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Proceedings ArticleDOI

Numerical Investigation of Wind Turbine Airfoils under Clean and Dusty Air Conditions

About: The article was published on 2020-06-15 and is currently open access. It has received 4 citations till now. The article focuses on the topics: Turbine & Airfoil.

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Washington University in St. Louis Washington University in St. Louis
Washington University Open Scholarship Washington University Open Scholarship
Mechanical Engineering and Materials Science
Independent Study
Mechanical Engineering & Materials Science
10-28-2019
Numerical Investigation of Wind Turbine Airfoils under Clean and Numerical Investigation of Wind Turbine Airfoils under Clean and
Dusty Air Conditions Dusty Air Conditions
Siyuan Chen
Washington University in St. Louis
Ramesh K. Agarwal
Washington University in St. Louis
Follow this and additional works at: https://openscholarship.wustl.edu/mems500
Recommended Citation Recommended Citation
Chen, Siyuan and Agarwal, Ramesh K., "Numerical Investigation of Wind Turbine Airfoils under Clean and
Dusty Air Conditions" (2019).
Mechanical Engineering and Materials Science Independent Study
. 100.
https://openscholarship.wustl.edu/mems500/100
This Final Report is brought to you for free and open access by the Mechanical Engineering & Materials Science at
Washington University Open Scholarship. It has been accepted for inclusion in Mechanical Engineering and
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1
Numerical Investigation of Wind Turbine Airfoils
under Clean and Dusty Air Conditions
Siyuan Chen
1
, Ramesh K. Agarwal
2
Washington University in St. Louis, St. Louis, MO 63130
This paper focuses on the simulation of the airflow around wind turbine airfoils
(S809 and S814) under both clean and dusty air conditions by using
Computational Fluid Dynamics (CFD). The physical geometries of the airfoils
and the meshing processes are completed in the ANSYS Mesh package ICEM.
The simulation is done by ANSYS FLUENT. For clean air condition, Spalart–
Allmaras (SA) model and realizable k-ε model are used. The results are
compared with the experimental data to test which model agrees better. For
dusty air condition, simulation of the two-phase flow is operated by realizable
k-ε model and discrete phase model (DPM) in different concentration of dust
particles (1% and 10% in volume). The results are compared with the data of
clean air to illustrate the effect of dust contamination on the lift and drag
characteristics of the airfoil.
Nomenclature
c
l
/C
L
=lift coefficient
c
d
/C
D
=drag coefficient
α=angle of attack/AOA
ρ
air
=density of air
ρ
p
=density of dust particles
μ=viscosity of air
Re=Reynolds number
Ma=Mach number
d
p
=diameter of dust particles
m󰇗
p
=mass flow rate of particles
Δt=time step
F
other
=other interaction forces
u󰇍
p
=velocity of particles
u󰇍
=velocity of airflow
1
Graduate Student, Computational Fluid Dynamics Laboratory, Dept. of Mechanical Engineering &
Materials Science.
2
William Palm Professor of Engineering, Dept. of Mechanical Engineering & Materials Science, Fellow
AIAA.

2
I. Introduction
Because of environmental concerns related to CO
2
emissions and global warming with use of fossil
fuels, there is currently great deal of interest in exploitation of renewable energy sources such as wind
energy among others. In the context of wind energy, great deal of research is being conducted on the
design of wind turbines and wind farms to extract maximum possible energy from the wind.
Optimization of aerodynamic performance of both Horizontal Axis Wind Turbines (HAWT) and
Vertical Axis Wind Turbines (VAWT) is being investigated. Several wind turbine airfoils/blades have
been analyzed and newer airfoils/blades are being analyzed in the literature. National Renewable
Energy Laboratory (NREL) in Colorado has led the effort in this research along with industry and
academia.
For HAWT, aerodynamic characteristics of S809 airfoil have been extensively studied in the
literature. S-series of airfoils are representative of many horizontal-axis wind-turbine (HAWT) airfoils;
S809 is a 21% thick low speed airfoil while S814 airfoil is 24% thick airfoil and there are other S-series
of airfoils of different thicknesses and cambers with different lift and drag characteristics. S809 and
S814 airfoils have been tested in a wind tunnel at the Delft University on Technology and at Ohio State
University and the results have been published [2,3], which are utilized in this paper for comparison
with the numerical results. However, there are very few publications that consider the influence of
dusty air condition on the aerodynamic performance of wind turbine airfoils. In 2017, Douvi, Margaris
and Davaris published a paper on the effect of dusty air effect on the aerodynamic performance of S809
airfoil [5].
The focus of this paper is on the evaluation of the aerodynamic performance of the S809 and S814
airfoils in clean air and dusty air by numerical simulation. Incompressible RANS equations are solved
with one-equation SA model and two-equation realizable k-ε model. The discrete phase, which consists
of dust particles in this case, is injected into the air flow and its effect is calculated using discrete phase
model (DPM) in FLUENT. By comparing the results of clean and dusty air conditions, conclusions
about the effects of dusty air condition on the aerodynamic performance of airfoils are drawn.
II. Numerical Method and Validation
A. Physical model and Mesh Process
The geometry models of airfoils are constructed using their coordinate’s data in Somers’s report [1].
The chord lengths of both airfoils are taken to be 1m. As shown in Figs. 2 and 4, the computational
domain consists of a semi-circle with radius 25m and a rectangle with 50m height and 25m width. The
airfoil is located at the center of the domain. Due to the turbulent boundary layer effects on the flow
field near the airfoil, mesh in this region is much denser than the mesh in the far field. ICEM is used for
mesh generation. Figure 5 demonstrates that the mesh is of high quality and is adequate for simulation.
The solutions are performed on a series of meshes and it is ensured that the solution is mesh
independent and the distance of first grid point from the airfoil surface y+ is less than 1.

3
(a) S809 airfoil
(b) S814 airfoil
Fig.1 Physical models of airfoils
1m
1m

4
Fig.2 Computational domain and mesh around S809 airfoil
aZoomed-in-view of mesh near S809 airfoil
airfoil
outlet
inlet

Citations
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Journal ArticleDOI
TL;DR: In this article , the effect of sand particle on dynamic stall characteristics is investigated under a sand-wind environment, where the authors adopted the unsteady CFD method and the discrete phase model (DPM) to simulate the dynamic stall characteristic of the S809 airfoil.

1 citations

13 Apr 2023
TL;DR: In this paper , the performance of the National Renewable Energy Laboratory (NREL) Phase VI wind turbine, designed to be insusceptible to surface roughness, undergoing either clean or dusty air was numerically investigated.
Abstract: The meteorological conditions markedly affect the energy efficiencies and cost/power rate of the wind turbines. This study numerically investigates the performance of the National Renewable Energy Laboratory (NREL) Phase VI wind turbine, designed to be insusceptible to surface roughness, undergoing either clean or dusty air. First, the numerical approach is validated against the available experimental data for clean air. Following this, the model is developed into a Lagrangian-Eulerian multiphase approach to comprehensively analyze the effects of the dusty air. The dependence of aerodynamic performance on the wind speed (= 5-25 m/s), particle diameter dp (= 0.025-0.9 mm) and angle of attack (= 0o-44o) is investigated. It is found that the turbine performance generally deteriorates in dusty conditions. But it becomes relatively acute for dp>0.1 mm and post-stall state. As such, the generated power is reduced by 4.3% and 13.3% on average for the air with the dp = 0.05 and 0.9 mm, respectively. The particles change the flow field profoundly, declining the pressure difference between the suction/pressure sides of the blade-airfoil, advancing the boundary layer separation, and strengthening the recirculation zones. The above changes account for a lower lift coefficient and higher drag coefficient.
References
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Book
01 Feb 1986
TL;DR: In this article, Navier-Stokes et al. discuss the fundamental principles of Inviscid, Incompressible Flow over airfoils and their application in nonlinear Supersonic Flow.
Abstract: TABLE OF CONTENTS Preface to the Fifth Edition Part 1: Fundamental Principles 1. Aerodynamics: Some Introductory Thoughts 2. Aerodynamics: Some Fundamental Principles and Equations Part 2: Inviscid, Incompressible Flow 3. Fundamentals of Inviscid, Incompressible Flow 4. Incompressible Flow Over Airfoils 5. Incompressible Flow Over Finite Wings 6. Three-Dimensional Incompressible Flow Part 3: Inviscid, Compressible Flow 7. Compressible Flow: Some Preliminary Aspects 8. Normal Shock Waves and Related Topics 9. Oblique Shock and Expansion Waves 10. Compressible Flow Through Nozzles, Diffusers and Wind Tunnels 11. Subsonic Compressible Flow Over Airfoils: Linear Theory 12. Linearized Supersonic Flow 13. Introduction to Numerical Techniques for Nonlinear Supersonic Flow 14. Elements of Hypersonic Flow Part 4: Viscous Flow 15. Introduction to the Fundamental Principles and Equations of Viscous Flow 16. A Special Case: Couette Flow 17. Introduction to Boundary Layers 18. Laminar Boundary Layers 19. Turbulent Boundary Layers 20. Navier-Stokes Solutions: Some Examples Appendix A: Isentropic Flow Properties Appendix B: Normal Shock Properties Appendix C: Prandtl-Meyer Function and Mach Angle Appendix D: Standard Atmosphere Bibliography Index

3,113 citations


"Numerical Investigation of Wind Tur..." refers background in this paper

  • ...Such a behavior of the velocity field affects the pressure field which reduces the lift and increase the drag [6]....

    [...]

  • ...One more interesting fact is that the cl-α curve does not pass through the origin, which means that non-zero lift force exists when angle of attack is zero; it is expected since the airfoil is not completely symmetrical and this asymmetry results in pressure difference between upper and lower part of the airfoil [6]....

    [...]

ReportDOI
01 Jan 1997
TL;DR: In this article, a 21-percent-thick laminar flow airfoil, the S809, for horizontal-axis wind-turbine applications, has been designed and analyzed theoretically and verified experimentally in the lowturbulence wind tunnel of the Delft University of Technology Low Speed Laboratory, The Netherlands.
Abstract: A 21-percent-thick, laminar-flow airfoil, the S809, for horizontal-axis wind-turbine applications, has been designed and analyzed theoretically and verified experimentally in the low-turbulence wind tunnel of the Delft University of Technology Low Speed Laboratory, The Netherlands. The two primary objectives of restrained maximum lift, insensitive to roughness, and low profile drag have been achieved. The airfoil also exhibits a docile stall. Comparisons of the theoretical and experimental results show good agreement. Comparisons with other airfoils illustrate the restrained maximum lift coefficient as well as the lower profile-drag coefficients, thus confirming the achievement of the primary objectives.

389 citations


"Numerical Investigation of Wind Tur..." refers methods in this paper

  • ...S809 and S814 airfoils have been tested in a wind tunnel at the Delft University on Technology and at Ohio State University and the results have been published [2,3], which are utilized in this paper for comparison with the numerical results....

    [...]

Journal ArticleDOI
TL;DR: In this article, a dynamical, two-phase flow model in two-and three-space coordinates is presented, where the gas-liquid flow is modeled by a Navier-Stokes system of equations in an Eulerian representation.

267 citations

Frequently Asked Questions (16)
Q1. What is the effect of dust particles on the aerodynamic performance of the wind turbine?

2. Injection of dust particles can generate negative effects on the aerodynamic performance of the wind turbine airfoil; the drag coefficient increases and the lift coefficient decreases resulting in a lower lift to drag ratio. 

For dusty air simulation, realizable k-ε model is chosen and the discrete phase model (DPM) in FLUENT is employed to inject the dust particles into the flow field. 

Due to the turbulent boundary layer effects on the flow field near the airfoil, mesh in this region is much denser than the mesh in the far field. 

4. The wind turbines will not only have erosion and degradation of blades in dusty environment but also poor power generation in countries where sand dust is very common in the environment e.g. countries in the Middle East. 

The discrete phase, which consists of dust particles in this case, is injected into the air flow and its effect is calculated using discrete phase model (DPM) in FLUENT. 

C. Discrete phase model (DPM)Currently there are two numerical methods for calculation of multiphase flows: the Euler-Lagrange approach and the Euler-Euler approach. 

2William Palm Professor of Engineering, Dept. of Mechanical Engineering & Materials Science, Fellow AIAA.I. IntroductionBecause of environmental concerns related to CO2 emissions and global warming with use of fossil fuels, there is currently great deal of interest in exploitation of renewable energy sources such as wind energy among others. 

By using realizable k-ε model and discrete phase model, results of dusty air condition are calculated and compared with results of clean air condition. 

3. Based on the comparison between results of 1% and 10% concentration of particles by volume in dusty air, it is found that larger concentration of dust particles has more detrimental effects on aerodynamic performance as expected and therefore on the power output of the wind turbine. 

Re is the relative Reynolds number, which is defined asRe ≡ ⃑ ⃑(4)Since the flow is regarded as incompressible and the temperature effects are very small, the energy equation is not considered. 

As α increases, linearly dependence no longer exists and the computed results are significantly different from the experimental data due to the effect of stall [8]. 

According to theformula,𝑅𝑒 = 𝜌 ∙ 𝑉 ∙ 𝑑𝜇with the density of air ρair=1.176674 kg/m3 and the viscosity of air μ=1.7894×10-5kg/m∙s, the velocity at the inlet is 22.8m/s and the Mach Number is 0.066.B. 

Results for S809 airfoil at different Reynolds Number under clean air conditionSince Re and free stream velocity V are linearly dependent with ρ, d and μ being unchanged, differentRe means different free stream velocity faced by the airfoil. 

The change in momentum of a sand particle through each control volume can be calculated by the following equation:F = 18𝜇𝐶 𝑅𝑒24𝜌 𝑑 𝑢 − 𝑢 + 

As shown in Figs. 2 and 4, the computational domain consists of a semi-circle with radius 25m and a rectangle with 50m height and 25m width. 

Figure 10 shows that the lift coefficient increases slightly when the Reynolds number increases from 1×106 to 1.5×106, which leads to change in lift to drag ratio.