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Simulating particle sedimentation in a flowing fluid using an immersed boundary-lattice Boltzmann method

机译:使用浸没边界晶格Boltzmann方法模拟流动流体中的颗粒沉降

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A combination of the lattice-Boltzmann and immersed-boundary methods is used to simulate the behaviour of circular particles in fluids, including their behaviour in stationary and flowing fluids. This method simulates the fluid domain with a regular Eulerian grid, and the non-grid uniform boundaries with a Lagrangian grid. The no-slip boundary condition of the fluid and particle boundaries is enforced by interpolating boundary forces. This simulation uses a direct-force method to achieve a slight deformation of solid particles. The correctness of the method is validated using simulations of the flow past an impulsive cylinder. Finally, the method is used to compare the particles' behaviour in stationary and flowing fluids. The result shows that a well-known 'drafting, kissing, and tumbling' (DKT) case occurs in the particle sedimentation in the stationary viscous fluid. In contrast, kissing occurs in the moving fluid, but no separating.
机译:格子-Boltzmann和浸没边界方法的组合用于模拟圆形颗粒在流体中的行为,包括它们在固定和流动的流体中的行为。 该方法用常规欧拉网格模拟流体域,与拉格朗日网格的非网格均匀边界。 通过内插边界力来强制流体和颗粒边界的无滑动边界条件。 该模拟使用直接力的方法来实现固体颗粒的轻微变形。 使用流过脉冲圆筒的流动仿验该方法的正确性。 最后,该方法用于比较静止和流动流体中的粒子的行为。 结果表明,众所周知的“起草,接吻和翻滚”(DKT)病例发生在静止粘性流体中的颗粒沉降中。 相比之下,在移动流体中发生接吻,但没有分离。

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