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Non-linearities and Coupling Effects on Floating Breakwaters Eigenvalues

机译:非线性和浮动防护者特征值的耦合效应

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We have seen, the consequences of non-linearities and coupling effects on floating breakwaters eigenvalues and take a prominent part in the design of floating breakwaters anchored on piles. For some exposed sites, the greatest problem is no longer set in terms of extreme loads but in terms of stiffness and of natural periods. So, we can draw four concrete conclusions from this analysis: For floating breakwaters linked on piles with linear stiffness, limitation of motions and anchorage loads is assured by setting all piles bending eigen-periods smallest than half of modal period of sea state spectrum and typically at most of the order of 1.0 to 1.5 s. RAO plotted on Fig. 1 shows that this usual approach is inadequate as early as anchorage stiffness is nonlinear. If equivalent linear damping verify alpha~2 > alpha~2 (1 - alpha~2)~2 > |mu|, or better 4alpha~4 > 4alpha~4 (1 - 2alpha~2) > |mu|, RAO is broken in two parts and low frequency amplification concerns only periods greater than 5 or 10 times eigenperiods. We must try to obtain a good enough linearity of anchorage stiffness, in order to eliminate the three risks of eigenperiod sliding, superharmonic resonances and combined resonances. This objective can induce us to increase the flexural rigidity of the pile. If the depth of water or the thickness of soft soil is too important, it can be more convenient to fill up piles with concrete than to increase wrongly the steel thickness. We must try to obtain a sufficient viscous damping of hull, may be alpha > 0.15 or 0.20, in order to restrict the motions amplitudes of floating breakwater, in particular for the sway, roll and yaw degrees of freedom. It must be convenient to eliminate bilge radius and maybe to have recourse to bilge keels. When the modal period or the significant height of the sea state is too large, typically greatest than respectively 4.0 s and 1.0 m, it must be convenient to renounce to use classical breakwater pontoons and to adopt any special feature as, for example, a floating semi submersible wave attenuator (ASB) [7].
机译:我们已经看到了非线性和耦合效应对浮动防护者特征值的后果,并在堆积在桩上的浮动防波堤设计中突出部分。对于一些暴露的网站,最大的问题是不再在极端载荷方面设置的,而是在僵硬和自然时期。因此,我们可以从该分析中汲取四个具体结论:对于在具有线性刚度的桩上连接的浮动防波堤,通过将所有桩弯曲的特征期 - 平于海区频谱的一半的均桩和通常的堆积,可以确保动作和锚固载荷的限制。大部分1.0至1.5秒的订单。 Rao绘制在图1中。图1显示,随着锚固刚度是非线性的,这种通常的方法是不充分的。如果等效的线性阻尼验证α〜2>α〜2(1 - α〜2)〜2> |或更好的4Alpha〜4> 4> 4(1 - 2 - 2Alpha〜2)> |,Rao是破碎的在两部分中,低频放大仅涉及大于5或10倍的特征百分之部。我们必须尝试获得足够的锚定刚度线性,以消除特征普通滑动,超高臂共振和组合共振的三种风险。该目标可以诱导我们增加桩的抗弯刚度。如果水的深度或软土的厚度太重要,可以更方便地填充混凝土而不是错误地增加钢厚度。我们必须尝试获得足够的羊毛的粘性阻尼,可以是alpha> 0.15或0.20,以限制浮动防波堤的动作幅度,特别是用于摇摆,卷和横摆程度的自由度。消除舱底半径必须方便,也许可以追索到舱底龙骨。当模态周期或海水的显着高度太大时,通常比分别为4.0秒和1.0米,更加放弃使用经典防波堤,并采用任何特殊功能,例如浮动半潜水波衰减器(ASB)[7]。

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