TY - JOUR
T1 - Aerodynamics of a two-dimensional flapping wing hovering in proximity of ground
AU - Zheng, Yunlong
AU - Qu, Qiulin
AU - Liu, Peiqing
AU - Qin, Yunpeng
AU - Agarwal, Ramesh K.
N1 - Funding Information:
The author(s) disclosed receipt of the following financial support for the research, authorship, and/or publication of this article: This work was partially supported by the National Natural Science Foundation of China (Nos. 11502012, 11772033, and 11721202).
Publisher Copyright:
© IMechE 2018.
PY - 2019/9/1
Y1 - 2019/9/1
N2 - The difference in aerodynamic forces of a two-dimensional flapping wing hovering in unbounded flow field and ground effect is studied. The unsteady laminar Navier–Stokes equations are solved by the finite volume method to simulate the flow field around the wing. In the unbounded flow field, the correspondence between the aerodynamic force, pressure distribution on wing, and typical vortex structures is established, and then the high-lift mechanism of the flapping wing is further explained. In the ground effect, based on the lift variation, the dimensionless height H/C (H is the height of the wing above ground and C is the chord length of the wing) can be divided into transition and ground effect regimes. In the transition regime (H/C > 2.5), the lift decreases with the decreasing height, and the ground indirectly impacts the vortices near wing by changing the shed vortices in space. In the ground effect regime (H/C < 2.5), the lift increases with the decreasing height, and the ground directly impacts the vortices near the wing.
AB - The difference in aerodynamic forces of a two-dimensional flapping wing hovering in unbounded flow field and ground effect is studied. The unsteady laminar Navier–Stokes equations are solved by the finite volume method to simulate the flow field around the wing. In the unbounded flow field, the correspondence between the aerodynamic force, pressure distribution on wing, and typical vortex structures is established, and then the high-lift mechanism of the flapping wing is further explained. In the ground effect, based on the lift variation, the dimensionless height H/C (H is the height of the wing above ground and C is the chord length of the wing) can be divided into transition and ground effect regimes. In the transition regime (H/C > 2.5), the lift decreases with the decreasing height, and the ground indirectly impacts the vortices near wing by changing the shed vortices in space. In the ground effect regime (H/C < 2.5), the lift increases with the decreasing height, and the ground directly impacts the vortices near the wing.
KW - Flapping wing
KW - ground effect
KW - high-lift mechanism
UR - http://www.scopus.com/inward/record.url?scp=85069038981&partnerID=8YFLogxK
U2 - 10.1177/0954410018819335
DO - 10.1177/0954410018819335
M3 - Article
AN - SCOPUS:85069038981
SN - 0954-4100
VL - 233
SP - 4316
EP - 4332
JO - Proceedings of the Institution of Mechanical Engineers, Part G: Journal of Aerospace Engineering
JF - Proceedings of the Institution of Mechanical Engineers, Part G: Journal of Aerospace Engineering
IS - 12
ER -