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Reducing the micro-structural scales enlarges the threshold pressure of a wetting transition.
The critical pressure necessary for a wetting transition is introduced.
This process requires that both interior phases contact the membrane, and proceeds through a wetting transition in which the contact angle between the dextran-rich aqueous phase droplet and the membrane increases.
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The microstructures indicate a reversible wetting transition between 1460 °C and 1500 °C.
The non-wetting to wetting transition in this system may be explained by formation of an oxygen-rich interphase at the liquid Al-sapphire interface.
As a result the temperature of TJ wetting transition should be lower than that of GB wetting transition TwGB.
Exaggerated grain growth was found close to the wetting transition and is explained by a temperature dependent anisotropy of the grain boundary mobility in conjunction with a high mobility of wetted grain boundaries.
This is because the wetting transition at the low-angle grain boundary is associated with the low value of the solid/liquid interfacial energy.
The grain boundary wetting transition occurs at the misorientation θ≈0.19b/RF, where b and RF are the Burgers vector of dislocation and the Frank's radius, respectively.
Ellipsometry monitoring of film thickness is intended to follow total towards pseudo-partial wetting transition, allowing to reconstruct the effective interface potential of the system, acting like the electrostatic counterpart to the mechanical Surface Force Apparatus.
The current work is dedicated to elucidating the underlying mechanisms of stability and wetting transition of underwater superhydrophobicity, providing novel strategies for durable and robust design, and introducing the applications in drag reduction and cavitation control.
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