微通道内屈服应力型流体的流变特性及多相流研究进展

doi:10.11949/0438-1157.20221091

摘要/Abstract

摘要：

屈服应力型流体（YSFs）是一种典型的非牛顿流体，因其丰富的流变特性被广泛关注。屈服应力是高浓度的粒子分散系统和凝胶状物质（多相乳液、微胶囊、3D打印复杂结构、药物输送凝胶等）的基本特征。本文对微通道内简单屈服应力型流体的流动特征和流变行为，及其流变性对多相流系统的影响进行了综述，剖析了受限空间内流体流动与流体流变性，及多相流动力学和界面现象的耦合机制，并对亟需推进的研究方向进行了展望。为微通道内屈服应力型流体的数值模拟、实验研究和应用提供参考。

关键词: 微通道, 非牛顿流体, 屈服应力型流体, 气泡, 液滴

Abstract:

Yield stress-type fluids (YSFs) are typical non-Newtonian fluid that have received extensive attention due to their rich rheological properties. Yield stress is an essential feature in high concentration particle dispersion systems and gelatinous substances, such as multiphase emulsions, microencapsule, 3D printing of complex structures and drug delivery. In this paper, the flow characteristics and rheological behavior of simple yield stress fluid and the effects of rheology on multiphase flow systems are reviewed. The coupling mechanism of the fluid flow and fluid rheology, the multiphase flow dynamics, and interfacial phenomena in confined spaces are analyzed. The research directions that need to be promoted are prospected. It provides a reference for numerical simulation, experimental research and application of yield stress-based fluids in microchannels.

Key words: microchannel, non-Newtonian fluid, yield stress fluid, bubble, droplet

中图分类号:

TQ 021.1

项星宇, 王忠东, 董艳鹏, 李守川, 朱春英, 马友光, 付涛涛. 微通道内屈服应力型流体的流变特性及多相流研究进展[J]. 化工学报, 2023, 74(2): 546-558.

Xingyu XIANG, Zhongdong WANG, Yanpeng DONG, Shouchuan LI, Chunying ZHU, Youguang MA, Taotao FU. Progress on rheological properties and multiphase flow of yield stress fluids in microchannels[J]. CIESC Journal, 2023, 74(2): 546-558.

图/表 6

图1 常见的简单屈服应力型流体模型[14]

Fig.1 The most common simple yield stress fluid models [14]

图2 屈服应力型流体在微通道内的层流流动及速度分布

Fig.2 Laminar flow and velocity profile of yield stress-type fluids in microchannels

图3 乳液 A（油体积分数Φ = 75%）的速度剖面经过了滑移速度校正（虚线是H-B方程预测的速度曲线）[49]

Fig.3 The velocity profile of emulsion A (oil volume fraction Φ = 75%) was corrected for slip velocity (the dashed line is the speed curve predicted by the H-B equation)[49]

图4 被罗丹明B标记的中性卡波姆凝胶的显微图像[57]

Fig.4 Micrograph of the neutral Carbopol gel covalently labelled with Rhodamine B [57]

图5 (a)T型通道处气泡生成的界面破裂图像；(b) T型通道中气泡破裂的时空图；(c)单个气泡形成时间tb和气泡长度l演变图[80]

Fig.5 (a) Different stages of the break-up mechanism inside the T-junction；(b) Spatiotemporal diagram of the break-up dynamic for a bubble train; (c) Typical evolution of the time to form one bubble tb and bubble length l as functions of the time [80]

图6 阶梯乳化微器件中液滴群的自组织行为[94]

Fig.6 Self-organizing behavior of droplet groups in step emulsification microdevices[94]

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