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Penetration thermodynamics

The equilibrium and dynamic behaviour of mixed monolayers of soluble and insoluble amphiphiles at fluid/liquid interfaces plays an important role in various technological and biological processes, which was studied in numerous publications [139-157], However, even for very simple systems, say, gaseous mixed monolayers, the thermodynamic analysis is not trivial. For more complicated systems (the formation of two-dimensional domains) such an analysis is very cumbersome due to mathematical difficulties. [Pg.164]

The main problem in the thermodynamic theory of penetration is to determine the dependence of the adsorption of a soluble surfactant on its bulk concentration for any given (constant) adsorption of the insoluble surfactant (surface concentration), and the onset of the surface pressure jump in mixed monolayers, caused by the adsorption of a soluble surfactant in the presence of the insoluble component. There exist several main theoretical approaches to the description of the penetration thermodynamics. One is based on the Gibbs adsorption equation for multicomponent monolayers [143-146], Another approach, initially proposed by Pethica [Pg.164]


The lower the value of the more likely it is that S is positive indicating a thermodynamic tendency for the process to occur. Longitudinal wave theory has been appHed to the defoamer spreading process as in equation 5 where P is the penetration depth of a spreading droplet of initial radius R, viscosity Tj, and density p. [Pg.465]

NaCl, interact with the sulphur and vanadium oxides emitted from the combustion of technical grade hydrocarbons and die salt spray to form Na2S04 and NaV03- These conosive agents function in two modes, either the acidic mode in which for example, the sulphate has a high SO3 thermodynamic activity, of in the basic mode when the SO3 partial pressure is low in the combustion products. The mechanism of coiTosion is similar to the hot coiTosion of materials by gases widr the added effects due to the penetration of tire oxide coating by tire molten salt. [Pg.320]

In some metal components it is possible to form oxides and carbides, and in others, especially those with a relatively wide solid solubility range, to partition the impurity between the solid and the liquid metal to provide an equilibrium distribution of impurities around the circuit. Typical examples of how thermodynamic affinities affect corrosion processes are seen in the way oxygen affects the corrosion behaviour of stainless steels in sodium and lithium environments. In sodium systems oxygen has a pronounced effect on corrosion behaviour whereas in liquid lithium it appears to have less of an effect compared with other impurities such as C and Nj. According to Casteels Li can also penetrate the surface of steels, react with interstitials to form low density compounds which then deform the surface by bulging. For further details see non-metal transfer. [Pg.429]

Tethering may be a reversible or an irreversible process. Irreversible grafting is typically accomplished by chemical bonding. The number of grafted chains is controlled by the number of grafting sites and their functionality, and then ultimately by the extent of the chemical reaction. The reaction kinetics may reflect the potential barrier confronting reactive chains which try to penetrate the tethered layer. Reversible grafting is accomplished via the self-assembly of polymeric surfactants and end-functionalized polymers [59]. In this case, the surface density and all other characteristic dimensions of the structure are controlled by thermodynamic equilibrium, albeit with possible kinetic effects. In this instance, the equilibrium condition involves the penalties due to the deformation of tethered chains. [Pg.46]

CVI is a special CVD process in which the gaseous reactants penetrate (or infiltrate) a porous structure which acts as a substrate and which can be an inorganic open foam or a fibrous mat or weave. The deposition occurs on the fiber (or the foam) and the structure isgradually densified to form a composite.The chemistry and thermodynamics of CVT are essentially the same as CVD but the kinetics is different, since the reactants have to diffuse inward through the porous structure and the by-products have to diffuse out.f l Thus, maximum penetration and degree of densification are attained in the kinetically limited low-temperature regime. [Pg.129]

In contrast, thermodynamic as well as spectroscopic properties of core water in AOT-reversed micelles are similar to those of pure water. Together with electrostatic considerations, this suggests that the penetration of counterions in the micellar core is negligible and that a relatively small number of water molecules are able to reconstruct the typical extended H-bonded structure of bulk water. [Pg.482]

Ogston, AG SUpananta, P, The Thermodynamics of Interaction between Sephadex and Penetrating Solntes, Biochemical Jonmal 116, 171, 1970. [Pg.617]

The convective diffusion equations presented above have been used to model tablet dissolution in flowing fluids and the penetration of targeted macro-molecular drugs into solid tumors [5], In comparison with the nonequilibrium thermodynamics approach described below, the convective diffusion equations have the advantage of theoretical rigor. However, their mathematical complexity dictates a numerical solution in all but the simplest cases. [Pg.33]

Figure 3 A hydrophobic permeant must negotiate through a complex series of diffu-sional and thermodynamic barriers as it penetrates into a cell. The lipid and protein compositions and charge distribution of the inner and outer leaflets of the membrane lipid bilayer can play limiting roles, particularly at the tight junction. Depending upon the permeant s characteristics, it may remain within the plasma membrane or enter the cytoplasm, possibly in association with cytosolic proteins, and partition into cytoplasmic membranes. Figure 3 A hydrophobic permeant must negotiate through a complex series of diffu-sional and thermodynamic barriers as it penetrates into a cell. The lipid and protein compositions and charge distribution of the inner and outer leaflets of the membrane lipid bilayer can play limiting roles, particularly at the tight junction. Depending upon the permeant s characteristics, it may remain within the plasma membrane or enter the cytoplasm, possibly in association with cytosolic proteins, and partition into cytoplasmic membranes.
In this chapter, the subscript 1 denotes the penetrant and subscript 2, the polymer. The term penetrant refers to solvents which have sufficient thermodynamic affinity for and interaction with the polymer. It is because of this interaction that penetrant diffusion exhibits a significant concentration dependence. This orientation excludes consideration of the permeation of small gaseous molecules. [Pg.458]

Particular cases are potassium selective potentiometric sensors based on cobalt [41] and nickel [38, 42] hexacyanoferrates. As mentioned, these hexacyanoferrates possess quite satisfactory redox activity with sodium as counter-cation [18]. According to the two possible mechanisms of such redox activity (either sodium ions penetrate the lattice or charge compensation occurs due to entrapment of anions) there is no thermodynamic background for selectivity of these sensors. In these cases electroactive films seem to operate as smart materials similar to conductive polymers in electronic noses. [Pg.440]

In membrane osmometry the two compartments of an osmometer are separated by a semi-permeable membrane only solvent molecule can penetrate through the semi-permeable membrane which is closed except for capillary tubes. The polymer solute remains confined to one side of the osmometer and the activity of the solvent is different in the two compartments. Because of the thermodynamic drive towards equilibrium a difference in liquid level in the two capillaries results. [Pg.104]


See other pages where Penetration thermodynamics is mentioned: [Pg.164]    [Pg.164]    [Pg.269]    [Pg.277]    [Pg.61]    [Pg.121]    [Pg.317]    [Pg.329]    [Pg.333]    [Pg.424]    [Pg.684]    [Pg.429]    [Pg.169]    [Pg.442]    [Pg.253]    [Pg.283]    [Pg.287]    [Pg.127]    [Pg.307]    [Pg.31]    [Pg.48]    [Pg.386]    [Pg.669]    [Pg.226]    [Pg.206]    [Pg.217]    [Pg.467]    [Pg.473]    [Pg.404]    [Pg.918]    [Pg.42]    [Pg.35]    [Pg.53]    [Pg.82]    [Pg.57]   


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