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首页> 外文期刊>Journal of Mechanical Science and Technology >The effect of non-equilibrium condensation on the coefficients of force with the angle of attack in the transonic airfoil flow of NACA0012
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The effect of non-equilibrium condensation on the coefficients of force with the angle of attack in the transonic airfoil flow of NACA0012

机译:非平衡冷凝对NACA0012跨音速翼型流中力系数和迎角的影响

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摘要

A transonic flow with a non-equilibrium condensation past NACA0012 profile whose aspect ratio AR is 1.0 with the angle of attack was analyzed by numerical analysis using a TVD scheme, and investigated using an intermittent indraft type supersonic wind tunnel. Transonic flows of 0.70–0.90 in free stream Mach number with variations of Φ0 and α were tested. For the same M∞ and α, the increase in stagnation relative humidity Φ0 caused a decrease in the drag coefficient of profile (that is total) which is composed of the components of form, viscous, wave and condensation; however, the lift coefficient up to Φ0 = 50% increased in the opposite direction. As an example, in the case of M∞ = 0.83, Φ0 = 50%, α = 3○ and T0 = 298 K, the decreasing rate of the coefficient of profile drag and the increasing rate of the lift coefficient compared to the case of Φ0 = 0% caused by non-equilibrium condensation amounted to 65% and 52%, respectively. In addition, for the same Φ0 and α, as the free stream Mach number M∞ increased, at first, the lift coefficient increased slightly, and then suddenly severely dropped, and finally remained nearly constant. The suddenly dropped free stream Mach number in CL became larger with an increase of Φ0. It turned out that the drag coefficients of form and viscous were almost independent of Φ0. The contribution of wave drag to the coefficient of profile drag for M∞ = 0.83, Φ0 = 30%, α = 3° and T0 = 298 K amounted to approximately 79%, and in the case of Φ0 = 60%, the contribution of the non-equilibrium condensation to the reduction in the coefficient of the profile drag compared to the case without condensation amounted to 75%. Especially, for the case of Φ0 = 0% and α = 0°, there was an oscillatory flow region around M∞ = 0.87.
机译:通过使用TVD方案的数值分析,分析了经过NACA0012轮廓且纵横比AR为1.0且攻角为非平衡的跨音速流,并使用间歇吸气式超音速风洞进行了研究。测试了自由流马赫数随Φ0和α变化的跨音速流0.70–0.90。对于相同的M∞和α,停滞相对湿度Φ0的增加导致轮廓(整体)阻力系数减小,该阻力由形式,粘性,波动和凝结组成。但是,升力系数Φ0= 50%沿相反方向增加。例如,在M∞= 0.83,Φ0= 50%,α= 3○和T0 = 298 K的情况下,轮廓阻力系数的减小率和升力系数的增大率与由非平衡缩合引起的Φ0= 0%分别为65%和52%。此外,对于相同的Φ0和α,随着自由流马赫数M∞的增加,起升系数略有增加,然后突然急剧下降,最后几乎保持恒定。 CL中突然下降的自由流马赫数随着Φ0的增加而变大。结果表明,形式和粘性的阻力系数几乎与Φ0无关。对于M∞= 0.83,Φ0= 30%,α= 3°和T0 = 298 K的情况,波浪阻力对轮廓阻力系数的贡献约为79%,而在Φ0= 60%的情况下,与没有凝结的情况相比,非平衡凝结导致轮廓阻力系数的降低。特别是对于Φ0= 0%和α= 0°的情况,在M∞= 0.87附近存在一个振荡流动区域。

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