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Interface forms

There is a fair amount of work reported with films at the mercury-air interface. Rice and co-workers [107] used grazing incidence x-ray diffraction to determine that a crystalline stearic acid monolayer induces order in the Hg substrate. Quinone derivatives spread at the mercury-n-hexane interface form crystalline structures governed primarily by hydrogen bonding interactions [108]. [Pg.552]

Figure 4c illustrates interfacial polymerisation encapsulation processes in which the reactant(s) that polymerise to form the capsule shell is transported exclusively from the continuous phase of the system to the dispersed phase—continuous phase interface where polymerisation occurs and a capsule shell is produced. This type of encapsulation process has been carried out at Hquid—Hquid and soHd—Hquid interfaces. An example of the Hquid—Hquid case is the spontaneous polymerisation reaction of cyanoacrylate monomers at the water—solvent interface formed by dispersing water in a continuous solvent phase (14). The poly(alkyl cyanoacrylate) produced by this spontaneous reaction encapsulates the dispersed water droplets. An example of the soHd—Hquid process is where a core material is dispersed in aqueous media that contains a water-immiscible surfactant along with a controUed amount of surfactant. A water-immiscible monomer that polymerises by free-radical polymerisation is added to the system and free-radical polymerisation localised at the core material—aqueous phase interface is initiated thereby generating a capsule sheU (15). [Pg.320]

The nature of the interface formed between very thin metallic films and substrates of various types has been studied extensively by AES, just as it has by XPS... [Pg.45]

We present here a simple experiment, conceived to test both the reptation model and the minor chain model, by Welp et al. [50] and Agrawal et al. [51-53]. Consider the HDH/DHD interface formed with two layers of polystyrene with chain architectures shown in Fig. 5. In one of the layers, the central 50% of the chain is deuterated. This constitutes a triblock copolymer of labeled and normal polystyrene, which is, denoted HDH. In the second layer, the labeling has been reversed so that the two end fractions of the chain are deuterated, denoted by DHD. At temperatures above the glass transition temperature of the polystyrene ( 100°C), the polymer chains begin to interdiffuse across the... [Pg.363]

In this section we characterize the minima of the functional (1) which are triply periodic structures. The essential features of these minima are described by the surface (r) = 0 and its properties. In 1976 Scriven [37] hypothesized that triply periodic minimal surfaces (Table 1) could be used for the description of physical interfaces appearing in ternary mixtures of water, oil, and surfactants. Twenty years later it has been discovered, on the basis of the simple model of microemulsion, that the interface formed by surfactants in the symmetric system (oil-water symmetry) is preferably the minimal surface [14,38,39]. [Pg.702]

An ordering phase transition is characterized by a loss of symmetry the ordered phase has less symmetry than the disordered one. Hence, an ordering process leads to the coexistence of different domains of the same ordered phase. An interface forms whenever two such domains contact. The thermodynamic behavior of this interface is governed by different forces. The presence of the underlying lattice and the stability of the ordered domains tend to localize the interface and to reduce its width. On the other hand, thermal fluctuations favor an interfacial wandering and an increase of the interface width. The result of this competition depends strongly on the order of the bulk phase transition. [Pg.121]

When speculating about the hypothetical structure of interfaces with minimal free energy, the diffuse interfaces formed by the properly grafted water-soluble... [Pg.137]

The most reliable methods of the preparation of stable adsorbents involve, however, a covalent attachment of the polymeric stationary phases to the solid supporting material. In addition, the more diffuse interfaces formed in this case (see Sect. 2.2) are often favourable for the separation of proteins. [Pg.148]

Phosphorus-containing surfactants are amphiphilic molecules, exhibiting the same surface-active properties as other surfactants. That means that they reduce the surface tension of water and aqueous solutions, are adsorbed at interfaces, form foam, and are able to build micelles in the bulk phase. On account of the many possibilities for alteration of molecular structure, the surface-active properties of phosphorus-containing surfactants cover a wide field of effects. Of main interest are those properties which can only be realized with difficulty or in some cases not at all by other surfactants. Often even quantitative differences are highly useful. [Pg.590]

Here, only one Interface forms as the reaction takes place initial at the surface of B". Once the AB-phase heis formed, gaseous A atoms must then diffuse through to the phase boundeuy in order for the reaction to occur. The wall of AB thus moves in two (2) dimensions instead of the three, in contTcist to the case of 4.2.2. [Pg.135]

Figure 4. The potential changes measured at the interfaces formed by the nonpolar solvent-wateiand polar solvent-wateisystems. Figure 4. The potential changes measured at the interfaces formed by the nonpolar solvent-wateiand polar solvent-wateisystems.
Smith, D. C. Cartz, L. (1973). Crystalline interface formed by polyacrylic acid and tooth enamel. Journal of Dental Research, 52, 1155. [Pg.192]

Very finely disperse solids, which are adsorbed at the liquid/liquid interfaces, forming films of particles around the disperse globules. Certain powders can very effectively stabilize against coalescence. The solid s particle size must be very small compared with the emulsion droplet size and must exhibit an appropriate angle of contact at the three-phase (oil/water/solid) boundary [141]. [Pg.269]

A binary suspension consists of equal masses of spherical particles of the same shape and density whose free falling velocities in the liquid are 1 mm/s and 2 mm/s, respectively. The system is initially well mixed and the total volumetric concentration of solids is 0.2. As sedimentation proceeds, a sharp interface forms between the clear liquid and suspension consisting only of small particles, and a second interface separates the suspension of fines from the mixed suspension. Using a suitable model for the behaviour of the system, estimate the falling rates of the two interfaces. It may be assumed that the sedimentation velocity uc in a concentrated suspension of voidage e is related to the free falling velocity u0 of the particles by ... [Pg.42]

The structure of the interface is of obvious interest to electrochemists. However, the interface forms only a small part of the two ad-... [Pg.6]

Database central point for all input and control data like optimization results with 50 tables, related queries and user interface forms. [Pg.208]

It is shown in Section 5.3.3 that, for coarse particles, the point of inflexion does not occur at a concentration which would be obtained in practice in a suspension, and therefore the particles will settle throughout at a constant rate until an interface forms between the clear liquid and the sediment when sedimentation will abruptly cease. With a highly flocculated suspension the point of inflexion may occur at a very low volumetric concentration. In these circumstances, there will be a wide range of concentrations for which the constant rate sedimentation is followed by a period of falling rate. [Pg.255]

Figure 4. HRTEM images of particles after the reduction, showing (a) the coalescence of three particles, (b) the coalescence of two crystallites with an interface formed in between and (c) the overlapping of different phases. Figure 4. HRTEM images of particles after the reduction, showing (a) the coalescence of three particles, (b) the coalescence of two crystallites with an interface formed in between and (c) the overlapping of different phases.
DOM also tends to be concentrated at boimdaries, such as the sediment-water and air-sea interfeces. The latter is also characterized by enrichments of POM, such as bacteria. Under calm conditions, the DOM and POM that collects at the air-sea interface forms a visible surfece slick or microlayer. On windy days, this organic matter can be whipped up into an emulsion that has the appearance of a very sturdy foam. DOM can also be transferred into the POM pool by adsorbing onto organic particles. [Pg.621]

Compared with the research interest in the passivation of anodes, especially materials with carbonaceous origins, there have been relatively few studies dedicated to the understanding of the interface formed between electrolytes and cathode surfaces. A... [Pg.102]

We will now deal with interfaces formed between organic and inorganic materials. The convention that will be followed is that for a generic A/B interface, A... [Pg.150]

A number of different types of such interfacial phases must be considered when dealing with bulk phases in their different physical states. Of special importance are the interfaces formed by contact of a bulk liquid with gaseous, liquid and solid phases whilst the problems connected with heterogeneous catalysis necessitate an examination of the properties of the solid-gas interface. [Pg.1]


See other pages where Interface forms is mentioned: [Pg.381]    [Pg.224]    [Pg.41]    [Pg.416]    [Pg.31]    [Pg.351]    [Pg.352]    [Pg.370]    [Pg.717]    [Pg.135]    [Pg.159]    [Pg.8]    [Pg.248]    [Pg.293]    [Pg.400]    [Pg.54]    [Pg.592]    [Pg.224]    [Pg.507]    [Pg.394]    [Pg.584]    [Pg.154]    [Pg.111]    [Pg.232]    [Pg.188]    [Pg.588]    [Pg.225]    [Pg.16]   


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