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带电胶体颗粒在水溶液中的近壁面热泳分析

王伟豪 周懿 赵玉刚 边坤 杨水金

王伟豪, 周懿, 赵玉刚, 等. 带电胶体颗粒在水溶液中的近壁面热泳分析[J]. 航空动力学报, 2026, 41(1):20240079 doi: 10.13224/j.cnki.jasp.20240079
引用本文: 王伟豪, 周懿, 赵玉刚, 等. 带电胶体颗粒在水溶液中的近壁面热泳分析[J]. 航空动力学报, 2026, 41(1):20240079 doi: 10.13224/j.cnki.jasp.20240079
WANG Weihao, ZHOU Yi, ZHAO Yugang, et al. Near-wall thermophoresis analysis of charged colloidal particle in aqueous media[J]. Journal of Aerospace Power, 2026, 41(1):20240079 doi: 10.13224/j.cnki.jasp.20240079
Citation: WANG Weihao, ZHOU Yi, ZHAO Yugang, et al. Near-wall thermophoresis analysis of charged colloidal particle in aqueous media[J]. Journal of Aerospace Power, 2026, 41(1):20240079 doi: 10.13224/j.cnki.jasp.20240079

带电胶体颗粒在水溶液中的近壁面热泳分析

doi: 10.13224/j.cnki.jasp.20240079
基金项目: 国家自然科学基金(51806157)
详细信息
    作者简介:

    王伟豪(1998-),男,硕士,主要从事通用航空新型动力技术研究

    通讯作者:

    周懿(1987-),女,副教授,博士,主要从事通用航空新型动力技术研究。E-mail:yzhou96@nuaa.edu.cn

  • 中图分类号: V237

Near-wall thermophoresis analysis of charged colloidal particle in aqueous media

  • 摘要:

    针对水溶液中带电胶体颗粒的近壁面热泳,基于颗粒运动参考系建立了数值模拟方法,并结合微流体技术搭建了实验验证平台,研究了不同双电层相对厚度时流体动力干扰对近壁面热泳的影响。结果表明:当颗粒向壁面移动时,存在一个拐点位置:在接近拐点位置时,远场流体流动方向与颗粒热泳相反且生成一对涡流,从而产生较强的流体动力干扰,导致颗粒的热泳系数加剧降低;当颗粒越过拐点位置,远场涡流区域扩大并压缩颗粒附近的反向涡流,从而产生强烈的流体动力干扰,导致热泳系数急剧下降。因此,该拐点位置代表了流体动力干扰对近壁面热泳的影响范围,且与双电层相对厚度有关:当双电层相对颗粒半径较厚时,流体动力干扰对近壁面热泳的影响范围可达颗粒半径的几百倍;而当双电层相对颗粒半径较薄时,影响范围则缩至接近颗粒直径量级的距离。系统研究流体动力干扰对近壁面热泳的影响,为应用于空间飞行器和电子器件散热的纳米流体强化传热提供理论指导和实验支持。

     

  • 图 1  带电胶体颗粒的近壁面热泳数值模型示意图

    Figure 1.  Schematic diagram of the numerical model for thermophoresis of charged colloidal particles near the wall surface

    图 2  距离壁面远时颗粒热泳系数的数值仿真结果与Rasuli等[17]分析解的比较图

    Figure 2.  Numerical simulation results of particle thermophoretic coefficients at a distance from the wall in comparison with the analytical solution of Rasuli, et al.[17]

    图 3  近壁面热泳实验系统示意图

    Figure 3.  Schematic of the near-wall thermophoretic experimental system

    图 4  当$ {\kappa _0}a = 0.01 $时,采用不同参考系求解的颗粒附近的无量纲轴向速度$ {u^*} $分布情况

    Figure 4.  Distribution of the dimensionless axial velocity $ {u^*} $ around the particle in two reference frames when $ {\kappa _0}a = 0.01 $

    图 5  $ {\kappa _0}a = 0.1 $时,不同颗粒-壁面之间的距离时无量纲轴向速度$ {u^*} $分布情况

    Figure 5.  Distribution of the dimensionless axial velocity $ {u^*} $ when $ {\kappa _0}a = 0.1 $ for different particle-wall distances

    图 6  $ {\kappa _0}a = 1 $时,不同颗粒-壁面之间的距离时无量纲轴向速度$ {u^*} $分布情况

    Figure 6.  Distribution of the dimensionless axial velocity $ {u^*} $ when $ {\kappa _0}a = 1 $ for different particle-wall distances

    图 7  $ {\kappa _0}a = 10 $时,不同颗粒-壁面之间的距离时无量纲轴向速度$ {u^*} $分布情况

    Figure 7.  Distribution of the dimensionless axial velocity $ {u^*} $ when $ {\kappa _0}a = 10 $ for different particle-wall distances

    图 8  热泳系数$ {D_{\mathrm{t}}} $随颗粒-壁面之间的距离与颗粒半径的比值${h^*}$的变化曲线

    Figure 8.  Variation of the thermophoretic coefficient $ {D_{\mathrm{t}}} $ with the ratio of the particle-wall distance to the particle radius ${h^*}$

    图 9  热泳系数比值$ \beta $的数值解与实验结果随颗粒-壁面之间的距离与颗粒半径之比${h^*}$的变化

    Figure 9.  Variations of numerical and experimental thermophoretic coefficients $ \beta $ with the ratio ${h^*}$ of the particle-wall distance to the particle radius

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出版历程
  • 收稿日期:  2024-02-05
  • 网络出版日期:  2025-10-14

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