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Computational fluid-structure interaction simulations for wind induced vibrations in silo groups

机译:筒仓中风致振动的计算流固耦合模拟

摘要

During a storm in October 2002, wind induced ovalling vibrations were observed on several empty silos of a closely spaced group consisting of 8 by 5 silos in theport of Antwerp (Belgium). First, a thorough understanding of the fluid flow around the group is required to clarify the underlying mechanisms for the vibration. Since the configuration and orientation of the group drastically change the pressure distribution on the silos of the group, the flow regime around and within the silo group has been simulated for 7 angles of incidence between 0 and 90, leaving other parameters unchanged (e.g. spacing ratio, Reynolds number,...). The flow regime shows similarities with the flow within tube arrays (e.g. heat exchangers) and the flow around rectangular cylinders. By a ‘one way coupling’ of static (time averaged) and dynamic (fluctuating) pressure loadings on the cylinder surfaces it is examined if the excitation of ovalling vibrations in the silo group is possible. Two probable causes of observable silo vibrations in the group are observed. The first, as a result of large static wind pressures and fluctuating drag and lift coefficients, might lead to rigid body motions of the statically deformed silos. The second, due to higher dynamic pressure oscillations, can excite ovalling oscillations in the third and fourth eigenmodes at the lee side of the group, corresponding with the lowest eigenfrequencies of the silos and the visually detected vibrations in 2002. Although it is shown by this ‘one way coupling’ that ovalling vibrations can be excited in the group, more advanced ‘two way coupled’ fluid-structure interaction simulations are required to determine the underlying mechanism inducing these aeroelastic deformations.
机译:在2002年10月的一场暴风雨中,在比利时安特卫普港,在一个由8乘5的筒仓组成的紧密间隔的几个空筒仓中,观察到风引起的椭圆振动。首先,需要彻底了解围绕该组的流体,以阐明振动的潜在机制。由于该组的配置和方向极大地改变了该组筒仓上的压力分布,因此已模拟了筒仓组周围和内部的流动状态,其入射角为0至90之间的7个,其他参数不变(例如,间距比) ,雷诺数,...)。流动状态显示出与管阵列(例如,热交换器)内的流动以及矩形圆柱体周围的流动相似。通过气缸表面上静态(时间平均)和动态(波动)压力载荷的“单向耦合”,检查是否可能激发筒仓组中的椭圆振动。在该组中,观察到了两个可能的筒仓振动的可能原因。首先,由于较大的静态风压和波动的阻力系数和升力系数,可能导致静态变形筒仓的刚体运动。第二个由于较高的动态压力振荡,可以激发该组背风的第三和第四本征模态的椭圆形振荡,这对应于筒仓的本征频率最低,并且在2002年是视觉检测到的振动。可以激发椭圆形振动的“单向耦合”,需要更高级的“双向耦合”流固耦合模拟,以确定引起这些气动弹性变形的潜在机理。

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