Surfactant-spreading and surface-compression disturbance on a thin viscous film

被引:46
|
作者
Bull, JL [1 ]
Nelson, LK
Walsh, JT
Glucksberg, MR
Schürch, S
Grotberg, JB
机构
[1] Univ Michigan, Dept Biomed Engn, Ann Arbor, MI 48109 USA
[2] Northwestern Univ, Robert R McCormick Sch Engn & Appl Sci, Dept Biomed Engn, Evanston, IL 60208 USA
[3] Univ Calgary, Dept Med Physiol, Calgary, AB T2N 4N1, Canada
[4] Univ Michigan, Dept Biomed Engn, Ann Arbor, MI 48109 USA
关键词
D O I
10.1115/1.2798049
中图分类号
Q6 [生物物理学];
学科分类号
071011 ;
摘要
Spreading of a new surfactant in the presence of a pre-existing surfactant distribution is investigated both experimentally and theoretically for a thin viscous substrate. The experiments are designed to provide a better understanding of the fundamental interfacial and fluid dynamics for spreading of surfactants instilled into the lung. Quantitative measurements of spreading rates were conducted using a fluorescent new surfactant that was excited by argon laser light as it spread on an air-glycerin interface in a petri dish. It is found that pre-existing surfactant impedes surfactant spreading. However, fluorescent microspheres used as surface markers show that pre-existing surfactant facilitates the propagation of a surface-compression disturbance, which travels aster than the leading edge of the new surfactant. The experimental results compare well with the theory developed using lubrication approximations. An effective diffusivity of the thin film system is found to be D-eff = (E*<(Gamma)over bar>)/(mu/(H) over bar), which indicates that the surface-compression disturbance propagates faster for larger background surfactant concentration, <(Gamma)over bar>, larger constant slope of the sigma*-Gamma* relation, -E*, and smaller viscous resistance, mu/<(Gamma)over bar>. Note that sigma* and Gamma* are the dimensional surface tension and concentration, respectively, mu is fluid viscosity, and (H) over bar is the unperturbed film thickness.
引用
收藏
页码:89 / 98
页数:10
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