Topic
Airfoil
About: Airfoil is a research topic. Over the lifetime, 24696 publications have been published within this topic receiving 337709 citations. The topic is also known as: aerofoil & wing section.
Papers published on a yearly basis
Papers
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01 Jan 1995
TL;DR: The development of special-purpose airfoils for horizontal-axis wind turbines (HAWTs) began in 1984 as a joint effort between the National Renewable Energy Laboratory (NREL), formerly the Solar Energy Research Institute (SERI), and Airfoils, Incorporated.
Abstract: The development of special-purpose airfoils for horizontal-axis wind turbines (HAWTs) began in 1984 as a joint effort between the National Renewable Energy Laboratory (NREL), formerly the Solar Energy Research Institute (SERI), and Airfoils, Incorporated. Since that time seven airfoil families have been designed for various size rotors using the Eppler Airfoil Design and Analysis Code. A general performance requirement of the new airfoil families is that they exhibit a maximum lift coefficient (c{sub l,max}) which is relatively insensitive to roughness effects. The airfoil families address the needs of stall-regulated, variable-pitch, and variable-rpm wind turbines. For stall-regulated rotors, better peak-power control is achieved through the design of tip airfoils that restrain the maximum lift coefficient. Restrained maximum lift coefficient allows the use of more swept disc area for a given generator size. Also, for stall-regulated rotors, tip airfoils with high thickness are used to accommodate overspeed control devices. For variable-pitch and variable-rpm rotors, tip airfoils having a high maximum lift coefficient lend themselves to lightweight blades with low solidity. Tip airfoils having low thickness result in less drag for blades having full-span pitch control. Annual energy improvements from the NREL airfoil families are projected to be 23% to 35% for stall-regulatedmore » turbines, 8% to 20% for variable-pitch turbines, and 8% to 10% for variable-rpm turbines. The improvement for stall-regulated turbines has been verified in field tests.« less
233 citations
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09 Jan 2006
TL;DR: In this article, the power flow through a plasma actuator is divided into four sinks: reactive power losses due to inadequate impedance matching of the power supply to the actuator, dielectric heating of actuator insulating materials, power required to maintain the atmospheric pressure plasma, and power coupled to the neutral gas flow by ion-neutral collisions.
Abstract: Electrohydrodynamic plasma actuators have proven effective for flow attachment in internal and external aerodynamics, and for modification of the lift, drag, and stall angle of airfoils. The performance of plasma actuators has been studied with such classical aerodynamic tools as wind tunnels, drag balances, Pitot tubes, smoke flow visualization, and fluid dynamic modeling programs. However, the physical processes and power flows that occur in plasma actuators, before the plasma ions transfer their momentum to the neutral background gas, are those of an electrical device. Optimization of such actuators needs to include the methods of electrical engineering and plasma physics, including classical electrical discharge physics. To implement a program of optimization, we have conceptually divided the power flow through a plasma actuator into the following four sinks: 1.) Reactive power losses due to inadequate impedance matching of the power supply to the actuator; 2.) Dielectric heating of the actuator insulating materials; 3.) Power required to maintain the atmospheric pressure plasma; and 4.) Power coupled to the neutral gas flow by ion-neutral collisions. These four power flows can be, and usually are, of comparable magnitude. In this paper, we review our progress in understanding and minimizing the first three power flows, and maximizing the fourth by adjustment of the actuator geometry and materials, as well as such plasma parameters as the RF frequency and RMS voltage.
232 citations
01 Jan 1944
TL;DR: Theoretical tunnel-wall corrections for an airfoil of finite thickness and camber in a two-dimensional flow wind tunnel were derived in this article, and the results were compared with the small amount of low-speed experimental data available, even for relatively large values of the chord-height ratio.
Abstract: Theoretical tunnel-wall corrections are derived for an airfoil of finite thickness and camber in a two-dimensional-flow wind tunnel. The theory takes account of the effects of the wake of the airfoil and of the compressibility of the fluid, and is based upon the assumption that the chord of the airfoil is small in comparison with the height of the tunnel. Consideration is given to the phenomenon of choking at high speeds and its relation to the tunnel-wall corrections. The theoretical results are compared with the small amount of low-speed experimental data available and the agreement is seen to be satisfactory, even for relatively large values of the chord-height ratio.
231 citations
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TL;DR: In this paper, a flying hot wire was used to measure the relative flow direction of hot-wire data at closely spaced points along the probe arc, and the data were obtained at several thousand locations in the flow field.
Abstract: Hot-wire measurements have been made in the boundary layer, the separated region, and the near wake for
flow past an NACA 4412 airfoil at mad mum lift. The Reynolds number based on chord was about 1,500,000.
Special care was taken to achieve a two-dimensional mean flow. The main instrumentation was a flying hot wire;
that is, a hot-wire probe mounted on the end of a rotating arm. The probe velocity was sufficiently high to avoid
the usual rectification problem by keeping the relative flow direction always within a range of ± 30 deg from the
probe ads. A digital computer was used to control synchronized sampling of hot-wire data at closely spaced
points along the probe arc. Ensembles of data were obtained at several thousand locations in the flowfield. The
data include Intermittency, two components of mean velocity, and twelve mean values for double, triple, and
quadruple products of two velocity fluctuations. No Information was obtained about the third (spanwise)
velocity component. An unexpected effect of rotor interference was identified and brought under reasonable
control. The data are available on punched cards in raw form and also after use of smoothing and interpolation
routines to obtain values on a fine rectangular grid aligned with the airfoil chord. The data are displayed In the
paper as contour plots.
230 citations
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TL;DR: In this article, a finite state induced flow model for the three-dimensional induced flow for a rotor was developed in a compact closed form, which does not presuppose anything about the source of lift on the rotating blades.
Abstract: In Part I of this two-part article, we developed a finite state induced flow model for a two-dimensional airfoil. In this second part, we develop a finite state induced flow model for the three-dimensional induced flow for a rotor. The coefficients of this model are found in a compact closed form. Although the model does not presuppose anything about the source of lift on the rotating blades, applications are given in which the Prandtl assumption is invoked. That is, the two-dimensional lift equations are used at each radial station, but with the inflow from the three-dimensional model. The results are shown to reduce (in several special cases) to Prandtl-Golds tein theory, Theodorsen theory, Loewy theory, dynamic inflow, and blade-element momentum theory. Comparisons with vortex-filament models and with experimental data in hover and forward flight also show excellent correlation.
230 citations