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Liquid-solid interactions strength

The parameter Sij determines the interaction strength between particles i and j. By choosing a different parameterisation for interactions between liquid particles and liquid and solid ones, the wetting behaviour can be simulated. Kondo et al. derived by energy considerations that the liquid-solid interaction strength sis depends on the pure liquid one su and the contact angle 0 [27]... [Pg.100]

The boundary condition is controlled by the extent to which the liquid feels a spatial corrugation in the surface energy of the solid. This depends on a number of interfacial parameters, including the strength of the liquid-liquid and liquid-solid interactions, the commensurability of the substrate and the liquid densities, characteristic sizes, and also the roughness of the interface. In order to quantify the slippage effect, the slip length. [Pg.20]

The attraction between solid primary particles is also parameterised using this approach. The solid-solid interaction strength is then set as a distinct fraction of the liquid-liquid one. The method of pairwise forces bears some peculiarities like a remaining net force on a flat surface. Nonetheless, as can be seen from Fig. 3.6, the method as has been used in our code relaxes to the correct static contact angle. Furthermore, it is easy to implement and proves to be robust.Please check if the sentence " It is sufficient that the force x2026 " is ok as edited.Just one shght modification added. [Pg.101]

Fig. 3.14 Final morphologies after complete drying at different feed parameters variation of solid-solid interaction strengths between 0.3, 0.7, and 1.0 times the liquid-liquid one and threshold values for crust stabilisation of 0, 5 and 10% liquid content... Fig. 3.14 Final morphologies after complete drying at different feed parameters variation of solid-solid interaction strengths between 0.3, 0.7, and 1.0 times the liquid-liquid one and threshold values for crust stabilisation of 0, 5 and 10% liquid content...
Most of the aforementioned methods use gas-phase feedstock, including CVD via the VLS mechanism in the presence of metal catalysts, evaporation at high temperatures without the use of metal catalysts, or laser vaporization in the presence of metal catalysts. Solution-liquid-solid methods have been explored in the presence of metal catalysts and under supercritical conditions. These two mechanisms can result in either tip or root growth, meaning that the catalysts can be either suspended in space at the tips of the growing nanowires, or anchored at the surface of the substrate, depending on the strength of interactions between the nanoparticles and the substrate. [Pg.155]

Therefore, in liquid-solid chromatographic systems selectivity in a separation is determined by the mobile phase solvent strength and interaction with the adsorbent. The general selectivity triangle... [Pg.149]

Figure 3.4 (Left) Phase diagram for purely hard sphere interaction potentiaf which shows only fluid (F) and crystalhne (C) phases. (Middle) A short-range (relative to particle size) interaction is added to the hard sphere potential. Then a dilute gas (G) phase can appear, as well as a metastahle hquid-hquid coexistence (L + L). (Right) The attractive interaction is long range and a complete phase diagram occurs, with gas, liquid, and crystalline solid phases. The triple hne (TL) temperature increases with increasing attractive interaction strength. Figure 3.4 (Left) Phase diagram for purely hard sphere interaction potentiaf which shows only fluid (F) and crystalhne (C) phases. (Middle) A short-range (relative to particle size) interaction is added to the hard sphere potential. Then a dilute gas (G) phase can appear, as well as a metastahle hquid-hquid coexistence (L + L). (Right) The attractive interaction is long range and a complete phase diagram occurs, with gas, liquid, and crystalline solid phases. The triple hne (TL) temperature increases with increasing attractive interaction strength.

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See also in sourсe #XX -- [ Pg.116 ]




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