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A Lattice Boltzmann-Immersed Boundary method to simulate the fluid interaction with moving and slender flexible objects

机译:一种格子Boltzmann浸入边界方法,用于模拟流体与移动和细长柔性物体的相互作用

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A numerical approach based on the Lattice Boltzmann and Immersed Boundary methods is proposed to tackle the problem of the interaction of moving and/or deformable slender solids with an incompressible fluid flow. The method makes use of a Cartesian uniform lattice that encompasses both the fluid and the solid domains. The deforming/moving elements are tracked through a series of Lagrangian markers that are embedded in the computational domain. Differently from classical projection methods applied to advance in time the incompressible Navier-Stokes equations, the baseline Lattice Boltzmann fluid solver is free from pressure corrector step, which is known to affect the accuracy of the boundary conditions. Also, in contrast to other immersed boundary methods proposed in the literature, the proposed algorithm does not require the introduction of any empirical parameter. In the case of rigid bodies, the position of the markers delimiting the surface of an object is updated by tracking both the position of the centre of mass of the object and its rotation using Newton's laws and the conservation of angular momentum. The dynamics of a flexible slender structure is determined as a function of the forces exerted by the fluid, its flexural rigidity and the tension necessary to enforce the filament inextensibility. For both rigid and deformable bodies, the instantaneous no-slip and impermeability conditions on the solid boundary are imposed via external and localised body forces which are consistently introduced into the Lattice Boltzmann equation. The validation test-cases for rigid bodies include the case of an impulsively started plate and the sedimentation of particles under gravity in a fluid initially at rest. For the case of deformable slender structures we consider the beating of both a single filament and a pair filaments induced by the interaction with an incoming uniformly streaming flow. © 2014 Elsevier Inc.
机译:提出了一种基于格子玻尔兹曼和浸入边界方法的数值方法,以解决运动和/或可变形的细长固体与不可压缩的流体相互作用的问题。该方法利用了同时包含流体域和固体域的笛卡尔均匀网格。通过嵌入在计算域中的一系列拉格朗日标记来跟踪变形/移动元素。与用于及时推广不可压缩的Navier-Stokes方程的经典投影方法不同,基线Lattice Boltzmann流体求解器没有压力校正器步骤,已知该步骤会影响边界条件的精度。而且,与文献中提出的其他浸入式边界方法相比,提出的算法不需要引入任何经验参数。在刚体的情况下,通过使用牛顿定律跟踪物体质心的位置及其旋转以及角动量守恒来更新界定物体表面的标记的位置。柔性细长结构的动力学取决于流体所施加的力,其弯曲刚度和强制细丝不可伸长性所需的张力。对于刚体和可变形体,固体边界上的瞬时防滑和不渗透性条件都是通过始终被引入Lattice Boltzmann方程的外力和局部力来施加的。刚体的验证测试用例包括脉冲启动的板和最初处于静止状态的流体在重力作用下的沉降情况。对于可变形的细长结构,我们考虑了单根细丝和一对细丝的跳动,它们是由与流入的均匀流动相互作用引起的。 ©2014爱思唯尔公司。

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