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CFD study on NACA 4415 airfoil implementing spherical and sinusoidal Tubercle Leading Edge

  • S. M. A. Aftab ,

    Contributed equally to this work with: S. M. A. Aftab, K. A. Ahmad

    Roles Conceptualization, Investigation, Methodology, Writing – original draft, Writing – review & editing

    Affiliation Dept of Aerospace Engineering, Universiti Putra Malaysia, Selangor, 43400, Malaysia

  • K. A. Ahmad

    Contributed equally to this work with: S. M. A. Aftab, K. A. Ahmad

    Roles Conceptualization, Investigation, Methodology, Writing – original draft

    aekamarul@upm.edu.my

    Affiliations Dept of Aerospace Engineering, Universiti Putra Malaysia, Selangor, 43400, Malaysia, Mechanical Engineering Department, College of Engineering, King Saud University, P.O. Box 800, Riyadh 11421, Saudi Arabia

CFD study on NACA 4415 airfoil implementing spherical and sinusoidal Tubercle Leading Edge

  • S. M. A. Aftab, 
  • K. A. Ahmad
PLOS
x

Correction

21 Nov 2017: Aftab SMA, Ahmad KA (2017) Correction: CFD study on NACA 4415 airfoil implementing spherical and sinusoidal Tubercle Leading Edge. PLOS ONE 12(11): e0188792. https://doi.org/10.1371/journal.pone.0188792 View correction

Abstract

The Humpback whale tubercles have been studied for more than a decade. Tubercle Leading Edge (TLE) effectively reduces the separation bubble size and helps in delaying stall. They are very effective in case of low Reynolds number flows. The current Computational Fluid Dynamics (CFD) study is on NACA 4415 airfoil, at a Reynolds number 120,000. Two TLE shapes are tested on NACA 4415 airfoil. The tubercle designs implemented on the airfoil are sinusoidal and spherical. A parametric study is also carried out considering three amplitudes (0.025c, 0.05c and 0.075c), the wavelength (0.25c) is fixed. Structured mesh is utilized to generate grid and Transition SST turbulence model is used to capture the flow physics. Results clearly show spherical tubercles outperform sinusoidal tubercles. Furthermore experimental study considering spherical TLE is carried out at Reynolds number 200,000. The experimental results show that spherical TLE improve performance compared to clean airfoil.

1. Introduction

Biomimetics is the art of studying and applying nature inspired designs in the field of engineering. Research utilizing Humpback whale tubercles has gained popularity over the past decade. Implementing tubercle design has shown to improve airfoil performance, dratstically reduce aeroacoustic noise and seperation bubble [16]. A detailed review on application of Humpback whale flipper design on various airfoils has been conducted by Aftab et al., [7]. Few of the previous parametric studies conducted considering TLE are reported below Aftab et al., [7].

  1. Study considering the variation of amplitude and wavelength Johari et al., [1], Zhang et al., [2, 8, 9], Lohry et al., [10] and Koun et al., [11].
  2. Custodio et al., [3] studied four planform geometries: rectangular finite span, infinite span, swept and idealized flipper model.
  3. Yoon et al., [12] studied the effect of waviness along the span, for 5 different waviness ratios (0.2, 0.4, 0.6, 0.8 and 1.0), in comparison with base line airfoil. Kim et al., [13] extended the previous study of Yoon et al., [12], studying the effect of 5 wavelengths (,,, and , S is span 1.5c) for fixed amplitude (0.5c).
  4. Goruney and Rockwell [14], studied the effect of TLE on a swept delta wing. Chen et al., [15] investigated the effect of the tubercles on the performance of a moderately swept delta wing. Chen et al., [16] further investigated the effect of tubercles on a highly swept delta wing.
    The above mentioned researchers as well as few others, such as Custodio et al., [3], Rostamzadeh et al., [4], Miklosovic et al., [5], Borg [6], Corsini et al, [17], Zhang et al., [8, 18] and Skillen et al., [19], have worked considering only the sinusoidal tubercles designs. Only one author Gawad [20, 21] has proposed spherical TLE design. Gawad [20, 21] conducted CFD study on NACA 0012 implementing spherical TLE and reported that, it performed better compared to the sinusoidal TLE.
    Aftab et al., [22] also carried out a numerical study for low Reynolds number flow. Five turbulence models were tested in the study, out of all RANS turbulence models tested, only transition SST turbulence model is suitable to capture the transition effects. The work on transition SST turbulence model reported by Langtry and Menter [23] and Menter et al., [24] is quite accurate to capture the separation bubble and other related phenomenon for low Reynolds number flows.
    The current study is on NACA 4415 airfoil profile with sinusoidal and spherical TLE. A parametric study is carried out between the two designs by varying the tubercle amplitude, inorder to determine which design is more suitable for NACA 4415 airfoil. This study is unique as an in-depth study comparing, tubercle design has not been reported in literature. Experimental testing in wind tunnel is also carried out, based on the best tubercle design.

2. Geometrical design

This section deals with the creation of the geomerty using CATIA V5R21.

2.1 Clean airfoil

The NACA 4415 profile of unit chord (c) is created using CATIA V5R21, as shown in Fig 1.

2.2 Sinusoidal tubercles

The sinusoidal tubercles have been modeled using the methodology suggested by Swanson et al., [25]. Three amplitudes are modeled 0.025c, 0.05c and 0.75c and the wavelength is kept constant at 0.25c as shown in Fig 2. The airfoil coordinates are modified at the leading edge in x direction without altering the y coordinates as shown in Eq (1) and (2). The subscript old indicates the clean wing and subscripts tm refers to the location of max thickness. The Amplitude A is used to modify the leading edge by a fraction of chord length. Profiles are generated using excel and later using macros these profiles are imported into CATIA V5R21 to generate the wing surface.

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Fig 2. Sinusoidal tubercles with different amplitudes and constant wavelength.

https://doi.org/10.1371/journal.pone.0183456.g002

2.3 Spherical tubercles

Gawad [[20, 21]] has proposed spherical design of tubercles, and also reported that the new spherical TLE design, improves the performance compared to sinusoidal TLE design. The spherical tubercles have been generated varying the radius of sphere as shown in Fig 3. Study by Aftab and Kamarul [26] noticed improvement in NACA 4415 airfoil performance implementing spherical TLE.

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Fig 3. Spherical tubercles with different amplitudes and constant wavelength.

https://doi.org/10.1371/journal.pone.0183456.g003

The major draw back noticed in the studies of Gawad [20, 21] and Aftab and Kamarul [26] was, they were based on unstructured meshing and unsuitable turbulence model. Gawad [20, 21] considered kω and Aftab and Kamarul [26] considered the one equation Spalart Allmaras turbulence model. The importance of selecting a proper turbulence model for low Reynolds number flows, has been discussed in detail by Aftab et al., [22].

2.4 Domain details

A rectangular domain is created around the wing with a width equal to span of the airfoil. The inlet and outlet are kept at a distance of −1.3c and 10.3c from the airfoil leading edge. The domain is extended 2c above and below the airfoil to avoid confinement effects. The domain is similar to one used by Corsini et al., [17]. Hex mesh is generated around the airfoil. Two zones are created for meshing, the inner zone close to the airfoil is used to obtain fine grid as shown in Fig 4. The wall y+ is calculated and the estimated distance is fixed 7.9 × 10−5m. The domain size is maintained for clean and TLE (sinusoidal and spherical) airfoils. The mesh for clean airfoil is as shown in Fig 5. The Figs 6 and 7 show the mesh on sinusoidal and spherical tubercle airfoils. The mesh density is varied making it coarse as it goes outward away from the surface of interest.

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Fig 5. O-grid structured mesh around clean airfoil with structured mesh.

https://doi.org/10.1371/journal.pone.0183456.g005

The growth ratio around the airfoils Figs 5, 6 and 7 is maintained at 1.05 in outward direction in order to capture the Boundary Layer (BL) effects. The wall y+ <1 is also maintained which is the main requirement for capturing the transition effects.

3. Numerical method

This section will cover the computational aspects as well as the previous validation study.

3.1 Computational aspects

Commercial simulation software ANSYS was used to carry out Steady state analysis considering, transition SST turbulence model. It has been well proven and designed for low Reynolds number aerodynamic applications. Transition SST uses four transport equations to model the transition behavior which has been clearly explained in previous work of Aftab et al., [22]. The model is more accurate and the computation time required is less. SIMPLE pressure velocity coupling is implemented and the simulation is carried out for 2nd order of accuracy and convergence criterion is set to 10−6.

Simulation is carried out from 0° till 18° Angle of Attack (AoA). The input parameters such as pressure, density and viscosity are considered at sea level conditions. The inlet velocity is kept at 1.76 ms−1 for a chord based of Reynolds number of 1.2 × 105. Mesh dependence study is carried out by varying mesh sizes, results showed that 0.55 million, 1.93 million and 2.5 million, mesh size is optimum for clean, sinusoidal and spherical airfoil respectively. The methodology followed for the current mesh dependency test, is similar to the study previously reported by Aftab et al., [22]. Thus above mentioned mesh sizes are utilized for the parametric study. The results obtained are described in detail in section 4.

3.2 Previous validation study

Aftab et al., [22] conducted an in depth CFD validation analysis considering NACA 4415 with experimental data of Karthikayen et al., [27]. The Cp plot Fig 8 shows the accuracy of Transition SST Turbulence model in capturing the separation bubble at 6° and complete separation at 18°. The values of the experimental study and the CFD study of Aftab et al., [22] were found to be in good agreement.

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Fig 8. Cp expt and γ-Reθ SST a) 6 degree AOA b) 18 degree AOA Aftab et al., [22].

https://doi.org/10.1371/journal.pone.0183456.g008

4 Results and discussion

This section discusses the results of the current study. Table 1, summarizes the basic details such as TLE amplitude and Reynolds number used in the current CFD study.

4.1 Sinusoidal TLE

Peformance comparision of sinusoidal TLE design with clean airfoil is discussed in this subsection. The parametric study is carried out considering sinusoidal TLE designs with three amplitudes (0.025c, 0.05c and 0.075c). The Cl vs AoA and Cd vs AoA results are as shown in Figs 9 and 10. In case of sinusoidal TLE the airfoil with tubercle amplitude 0.025c, performed better than other two sinusoidal TLE design.

Table 2 provides an in depth comparison of clean airfoil and sinusoidal TLE of amplitude 0.025c.

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Table 2. Cl, Cd and L/D for clean airfoil and sinusoidal TLE airfoil with 0.025c and 0.25c.

https://doi.org/10.1371/journal.pone.0183456.t002

The comparison of Cl, Cd and L/D vs AoA for clean and the best performing sinusoidal TLE, is as shown in Table.2. The results clearly indicate that at 0, 6, 12 and 18 degree AoA, the clean airfoil constantly generates more lift and less drag than the sinusoidal TLE. The L/D ratios show that at 6° and 18° the values for both clean and sinusoidal TLE are quite close, but still the clean airfoil outperforms the sinusoidal TLE.

4.2 Spherical TLE

The parametric study varying the amplitude (0.025c, 0.05c and 0.075) is carried out considering spherical TLE. The Cl vs AoA and Cd vs AoA results are as shown in Figs 9 and 10. Results show that out of the three amplitudes considered, the spherical tubercle with 0.025c performed better than other two spherical TLE design.

Table 3, shows the comparison of Cl, Cd and L/D vs AoA, for clean and the best performing spherical TLE. The results clearly indicate that at 0 and 12 degree AoA the clean airfoil constantly generates more lift and less drag than the spherical TLE. At 0° AoA the TLE airfoil reduced lift by 4.55% and increased drag by 17%, resulting in a decrement of L/D by 18.4%. At 6° AoA the TLE shows a lift reduction by only 3.86% and drag reduction by almost 2%, thus an overall decrease in L/D of only 1.93% is noticed. At 18° AoA the spherical TLE airfoil, outperforms the clean airfoil. The spherical TLE airfoil shows an increase in lift by 5.96% and decrease in drag by 2.67%. The overall L/D ratio at 18° shows an improvement by 6.25% due to the presence of spherical TLE. Tables 2 and 3 clearly show that both the TLE designs reduce L/D significantly. But spherical TLE performs better than sinusoidal TLE.

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Table 3. Cl, Cd and L/D for clean airfoil and spherical TLE airfoil with 0.025c and 0.25c.

https://doi.org/10.1371/journal.pone.0183456.t003

5. Spherical tubercle working mechanism

Inorder to understand the behavior of flow around a spherical TLE, a close up of velocity vectors is plotted. The Figs 11 to 14 show velocity vectors downstream of TLE, at 0.35c, 0.4c, 0.5c and 0.55c from the leading edge of the airfoil. The velocity vectors behind the TLE, show that the TLE produces eddies which travel downstream along the chord. These eddies create flow instability further downstream and introduces vortices inside the boundary layer, thereby acting as Sub Boundary Layer Vortex Generators (SBVG). These vortices help in reattaching the BL, thereby increasing the aerodynamic performance. It is quite noticeable that no vortices were generated by TLE from the leading edge location. The TLE did induce eddies downstream, but a proper vortex formation is seen quite far from the TLE location. At 0.35c a vortex pattern is noticed, two vortices were generated within the boundary layer. A clock wise and counter clockwise vortex pattern is visible inside the BL Fig 11. The energy from the BL is sucked into the two vortices, this behavior shows that TLE act as SBVG. The size of the twin vortices grows bigger at 0.4c, as shown in Fig 12. At 0.5c these twin vortices start interacting with each other and behave similar to a standard Vortex Generator (VG). The height of the recirculation zone reaches the BL height Fig 13. At 0.55c Fig 14, the vortices lose their energy and completely disappears.

6. Experimental study on NACA 4415 airfoil with spherical TLE

Based on the CFD parametric study results, spherical tubercle showed improved performance compared to sinusoidal TLE. Thus spherical TLE with A 0.025c and W 0.25c is fabricated as shown in Fig 15. The airfoil along with the mounting holes is designed using CATIA V5R21. The chord length of the airfoil is 0.3m and the span is 0.98m. Tubercle airfoil is fabricated using CNC machine, soft wood which is light weight and easy to fabricate is used. Fine surface finishing is obtained initially by sanding and later by painting the top and bottom surfaces. The airfoil is mounted inside the test section as shown in Fig 15.

The experimental study on the optimum spherical TLE configuration is carried out in the wind tunnel. The low speed wind tunnel is available at Universiti Putra Malaysia (UPM). Fig 16 shows the basic schematic of the UPM-T-1000 suction type open loop wind tunnel. The honey comb inlet houses, large screens in order to reduce the turbulence of the incoming airflow. The transparent test section is 1m × 1m × 2.5m and houses a 6 axis load balance system on which the model is mounted. The load balance is connected to the data acquisition computer. The computer is installed with Data Acquisition Reduction and Control (DARCS) software, which helps in, calibration, controlling the pitching angle and load measurements on the model.

6.1 Calibration

In order to ensure the correctness of the results the calibration of the force balance is carried out. Table 4 shows the range and accuracy of the force balance.

The calibration is carried by mounting the calibration rig on to the balance as shown in the Fig 17. The weight block is initially weighed on a digital scale, upon mounting the force exerted by the weight block is noted.

6.2 Data Acquisition System (DAQ)

The Data Acquisition System (DAQ) gathers information from the six component force balance. The balance is equipped with transducers that converts the lift, drag, moment and side forces into electrical signals. These signals are very weak of the order of millivolts which need to be amplified. An Analog to Digital convertor is used to convert the voltage to a digital signal. This digital signal is analyzed using the DARCs software.

Two pitot gauges, are used to measure the speed of air inside the tunnel. One is connected to the digital manometer. The other pitot is connected to the computer. This helps in double checking the airspeed inside the wind tunnel.

The values of Cl, Cd, velocity and AoA are all recorded using the DARCs software. The raw data from the DARCs software is checked for consistency. Standard procedure is followed to calculate the mean and standard deviation, for the data obtained from the wind tunnel and graphs are plotted.

6.3 Blockage correction

Standard blockage correction analysis, recommended in Pope and Harper [29] is applied for the aerodynamic data.

The solid blockage correction for a general shape is given by

K1 = 0.74 for a horizontal modeal and 0.52 for a vertical model. S is the working section area and VB is the body volume.

The wake blockage ϵwb is given by where c is the wing chord and Cdu is the uncorrected drag coefficient.

6.4 Experimental study results and discussion

Table 5 shows the values of Cl and Cd variation from 0°AoA to 30°AoA. For each AoA three trials are carried out, and each trial consists of 15 data points, in order to determine the mean, and standard deviation.

The Fig 18 shows the variation of lift from 0° to 30°AoA. The TLE airfoil maintains lift over the airfoil without sudden drop at higher AoA. It can be noticed from the Table 5 that spherical TLE airfoil maintains stable lift even at higher AoA.

Fig 19 shows the variation of Cd vs AoA. As expected the drag increases with increase in AoA. The values increase exponentially with increasing AoA, with a max drag of 0.576387 at 30° AoA.

Fig 20 shows the plot of lift to drag ratio. The TLE airfoil produces max L/D of about 17.38 at 6° AoA.

6.5 Comparison of TLE and clean airfoil

The current spherical TLE experimental work is carried out at the same Reynolds numbers as in the study by Fouatih et al., [30]. The Fig 21 shows the comparison of Cl vs AoA for the current experimental work, with the previous work of Fouatih et al., [30] on NACA 4415. In the current experimental study, the TLE airfoil at 0° produces higher Cl, compared to clean airfoil. Further increasing the AoA, to 6°, 12° and 18° the clean airfoil Cl values are better than the TLE airfoil Fig 21 [Data is provided in S1S4 Data].

Fig 22 [Data is provided in S1S4 Data] shows the variation of Cd vs AoA. At 0° AoA the TLE airfoil Cd value is higher than the clean airfoil. The TLE airfoil outperforms the clean airfoil of Fouatih et al., [30] at other AoA. Thus these lower values of Cd are reflected in the overall performance improvement.

The performance of an airfoil is measured by its L/D, TLE airfoil clearly outperforms the clean airfoil as shown in Table 6 and Fig 23 [Data is provided in S1S4 Data]. The TLE airfoil outperforms the clean airfoil from 0° to 12°, TLE increases performance by 67.3%, 14% and 17.6%, respectively. At 12°Clmax for Fouatih et al., [30] is low compared to the current TLE airfoil. At 18° the L/D ratio reduces by 3.23% compared to clean airfoil.

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Table 6. Cl, Cd and L/D for clean airfoil and spherical TLE airfoil with A 0.025c and W 0.25c.

https://doi.org/10.1371/journal.pone.0183456.t006

6.6 Comparison of TLE and VG

In this section the result of NACA 4415 spherical TLE are compared with the results of Fouatih et al., [30] on NACA 4415 airfoil with VG. Fouatih et al., [30] studied the performance improvement by installing triangular VG. The VG’s were located at 0.3c, and the VG orientation was set at 12° AoA to the free stream. Table 7 compares the results ofthe current TLE experimental work along with the experiment of Fouatih et al., [30] on clean airfoil and airfoil with VG.

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Table 7. Cl, Cd and L/D for VG airfoil and spherical TLE airfoil with A 0.025c and W 0.25c.

https://doi.org/10.1371/journal.pone.0183456.t007

Fig 24 shows the variation Cl vs AoA. The VG airfoil produces higher lift throughout the AoA range, except at 0°. Clean airfoil too produces higher lift in comparison with TLE airfoil. The airfoil with VG configuration produces less drag till 12°. After 12° the VG airfoil produces substantially higher drag than the clean airfoil and the TLE airfoil as shown in Fig 25. Overall TLE airfoil produces, less drag comparatively.

The L/D ratio Fig 26, gives a much clearer picture. The VG airfoil performs better at low AoA below 10°. The current experimental study shows that, spherical TLE airfoil surpasses the performance of both clean airfoil and VG airfoil in between 10° to 18°.

Conclusion

Important conclusions from the current CFD study are as follows.

  1. Both in case of sinusoidal and spherical TLE, it can be observed that smaller amplitude 0.025c tubercles performed better.
  2. From the above analysis, both sinusoidal and spherical TLE, reduce L/D max significantly, but the reduction of L/D max is less in case of spherical TLE than sinusoidal TLE.
  3. The current study shows that, spherical TLE reduces the formation of separation bubble and outperforms the clean airfoil and sinusoidal airfoil at 18° AoA.

Important conclusions from the experimental study are as follows.

  1. Results show that L/D of spherical TLE airfoil outperforms the clean airfoil.
  2. Comparison of spherical TLE and VG shows that, TLE outperforms the VG airfoil and clean airfoil above 10° AoA thus improving the Clmax.
  3. In case of CFD study the Reynolds number used was 120,000 and experimental study is carried out for Reynolds number 200,000. The results for both the cases shows that spherical tubercle behavior is Reynolds number dependent.

Acknowledgments

The authors would like to acknowledge the support provided by the Ministry of Science, Technology and Innovation (MOSTI), Malaysia, for providing funds through the e-science fund, grant no 04-01-04-SF2206, for the current research. The authors are also grateful for the facilities provided by the College of Engineering Research Center at King Saud University, for this work.

References

  1. 1. Johari H., Henoch C. W., Custodio D., and Levshin A., “Effects of leading-edge protuberances on airfoil performance”, AIAA Journal, vol. 45, no. 11, pp. 2634–2642, 2007.
  2. 2. Zhang M., Wang G., and Xu J., “Experimental study of flow separation control on a low-Re airfoil using leading-edge protuberance method”, Experiments in Fluids, vol. 55, no. 4, pp. 1–13, 2014.
  3. 3. D. Custodio, C. Henoch, and H. Johari, “Aerodynamic Characteristics of Finite-Span Wings with Leading Edge Protuberances”, 50th AIAA Aerospace Sciences Meeting Including the New Horizons Forum and Aerospace Exposition, no. 0054, pp. 1–12, 2012.
  4. 4. N. Rostamzadeh, R. Kelso, B. Dally, and K. L. Hansen, “The Effect of Wavy Leading Edge Modification on NACA 0021 Airfoil characteristics”, 18th Australian Fluid Mechanics conference, 1–4, 2012.
  5. 5. Miklosovic D. S., Murray M. M., and Howle L. E., “Experimental evaluation of sinusoidal leading edges”, Journal of Aircraft, vol. 44, no. 4, pp. 1404–1408, 2007.
  6. 6. Borg J., “The effect of leading edge serrations on dynamic stall”, 2012.
  7. 7. Aftab S. M. A., Razak N. A., Rafie A. M., and Ahmad K. A., “Mimicking the humpback whale: An aerodynamic perspective”, Progress in Aerospace Sciences, vol. 84, pp. 48–69, 2016.
  8. 8. Zhang M., Wang G., and Xu J., “Aerodynamic control of low-Reynolds-number airfoil with leading-edge protuberances”, AIAA Journal, vol. 51, no. 8, pp. 1960–1971, 2013.
  9. 9. Zhang M., Wang G., and Xu J., “Effect of Humpback Whale-like Leading-Edge Protuberances on the Low Reynolds Number Airfoil Aerodynamics”, in Fluid-Structure-Sound Interactions and Control, Springer, pp. 107–113, 2014.
  10. 10. M. W. Lohry, L. Martinelli, and J. S. Kollasch, “Genetic Algorithm Optimization of Periodic Wing Protuberances for Stall Mitigation”, 31st AIAA Applied Aerodynamics Conference, AIAA, no. 2905, pp. 1–13, 2013.
  11. 11. Kouh J. S., Lin H. T., Lin T. Y., Yang C. Y., and Bryan-Steven Nelson, “Numerical study of Aerodynamic characteristic of protuberances wing in low reynolds number”, in FLUCOME 2011, pp. 1–6, 2011.
  12. 12. Yoon H., Hung P., Jung J., and Kim M., “Effect of the wavy leading edge on hydrodynamic characteristics for flow around low aspect ratio wing”, Computers & Fluids, vol. 49, no. 1, pp. 276–289, 2011.
  13. 13. Kim M. J., Yoon H. S., Jung J. H., Chun H. H., and Park D. W., “Hydrodynamic characteristics for flow around wavy wings with different wave lengths”, International Journal of Naval Architecture and Ocean Engineering, vol. 4, no. 4, pp. 447–459, 2012.
  14. 14. Goruney T. and Rockwell D., “Flow past a delta wing with a sinusoidal leading edge: near-surface topology and flow structure”, Experiments in fluids, vol. 47, no. 2, pp. 321–331, 2009.
  15. 15. Chen H., Pan C., and Wang J., “Effects of sinusoidal leading edge on delta wing performance and mechanism”, Science China Technological Sciences, vol. 56, no. 3, pp. 772–779, 2013.
  16. 16. Chen H. and Wang J.-J., “Vortex structures for flow over a delta wing with sinusoidal leading edge”, Experiments in Fluids, vol. 55, no. 6, pp. 1–9, 2014.
  17. 17. Corsini A., Delibra G., and Sheard A. G., “On the Role of Leading-Edge Bumps in the Control of Stall Onset in Axial Fan Blades”, Journal of Fluids Engineering, vol. 135, no. 8, p. 081104, 2013.
  18. 18. Zhang L. H., Li W. J., and Yin J. X., “Numerical Simulation of Bionic Wing for Drag Reduction”, Advanced Materials Research, vol. 602, pp. 1761–1764, 2013.
  19. 19. Skillen A., Revell A., Pinelli A., Piomelli U., and Favier J., “Flow over a Wing with Leading-Edge Undulations”, AIAA Journal, vol. 53, no. 2, pp. 464–472, 2014.
  20. 20. Gawad A. F. A., “Numerical Simulation Of The Effect Of Leading-Edge Tubercles On The Flow Characteristics Around An Airfoil”, in International Mechnaical Engineering Congresss & Exposition, 2012.
  21. 21. Gawad A. F. A., “Utilization of Whale-Inspired Tubercles as a Control Technique to Improve Airfoil Performance”, Transaction on Control and Mechanical Systems, vol. 2, no. 5, 2013.
  22. 22. Aftab S. M. A., Rafie A. M., Razak N. A., and Ahmad K. A., “Turbulence Model Selection for Low Reynolds Number Flows”, PloS one, vol. 11, no. 4, p. e0153755, 2016.
  23. 23. Langtry R. B. and Menter F. R., “Correlation-based transition modeling for unstructured parallelized computational fluid dynamics codes”, AIAA Journal, vol. 47, no. 12, pp. 2894–2906, 2009.
  24. 24. Menter F. R., Langtry R.B., Likki S., Suzen Y., Huang P., and Volker S., “A correlation-based transition model using local variables-Part I: model formulation”, Journal of Turbomachinery, vol. 128, no. 3, pp. 413–422, 2006.
  25. 25. T. Swanson and K. Isaac, “Biologically Inspired Wing Leading Edge for Enhanced Wind Turbine and Aircraft Performance”, 6th AIAA Theoretical Fluid Mechanics Conference,. AIAA, (3533), pp. 1–10, 2011.
  26. 26. Aftab S. M. A. and Ahmad K. A., “NACA 4415 Wing Modification Using Tubercles-A Numerical Analysis”, in Applied Mechanics and Materials, vol. 629, pp. 30–35, 2014.
  27. 27. N. Karthikeyan, S. Sudhakar and P. Suriyanarayanan, “Experimental studies on the effect of leading edge tubercles on laminar separation bubble”, in proceedings 52nd Aerospace Sciences Meeting, AIAA, 2014, no.1279, pp. 1–16.
  28. 28. Wisuda, “UPM External Balance Specification”, 2012.
  29. 29. Pope A. and Harper J. J., “Low Speed Wind Tunnel Testing”, John Wiley & Sons New York, 1966.
  30. 30. Fouatih O. M., Medale M., Imine O., and Imine B., “Design optimization of the aerodynamic passive flow control on NACA 4415 airfoil using vortex generators”, European Journal of Mechanics-B/Fluids, vol. 56, pp. 82–96, 2016.