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首页> 外文期刊>Chemical Engineering Science >Deformation and breakup of stretching bridges of Newtonian and shear-thinning liquids:comparison of one-and two-dimensionalmodels
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Deformation and breakup of stretching bridges of Newtonian and shear-thinning liquids:comparison of one-and two-dimensionalmodels

机译:牛顿流体和剪切稀化液体的拉伸桥的变形和破裂:一维模型和二维模型的比较

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摘要

Deformation and breakup of bridges of Newtonian and non-Newtonian fluids held captive between two disks that are separated from one another at a constant speed are studied computationally. When the liquid bridge is at the incipience of breakup, a thin liquid thread connects two large volumes of fluid that are pendant from and sessile on the top and bottom disks. High viscosity and elasticity are known from experiments to lead to formation of long threads: these are precursors of satellite droplets which are usually unwanted in applications such as ink-jet printing. To investigate the role of shear-thinning in suppressing long threads and to separate the effect of elasticity from shear-thinning, the rheology of non-Newtonian fluids is described here by a Carreau model which simply accounts for shear-thinning behavior. When the dynamics is axially symmetric with respect to the common axis of the bridge and the disks, the physics is described by a spatially two-dimensional (2-D) theory. In addition to this fully 2-D theory, a one-dimensional (1-D) theory based on the slender-jet approximation is also developed here. Both the 2-D and l-D problems are solved by a method of lines employing the finite element method for spatial discretization and an adaptive finite difference technique for time integration. The computational results show that the limiting bridge length Ld at breakup increases with increasing stretching speed U for both Newtonian and shear-thinning fluids. However, in the case of high-viscosity bridges, as compared to a Newtonian fluid with viscosity equal to the zero shear-rate viscosity of a shear-thinning fluid, the rate at which Ld of a shear-thinning fluid varies with U becomes less pronounced as U increases. Furthermore, in the case of low-viscosity bridges, the axial location along the thread at which the bridge breaks switches from the vicinity of the bottom of the bridge to its top and then back to its bottom again as U is increased. This switch in the breakup location has important implications in determining the fate of satellite droplets if any are formed. It is also shown that both the shape of the bridge and that of the liquid thread are profoundly affected by shear-thinning behavior. l-D models have of course been previously used but often without direct comparison to experimental measurements or predictions made with exact 2-D models. It is shown here for the first time that 1-D models are remarkably accurate at low stretching speeds but fail at high stretching speeds. Furthermore, it is demonstrated that as the bridges thin, the dynamics in the vicinity of the location where the bridge radius is smallest follow scaling laws recently developed by others who have analyzed the local behavior of the governing equations close to pinch-off.
机译:通过计算研究了以恒定速度相互分离的两个盘之间俘获的牛顿流体和非牛顿流体的桥梁的变形和破裂。当液桥刚开始破裂时,细的液线连接两个大体积的流体,这些流体悬垂在顶盘和底盘上,并固定在顶盘和底盘上。从实验中知道,高粘度和高弹性会导致形成长线:这些是卫星液滴的前体,通常在诸如喷墨印刷等应用中是不需要的。为了研究剪切稀化在抑制长螺纹中的作用并将弹性与剪切稀化分开的作用,此处用Carreau模型描述了非牛顿流体的流变学,该模型简单地解释了剪切稀化行为。当动力学相对于桥和圆盘的公共轴轴向对称时,通过空间二维(2-D)理论描述物理学。除了这种完全二维的理论,这里还发展了基于细长射流近似的一维(1-D)理论。通过采用有限元方法进行空间离散化和采用自适应有限差分技术进行时间积分的线法可以解决二维和二维问题。计算结果表明,牛顿流体和剪切稀化流体的破裂极限桥长度Ld随拉伸速度U的增加而增加。但是,在高粘度桥的情况下,与粘度等于剪切稀化流体的零剪切速率粘度的牛顿流体相比,剪切稀化流体的Ld随U变化的速率变小。随着U的增加而明显变大。此外,在低粘度桥的情况下,随着U的增加,沿着桥断裂处的螺纹的轴向位置从桥的底部附近切换到其顶部,然后再次回到其底部。分解位置的这种转换对于确定卫星液滴的形成有重要意义。还表明,桥的形状和液线的形状都受到剪切稀化行为的深刻影响。当然,以前曾使用过l-D模型,但通常没有与使用精确2-D模型进行的实验测量或预测进行直接比较。此处首次显示一维模型在低拉伸速度下非常精确,但在高拉伸速度下失败。此外,已经证明,随着桥梁的变薄,桥梁半径最小的位置附近的动力学遵循其他人最近开发的比例定律,这些人分析了控制方程的局部行为接近于夹断。

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