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Numerical study of blowing and suction slot geometry optimization on NACA 0012 airfoil

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In this article, the effects of jet width on blowing and suction flow control were evaluated for a NACA 0012 airfoil, and the results showed that when the blowing jet width increases, the lift-to-drag ratio rises continuously in tangential blowing and decreases quasi-linearly in perpendicular blowing.
Abstract
The effects of jet width on blowing and suction flow control were evaluated for a NACA 0012 airfoil. RANS equations were employed in conjunction with a Menter’s shear stress turbulent model. Tangential and perpendicular blowing at the trailing edge and perpendicular suction at the leading edge were applied on the airfoil upper surface. The jet widths were varied from 1.5% to 4% of the chord length, and the jet velocity was 0.3 and 0.5 of the free-stream velocity. Results of this study demonstrated that when the blowing jet width increases, the lift-to-drag ratio rises continuously in tangential blowing and decreases quasi-linearly in perpendicular blowing. The jet widths of 3.5% and 4% of the chord length are the most effective amounts for tangential blowing, and smaller jet widths are more effective for perpendicular blowing. The lift-to-drag ratio improves when the suction jet width increases and reaches its maximum value at 2.5% of the chord length.

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Book ChapterDOI

Boundary Layer Theory

TL;DR: The boundary layer equations for plane, incompressible, and steady flow are described in this paper, where the boundary layer equation for plane incompressibility is defined in terms of boundary layers.
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Application of flow control strategy of blowing, synthetic and plasma jet actuators in vertical axis wind turbines

TL;DR: In this paper, the upward-parabola blowing jet flow control strategy for VAWTs is proposed to suppress the flow separation in advance, which can significantly enhance the aerodynamic performance by using significantly low energy consumption.
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Three-dimensional suction flow control and suction jet length optimization of NACA 0012 wing

TL;DR: In this article, a three-dimensional suction flow control study was performed to investigate the aerodynamic characteristics of a rectangular wing with a NACA 0012 airfoil section, and the optimum suction jet length was determined.
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Passive flow control for aerodynamic performance enhancement of airfoil with its application in Wells turbine – Under oscillating flow condition

TL;DR: In this article, the authors employed an entropy generation minimization method to examine the impact of the flow control method on the entropy generation characteristics around the turbine blade, which is performed using a time-dependent CFD model of isolated NACA airfoil, which refers to the turbine blades under sinusoidal flow boundary conditions, which emulates the actual operating conditions.
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Enhancement of performance of wave turbine during stall using passive flow control: First and second law analysis

TL;DR: In this article, the authors used an entropy generation minimization method to examine the impact of the multi-suction slots method on the entropy generation characteristics around the turbine blade and found that the airfoil with three suction slots located at 40, 55% and 90% from leading edge in chord percentage gave the highest torque coefficient by 267% before the stall and 51% after the stall.
References
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Book

Boundary layer theory

TL;DR: The flow laws of the actual flows at high Reynolds numbers differ considerably from those of the laminar flows treated in the preceding part, denoted as turbulence as discussed by the authors, and the actual flow is very different from that of the Poiseuille flow.
Book ChapterDOI

Boundary Layer Theory

TL;DR: The boundary layer equations for plane, incompressible, and steady flow are described in this paper, where the boundary layer equation for plane incompressibility is defined in terms of boundary layers.

Airfoil section characteristics as affected by variations of the Reynolds number

TL;DR: In this paper, the results of an investigation of a systematically chosen representative group of related airfoils conducted in the NACA variable-density wind tunnel over a wide range of Reynolds number extending well into the flight range are presented.
Journal ArticleDOI

Post-stall flow control on an airfoil by local unsteady forcing

TL;DR: In this article, the authors used a Reynolds-averaged two-dimensional computation of a turbulent flow over an airfoil at post-stall angles of attack, and showed that the massively separated and disordered unsteady flow can be effectively controlled by periodic blowing-suction near the leading edge with low-level power input.
Journal ArticleDOI

Numerical investigation of synthetic-jet flowfields

TL;DR: In this article, the flowflelds surrounding a synthetic-jet actuating device are investigated numerically by direct simulation, and solutions are obtained to the unsteady compressible Navier-Stokes equations for both the interior of the actuator cavity and for the external jet flowfield.
Related Papers (5)
Frequently Asked Questions (24)
Q1. What have the authors contributed in "Numerical study of blowing and suction slot geometry optimization on naca 0012 airfoil" ?

Results of this study demonstrated that when the blowing jet width increases, the lift-to-drag ratio rises continuously in tangential blowing and decreases quasi-linearly in perpendicular blowing. 

Further works are needed to investigate some essential suction/blowing parameters, including the number of slots, slot arrangements, and synthetic jet parameters. 

A low free-stream turbulence level was used to match the wind tunnel characteristics, such that the stream turbulence intensity was selected as less than 0.1%. 

Methods of flow control to achieve transition delay, separation postponement, lift enhancement, drag reduction, turbulence augmentation, and noise suppression have been considered [2]. 

When the jet width varied from 1.5% to 4% of the chord length, the lift and drag coefficients decreased by approximately 23% and 16%, respectively, under A = 0.5 and an angle of attack of 14°. 

With increasing jet width, the lift coefficient increases continuously until a jet width of 2.5% of the chord length and then insignificantly decreases. 

Increasing blowing jet width improves the lift-to-drag ratio continuously for tangential blowing and reduces it constantly and quasilinearly for perpendicular blowing. 

perpendicular blowing decreases the lift-to-drag ratio before stall angle intensively and increases the aerodynamic characteristics after stall, for instance, perpendicular blowing increased the lift-to-drag ratio by 17.5% at an angle of attack of 18°. 

To simulate the turbulent flow, eddy or turbulent viscosity distribution was employed rather than the Reynolds stress tensor through eddy viscosity turbulent models, including algebraic or zero-equation models, one-equation models, and two-equation models. 

Jet widths of 3.5% and 4% of the chord length appear to be the most effective choice for tangential blowing at the airfoil trailing edge. 

Under an angle of attack of 14° and a blowing amplitude of 0.5, the lift coefficient increased to 1.157 and 1.163 for blowing jet widths of 1.5% and 4.0% of the chord length, respectively. 

With the use of perpendicular suction, not only the lift-to-drag ratio increases dramatically but also the stall angle delays effectively. 

the authors indicate that smaller blowing jet widths provide more positive effects for using perpendicular blowing to minimize drag and larger jet widths are effective to maximize it. 

The lift-to-drag ratio increased by approximately 17% for tangential blowing under H = 4%, A = 0.5, and Lj = 0.8C from the leading edge, with an angle of attack of 18°. 

the maximum errors for lift and drag coefficients in the k-ε realizable model at an angle of attack of 14° were 17% and 25%, respectively. 

The lift-to-drag ratio increases continually up to jet widths of 3.5% to 4% of the chord length along with jet width and then decreases. 

As mentioned earlier, the blowing jet amplitude has an insignificant effect on aerodynamic coefficients and poses only a 2% increase in the lift-to-drag ratio. 

The variations in lift and drag coefficients with jet width are almost negligible at low angles of attack, although they have shown significant changes with the increment of angle of attack. 

the lift-to drag ratio increased by 17% under a jet amplitude of 0.5, a jet width of 4% of the chord length, and an angle of attack of 18°. 

Techniques developed to manipulate the boundary layer, either to increase the lift or decrease the drag, are classified under the general heading ofboundary layer control or flow control [1]. 

12-14 present the lift, drag, and lift-to-drag ratio versus jet width with blowing jet amplitudes of 0.3 and 0.5 for tangential blowing at the trailing edge, respectively. 

The interval size was reduced to 0.00125 for blowing and suction slots, as indicated in Fig. 4.The residuals in all simulations were continued until the lift and drag coefficients reach a full convergence. 

The earliest known experimental works [4-6] on boundary layer suction for wings, primarily in the wind tunnel, were conducted in the late 1930s and the 1940s. 

the variations of tangential blowing parameters have a remarkable effect on the lift coefficient and a marginal effect on the drag coefficient.