Zheng Hongyu, Xie Fangfang, Zheng Yao, Ji Tingwei, Zhu Zaoxu
Center for Engineering and Scientific Computation, and School of Aeronautics and Astronautics Zhejiang University, Zhejiang 310027, China.
Phys Rev E. 2019 Jun;99(6-1):063109. doi: 10.1103/PhysRevE.99.063109.
In the present study, we use the dynamic mesh method based on the radial basis function interpolation for the two-dimensional simulation of harmonically oscillating NACA0015 airfoil. Under various flapping frequencies, heaving and pitching amplitudes, the observed wake flows can be divided into seven types, including the Bénard-von Kármán (BvK) vortex street, the reversed BvK (RBvK) vortex street, the 1P wake, the mP wake, the 2P+mS wake, the 2S+mS wake, and the mS wake, where m is around 4 and xS+yP signifies x single vortices and y vortex pairs shedding per oscillation period. Then we have constructed two phase diagrams of the wake types in terms of the flapping frequency, heaving and pitching amplitudes. Importantly, we have combined the propulsion performance of the flapping airfoil with the wake map and found that α(T/4), the angle of attack at t=T/4, can determine the wake type: negative value corresponding to drag-dominated wakes, while positive value corresponding to thrust dominated flow wakes. With the increase of α(T/4), the wake transforms from the mP to 2S+mS then to RBvK and eventually to 1P wake. Furthermore, the coherent structure analysis and spectral analysis are conducted for all the types of wakes by using dynamic mode decomposition. And there is a positive correlation between the strengths of vortices shedding at i times flapping frequency and the modulus of the ith dynamic mode decomposition mode, which can further reveal the differences among different types of wakes.
在本研究中,我们使用基于径向基函数插值的动态网格方法对谐波振荡的NACA0015翼型进行二维模拟。在各种拍动频率、升沉和俯仰幅度下,观察到的尾流可分为七种类型,包括贝纳德-冯·卡门(BvK)涡街、反向BvK(RBvK)涡街、1P尾流、mP尾流、2P + mS尾流、2S + mS尾流和mS尾流,其中m约为4,xS + yP表示每个振荡周期有x个单个涡旋和y个涡旋对脱落。然后,我们根据拍动频率、升沉和俯仰幅度构建了两个尾流类型的相图。重要的是,我们将拍动翼型的推进性能与尾流图相结合,发现α(T/4),即t = T/4时的攻角,可以决定尾流类型:负值对应于阻力主导的尾流,而正值对应于推力主导的流动尾流。随着α(T/4)的增加,尾流从mP转变为2S + mS,然后转变为RBvK,最终转变为1P尾流。此外,通过使用动态模态分解对所有类型的尾流进行了相干结构分析和频谱分析。并且在i倍拍动频率下脱落的涡旋强度与第i个动态模态分解模式的模之间存在正相关,这可以进一步揭示不同类型尾流之间的差异。