Two-Step Stall Characteristic of an Airfoil with a Single Leading-Edge Protuberance

被引:24
作者
Cai, Chang [1 ]
Zuo, Zhigang [1 ]
Morimoto, Masahiro [2 ]
Maeda, Takao [2 ]
Kamada, Yasunari [2 ]
Liu, Shuhong [1 ]
机构
[1] Tsinghua Univ, State Key Lab Hydrosci & Engn, Dept Thermal Engn, Beijing 100084, Peoples R China
[2] Mie Univ, Div Mech Engn, Tsu, Mie 5148507, Japan
基金
中国国家自然科学基金;
关键词
FLOW; TUBERCLES; PERFORMANCE; HYSTERESIS;
D O I
10.2514/1.J055921
中图分类号
V [航空、航天];
学科分类号
08 ; 0825 ;
摘要
An experimental investigation has been conducted to examine the influence of a single leading-edge protuberance on the performance of a baseline NACA 634-021 airfoil. Static aerodynamic forces of the airfoils have been measured as the angle of attack increased and decreased. A hysteresis loop of the lift coefficient around the stall angle is observed for the baseline airfoil, with a sharp decline of the lift coefficient during angle-of-attack increase and a delayed recovery during angle-of-attack decrease. It was discovered for the first time that both the decline and the recovery of the lift coefficient of the modified airfoil with a single leading-edge protuberance included two steps. When the first step happened, the lift coefficient reached an intermediate value between the maximum value and the poststall value of the baseline airfoil, and it remained almost constant within a range of angles of attack. Surface tuft visualization revealed that, during the first step of stall, one side of the modified airfoil was stalled with leading-edge separation, whereas the other side remained in a nonstall condition. When the second step of stall happened, both sides of the modified airfoil were stalled, except for an attached flow on the protuberance peak. This one-sided stall phenomenon indicated that one important role of the leading-edge protuberance might be confining the local stall region from extending spanwise, which is similar to the effect of a wing fence.
引用
收藏
页码:64 / 77
页数:14
相关论文
共 39 条
[1]  
Arai H., 2010, J. Aero Aqua Bio-mech, V1, P18, DOI [10.5226/jabmech.1.18, DOI 10.5226/JABMECH.1.18]
[2]   Tubercles and Their Applications [J].
Bolzon, Michael D. ;
Kelso, Richard M. ;
Arjomandi, Maziar .
JOURNAL OF AEROSPACE ENGINEERING, 2016, 29 (01)
[3]   Spanwise variation in the unsteady stalling flowfields of two-dimensional airfoil models [J].
Broeren, AP ;
Bragg, MB .
AIAA JOURNAL, 2001, 39 (09) :1641-1651
[4]  
Bushnell D. M., 1991, J FLUIDS ENG, V113, P5, DOI [10. 1115/1. 2926497 JFEGA4 0098-2202, DOI 10.1115/1.2926497JFEGA40098-2202]
[5]  
BUSHNELL DM, 1991, ANNU REV FLUID MECH, V23, P65, DOI 10.1146/annurev.fl.23.010191.000433
[6]  
Cai C., 2017, J FLUIDS ENG
[7]   Numerical investigations of hydrodynamic performance of hydrofoils with leading-edge protuberances [J].
Cai, Chang ;
Zuo, Zhigang ;
Liu, Shuhong ;
Wu, Yulin .
ADVANCES IN MECHANICAL ENGINEERING, 2015, 7 (07) :1-11
[8]  
Camara J., 2013, 51 AIAA AER SCI M DA
[9]  
Carreira Pedro H., 2008, P 46 AIAA AER SCI M
[10]  
Coleman HW., 2009, Experimentation, Validation, and Uncertainty Analysis for Engineers, DOI [DOI 10.1002/9780470485682, 10.1002/9780470485682.]