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Surface partially wettable

Immersional wetting (fig. 5.8c) takes place if the solid is completely wet, that is, it is the result of spreading for S > 0 during the entire process, as in case (a). It is a less general phenomenon than adhesional wetting. It is noted that forced immersion of only partially wettable objects in a liquid leads in practice to the entrainment of air bubbles on the surface. [Pg.576]

Fig. 2 Contact angle versus wettability of a substrate surface. When angle 0 is > 90°, liquid will not wet the surface when angle 0 is <90°, liquid will wet surface partially when angle 0 = 0°, complete spreading wetting of the surface by the liquid. Spreading occurs only if 5 >0. Spreading coefficient S = 7sv (7lv + 7sl) S = solid, L = liquid, A = air. where 7sa = surface energy of the substrate (e.g., polymer surfaces), 7la = surface tension of the liquid and 7sl = interfacial tension... Fig. 2 Contact angle versus wettability of a substrate surface. When angle 0 is > 90°, liquid will not wet the surface when angle 0 is <90°, liquid will wet surface partially when angle 0 = 0°, complete spreading wetting of the surface by the liquid. Spreading occurs only if 5 >0. Spreading coefficient S = 7sv (7lv + 7sl) S = solid, L = liquid, A = air. where 7sa = surface energy of the substrate (e.g., polymer surfaces), 7la = surface tension of the liquid and 7sl = interfacial tension...
Monolayers of nanoparticles at liquid-fluid interfaces have attracted considerable attention over several decades [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17]. Among others, the examinations focused on thin-layer preparation [10, 18, 19, 20, 21, 22, 23], emulsion stabilisation [15, 24] and particle characterisations [25, 26, 27]. The Stober silica (synthesised by controlled hydrolysis of tetraethylorthosilicate in ethanol in the presence of ammonia and water) [28] has many advantageous properties for model investigations. The nearly spherical particles show a narrow size distribution and are compact above a certain particle size (around 20 nm diameter) [29]. The particles, on the one hand, show partial wettability and, on the other hand, form a weakly cohesive two-dimensional dispersion at the water-air interface [10, 14]. All that makes them suitable to determine the total repulsive interparticle energies in a film balance by measuring the effective surface tension of the monoparticulate layer [30, 31, 32, 33, 34, 35, 36]. [Pg.54]

We have previously discussed antibiotic-loaded cements produced by mixing the desired antibiotic with the PMMA cement. In this way, antibiotic elution and absorption are almost completely related to a surface phenomenon. Elution rates are dictated by several factors such as the porosity of the cement, surface area, wettability of the polymer, and the type and amount of antibiotic [1]. Increasing the porosity of the cement also increases drug elution [ 154]. A study by van de Belt et al. [83] showed that the initial release of gentamicin from an acrylic polymer matrix is partially a surface phenomenon, whereas the total amount released depends on bulk porosity. Therefore, a combination of surface roughness and porosity could improve the release kinetics of... [Pg.400]

Figure 6.1 schematically depicts the three interactions between a liquid droplet and a surface. These three interactions are actually governed by the movement of the contact line. When the liquid first wets the surface, the contact line advances outward, and the first information one seeks is wettability. The adjectives to describe the surface are wettable and non-wettable. As for the liquid, it will either wet or partially wet the surface or repel from it. As discussed in Chap. 5, wettability is measured by the advancing angle Oa- Once the liquid partially wets the surface, a static sessile drop is formed. There exist two interactions between the sessile drop and the surface. In the vertical direction, it is the adhesion and it is measured by the receding angle 0r. The only motion for the contact line is receding, and an interface (liquid-solid) is eliminated when the liquid droplet is detached from the surface. [Pg.125]

It is necessary to make additional comments on a-fihns and P-films in the case of partial wetting. If we increase the vapor pressure over partially wettable surfaces from p = 0 to the saturation pressure, p then we can observe the formation of only a-films on the solid substrate. The thickness of these films changes correspondingly (according to Equation 2.3 and Figure 2. 3) from zero at p = 0 to to = 70 A [1]. However, P-fihns cannot be obtained in the course of the adsorption process they can be obtained only by decreasing the thickness of very thick films down to the equilibrium thickness of the P-film. This is why a-films are referred to as adsorption films (because they can be obtained in the course of adsorption), and P-fihns are referred to as wetting films. [Pg.39]

Sec. Ill is concerned with the description of models with directional associative forces, introduced by Wertheim. Singlet and pair theories for these models are presented. However, the main part of this section describes the density functional methodology and shows its application in the studies of adsorption of associating fluids on partially permeable walls. In addition, the application of the density functional method in investigations of wettability of associating fluids on solid surfaces and of capillary condensation in slit-like pores is presented. [Pg.171]

The structure of the surface may be modified in other ways to enhance its reactivity and wettability. Frequently, the effect is partial oxidation, with the formation of C—OH and C=0 groups with polypropylene, especially, rather powerful methods of treatment may be necessary, and sometimes they are employed in combination with priming. Some typical surface treatments are as follows. [Pg.213]

The above distinction between non-reactive and reactive systems does not take into account the possible effect on reactivity and wettability of the furnace atmosphere. The concentration of dissolved oxygen in the liquid close to the S/L/V triple line will lie between two limits. The first of these is that for congruent dissolution of the oxide. This can be calculated using equations (6.8) by assuming that local equilibrium is established between the liquid metal and the oxide at the interface. This limit will be identified as Xq where the superscript I denotes its relevance to the interface. The second limit, Xq(Po2) at the liquid surface, is determined by equilibration with the furnace atmosphere in which the oxygen partial pressure is Pq2 (see Figure 6.3). Note that even if Xq and Xq can be calculated, it is impossible in practice to calculate the actual value of XQ at the... [Pg.202]

Sheets of PVC were subjected to argon plasma immersion ion implantation over various exposure times (from 900 to 10,800 s) and the effect of exposure time on the composition, roughness and wettability of the PVC sheets investigated. It was found that the wettability of samples increased with surface treatment and that the hydrophobic character of samples treated for shorter periods recovered either partially or completely. Samples exposed for the longest time remained highly hydrophilic. 21 refs. BRAZIL... [Pg.50]

While the focus of this overview has to this point been on API physical properties that are directly affected by milling (particle size and, hence, surface area), it is important to note that other API properties may be affected by milling. For example, milling is known to induce loss of crystallinity, through compressive or impact force and/or exposure to elevated temperatures. This is typically undesirable, as amorphous solids are usually less chemically and physically stable than crystalline solids. It is expected that much of the amorphous content is localized at the particles surfaces, so while the overall amorphous content may be low, its impact on particle-particle interactions in formulation can be significant. ° Milled compounds that are partially amorphous or that have different surface energies can have different wettability or different flow properties compared with unmilled API. In some cases, these differences are caused by recrystallization of amorphous material upon storage.P ... [Pg.2349]

The lipophilic character of the sorbent increases from RP-2 to RP-18, but it is also determined by the surface density of hydrophobic residues. Consequently, silicas are reacted to a different degree, either totally (100%) or partially (i.e., 50% of the reactive silanol groups) in order to obtain materials of various hy-drophobidty and wettability. [Pg.1638]

Chemical heterogeneity of a surface is an important property affecting adhesion, adsorption, wettability, biocompatibility, printability and lubrication behavior of a surface. It seriously affects gas and liquid adsorption capacity of a substrate and also the extent of a catalysis reaction. As an example, the partial oxidation of carbon black surfaces has an important, influence on their adsorptive behavior. In a chemically heterogeneous catalyst, the composition and the chemical (valence) state of the surface atoms or molecules are very important, and such a catalyst may only have the power to catalyze a specific chemical reaction if the heterogeneity of its surface structure can be controlled and reproduced during the synthesis. Thus in many instances, it is necessary to determine the chemical... [Pg.7]

Changing the wettability of the liquid can also be used to decrease the capillary forces. Creating a water-repellent surface is a means to reach this goal. Two kinds of bonds, Si-H and Si-F, make the silica surface hydrophobic or partially hydrophobic. Precursors bearing these special functional groups can be found in the literature [20,21]. [Pg.274]

Another mechanism proposed by some authors for the enhanced hydrophobicity evokes a closure of large micropores in cell walls [43]. Indeed, change in crystallinity of cellulose or conformational reorganization of polymeric components of wood could lead to more perfectly aligned bonds which may no longer be separable by intrusion of water. This would explain why water drops are not absorbed in wood for certain experimental conditions as seen in wettability with water measurements. Blantocas et al. [44] and Ramos et al. [45] observed partial closure of surface pores in wood following ion irradiation. For low ion energies, ion bombard-... [Pg.55]


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