Experimental study of the heated contact line region for a pure fluid and binary fluid mixture in microgravity

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• 作者：Thao T.T. Nguyen^a ; ^{nguyen.thaoche@gmail.com} ; Akshay Kundan^a ; ^{akshaykundan@gmail.com} ; Peter C. Wayner Jr.^a ; ^{wayner@rpi.edu} ; Joel L. Plawsky^a ; ^{plawsky@rpi.edu} ; David F. Chao^b ; ^{david.f.chao@nasa.gov} ; Ronald J. Sicker^b ; ^{ronald.j.sicker@nasa.gov}
• 关键词：Contact line region ; Ideal liquid mixture ; Concentration ; Heat pipe
• 刊名：Journal of Colloid and Interface Science
• 出版年：2017
• 出版时间：15 February 2017
• 年：2017
• 卷：488
• 期：Complete
• 页码：48-60
• 全文大小：3537 K
• 卷排序：488

文摘

Understanding the dynamics of phase change heat and mass transfer in the three-phase contact line region is a critical step toward improving the efficiency of phase change processes. Phase change becomes especially complicated when a fluid mixture is used. In this paper, a wickless heat pipe was operated on the International Space Station (ISS) to study the contact line dynamics of a pentane/isohexane mixture. Different interfacial regions were identified, compared, and studied. Using high resolution (50×), interference images, we calculated the curvature gradient of the liquid-vapor interface at the contact line region along the edges of the heat pipe. We found that the curvature gradient in the evaporation region increases with increasing heat flux magnitude and decreasing pentane concentration. The curvature gradient for the mixture case is larger than for the pure pentane case. The difference between the two cases increases as pentane concentration decreases. Our data showed that the curvature gradient profile within the evaporation section is separated into two regions with the boundary between the two corresponding to the location of a thick, liquid, “central drop” region at the point of maximum internal local heat flux. We found that the curvature gradients at the central drop and on the flat surfaces where condensation begins are one order of magnitude smaller than the gradients in the corner meniscus indicating the driving forces for fluid flow are much larger in the corners.