An Evaluation of Measurements of Solid/Liquid Interfacial Energies in Metallic Alloy Systems by the Groove Profile Method

2007 ◽  
Vol 38 (7) ◽  
pp. 1563-1569 ◽  
Author(s):  
H. Jones
1993 ◽  
Vol 126-128 ◽  
pp. 695-698
Author(s):  
Simeon Agathopoulos ◽  
A. Tsoga ◽  
P. Nikolopoulos

2008 ◽  
Vol 41 (17) ◽  
pp. 175302 ◽  
Author(s):  
S Akbulut ◽  
Y Ocak ◽  
N Maraşlı ◽  
K Keşlioğlu ◽  
H Kaya ◽  
...  

2007 ◽  
Vol 78 (7) ◽  
pp. 072217 ◽  
Author(s):  
C. J. Long ◽  
J. Hattrick-Simpers ◽  
M. Murakami ◽  
R. C. Srivastava ◽  
I. Takeuchi ◽  
...  

2011 ◽  
Vol 2 ◽  
pp. 145-151 ◽  
Author(s):  
Glen McHale ◽  
Michael I Newton ◽  
Neil J Shirtcliffe ◽  
Nicasio R Geraldi

In the wetting of a solid by a liquid it is often assumed that the substrate is rigid. However, for an elastic substrate the rigidity depends on the cube of its thickness and so reduces rapidly as the substrate becomes thinner as it approaches becoming a thin sheet. In such circumstances, it has been shown that the capillary forces caused by a contacting droplet of a liquid can shape the solid rather than the solid shaping the liquid. A substrate can be bent and folded as a (pinned) droplet evaporates or even instantaneously and spontaneously wrapped on contact with a droplet. When this effect is used to create three dimensional shapes from initially flat sheets, the effect is called capillary origami or droplet wrapping. In this work, we consider how the conditions for the spontaneous, capillary induced, folding of a thin ribbon substrate might be altered by a rigid surface structure that, for a rigid substrate, would be expected to create Cassie–Baxter and Wenzel effects. For smooth thin substrates, droplet wrapping can occur for all liquids, including those for which the Young’s law contact angle (defined by the interfacial tensions) is greater than 90° and which would therefore normally be considered relatively hydrophobic. However, consideration of the balance between bending and interfacial energies suggests that the tendency for droplet wrapping can be suppressed for some liquids by providing the flexible solid surface with a rigid topographic structure. In general, it is known that when a liquid interacts with such a structure it can either fully penetrate the structure (the Wenzel case) or it can bridge between the asperities of the structure (the Cassie–Baxter case). In this report, we show theoretically that droplet wrapping should occur with both types of solid–liquid contact. We also derive a condition for the transition between the Cassie–Baxter and Wenzel type droplet wrapping and relate it to the same transition condition known to apply to superhydrophobic surfaces. The results are given for both droplets being wrapped by thin ribbons and for solid grains encapsulating droplets to form liquid marbles.


2009 ◽  
Vol 487 (1-2) ◽  
pp. 103-108 ◽  
Author(s):  
Y. Kaygısız ◽  
S. Akbulut ◽  
Y. Ocak ◽  
K. Keşlioğlu ◽  
N. Maraşlı ◽  
...  

Author(s):  
Alfredo Calvimontes

In this study, the values of the interfacial energies of seven different polymer-water systems obtained by Sessile Drop Accelerometry (SDACC) are compared with the values obtained by the Young’s-equation-based Owens-Wendt method. The SDACC laboratory instrument –a combination of a drop shape analyzer with high-speed camera and a microgravity tower- and the evaluation algorithms, are designed to measure the interfacial energies as a function of the geometrical changes of a sessile droplet shape due to the effect of “switching off” gravity during the experiment. The method bases on Thermodynamics of Interfaces and differs from the conventional aproach of the two hundred-years-old Young’s equation in that it assumes a thermodynamic equilibrium between interfaces, rather than a balance of forces on a point of the solid-liquid-gas contour line. A comparison of the mathematical model that supports the SDACC method with the widely accepted Young`s equation is discussed in detail in this study.


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