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首页> 外文期刊>Advances in Engineering Software >Binary collision of drops in simple shear flow at finite Reynolds numbers:Geometry and viscosity ratio effects
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Binary collision of drops in simple shear flow at finite Reynolds numbers:Geometry and viscosity ratio effects

机译:有限雷诺数下简单剪切流中液滴的二元碰撞:几何和粘度比效应

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摘要

The collision of two equal-size drops in an immiscible phase undergoing a shear flow is simulated over a range of viscosity ratios (λ) and different geometries. The full Navier-Stokes equations are solved by a finite difference/front tracking method. Based on experimental data, different cases were simulated by changing the offset, size of drops, and viscosity ratio. The distance between drop centres along the velocity gradient direction (z) was measured as a function of time. It was found that Az increases after collision and reaches a new steady-state value after separation. The values of Az, during the interaction, increases with increasing initial offset. Our results show that the time of approaching of drops at low initial offset is greater than the other cases, but the maximum deformation is the same for equal drop sizes. The deformation decreases with decreasing the size of drops. As the initial offset increases, the drops rotate more quickly and the available contact time for film drainage decreases. We found that the trajectories of drops in the approaching stage are different owing to the different initial offsets. However, after the drops come into contact, it observed that they follow the same trajectories. As A increases, the drops rotate more slowly, and the point at which the drops separate is delayed. The trajectories of drops become more symmetric with the increased λ.
机译:在一定的粘度比(λ)和不同的几何形状范围内,模拟了两个大小相等的液滴在不混溶相中经历剪切流的碰撞。完整的Navier-Stokes方程通过有限差分/前跟踪方法求解。根据实验数据,通过改变偏移量,液滴大小和粘度比来模拟不同情况。测量沿速度梯度方向(z)的墨滴中心之间的距离作为时间的函数。发现碰撞后Az增加,分离后达到新的稳态值。在交互过程中,Az的值随初始偏移的增加而增加。我们的结果表明,在低初始偏移下,液滴接近的时间比其他情况要长,但是对于相同的液滴大小,最大变形是相同的。变形随着液滴尺寸的减小而减小。随着初始偏移量的增加,墨滴旋转得更快,并且可用于排墨的接触时间减少。我们发现,由于初始偏移量的不同,液滴在接近阶段的轨迹也有所不同。但是,在液滴接触后,观察到它们遵循相同的轨迹。随着A的增加,墨滴旋转得更慢,并且墨滴分离的点被延迟。液滴的轨迹随着λ的增加而变得更加对称。

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