Numerical studies of undulation control on dynamic stall for reverse flows

The delayed detached-eddy simulation with adaptive coefficient (DDES-AC) method is used to simulate the baseline and leading-edge undulation control of dynamic stall for the reverse flow past a finite-span wing with NACA0012 airfoil. The numerical results of the baseline configuration are compared w...

Full description

Saved in:
Bibliographic Details
Published inActa mechanica Sinica Vol. 36; no. 2; pp. 290 - 305
Main Authors Wang, Biao, Liu, Jian, Yang, Yunjun, Xiao, Zhixiang
Format Journal Article
LanguageEnglish
Published Beijing The Chinese Society of Theoretical and Applied Mechanics; Institute of Mechanics, Chinese Academy of Sciences 01.04.2020
Springer Nature B.V
China Aerodynamics Research and Development Center,Mianyang 621000,China%China Academy of Aerospace Aerodynamics,Beijing 100074,China
School of Aerospace Engineering,Tsinghua University,Beijing 100084,China%School of Aerospace Engineering,Tsinghua University,Beijing 100084,China
EditionEnglish ed.
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:The delayed detached-eddy simulation with adaptive coefficient (DDES-AC) method is used to simulate the baseline and leading-edge undulation control of dynamic stall for the reverse flow past a finite-span wing with NACA0012 airfoil. The numerical results of the baseline configuration are compared with available measurements. DDES and DDES-AC perform differently when predicting the primary and secondary dynamic stalls. Overall, DDES-AC performs better owing to the decrease of grey area between the strong shear layer and the fully three-dimensional separated flow. Moreover, the effects of the undulating leading-edge on the forces, lift gradients, and instantaneous flow structures are explored. Compared with the uncontrolled case, the lift gradient in the primary dynamic stall is reduced from 18.4 to 8.5, and the secondary dynamic stall disappears. Therefore, periodic unsteady air-loads are also reduced. Additionally, the control mechanism of the wavy leading edge (WLE) is also investigated by comparison with the straight leading edge (SLE). No sudden breakdown of strong vortices is the main cause for WLE control.
ISSN:0567-7718
1614-3116
DOI:10.1007/s10409-020-00950-7