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Identification of hydrodynamic coefficients from experiment of vortex-induced vibration of slender riser model 被引量:6
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作者 TANG GuoQiang LU Lin +3 位作者 TENG Bin PARK HanI1 SONG JiNing ZHANG JianQiao 《Science China(Technological Sciences)》 SCIE EI CAS 2011年第7期1894-1905,共12页
One of the challenges in predicting the dynamic response of deepwater risers under vortex-induced vibration (VIV) is that it runs short of believable fluid loading model. Moreover, the hydrodynamic loading is also d... One of the challenges in predicting the dynamic response of deepwater risers under vortex-induced vibration (VIV) is that it runs short of believable fluid loading model. Moreover, the hydrodynamic loading is also difficult to be measured directly in the VIV experiments without disturbing the fluid field. In the present work, by means of a finite element analysis method based on the experimental data of the response displacements, the total instantaneous distributions of hydrodynamic forces together with the hydrodynamic coefficients on the riser model with large aspect ratio (length/ddiameter) of 1750 are achieved. The steady current speeds considered in the experiments of this work are ranging from 0.15 rn/s to 0.60 m/s, giving the Reynolds Number between 2400 and 9600. The hydrodynamic coefficients are evaluated at the fundamental frequency and in the higher order frequency components for both in-line and cross-flow directions. It is found that the Root-Mean Squared hydrodynamic forces of the higher order response frequency are larger than those of the fundamental response frequency. Negative lift or drag coefficients are found in the numerical results which is equivalent to the effect of fluid damping. 展开更多
关键词 vortex-induced vibration deepwater riser hydrodynamic coefficients finite element method dynamic response
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Modelling of multi-bodies in close proximity under water waves——Fluid resonance in narrow gaps
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作者 LU Lin TENG Bin +2 位作者 CHENG Liang SUN Liang CHEN XiaoBo 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS 2011年第1期16-25,共10页
Viscous fluid model and potential flow model with and without artificial damping force(f=-μV,μthe damping coefficient and V the local averaging flow velocity)are employed in this work to investigate the phenomenon o... Viscous fluid model and potential flow model with and without artificial damping force(f=-μV,μthe damping coefficient and V the local averaging flow velocity)are employed in this work to investigate the phenomenon of fluid resonance in narrow gaps between multi-bodies in close proximity under water waves.The numerical results are compared with experimental data available in the literature.The comparison demonstrates that both the viscous fluid model and the potential flow model are able to predict the resonant frequency reasonably well.However the conventional potential flow model(without artificial damping term)significantly over-predicts the wave height in narrow gaps around the resonant frequency.In order to calibrate the appropriate damping coefficient used for the potential model and make it work as well as the viscous fluid model in predicting the resonant wave height in narrow gaps but with little computational efforts,the dependence of damping coefficientμon the body geometric dimensions is examined considering the parameters of gap width Bg,body draft D,body breadth ratio Br and body number n(n=2,3),where Br=BB/BA for the case of two bodies(Body A and Body B)with different breadths of BA and BB,respectively.It was confirmed that the damping coefficient used for the potential flow model is not sensitive to the geometric dimensions and spatial arrangement.It was found thatμ∈[0.4,0.5]may guarantee the variation of Hg/H0 with kh to be generally in good agreement with the experimental data and the results of viscous fluid model,where Hg is the excited wave height in narrow gaps under various dimensionless incident wave frequencies kh,H0 is the incident wave height,k=2π/L is the wave number and h is the water depth. 展开更多
关键词 narrow gap fluid resonance water wave viscous fluid model potential flow model finite element method boundary element method
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