| Project/Area Number |
06650209
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| Research Category |
Grant-in-Aid for General Scientific Research (C)
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| Allocation Type | Single-year Grants |
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| Research Field |
Fluid engineering
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| Research Institution | EHIME UNIVERSITY |
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Principal Investigator |
AYUKAWA Kyozo EHIME UNIV., Faculty of Engng.Professor, 工学部, 教授 (30036230)
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| Co-Investigator(Kenkyū-buntansha) |
KAWAHARA Genta EHIME UNIV., Faculty of Engng.Associate Professor, 工学部, 助教授 (50214672)
OCHI Junji EHIME UNIV., Faculty of Engng.Professor, 工学部, 教授 (00036245)
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| Project Period (FY) |
1994 – 1995
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| Project Status |
Completed (Fiscal Year 1995)
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| Budget Amount *help |
¥2,000,000 (Direct Cost: ¥2,000,000)
Fiscal Year 1995: ¥600,000 (Direct Cost: ¥600,000)
Fiscal Year 1994: ¥1,400,000 (Direct Cost: ¥1,400,000)
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| Keywords | Flow around a rectangular cylinder / Fluctuating frequency in a wake / Control / Critical shape / Discrete vortex method |
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| Research Abstract |
Numerical simulation by discrete vortex method was carried out on the alternative control between wholly separated flow and periodically reattached flow, triggered off by suction at a leading edge of a rectangular cylinder near the critical shape in a uniform flow. Experiments were executed after preparing rectangular cylinders with the suction slot at the leading edge connected to a suction device in which suction speed and operating time were controllable, based on the results of the numerical simulation. The main results obtained through the simulation and the experiments are the following.
1.In the flow around a cylinder with the critical shape, fluctuation in wholly separated flow appeared in the flow around a cylinder with small side-to-height ratio are superposed on periodically reattached flow appeared in the one with large side-to-height ratio. They appear intermittently in the experiment, while supperposed wave form appears in the simulation.
2.In the numerical simulation, the
… More
flow was transferred to the periodically reattached flow by a single suction which had 0.4-0.7 times speed in the incident flow and 1/30 of fluctuating period in the wholly separated flow for the operating time, and the transferred flow returned to the critical flow after a while. The suction width with a half of the height of cylinder was suitable to the transition. This control was possible in the range of side-height ratio between 3.6 and 4.0 at which the critical shape was realized in the numerical simulation.
3.In the experiment, the critical shape was realized at 2.7 of side-height ratio at low Reynolds number and 2.3 at high Reynolds number. The results were similar qualitatively to those of the numerical simulation, but, quantitatively, some differences appeared such as the transition occurred at 0.7-1.0 times of the suction speed higher and for 0.1-0.4 times fluctuating period in the wholly separated flow of operating time longer than the numerical results, and the suitable width for the suction control was below 0.2 times the height.
4.We have some problems to be investigated such as the differences above-mentioned and the retarded transition occurred at a few periods after the suction. Less
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