摘要:
由于Lagrange粒子法的本质，固壁边界条件的施加一直是光滑粒子动力学方法的难点之一。本文从固壁边界的物理原理出发，应用多层虚粒子表征固壁边界，提出了一种新型固壁边界施加模型。将虚粒子看作流体的扩展，计算中虚粒子密度保持不变，压力、速度等参数通过对流体粒子的插值获得，虚粒子有条件的参与控制方程的计算，对流体的密度/压力产生影响，通过压力梯度隐式地表征壁面与流体之间的作用强度并对流体粒子施加沿壁面法线方向的斥力作用，防止流体粒子对壁面的穿透。数值算例测试结果表明，与现有固壁边界施加方法相比，本文方法更加符合流体与固壁边界作用的物理原理，可以简单、有效地施加固壁边界条件，方便地应用于具有复杂几何边界的问题，获得稳定的流场形态、规则的粒子秩序及良好的速度、压力等参量的分布。
Abstract:
As the smoothed particle hydrodynamics (SPH) is a truly Lagrangian meshfree method, the implementation of solid boundary condition has been one of the key problems that hinder SPH from applying to lots of engineering problems. In order to treat the boundary conditions e?ciently, based on the boundary-fluid interaction principles, a new boundary treatment method is proposed. In this method, the solid boundary is represented implicitly by several layers of dummy particles along the boundary line. During the simulation, the dummy particles are treated as an extension of the fluid phase. The densities of dummy particles are kept constant, and the pressures and velocities are interpolated from the nearby fluid particles at each time step. Dummy particles can be involved in the calculation of the continuity equation conditionally and exert influences on the density/pressure field of the fluid phase. Then, for the fluid particles that approach the solid boundary, local pressure gradients are used to represent the dummy-fluid particle pair’s interaction strength and act as the boundary force term implicitly, which is tuned to be repulsive only and normal to the boundary. Thus, large pressure gradients mean strong boundary-fluid interaction strength, and the boundary force from the dummy particles should also be large enough to prevent the fluid particles from penetrating the solid boundary;and on the contrary, small pressure gradients mean weak boundary-fluid interaction strength and the boundary force becomes soft and little disturbs the flow field. Results of numerical tests demonstrate that, compared with the existing boundary treatment methods, the new method is in better accordance with the physical principles of the fluid-boundary interaction, and is able to treat arbitrary solid boundaries with limited modeling and computational costs. With the help of this new boundary treatment method, the stable flow field, well-ordered particle distribution, smooth velocity and pressure fields could be obtained. Theoretically, this new boundary treatment method could be directly used in three-dimensional multi-phase problems. Further tests are planned to be carried out; meanwhile, expanding the new boundary treatment method to rigid-fluid interaction problems is also a work in the future.
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