DIFFERENCE-FREQUENCY WAVE LOADS ON A LARGE BODY IN MULTI-DIRECTIONAL WAVES

Abstract The second-order difference-frequency wave forces on a large three-dimensional body in multi-directional waves are computed by the boundary integral equation method and the so-called FML formulation (assisting radiation potential method). Semi-analytic solutions for a bottom-mounted vertical circular cylinder are also developed to validate the numerical method. Difference-frequency wave loads on a bottom-mounted vertical cylinder and stationary four legs of the ISSC tension-leg platform (TLP) are presented for various combinations of incident wave frequencies and headings. These force quadratic transfer functions (QTF) can directly be used in studying slowly varying wave loads in irregular short-crested seas described by a particular directional spectrum. From our numerical results, it is seen that the slowly varying wave loads are in general very sensitive to the directional spreading function of the sea, and therefore wave directionality needs to be taken into account in relevant ocean engineering applications. It is also pointed out that the uni-directionality of the sea is not necessarily a conservative assumption when the second-order effects are concerned.

[1]  Moo-Hyun Kim,et al.  The complete second-order diffraction solution for an axisymmetric body Part 1. Monochromatic incident waves , 1989, Journal of Fluid Mechanics.

[2]  P. S. Teigen The response of a TLP in short-crested waves. [Tension leg platform] , 1983 .

[3]  Moo-Hyun Kim,et al.  SLOWLY-VARYING WAVE DRIFT FORCES IN SHORT-CRESTED IRREGULAR SEAS , 1989 .

[4]  J N Newman,et al.  FIRST- AND SECOND-ORDER WAVE EFFECTS ON A SUBMERGED SPHEROID , 1991 .

[5]  Odd M. Faltinsen,et al.  Sea loads on ships and offshore structures , 1990 .

[6]  Moo-Hyun Kim,et al.  Second-order sum-frequency wave loads on large-volume structures* , 1991 .

[7]  R. Eatock Taylor,et al.  Variability of hydrodynamic load predictions for a tension leg platform , 1986 .

[8]  K L Mitchell,et al.  ADVANCES IN THE PREDICTION OF LOW FREQUENCY DRIFT BEHAVIOUR , 1988 .

[9]  D. Yue,et al.  The complete second-order diffraction solution for an axisymmetric body Part 2. Bichromatic incident waves and body motions , 1990, Journal of Fluid Mechanics.

[10]  L. E. Borgman,et al.  The wadic project: A comprehensive field evaluation of directional wave instrumentation , 1989 .

[11]  Fritz John,et al.  On the motion of floating bodies II. Simple harmonic motions , 1950 .

[12]  J. N. Newman Second-order, slowly-varying Forces on Vessels in Irregular Waves , 1974 .

[13]  A. G. Abul-Azm,et al.  SECOND-ORDER DIFFRACTION LOADS ON TRUNCATED CYLINDERS , 1988 .

[14]  R. Isaacs,et al.  Applied Mathematics , 1901, Nature.

[15]  F. John On the motion of floating bodies. I , 1949 .

[16]  J. N. Newman,et al.  THE COMPUTATION OF SECOND-ORDER WAVE LOADS , 1991 .

[17]  Bernard Molin,et al.  Second-order diffraction loads upon three-dimensional bodies , 1979 .

[18]  T. Matsui Computation of Slowly Varying Second-Order Hydrodynamic Forces on Floating Structures in Irregular Waves , 1989 .

[19]  S. M. Hung,et al.  SECOND ORDER DIFFRACTION FORCES ON A VERTICAL CYLINDER IN REGULAR WAVES , 1987 .