NACA4412 and the analysis of the data.
Lift increase at the angle of attack increase at certain point and at this point it become maximum. After that if the
angle of attack is increased by further, drag become the dominant factor and the wind enters the stall mode.
Keywords: Air Foil, Angle of attack, Drag Force, Lift Force
I. INTRODUCTION
The purpose of this report is to present an Introduction to structure and theory of wings. Also, it includes some
background information on wind tunnels and wind tunnel testing. Lastly, this report describes the procedure for testing the
NACA 4412 airfoil and presents a number of graphs and tables evaluating the data obtained through these tests. The
objective is to find the angle of attack at which the lift is maximized in order to get the best performance of this wing when
in flight.
This report is based on the research on basic aerodynamics of wings and fundamentals of wind tunnel testing. In
addition, it will present the results from testing the NACA 4412. This data is then presented through tables and graphs using
Microsoft Excel.
II. AIM OF EXPERIMENT
The present research describes the application of different turbulence models for flow around NACA 4412 aerofoil
at angle of attack 15 degree, 20 degree, 22.5 degree. It is designed to investigate the change in the structure of the flow as a
function of using different turbulence models, to investigate the performance of these turbulence models and to compare
them with the available accurate experimental data. An improved understanding of the physical characteristics of separation
on the aerofoil sections and in the region of the trailing edge is of direct value for the improvement of high life wings for
aircraft. The configuration were planned with the knowledge that a small intermittent separated region will be formed at
angle of attack a = 15º, that corresponds to the position of maximum lift of a NACA 4412 aerofoil section
III. WIND TUNNEL TESTING OF THE AIRFOIL
Wind tunnel testing is a crucial step in the design of an aircraft. It can give quite accurate information on the
performance of an aircraft or a section of an aircraft by taking data on a scale model. This can save enormous amounts of
money by testing models instead of prototypes. It is also much safer to test in a wind tunnel than out in the open. The
following section covers the theory of the wind tunnels and procedures for testing the NACA 4412 airfoil.
IV. THEORY OF WIND TUNNELS
All wind tunnels can be divided into one of two types: open circuit (also called “straight through”) or closed circuit
(also called “return flow”) 6. Open circuit wind tunnels pull the air from the environment into the tunnel and release the air
back into the environment, whereas the closed circuit continually circulates the same air throughout the tunnel. The wind
tunnel we used is a single return flow wind tunnel, shown in Figure.
Figure: The wind tunnel we used to test our airfoil.
Analysis of wings using Airfoil NACA 4412 at different
angle of attack
International Journal of Modern Engineering Research (IJMER)
www.ijmer.com Vol. 3, Issue. 3, May.-June. 2013 pp-1467-1469 ISSN: 2249-6645
www.ijmer.com 1468 | Page
Closed circuit wind tunnels are advantageous over open circuit wind tunnels for the following reasons: the quality
of the flow can be easily controlled with screens and corner turning vanes; less energy is required to create an airflow of a
given size and velocity; the wind tunnel runs more quietly. The disadvantages are the initial expense of building and need to
change the air if it is significantly heated or polluted with smoke from smoke testing or engines7. Fortunately, neither of the
disadvantages affected us.
V. TURBULENCE MODELS
The inlet boundary velocity Uwas set to 18.4 m/sec for all turbulence models for direct comparison with the
flying hot-wires measurements. The corresponding Reynolds number is 0.36 x 106 based on the chord c of the airfoil (250
mm). A computational grid of 150 ×150 was fixed for all models. Three different turbulence models were used, two equation
models such as Realizable and RNG k-Reynolds and Reynolds Stress Model (RSM). These models selected because they are
most widely used in aerodynamic industry, and they have well documented strength. Also these models proved to have a
superior performance for flows involving strong streamline curvature. All computations have been performed on the same
grid to ensure that the presented solution for each model will be compared with each other. Flow conditions around the
airfoil were built up by finite element analysis using FLUENT 5 software by Fluent Inc.
VI. FIGURES AND TABLES
Figure 1 Pressure coefficient (for angle of attack 15)
Figure 2 Friction coefficient (for angle of attack 15)
International Journal of Modern Engineering Research (IJMER)
www.ijmer.com Vol. 3, Issue. 3, May.-June. 2013 pp-1467-1469 ISSN: 2249-6645
www.ijmer.com 1469 | Page
VII. CONCLUSION
One of the most important aspects of a turbulence model for aerodynamic applications is its ability to accurately
predict adverse pressure gradient boundary-layer flows. It is especially important that a model be able to predict the location
of flow separation and the wake behavior associated with it.
This study found that the turbulence models had captured the physics of unsteady separated flow. The resulting
surface pressure coefficients, skin friction, velocity vectors, and Reynolds stresses are compared with flying hot wire
experimental data, and the models produce very similar results. Also excellent agreements between computational and
experimental surface pressures and skin friction were observed.
REFERENCES
[1] Badran O.O. 1993. A flying hot-wire study of separated flows. Ph.D thesis. University of Bradford, UK.
[2] Rumsey, C. L., Gatski, T. B. 2001. Recent turbulence model advances applied to multielement airfoil computations. Journal of
aircraft, vol. 38, no. 5.
[3] O.O.Badran. O.O. and Bruun, H.H. 2003. Turbulent flow over a NACA 4412 airfoil at angle of attack 15 degree. Proceedings of
FEDSM’03, 4th ASME_JSME Joint Fluids Engineering Conference, Honolulu, Hawaii, USA, July 6-11, 2003.
[4] Adair D.1987. Characteristics of a trailing flap flow with small separation. Experiments in Fluids 5, 114-128.
[5] Adair D. and Horne W.C. 1989. Turbulent separated flow over and downstream of a two-element airfoil. Experiments in Fluids 7,
531-541.
[6] Al-Kayiem H.H and Bruun H.H. 1991. Evaluation of a flying x hot-wire probe system. Meas. Sci. Technol. 2, 374-380.
[7] Coles D. and Wadcock A. (1979). Flying-hot-wire study of flow past an NACA 4412 airfoil at maximum lift. AIAA 17:4, 321-329.
[8] Nakayama A. 1985. Characteristics of the flow around conventional and supercritical airfoils. J. Fluid Mech 160, 155-179.
[9] Seetharam H.C. and Wentz W.H. 1977. Experimental investigation of subsonic turbulent separated boundary layers on an airfoil. J.
Aircraft 14:1, 51-55.
[10] Simpson R.L, Chew Y.T. and Shivaprasad B.G. (1981). The structure of a separating turbulent boundary layer. Part 1: Mean flow
and Reynolds stresses. J. Fluid Mech 113, 23-53.
[11] Thompson B.E and Whitelaw J.H. (1984). Flying hot-wire anemometry. Experiments in fluids 2, 47-55.
[12] Wadcock A.J. (1978). Flying hot-wire study of two-dimensional turbulent separation on an NACA 4412 airfoil at maximum lift.
Ph.D. Thesis, C.I.T, USA.
[13] Maddah, S. R. Gough, T. Pierscionek, B. Bruun, H.H.. 2002. Investigation of slat heel effect on the flow field over multi-element
aerofoils. Experimental Thermal and Fluid Science, Volume 25, Issue 8, February 2002, Pages 651-658
[14] Burns, T.F., and Mueller, T.J. (1982). "Experimental Studies of the Eppler 61 airfoil at low Reynolds numbers". AIAA 20th
Aerospace Science Meeting, Orland, Florida.
[15] Hastings, R. C., and William, B.R. (1984). "Studies of the flow field near an NACA 4412 aerofoil at nearly maximum lift. Royal
Aircraft Establishment, Hants., Tech. Memo, AERO 2026, pp.1-11.

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Analysis of wings using Airfoil NACA 4412 at different angle of attack

  • 1. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol. 3, Issue. 3, May.-June. 2013 pp-1467-1469 ISSN: 2249-6645 www.ijmer.com 1467 | Page Mahendra Agrawal, ¹ Gaurav Saxena² 1 Department of mechanical engineering, Assistant professor, SRCEM banmore, RGPV University, India 2 Department of mechanical engineering SRCEM banmore, RGPV University, India Abstract: The purpose of this paper is to analysis the basic aerodynamic theory of wings and the provide an introduction to wind tunnel testing. This is followed by the result from the wind tunnel testing of a NACA4412 and the analysis of the data. Lift increase at the angle of attack increase at certain point and at this point it become maximum. After that if the angle of attack is increased by further, drag become the dominant factor and the wind enters the stall mode. Keywords: Air Foil, Angle of attack, Drag Force, Lift Force I. INTRODUCTION The purpose of this report is to present an Introduction to structure and theory of wings. Also, it includes some background information on wind tunnels and wind tunnel testing. Lastly, this report describes the procedure for testing the NACA 4412 airfoil and presents a number of graphs and tables evaluating the data obtained through these tests. The objective is to find the angle of attack at which the lift is maximized in order to get the best performance of this wing when in flight. This report is based on the research on basic aerodynamics of wings and fundamentals of wind tunnel testing. In addition, it will present the results from testing the NACA 4412. This data is then presented through tables and graphs using Microsoft Excel. II. AIM OF EXPERIMENT The present research describes the application of different turbulence models for flow around NACA 4412 aerofoil at angle of attack 15 degree, 20 degree, 22.5 degree. It is designed to investigate the change in the structure of the flow as a function of using different turbulence models, to investigate the performance of these turbulence models and to compare them with the available accurate experimental data. An improved understanding of the physical characteristics of separation on the aerofoil sections and in the region of the trailing edge is of direct value for the improvement of high life wings for aircraft. The configuration were planned with the knowledge that a small intermittent separated region will be formed at angle of attack a = 15º, that corresponds to the position of maximum lift of a NACA 4412 aerofoil section III. WIND TUNNEL TESTING OF THE AIRFOIL Wind tunnel testing is a crucial step in the design of an aircraft. It can give quite accurate information on the performance of an aircraft or a section of an aircraft by taking data on a scale model. This can save enormous amounts of money by testing models instead of prototypes. It is also much safer to test in a wind tunnel than out in the open. The following section covers the theory of the wind tunnels and procedures for testing the NACA 4412 airfoil. IV. THEORY OF WIND TUNNELS All wind tunnels can be divided into one of two types: open circuit (also called “straight through”) or closed circuit (also called “return flow”) 6. Open circuit wind tunnels pull the air from the environment into the tunnel and release the air back into the environment, whereas the closed circuit continually circulates the same air throughout the tunnel. The wind tunnel we used is a single return flow wind tunnel, shown in Figure. Figure: The wind tunnel we used to test our airfoil. Analysis of wings using Airfoil NACA 4412 at different angle of attack
  • 2. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol. 3, Issue. 3, May.-June. 2013 pp-1467-1469 ISSN: 2249-6645 www.ijmer.com 1468 | Page Closed circuit wind tunnels are advantageous over open circuit wind tunnels for the following reasons: the quality of the flow can be easily controlled with screens and corner turning vanes; less energy is required to create an airflow of a given size and velocity; the wind tunnel runs more quietly. The disadvantages are the initial expense of building and need to change the air if it is significantly heated or polluted with smoke from smoke testing or engines7. Fortunately, neither of the disadvantages affected us. V. TURBULENCE MODELS The inlet boundary velocity Uwas set to 18.4 m/sec for all turbulence models for direct comparison with the flying hot-wires measurements. The corresponding Reynolds number is 0.36 x 106 based on the chord c of the airfoil (250 mm). A computational grid of 150 ×150 was fixed for all models. Three different turbulence models were used, two equation models such as Realizable and RNG k-Reynolds and Reynolds Stress Model (RSM). These models selected because they are most widely used in aerodynamic industry, and they have well documented strength. Also these models proved to have a superior performance for flows involving strong streamline curvature. All computations have been performed on the same grid to ensure that the presented solution for each model will be compared with each other. Flow conditions around the airfoil were built up by finite element analysis using FLUENT 5 software by Fluent Inc. VI. FIGURES AND TABLES Figure 1 Pressure coefficient (for angle of attack 15) Figure 2 Friction coefficient (for angle of attack 15)
  • 3. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol. 3, Issue. 3, May.-June. 2013 pp-1467-1469 ISSN: 2249-6645 www.ijmer.com 1469 | Page VII. CONCLUSION One of the most important aspects of a turbulence model for aerodynamic applications is its ability to accurately predict adverse pressure gradient boundary-layer flows. It is especially important that a model be able to predict the location of flow separation and the wake behavior associated with it. This study found that the turbulence models had captured the physics of unsteady separated flow. The resulting surface pressure coefficients, skin friction, velocity vectors, and Reynolds stresses are compared with flying hot wire experimental data, and the models produce very similar results. Also excellent agreements between computational and experimental surface pressures and skin friction were observed. REFERENCES [1] Badran O.O. 1993. A flying hot-wire study of separated flows. Ph.D thesis. University of Bradford, UK. [2] Rumsey, C. L., Gatski, T. B. 2001. Recent turbulence model advances applied to multielement airfoil computations. Journal of aircraft, vol. 38, no. 5. [3] O.O.Badran. O.O. and Bruun, H.H. 2003. Turbulent flow over a NACA 4412 airfoil at angle of attack 15 degree. Proceedings of FEDSM’03, 4th ASME_JSME Joint Fluids Engineering Conference, Honolulu, Hawaii, USA, July 6-11, 2003. [4] Adair D.1987. Characteristics of a trailing flap flow with small separation. Experiments in Fluids 5, 114-128. [5] Adair D. and Horne W.C. 1989. Turbulent separated flow over and downstream of a two-element airfoil. Experiments in Fluids 7, 531-541. [6] Al-Kayiem H.H and Bruun H.H. 1991. Evaluation of a flying x hot-wire probe system. Meas. Sci. Technol. 2, 374-380. [7] Coles D. and Wadcock A. (1979). Flying-hot-wire study of flow past an NACA 4412 airfoil at maximum lift. AIAA 17:4, 321-329. [8] Nakayama A. 1985. Characteristics of the flow around conventional and supercritical airfoils. J. Fluid Mech 160, 155-179. [9] Seetharam H.C. and Wentz W.H. 1977. Experimental investigation of subsonic turbulent separated boundary layers on an airfoil. J. Aircraft 14:1, 51-55. [10] Simpson R.L, Chew Y.T. and Shivaprasad B.G. (1981). The structure of a separating turbulent boundary layer. Part 1: Mean flow and Reynolds stresses. J. Fluid Mech 113, 23-53. [11] Thompson B.E and Whitelaw J.H. (1984). Flying hot-wire anemometry. Experiments in fluids 2, 47-55. [12] Wadcock A.J. (1978). Flying hot-wire study of two-dimensional turbulent separation on an NACA 4412 airfoil at maximum lift. Ph.D. Thesis, C.I.T, USA. [13] Maddah, S. R. Gough, T. Pierscionek, B. Bruun, H.H.. 2002. Investigation of slat heel effect on the flow field over multi-element aerofoils. Experimental Thermal and Fluid Science, Volume 25, Issue 8, February 2002, Pages 651-658 [14] Burns, T.F., and Mueller, T.J. (1982). "Experimental Studies of the Eppler 61 airfoil at low Reynolds numbers". AIAA 20th Aerospace Science Meeting, Orland, Florida. [15] Hastings, R. C., and William, B.R. (1984). "Studies of the flow field near an NACA 4412 aerofoil at nearly maximum lift. Royal Aircraft Establishment, Hants., Tech. Memo, AERO 2026, pp.1-11.