Adsorption at the solid–liquid interface as the source of contact angle dependence on the curvature of the three-phase line

2010 ◽  
Vol 161 (1-2) ◽  
pp. 171-180 ◽  
Author(s):  
C.A. Ward ◽  
K. Sefiane
Keyword(s):  
Contact Angle ◽  
Liquid Interface ◽  
Phase Line ◽  
Angle Dependence ◽  
Three Phase ◽  
Solid Liquid Interface ◽  
Solid Liquid

Dependence of the Contact Angle on Adsorption at the Solid-Liquid Interface

2010 ◽  
Author(s):  
C. A. Ward
Keyword(s):  
Surface Tension ◽  
Contact Angle ◽  
Pressure Range ◽  
Line Tension ◽  
Liquid Interface ◽  
Fluid Interfaces ◽  
Phase Line ◽  
Three Phase ◽  
Solid Liquid Interface ◽  
Solid Liquid

A method for determining the surface tension of solid-fluid interfaces has been proposed. For a given temperature and fluid-solid combination, these surface tensions are expressed in terms of material properties that can be determined by measuring the amount of vapor adsorbed on the solid surface as a function of xV, the ratio of the vapor-phase pressure to the saturation-vapor pressure. The thermodynamic concept of pressure is shown to be in conflict with that of continuum mechanics, but is supported experimentally. This approach leads to the prediction that the contact angle, θ, can only exist in a narrow pressure range and that in this pressure range, the solid-vapor surface tension is constant and equal to the surface tension of the liquid-vapor interface, γLV. The surface tension of the solid-liquid interface, γSL, may be expressed in terms of measurable properties, γLV and θ: γSL = γLV(1 − cosθ). The value of θ is predicted to depend on both the pressure in the liquid at the three-phase, line x3L, and the three-phase line curvature, Ccl. We examine these predictions using sessile water droplets on a polished Cu surface, maintained in a closed, constant volume, isothermal container. The value of θ is found to depend on the adsorption at the solid-liquid interface, nSL = nSL(x3L,Ccl). The predicted value of θ is compared with that measured, and found to be in close agreement, but no effect of line tension is found.

Adsorption of azacrown ethers at solid–liquid interface. Contact angle and neutron reflectivity study

2009 ◽  
Vol 256 (1) ◽  
pp. 274-279 ◽  
Author(s):  
Kamil Wojciechowski ◽  
Anna Brzozowska ◽  
Sebastien Cap ◽  
Witold Rzodkiewicz ◽  
Thomas Gutberlet
Keyword(s):  
Contact Angle ◽  
Liquid Interface ◽  
Neutron Reflectivity ◽  
Azacrown Ethers ◽  
Interface Contact ◽  
Solid Liquid Interface ◽  
Solid Liquid

scholarly journals 3D Numerical Analysis of the Asymmetric Three-Phase Line of Floating Zone for Silicon Crystal Growth

Crystals ◽  
2020 ◽  
Vol 10 (2) ◽  
pp. 121 ◽  
Author(s):  
Xue-Feng Han ◽  
Xin Liu ◽  
Satoshi Nakano ◽  
Hirofumi Harada ◽  
Yoshiji Miyamura ◽  
...  
Keyword(s):  
Heat Transfer ◽  
Silicon Crystal ◽  
Three Dimensional ◽  
Heat Transfer Fluid ◽  
Floating Zone ◽  
Phase Line ◽  
Three Phase ◽  
Em Field ◽  
Solid Liquid Interface ◽  
Solid Liquid

A numerical simulation has been carried out to study the asymmetric heat transfer, fluid flow, and three-phase line to explain the phenomenon of the spillage of the melt in floating zone (FZ) silicon growth. A three-dimensional high-frequency electromagnetic (EM) field is coupled with the heat transfer in the melt and crystal calculation domains. The current density along the three-phase line is investigated to demonstrate the inhomogeneous heating along the three-phase line. The asymmetric heating is found to affect the flow pattern and temperature distribution of the melt. The three-dimensional solid–liquid interface results show that, below the current supplies, the interface is deflected due to strong heating below the current supplies. The calculated asymmetric three-phase line shows a similar trend as the experimentally observed results. The results indicate that the re-melting and spillage phenomenon could occur below the current supplies.

Metastable Nanobubbles at the Solid–Liquid Interface Due to Contact Angle Hysteresis

Langmuir ◽  
2015 ◽  
Vol 31 (3) ◽  
pp. 982-986 ◽  
Author(s):  
Takashi Nishiyama ◽  
Yutaka Yamada ◽  
Tatsuya Ikuta ◽  
Koji Takahashi ◽  
Yasuyuki Takata
Keyword(s):  
Contact Angle ◽  
Contact Angle Hysteresis ◽  
Liquid Interface ◽  
Solid Liquid Interface ◽  
Solid Liquid

scholarly journals Polar effects at solid/liquid interfaces

1970 ◽  
Vol 48 (5) ◽  
pp. 865-866 ◽  
Author(s):  
A. C. Lowe ◽  
A. C. Riddiford
Keyword(s):  
Contact Angle ◽  
Free Energy ◽  
Unit Area ◽  
Liquid Interface ◽  
Liquid Interfaces ◽  
Advancing Contact Angle ◽  
Solid Liquid Interface ◽  
Glass Surfaces ◽  
Solid Liquid

Studies of the advancing contact angle of water upon several alkylchlorosilaned glass surfaces at 22 °C lead to the view that, at zero or very low interfacial velocities, the free energy per unit area of the solid/liquid interface is governed by both dispersive and polar forces. At higher velocities, the polar forces may be neglected.

Role of titanium on the reactive spreading of lead-free solders on alumina

2006 ◽  
Vol 21 (12) ◽  
pp. 3222-3233 ◽  
Author(s):  
Laurent Gremillard ◽  
Eduardo Saiz ◽  
Velimir R. Radmilovic ◽  
Antoni P. Tomsia
Keyword(s):  
Contact Angle ◽  
Sessile Drop ◽  
Triple Line ◽  
Contact Angles ◽  
Liquid Interface ◽  
Liquid Front ◽  
Wide Variability ◽  
Solid Liquid Interface ◽  
Lead Free Solders ◽  
Solid Liquid

The wetting of Sn3Ag-based alloys on Al2O3 has been studied using the sessile-drop configuration. Small additions of Ti decrease the contact angle of Sn3Ag alloys on alumina from 115° to 23°. Adsorption of Ti-species at the solid–liquid interface prior to reaction is the driving force for the observed decrease in contact angle, and the spreading kinetics is controlled by the kinetics of Ti dissolution into the molten alloy. The addition of Ti increases the transport rates at the solid–liquid interface, resulting in the formation of triple-line ridges that pin the liquid front and promote a wide variability in the final contact angles.

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