Zholob S A, Makievski A V, Miller R, Fainerman V B
Physicochemical Centre, Donetsk Medical University, 16 Ilych Avenue, Donetsk 83003, Ukraine.
Adv Colloid Interface Sci. 2007 Oct 31;134-135:322-9. doi: 10.1016/j.cis.2007.04.011. Epub 2007 May 1.
The standard technique for measuring surface or interfacial tension by drop profile analysis requires two main steps: (i) acquisition of drop/bubble images and determination of the profile coordinates via edge detection techniques; (ii) fitting of the theoretical drop/bubble profile to the experimental coordinates using the interfacial tension gamma as adjustable parameter. As to edge detection technique, usually the position of the maximum grey level gradient is assumed to be the drop edge. In order to increase the accuracy of edge detection the procedure of fitting a normal distribution function to the experimental grey level gradients yields accurate results when the drop edge is located into the distribution centre. Conventional algorithms use the arc length along the drop profile as independent variable and fit in a vertical, horizontal or normal direction to the experimental shape coordinates, requiring that the coordinates have to be interpolated between experimental points. For small drops having an almost spherical shape, this technique leads to rather large errors. To avoid this interpolation problem a transformation of the Gauss-Laplace equation into polar coordinates can provide higher accuracy. For this, the angle of rotation is used as independent variable and the origin of the coordinate system is located exactly between the drop apex and the capillary tip at which the drop or bubble is formed.
(i)采集液滴/气泡图像,并通过边缘检测技术确定轮廓坐标;(ii)使用界面张力γ作为可调参数,将理论液滴/气泡轮廓拟合到实验坐标上。关于边缘检测技术,通常假定最大灰度梯度的位置为液滴边缘。为了提高边缘检测的准确性,当液滴边缘位于分布中心时,将正态分布函数拟合到实验灰度梯度的过程会产生准确的结果。传统算法使用沿液滴轮廓的弧长作为自变量,并在垂直、水平或法线方向上拟合实验形状坐标,这要求坐标必须在实验点之间进行插值。对于几乎呈球形的小液滴,这种技术会导致相当大的误差。为了避免这种插值问题,将高斯 - 拉普拉斯方程转换为极坐标可以提供更高的精度。为此,使用旋转角度作为自变量,并且坐标系的原点恰好位于形成液滴或气泡的液滴顶点和毛细管尖端之间。