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Matrix particles

Hqq are the average number, the activity of the matrix particles, and the Hamiltonian of the matrix system, respectively. The grand potential of this system is... [Pg.300]

Motivated by a puzzling shape of the coexistence line, Kierlik et al. [27] have investigated the model with Lennard-Jones attractive forces between fluid particles as well as matrix particles and have shown that the mean spherical approximation (MSA) for the ROZ equations provides a qualitatively similar behavior to the MFA for adsorption isotherms. It has been shown, however, that the optimized random phase (ORPA) approximation (the MSA represents a particular case of this theory), if supplemented by the contribution of the second and third virial coefficients, yields a peculiar coexistence curve. It exhibits much more similarity to trends observed in... [Pg.306]

However, as follows from the results presented in Fig. 1(b), the behavior of the PMF for the case of adsorbed dispersion in the matrix at Pm< m — 0.386 contains interesting features in addition to those shown in Fig. 1(a). We observe that the PMF is modulated by the presence of solvent species and in addition is modulated by the presence of matrix particles. The structural repulsive barrier appears, due to matrix particles. An additional weak attractive minimum exists at separations corresponding to matrix-separated colloids. It is interesting that the effects of solvent modulation of the PMF in the adsorbed dispersion are seen for matrix separated colloids. The matrix particles are larger than colloids adsorption of solvent species on the surface of a matrix particle is stronger than on the surface of a colloid. Therefore, the solvent modulating effects of the PMF result from colloids separated by a matrix particle covered by a single layer of solvent species. [Pg.311]

The effects of confinement due to matrix species on the PMF between colloids is very well seen in Fig. 1(c). At a small matrix density, only the solvent effects contribute to the formation of the PMF. At a higher matrix density, the solvent preserves its role in modulating the PMF however, there appears another scale. The PMF also becomes modulated by matrix species additional repulsive maxima and attractive minima develop, reflecting configurations of colloids separated by one or two matrix particles or by a matrix particle covered by the solvent layer. It seems very difficult to simulate models of this sort. However, previous experience accumulated in the studies of bulk dispersions and validity of the PY closure results gives us confidence that the results presented are at least qualitatively correct. [Pg.311]

Let us proceed with the description of the results from theory and simulation. First, consider the case of a narrow barrier, w = 0.5, and discuss the pair distribution functions (pdfs) of fluid species with respect to a matrix particle, gfm r). This pdf has been a main focus of previous statistical mechanical investigations of simple fluids in contact with an individual permeable barrier via integral equations and density functional methodology [49-52]. [Pg.314]

Principles and Characteristics Supercritical fluid extraction uses the principles of traditional LSE. Recently SFE has become a much studied means of analytical sample preparation, particularly for the removal of analytes of interest from solid matrices prior to chromatography. SFE has also been evaluated for its potential for extraction of in-polymer additives. In SFE three interrelated factors, solubility, diffusion and matrix, influence recovery. For successful extraction, the solute must be sufficiently soluble in the SCF. The timescale for diffusion/transport depends on the shape and dimensions of the matrix particles. Mass transfer from the polymer surface to the SCF extractant is very fast because of the high diffusivity in SCFs and the layer of stagnant SCF around the solid particles is very thin. Therefore, the rate-limiting step in SFE is either... [Pg.85]

HPLC offers superior resolution due to the reduction in bead particle size. The diffusional distance inside the matrix particles is minimized, resulting in sharper peaks than those obtained when low-pressure systems are employed. [Pg.156]

Figure 25.8 Conceptual view of a saturated porous medium with colloids. The black dots represent the contaminant that is dissolved, sorbed on soil matrix particles, or sorbed on colloids. The colloids themselves can sorb on the soil matrix. Adapted from Corape ioglu and Jiang (1993). Figure 25.8 Conceptual view of a saturated porous medium with colloids. The black dots represent the contaminant that is dissolved, sorbed on soil matrix particles, or sorbed on colloids. The colloids themselves can sorb on the soil matrix. Adapted from Corape ioglu and Jiang (1993).
One important aspect of method development in SFE is that the extractability of analytes from sample matrices is strongly dependent upon the nature or type of the sample matrix. The efficiency of the extraction of a discrete set of analytes needs to be optimized for that set of analytes from a standard matrix and also optimized for the extractability of those specific analytes from a particular sample matrix. However, the optimum set of parameters for both of these cases may be distinctly different. This is due to the analytes, depending on the nature of the sample matrix, having an affinity for the physical outside surface of the matrix or actually being present within the sample matrix particles. This affinity results in either the predominance of a solubility mechanism, a diffusion type mechanism or a physical adsorption type mechanism. Therefore, the optimum extraction conditions will vary if the sample of interest is a polymer, soil or vegetable matrix. [Pg.355]

For the fluidized bed process the bed expansion as a consequence of an increase in linear flow rate has to be considered. In a simplified picture diffusive transport takes place in a boundary layer around the matrix particle which is frequently renewed, this frequency being dependent on velocity and voidage, as long as convective effects, e.g. the movement of particles are neglected. Rowe [74] has included these considerations into his correlation for kf in fluidized beds, which is applicable for a wide range of Reynolds numbers, including the laminar flow regime where fluidized bed adsorption of proteins takes place (Eq. 19). The exponent m is set to 1 for a liquid fluidized bed, a represents the proportionality factor in the correlation for packed beds (Eq. 18) and is assumed as 1.45. [Pg.215]

In other applications the pattern of evolution of styrene, butadiene and acrylonitrile as a function of temperature has provided a unique way for classifying different types of ABS. The loss of the antioxidant butylated hydroxytoluene (BHT) was also detected by MS preceding EVA copolymer degradation [165] BHT was identified at a concentration level of 20 ppm. Lehrle and co-workers [52] have described a successful controlled release system for the stabilisation of rubber by encapsulating efficient but rather mobile antioxidants to prevent loss from the host polymer. The performance of the controlled-release of the antioxidant BHT from alginate matrix particles was studied by means of DSC, TG and TG-MS. Polyisoprene rubber is more resistant to oxidation when protected in this way than by the equivalent concentration of unencapsulated antioxidant. [Pg.26]

The analysis of particle size distribution required an assumption of particle shape all encapsulated particles were assumed to be ellipsoids. To verify this assumption, single particles were reconstructed in three-dimensions. The reconstructed particles were remarkably symmetrical no significant spurs or convexities were observed. In these observations of three-dimensional in situ matrix particles, no geometries inconsistent with ellipsoids were discovered. Therefore, for the analysis of particle size distribution, all particles were assumed to be ellipsoidal. [Pg.27]

The present study attempts to elucidate mechanisms for vanadium migration between a Eu3+-exchanged zeolite Y and an AAA-alumina matrix. Eu3+ was used since it can readily be tracked with various spectroscopies. Moreover, effects of different vanadium precursors on migration will be a major focus of the paper because the nature of such precursors has been reported to control zeolite-vanadium interactions (28). SEM/EDX analyses are useful tools for tracking metal migration. Spot analyses on either Y zeolite or matrix particles will be reported since these FCC components show quite different morphologies. [Pg.189]

For diffusion in amorphous polymers at temperatures above their glass point, Tg, one can assume a behavior with some analogy to a liquid. On the other hand the Stokes-Einstein Eq. (6-4) for liquids was derived under the assumption that the diffusing particle is much larger in size than the matrix particles. If we let the matrix be a... [Pg.175]

Studies on the rheology of two-phase particulate systems suggest the existence of a deformation threshold that depends on the concentration of particles in the composite. Below this threshold (—68 vol.% for spherical particles), deformation occurs primarily by the flow of the composite matrix. Particles increase the effective viscosity of the matrix by absorbing energy and by forming clusters. [Pg.153]

The morphology of the matrix on which we wish to make a SFE can have an enormous influence on the efficiency of the extraction rate. Generally a rapid and complete extraction depends upon the relative size of the matrix particles, the smaller being the better. This is due principally to the short internal distance that the solute must cover in order to attain the core of the supercritical fluid solution. Some studies have shown that the geometrical form can also have an influence on the rate and efficacity of the extraction. As in the case of an extraction solid-liquid, an increase in the porosity of the matrix will lead to an efficient and rapid extraction. [Pg.129]

Simplified mass transport steps in the SFE of an analyte from a matrix particle. (Adapted from Reference 4.)... [Pg.129]

F. 8. Rate of salt uptake from 0.02 N salt solution by thermally r nerable plum pudding resins containing the same De-Acidite G and Zeo-K.arb 226 plums, and 30% matrix by weight, as a function of the nature of matrix. Particle size 14-52 mesh, BSS, base resin to acid resin ratio 2 5. (1) ethyl cellulose (2) polysalt (3) crosslinked poly (vinyl alcohol) (4) normal De-Acidite G and Zeo-I b 226 mixed bed... [Pg.102]


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See also in sourсe #XX -- [ Pg.166 ]




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A-particle density matrices

Density matrix single-particle

Electron correlation 2-particle density matrix

Fock particle density matrices

Free particle density matrix

Hamiltonian matrix, many-particle

Interaction particles/polymer matrix

Magnetic materials particle/matrix interactions

Many-electron methods 2-particle density matrix

Matrix-assisted particle-desorption techniques

Matrix-particle interaction

One-particle density matrices

One-particle reduced density matrix

Orientation of filler particle in a matrix

Particle bombardment matrix effects

Particle distribution in matrix

Particle-hole density matrix

Particle-matrix interface

Particle/matrix adhesion

Particle/matrix debonding

Polymeric matrix particles

Properties of the One-Particle Density Matrix

Relation between particle and antiparticle matrix elements

Role of Rubber Particle Cavitation on the PA Matrix Toughening

Two-particle matrix

Two-particle reduced Hamiltonian matrices

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