Experimental study of local scour around subsea caissons in steady currents

Abstract Local scour of sediments around subsea caisson structures was investigated experimentally by carrying out flume tests. The horizontal shape of the caissons is rectangular and the incident directions of the flow were 0°, 45° and 90°, with 0° representing flow parallel to the long boundary of the caisson and 90° representing flow parallel to the short boundary of the caisson. The study was focused on the low caissons whose vertical dimensions were equal to or less than their horizontal dimensions. It was found from the test results that the horseshoe vortex played a less important role compared with the velocity amplification at the sharp corners of the caisson if its height is smaller than its horizontal dimension. As the incident angle of flow is either 0° or 90°, scour started at the two upstream corners of the caisson, while scour at the centre of the upstream boundary did not start until the scour pits at the side corners extended there. This was also true for the case with 45° incident angle of the flow. The development of the scour depth was fitted according the exponential function and the hyperbolic function. It was found that the hyperbolic function fits the experimental data better than the exponential function because its correlation factor is larger.

[1]  Y Mao,et al.  THE INTERACTION BETWEEN A PIPELINE AND AN ERODIBLE BED , 1987 .

[2]  Ming Zhao,et al.  Numerical Modeling of Local Scour Below a Piggyback Pipeline in Currents , 2008 .

[3]  Marian Muste,et al.  Similitude of Large-Scale Turbulence in Experiments on Local Scour at Cylinders , 2006 .

[4]  Fangjun Li,et al.  Numerical Model for Local Scour under Offshore Pipelines , 1999 .

[5]  Dongfang Liang,et al.  Numerical modeling of flow and scour below a pipeline in currents: Part II. Scour simulation , 2005 .

[6]  B. Sumer,et al.  The mechanics of scour in the marine environment , 2002 .

[7]  R. Soulsby,et al.  Threshold of Sediment Motion in Coastal Environments , 1997 .

[8]  Jean-Louis Briaud,et al.  SRICOS: Prediction of Scour Rate in Cohesive Soils at Bridge Piers , 1999 .

[9]  Jørgen Fredsøe,et al.  TIME SCALE OF SCOUR AROUND A VERTICAL PILE , 1992 .

[10]  Subhasish Dey,et al.  Characteristics of Horseshoe Vortex in Developing Scour Holes at Piers , 2007 .

[11]  R. Soulsby Dynamics of marine sands , 1997 .

[12]  Ming Zhao,et al.  Experimental and numerical investigation of local scour around a submerged vertical circular cylinder in steady currents , 2010 .

[13]  Shuming Yan,et al.  Steady current induced seabed scour around a vibrating pipeline , 2006 .

[14]  Fangjun Li,et al.  Prediction of Lee-Wake Scouring of Pipelines in Currents , 2001 .

[15]  Ming Zhao,et al.  Numerical investigation of local scour below a vibrating pipeline under steady currents , 2010 .

[16]  Bruce W. Melville,et al.  THE PHYSICS OF LOCAL SCOUR AT BRIDGE PIERS , 2008 .

[17]  B. Melville,et al.  Scale Effect in Pier-Scour Experiments , 1998 .

[18]  B. Brørs Numerical Modeling of Flow and Scour at Pipelines , 1999 .

[19]  C. Baker The position of points of maximum and minimum shear stress upstream of cylinders mounted normal to flat plates , 1985 .

[20]  Lin Lu,et al.  Numerical simulation of the equilibrium profile of local scour around submarine pipelines based on renormalized group turbulence model , 2005 .

[21]  H. W. Shen,et al.  Local Scour Around Cylindrical Piers , 1977 .