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Solutes at the Surface of Water

Up to this point the surfaces between pure water and its vapor (or air), or another liquid, or a solid substrate have been dealt with. The situation at the free surface of an aqueous solution is also relevant in the present context. The behaviour of simple ions at the surface is dealt with first, and that of non-electrolytes and of surface active agents, ionic or non-ionic, is dealt with in the following sections. [Pg.154]


Electrode and Nafion film Platinum disk electrode (area = 0.28 cm2) was fabricated as previously described (27). A solution of Nafion (EW = 1100) 5% w/v in a mixture of lower aliphatic alcohols and 10% water was obtained from Aldrich and diluted with methanol to give a stock solution of 0.35% w/v. Films of Nafion-glucose oxidase were formed by syringing aliquot (20 pi) of the mixed solution (86.7 pi of Nafion stock solution and 13.3 pi of glucose oxidase solution) at the surface of the platinum electrode. The solvents were left to evaporate at room temperature for at least 30 min. The extra amount of GOD was... [Pg.38]

Surface films of proteins. Although most proteins are soluble in water they are usually sufficiently adsorbed to leave the interior of a solution almost completely for the surfaoe, provided this is large enough. Also, if a protein is placed in a suitable manner at the surface of water, it will often spread out to a thin film, which is of the order one amino-acid in thickness not only is the protein arranged in a monomolecular layer on the surface, but the complex protein molecules are themselves unfolded so that every amino-acid has its own place on the surface. Hence proteins can be studied by methods appropriate for insoluble films. [Pg.87]

Few experiments allow one to bridge gas-phase electron transfer mechanism to liquid (or condensed)-phase electron transfer reactions. The major problem is to model the so-called solvent coordinates in the gas phase. Of course, clusters seems to be the ideal medium to build solvent effects in a stepwise manner. However, clusters are much colder than liquids, with the consequence that only a limited number of isomers are explored, as compared with the room temperature configurations involved in liquid processes. Discrepancies are observed in the case of cluster solvation of ionic molecules in clusters Nal remains at the surface of water clusters whereas it dissolves in bulk water [275]. Clusters thus do not allow one to explore in a single step all the aspects of a liquid-phase electron-transfer reaction. Their main advantage arises from this limitation since they allow one to study separate aspects of the solution processes. [Pg.3051]

As mentioned above, the hydrophilic head group may be unionised [e.g., alcohols or poly(ethylene oxide) (PEO) alkane or alkyl phenol compounds], weakly ionised (e.g., carboxylic acids), or strongly ionised (e.g., sulphates, sulphonates, and quaternary ammonium salts). The adsorption of these different surfactants at the A/W and O/W interfaces depends on the nature of the head group. With nonionic surfactants, repulsion between the head groups is small and these surfactants are usually strongly adsorbed at the surface of water from very dilute solutions. Nonionic surfactants have much lower cmc values when compared to ionic surfactants with the same alkyl chain length typically, the cmc is in the region of... [Pg.59]

Adsorption of organic solutes at the surface of suspended particles, that is, the mineral water interface, can be also characterized by specific coordinalive... [Pg.300]

In Chapter 4, Section III, attention was drawn to the Breuer-Robb (53) reactivity series of uncharged water-soluble polymers with anionic surfactants the reactivity followed the sequence PVA < PEO < MeC < PVAc < PPO PVP. Reactivity seemed to increase with increasing hydrophobic nature, and hence surface activity (19), of the polymer. An important implication is that those polymers that are reactive form mixed films at the surface of water when mixed with surfactants. Note that even though Jones (54), the pioneer of the surface tension method to assess interaction between polymer and surfactant in aqueous solution, utilized such measurements as an indicator of interaction in solution, he does not seem to have drawn any inferences of mixed film formation at the air/water interface—or its implications—at least in his early work. [Pg.212]

When dezincification occurs in service the brass dissolves anodically and this reaction is electrochemically balanced by the reduction of dissolved oxygen present in the water at the surface of the brass. Both the copper and zinc constituents of the brass dissolve, but the copper is not stable in solution at the potential of dezincifying brass and is rapidly reduced back to metallic copper. Once the attack becomes established, therefore, two cathodic sites exist —the first at the surface of the metal, at which dissolved oxygen is reduced, and a second situated close to the advancing front of the anodic attack where the copper ions produced during the anodic reaction are reduced to form the porous mass of copper which is characteristic of dezincification. The second cathodic reaction can only be sufficient to balance electrochemically the anodic dissolution of the copper of the brass, and without the support of the reduction of oxygen on the outer face (which balances dissolution of the zinc) the attack cannot continue. [Pg.189]

In the case of liquid/liquid interfaces we have the experiments of W. C. McC. Lewis (1908), who examined the relations at the surface of separation between an aqueous solution and paraffin oil or mercury. If o-, a are the surface tensions between paraffin oil and pure water and the solution, respectively, it was found that cr < [Pg.439]

FIGURE 8.15 The events that take place at the interface of a solid ionic solute and a solvent (water). When the ions at the surface of the solid become hydrated, they move off into the solution. [Pg.441]

Fig. 22—Contact angle and film thickness of FDTE SAMs on the DLC surfaces as a function of the immersing time in a 10 mM FDTE solution at the temperature of 60°C (a) contact angle value and film thickness, (b) water contact angle of the FDTS SAM with an immersing time of 12 h. Fig. 22—Contact angle and film thickness of FDTE SAMs on the DLC surfaces as a function of the immersing time in a 10 mM FDTE solution at the temperature of 60°C (a) contact angle value and film thickness, (b) water contact angle of the FDTS SAM with an immersing time of 12 h.
MEEKC is a CE mode similar to MEKC, based on the partitioning of compounds between an aqueous and a microemulsion phase. The buffer solution consists of an aqueous solution containing nanometer-sized oil droplets as a pseudo-stationary phase. The most widely used microemulsion is made up of heptane as a water-immiscible solvent, SDS as a surfactant and 1-butanol as a cosurfactant. Surfactants and cosurfactants act as stabilizers at the surface of the droplet. [Pg.349]

Aluminum Citrate. Aluminum citrate can be used as a crosslinker for many polymers the gels are made of low concentrations of polymer and aluminum citrate in water. This crosslinker provides a valuable tool, in particular, for in-depth blockage of high-permeability regions of rock in heterogeneous reservoirs. The formulations can be mixed as a homogeneous solution at the surface. [Pg.116]

The basic assumption for a mass transport limited model is that diffusion of water vapor thorugh air provides the major resistance to moisture sorption on hygroscopic materials. The boundary conditions for the mass transport limited sorption model are that at the surface of the condensed film the partial pressure of water is given by the vapor pressure above a saturated solution of the salt (Ps) and at the edge of the diffusion boundary layer the vapor pressure is experimentally fixed to be Pc. The problem involves setting up a mass balance and solving the differential equation according to the boundary conditions (see Fig. 10). [Pg.715]

The boundary conditions for the system are (1) that at the surface of the hygroscopic material the partial pressure of water is determined by that of the saturated salt solution (Ps) and (2) that at a characteristic distance from the surface (8) the partial pressure of water vapor is given by the chamber pressure (Pc). [Pg.716]


See other pages where Solutes at the Surface of Water is mentioned: [Pg.154]    [Pg.155]    [Pg.157]    [Pg.159]    [Pg.161]    [Pg.154]    [Pg.155]    [Pg.157]    [Pg.159]    [Pg.161]    [Pg.284]    [Pg.147]    [Pg.147]    [Pg.541]    [Pg.137]    [Pg.494]    [Pg.541]    [Pg.512]    [Pg.65]    [Pg.224]    [Pg.44]    [Pg.235]    [Pg.78]    [Pg.18]    [Pg.181]    [Pg.699]    [Pg.418]    [Pg.115]    [Pg.646]    [Pg.495]    [Pg.454]    [Pg.495]    [Pg.219]    [Pg.561]    [Pg.392]    [Pg.263]    [Pg.275]    [Pg.646]    [Pg.443]    [Pg.234]    [Pg.147]   


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Solute surface

Solutes water

Solution, surface

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