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Dispersion layers

The jet-plume model only simulates vertical jets. Terrain is assumed to be flat and unobstructed. Application is limited to surface roughness mush less than the dispersing layer. User experti.se is required to ensure that the selected runtime options are self-consistent and actually reflect the physical release conditions. Documentation needs improvement there is little guidance... [Pg.351]

Routh and Russel [10] proposed a dimensionless Peclet number to gauge the balance between the two dominant processes controlling the uniformity of drying of a colloidal dispersion layer evaporation of solvent from the air interface, which serves to concentrate particles at the surface, and particle diffusion which serves to equilibrate the concentration across the depth of the layer. The Peclet number, Pe is defined for a film of initial thickness H with an evaporation rate E (units of velocity) as HE/D0, where D0 = kBT/6jT ir- the Stokes-Einstein diffusion coefficient for the particles in the colloid. Here, r is the particle radius, p is the viscosity of the continuous phase, T is the absolute temperature and kB is the Boltzmann constant. When Pe 1, evaporation dominates and particles concentrate near the surface and a skin forms, Figure 2.3.5, lower left. Conversely, when Pe l, diffusion dominates and a more uniform distribution of particles is expected, Figure 2.3.5, upper left. [Pg.97]

Fig. 74 Relative tinctorial strength of irradiated dispersion layers containing Pigment Orange 5 of different particle sizes (white reductions). Fig. 74 Relative tinctorial strength of irradiated dispersion layers containing Pigment Orange 5 of different particle sizes (white reductions).
The nodules rest as a mono-disperse layer of potato-like balls on unconsolidated pelagic sediments down to 5500 m water depth. [Pg.431]

Calculation of lengths of layers at the task of regime parameters was spent on the basis of the standard techniques of definition heat transmission in disperse layers of nozzles with drains of heat and without drains of heat, and were based on the given experiments. It is necessary to emphasize, that success of tests depends on correctness of calculation of lengths of layers of nozzles. [Pg.559]

The Important component of calculation have Aa and Ar in which processes of carry of heat in a disperse layer are considered all. [Pg.560]

As discussed in more detail in Chapter 6, the phthalocyanines are either metallized or metal free. The metal compounds can contain either two monovalent metal atoms, a divalent metal atom, or a tri- or tetravalent metal atom with one or two associated ligands. The phthalocyanines can exist in several ciystalline forms. Most studies have been made of vapor-deposited or dispersion layers. [Pg.441]

The residence time for the oil drops in the dispersion layer is 5 min and from Equation 6.15.2 Vd =Vl. Therefore, the interfacial area is... [Pg.313]

Film-coating is the formation of an adhering dispersion layer as a result of the drag force exerted by the substrate during withdrawal from a dispersion. To achieve pure fihn-coating, the capillary suction of the porous substrate must be suppressed. The thickness of the entrained dispersion layer increases with increasing withdrawal speed and increasing dispersion viscosity. The contact... [Pg.151]

In contrast, if the layer thickness is too large the viscosity will also be increased as a result of repulsion this occurs due to the much higher effective volume fraction of the dispersion compared to the core volume fraction. If the effective volume fraction of particles plus dispersant layer is calculated geometrically, it can be seen to depend on the thickness of that adsorbed layer, as illustrated in Figure 11.5. [Pg.213]

The effective volume fraction increases with a relative increase of the dispersant layer thickness. Even at 10% volume fraction, a maximum packing (< = 0.67) is soon reached, with an adsorbed layer thickness that is comparable to the particle radius. In this case, overlap of the steric layers wiU result in significant increases in viscosity. Such considerations may help to explain why solids loading can be severely Hmited, especially with small particles. In practice, soUds loading curves can be used to characterize the system, and take the form of those illustrated in Figure 11.6... [Pg.213]

Next, in two layers system consisting of diamond- dispersed layer and only matrix, effect of thickness of the diamond layer on the residual stresses was evaluated. In radial stress, the maximum compressive and tensile stresses in the diamond layer and in the interface of the layers became smaller in the thinner layer. In three layers system consisting of diamond- high, low dispersed layers (40 and 70 vol%) and matrix, influence of insertion of middle layer on the maximum stresses was compared with the two layers system. The residual stresses in each layer seems to become reduced by the insertion of middle layer. [Pg.292]

The physical interpretation of the load factors is that a liquid flow should be transported through the interface, and this transport is augmented by the density difference and decreased by the continuous phase viscosity. The liquid load factor accounts for transport of both phases through the interface, while the other two only transport the applicable dispersed phase. Flence, the liquid load factor is in line with the new separator design philosophy proposed by Polderman et al. (12, 15), while the oil and water load factors are in line with the dispersion layer theory developed by Jeelani and Flartland (16-20) (for the corresponding dispersed phase). [Pg.668]

For the past 15 years, Flartland and coworkers have developed a theory referred to here as the dispersion layer theory (20). The theory has been developed for batch tests, and has the following assumptions ... [Pg.668]


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