Steady lift-force generation on a circular cylinder utilising a longitudinal vortex: Influence of geometrical parameters

2021 ◽  
Vol 212 ◽  
pp. 104612
Author(s):  
Withun Hemsuwan ◽  
Kasumi Sakamoto ◽  
Tsutomu Takahashi
2021 ◽  
Vol 87 (894) ◽  
pp. 20-00375-20-00375
Author(s):  
Kasumi SAKAMOTO ◽  
Withun HEMSUWAN ◽  
Tsutomu TAKAHASHI

2016 ◽  
Vol 2016 (0) ◽  
pp. 0617
Author(s):  
Tsutomu TAKAHASHI ◽  
Kasumi SAKAMOTO ◽  
Withun HEMSUWAN ◽  
Yumiko YOSHITAKE

2013 ◽  
Vol 284-287 ◽  
pp. 557-561
Author(s):  
Jie Li Fan ◽  
Wei Ping Huang

The two-degrees-of-freedom VIV of the circular cylinder with high mass-ratio is numerically simulated with the software ANSYS/CFX. The VIV characteristic is analyzed in the different conditions (Ur=3, 5, 6, 8, 10). When Ur is 5, 6, 8 and 10, the conclusion which is different from the cylinder with low mass-ratio can be obtained. When Ur is 3, the frequency of in-line VIV is twice of that of cross-flow VIV which is equal to the frequency ratio between drag force and lift force, and the in-line amplitude is much smaller than the cross-flow amplitude. The motion trace is the crescent. When Ur is 5 and 6, the frequency ratio between the drag force and lift force is still 2, but the main frequency of in-line VIV is mainly the same as that of cross-flow VIV and the secondary frequency of in-line VIV is equal to the frequency of the drag force. The in-line amplitude is still very small compared with the cross-flow amplitude. When Ur is up to 8 and 10, the frequency of in-line VIV is the same as the main frequency of cross-flow VIV which is close to the inherent frequency of the cylinder and is different from the frequency of drag force or lift force. But the secondary frequency of cross-flow VIV is equal to the frequency of the lift force. The amplitude ratio of the VIV between in-line and cross-flow direction is about 0.5. When Ur is 5, 6, 8 and 10, the motion trace is mainly the oval.


2020 ◽  
Vol 15 (30) ◽  
pp. 81-92
Author(s):  
Hossein Sadeghi ◽  
Mehrshad Yassari ◽  
Mohsen Pourfallah ◽  
Mohammad Molla Alipour ◽  
Ahmad Ali Rabienataj Darzi ◽  
...  

1988 ◽  
Vol 1988 (37) ◽  
pp. 73-82
Author(s):  
K. FUJITA ◽  
Y. IKEGAMI ◽  
K. KOBAYASHI ◽  
M. OHASHI

Fluids ◽  
2020 ◽  
Vol 5 (2) ◽  
pp. 59
Author(s):  
Xiaohui Su ◽  
Kaixuan Zhang ◽  
Juan Zheng ◽  
Yong Zhao ◽  
Ruiqi Han ◽  
...  

In the paper, a novel flapping mode is presented that can generate high lift force by a dragonfly wing in hover. The new mode, named partial advanced mode (PAM), starts pitching earlier than symmetric rotation during the downstroke cycle of the hovering motion. As a result, high lift force can be generated due to rapid pitching coupling with high flapping velocity in the stroke plane. Aerodynamic performance of the new mode is investigated thoroughly using numerical simulation. The results obtained show that the period-averaged lift coefficient, CL, increases up to 16% compared with that of the traditional symmetrical mode when an earlier pitching time is set to 8% of the flapping period. The reason for the high lift force generation mechanism is explained in detail using not only force investigation, but also by analyzing vortices produced around the wing. The proposed PAM is believed to lengthen the dynamic stall mechanism and enhance the LEV generated during the downstroke. The improvement of lift force could be considered as a result of a combination of the dynamic stall mechanism and rapid pitch mechanism. Finally, the energy expenditure of the new mode is also analyzed.


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