化工学报 ›› 2024, Vol. 75 ›› Issue (6): 2180-2189.DOI: 10.11949/0438-1157.20240210
收稿日期:
2024-02-27
修回日期:
2024-03-20
出版日期:
2024-06-25
发布日期:
2024-07-03
通讯作者:
朱春英
作者简介:
赵赫(1999—),女,硕士研究生,zhzhaohezh@tju.edu.cn
基金资助:
He ZHAO(), Yingjie FEI, Chunying ZHU(), Taotao FU, Youguang MA
Received:
2024-02-27
Revised:
2024-03-20
Online:
2024-06-25
Published:
2024-07-03
Contact:
Chunying ZHU
摘要:
采用高速摄像机研究了微通道内高黏流体中纳米颗粒稳定的气泡在流动过程中的形态及其对下游对称Y型分岔口处气泡破裂的影响。在直通道内运动气泡呈现出弹状、哑铃状和手榴弹状3种形态,气泡的形态主要受分散相流率影响。Y型分岔口处气泡的破裂流型主要为部分阻塞破裂,吸附有纳米颗粒的气泡的破裂周期较常规气泡更大,其破裂周期之差ΔTb随毛细管数Ca变化呈现出3种不同的规律:当Ca > 0.042时,ΔTb为正且与Ca呈正相关;当Ca < 0.042时,存在ΔTb为正且与Ca呈负相关和ΔTb为负且与Ca呈正相关两种情况。此外,变形气泡在Y型分岔口处呈现非对称破裂行为,其破裂的非对称性与气泡的变形程度相关,当Ca大于临界毛细管数CaCr时气泡尾部直径减小的速度加快,从而加剧气泡的变形,气泡破裂的非对称性显著增大。研究表明,吸附纳米颗粒的气泡的CaCr值与无颗粒体系中气泡相同,但吸附有纳米颗粒的手榴弹状气泡的形变程度更大,破裂的非对称性也更明显。
中图分类号:
赵赫, 费滢洁, 朱春英, 付涛涛, 马友光. 高黏体系中纳米颗粒稳定气泡的形变及破裂行为[J]. 化工学报, 2024, 75(6): 2180-2189.
He ZHAO, Yingjie FEI, Chunying ZHU, Taotao FU, Youguang MA. Deformation and breakup behavior of nanoparticle-stabilized bubbles in high-viscosity systems[J]. CIESC Journal, 2024, 75(6): 2180-2189.
图4 纳米流体中气泡形态流型(数据点为纳米流体体系,点划线表示无颗粒流体中弹状气泡转变为哑铃状气泡的转变线,虚线表示无颗粒流体中哑铃状气泡转变为手榴弹状气泡的转变线)
Fig.4 Flow pattern diagram of bubble shape in nanofluid (data for nanofluid system, dot-dash line is transition line from slug bubbles to dumbbell bubbles in particle-free fluid, dash line is transition line from dumbbell bubbles to grenade bubbles in particle-free fluid)
图7 分散相流量对气泡头尾部曲率的影响(Qc= 1.8 ml·min-1)菱形—无颗粒流体体系;三角形—纳米流体体系;实心符号—弹状气泡;空心符号—哑铃状气泡;半实心符号—手榴弹状气泡
Fig.7 Effect of dispersed phase flow rate on curvatures of bubble head and tail (Qc = 1.8 ml·min-1)rhombus—particle-free fluid system; triangle—nanofluid system; solid symbols—slug bubbles; hollow symbols—dumbbell bubbles; semi-solid symbols—grenade bubbles
图11 Y型分岔口处气泡破裂过程中最小颈部宽度随时间的演化(Qc = 1.0 ml·min-1,Qd = 1.0 ml·min-1)
Fig.11 Evolution of minimum neck width with time for breakup of bubble in microfluidic Y-junction (Qc = 1.0 ml·min-1, Qd = 1.0 ml·min-1)
图12 Y型分岔口处气泡破裂过程中最小颈部宽度的减薄速率随时间的演化(Qc = 1.0 ml·min-1,Qd = 1.0 ml·min-1)
Fig.12 Evolution of thinning rate of minimum neck width with time for breakup of bubble in microfluidic Y-junction (Qc = 1.0 ml·min-1, Qd = 1.0 ml·min-1)
图13 颈部突然细化阶段两类气泡颈部曲线的对比(Qc = 1.0 ml·min-1,Qd = 1.0 ml·min-1)
Fig.13 Comparison of neck curves of two types of bubble during sudden thinning stage of the neck (Qc = 1.0 ml·min-1, Qd = 1.0 ml·min-1)
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