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Interfacial tension measurement of immiscible liq uids using a capillary tube

机译:使用毛细管测量不混溶液体的界面张力

摘要

The interfacial tension of immiscible liquids is an important thermophysical property that is useful in the behavior of liquids both in microgravity (Martinez et al. (1987) and Karri and Mathur (1988)) and in enhanced oil recovery processes under normal gravity (Slattery (1974)). Many techniques are available for its measurement, such as the ring method, drop weight method, spinning drop method, and capillary height method (Adamson (1960) and Miller and Neogi (1985)). Karri and Mathur mention that many of the techniques use equations that contain a density difference term and are inappropriate for equal density liquids. They reported a new method that is suitable for both equal and unequal density liquids. In their method, a capillary tube forms one of the legs of a U-tube. The interfacial tension is related to the heights of the liquids in the cups of the U-tube above the interface in the capillary. Our interest in this area arose from a need to measure small interfacial tension (around 1 mN/m) for a vegetable oil/silicon oil system that was used in a thermocapillary drop migration experiment (Rashidnia and Balasubramaniam (1991)). In our attempts to duplicate the method proposed by Karri and Mathur, we found it quite difficult to anchor the interface inside the capillary tube; small differences of the liquid heights in the cups drove the interface out of the capillary. We present an alternative method using a capillary tube to measure the interfacial tensions of liquids of equal or unequal density. The method is based on the combined capillary rises of both liquids in the tube.
机译:不混溶液体的界面张力是重要的热物理性质,可用于液体在微重力下的行为(Martinez等(1987)和Karri和Mathur(1988))以及在正常重力下增强油采收率的过程(Slattery( 1974))。许多技术可用于其测量,例如环法,液滴重量法,纺丝液滴法和毛细管高度法(Adamson(1960)以及Miller和Neogi(1985))。 Karri和Mathur提到,许多技术使用的方程式包含密度差项,不适用于等密度液体。他们报告了一种适用于等密度和不等密度液体的新方法。在他们的方法中,毛细管形成了U型管的支腿之一。界面张力与毛细管中界面上方的U型管杯中液体的高度有关。我们对该领域的兴趣来自对用于热毛细管液滴迁移实验的植物油/硅油系统的小界面张力(约1 mN / m)的测量(Rashidnia和Balasubramaniam(1991))。在尝试复制Karri和Mathur提出的方法时,我们发现很难将界面固定在毛细管内。杯中液体高度的微小差异使界面脱离了毛细管。我们提出了一种使用毛细管来测量密度相等或不相等的液体的界面张力的替代方法。该方法基于管中两种液体的总毛细管上升。

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