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A CFD analysis of the flow over a side-supported sphere with localised synthetic jet

机译:用局部合成射流对侧支撑球面上的流动进行CFD分析

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The application of synthetic jet in a cross flow has been studied numerically in mostly two-dimensional configurations. The synthetic jet is becoming a useful technological tool for flow control. For aerodynamic applications this would be beneficial in reducing fuel consumption by increasing the efficiency of the flow over solid geometries. The present numerical simulation is conducted on a three-dimensional bluff body, a side-supported sphere, in a cross flow. The computational model was constructed based upon the experimental work conducted by the authors [6,16]. The synthetic jet was modelled numerically based upon the harmonic sinusoidal motion of the actuator used in the physical experiments. An open type boundary condition was used in the ANSYS CFX commercial CFD package that has not been previously developed using this software to produce the zero net mass flow condition whilst generating the required velocity profile. The synthetic jet asymmetrical and localised, was located at three different angles of incidence 6.5°, 76° and 100°. The cross flow was set at the Reynolds number of 5 × 10~4. Since the flow over the side-supported sphere at this Reynolds number is unsteady and the synthetic jet is inherently an oscillating turbulent shear flow it was required to conduct a transient CFD analysis. Two different turbulence models were used to predict separation of the unsteady flow field with the SST turbulence model proving to be most accurate when compared to the experimental data. It was found that the synthetic jet at all angles of incidence improved the surface pressure distribution before separation relative to the baseline case. Post separation the localised synthetic jet increased the crosswise vorticity in the wake region at 6.5°. With the synthetic jet at 76° and 100° produced a similar result by decreasing the size of the wake and streamlining the flow through a breaking up crosswise vorticity in the wake region. Further the interference flow at the support-sphere junction was streamlined leading to a slight decrease in the drag.
机译:合成射流在错流中的应用已在大多数二维结构中进行了数值研究。合成射流正成为控制流量的有用技术工具。对于空气动力学应用,这将有利于通过增加实体几何形状上的流动效率来减少燃料消耗。当前的数值模拟是在三维流线形体(侧支撑球体)上以交叉流的形式进行的。该计算模型是根据作者的实验工作构建的[6,16]。基于物理实验中使用的执行器的谐波正弦运动,对合成射流进行了数值建模。在ANSYS CFX商业CFD软件包中使用了开放类型的边界条件,该条件以前并未使用该软件进行开发,无法在产生所需速度曲线的同时产生零净质量流量条件。合成射流不对称且局部分布,分别位于入射角6.5°,76°和100°的三个不同角度。错流设定为雷诺数为5×10〜4。由于在此雷诺数下流经侧支撑球体的流量不稳定,并且合成射流本质上是振荡湍流剪切流,因此需要进行瞬态CFD分析。使用两种不同的湍流模型来预测非稳态流场的分离,其中与实验数据相比,SST湍流模型被证明是最准确的。已经发现,相对于基线情况,合成射流在所有入射角均改善了分离前的表面压力分布。分离后,局部合成射流增加了尾流区6.5°处的横向涡度。在76°和100°的合成射流下,通过减小尾流尺寸并通过尾流区域内的横向涡旋破裂使流线流线化,产生了相似的结果。此外,简化了支撑-球体交界处的干扰流,从而导致阻力略有下降。

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