The Howard P. Isermann Department of Chemical and Biological Engineering, Rensselaer Polytechnic Institute, Troy, NY 12180, USA.
NASA Glenn Research Center, Cleveland, OH 44135, USA.
J Colloid Interface Sci. 2017 Feb 15;488:48-60. doi: 10.1016/j.jcis.2016.10.082. Epub 2016 Oct 28.
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.
理解三相接触线区域相变的热质传递动力学是提高相变过程效率的关键步骤。当使用流体混合物时,相变变得特别复杂。在本文中,无芯热管在国际空间站(ISS)上运行,以研究戊烷/异己烷混合物的接触线动力学。不同的界面区域被识别、比较和研究。我们使用高分辨率(50×)的干涉图像,计算了热管边缘接触线区域液-气界面的曲率梯度。我们发现,随着热流密度的增大和戊烷浓度的降低,蒸发区的曲率梯度增大。混合物情况下的曲率梯度大于纯戊烷情况下的曲率梯度。随着戊烷浓度的降低,两种情况之间的差异增大。我们的数据表明,蒸发段内的曲率梯度分布分为两个区域,两个区域的边界对应于最大内部局部热流密度处的厚液“中心液滴”区域。我们发现,在中心液滴和开始冷凝的平坦表面上的曲率梯度比在角落弯月面的梯度小一个数量级,这表明在角落处的流体流动驱动力要大得多。