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Stratified - layer

The dross from this operation contains considerable quantities of copper and lead as well as other valuable metals. Separation and recovery is economically imperative. The dross is treated to produce readily separated stratified layers of slag, speiss, matte, and lead. Two processes are primarily used. [Pg.42]

It is likely that some backmixing occurs, especially in the first reactor where fluid viscosities are relatively low. As polymerization proceeds and viscosity increases, the stratified layer condition cited above is gradually approached. [Pg.100]

Has limited applicability at sites with confined aquifers and stratified layers soil heterogeneities may limit effectiveness. [Pg.1006]

Kerkhof and Moulijn [30] suggested that a supported catalyst may be modeled as a stack of sheets of support material, with cubic crystals representing the supported particles. They used this stratified layer model, illustrated in Fig. 3.9b, to calculate the intensity ratio /P//s for electron trajectories perpendicular to the support sheets, assuming exponential attenuation of the electrons in the particles and the support. [Pg.66]

Figure 3.9 Models used in the quantitative analysis of XPS spectra of supported catalysts, a) particles on a semi-infinite support b) stratified layer model with cubic particles on sheets of support material as used by Kerkhof and Moulijn [30] c) particles with characteristic dimensions which have the same dispersion, giving nearly the same particle/support intensity ratio in XPS in the randomly oriented layer model according to Kuipers el al. [311. Figure 3.9 Models used in the quantitative analysis of XPS spectra of supported catalysts, a) particles on a semi-infinite support b) stratified layer model with cubic particles on sheets of support material as used by Kerkhof and Moulijn [30] c) particles with characteristic dimensions which have the same dispersion, giving nearly the same particle/support intensity ratio in XPS in the randomly oriented layer model according to Kuipers el al. [311.
Quantitative determination of the absolute distance from the surface to a labeled cell membrane at a cell/substrate contact region can be based on the variation of F(d) with 0.(1O6) This effort is challenging because corrections have to be made for 0-dependent reflection and transmission through four stratified layers (glass, culture medium, membrane, and cytoplasm), all with different refractive indices. For 3T3 cells, Lanni et a//1065 derived a plasma membrane/substrate spacing of 49 nm for focal contacts and 69 nm for close contacts elsewhere. They were also able to calculate an approximate refractive index for the cytoplasm of 1.358 to 1.374. [Pg.326]

Another complication in the quantitation of TIRF on cells is the effect of the membrane thickness itself on the profile of the evanescent wave. Reichert and Truskey<105) have calculated that, in theory, the thickness of the membrane should have a negligible effect on the fluorescence and that a simplified theory of three stratified layers (glass/water/cytoplasm) should be adequate. The theory approximates for simplicity that scattering plays a negligible role and that fluorescence intensity versus angle of observation and fluorescence lifetime are not functions of distance to the interface z. Experiments that... [Pg.326]

Human skin is divided into two regions the epidermis and dermis (Figure 2.1). The epidermis is composed of four stratified layers (in ascending order strata basale. [Pg.33]

In addition, plant roots invade rock cracks and speed up rock breakdown into small particles. After mountains form by the upward thrust of rock, erosion tears them down, and the resulting silt is deposited in stratified layers. This process repeats, leaving clay deposits. [Pg.153]

In addition to describing the conformation of the hydrocarbon chains for amphiphilic molecules at the A/W interface, external reflectance infrared spectroscopy is also capable of describing the orientation of the acyl chains in these monolayers as a function of the monolayer surface pressure. The analysis of the orientation distribution for an infrared dipole moment at the A/W interface proceeds based on classical electromagnetic theory of stratified layers (2). In particular, when parallel polarized radiation interacts with the A/W interface, the resultant standing electric field has contributions from both the z component of the p-polarized radiation normal to the interface, as well as the x component of the p-polarized radiation in the plane of the interface. The E field distribution for these two... [Pg.198]

As light propagates through the stratified layers, it is affected by two basic mechanisms, shown in Figure 3.2. The first mechanism concerns the transmission of the light through a film, and the second arises from reflection and refraction at an interface. An additional subscript, (0,1), has been added to denote whether the electric field exists either at the inside front surface of a film, or at the inside back surface of a film, respectively. In both cases, these interactions induce the following linear transformations ... [Pg.47]

Laminar flow is characterised by streamlines - stratified layers ... [Pg.60]

The deep-water observations with conductivity, temperature, depth (CTD) profilers performed in the Black Sea during the past two decades allowed one to distinguish the near-bottom mixed layer (NBML). In Fig. 3b, we present profiles of the potential temperature (T ), salinity (S), and potential density (ct ) of the Black Sea waters in the layer from 1500 to 2100 m obtained by averaging of 46 CTD profiles observed in 1985-1992 in different regions of the deep-sea area. In all three profiles shown in Fig. 3b, a distinct upper boundary of the NBML is traced at depths from 1750 to 1800 m. Above it, up to a depth of 1700 m, one finds a layer with increased vertical gradients of T , S, and a with a thickness about 100 m it separates NBML from the deep stratified layer. [Pg.224]

Before assessing how a chemical moves in the environment, the relevant media, or compartments, must be defined. The environment can be considered to be composed of four broad compartments—air, water, soil, and biota (including plants and animals)—as shown in Fig. 6.6. Various approaches to modeling the environment have been described.14-16 The primary difference in these approaches is the level of spatial and component detail included in each of the compartments. For example, the most simplistic model considers air as a lumped compartment. A more advanced model considers air as composed of air and aerosols, composed of species such as sodium chloride, nitric and sulfuric acids, soil, and particles released anthropogenically.17 A yet more complex model considers air as composed of air in stratified layers, with different temperatures and accessibility to the earth s surface, and aerosols segmented into different size classes.16 As the model complexity increases, its resolution and the data demands also increase. Andren et al.16 report that the simplest of models with lumped air, water, and soil compartments is suitable for... [Pg.226]

In slow-moving water bodies such as lakes and ocean basins, suspended solids falling to the bottom produce a well-stratified layer of bottom sediment. This is stratified in terms of age with the oldest sediment at the bottom (where when suitably pressurised in can form rock) and the... [Pg.332]

Hi) UV/visible spectroscopy. In comparison with IR and fluorescence spectroscopic techniques, UV/visible spectroscopy is only occasionally used for characterizing monolayers. It can be applied if the monolayer contains molecules with 7i-electron systems of which the electron transitions are in the UV/visible part of the spectrum. By measuring polarized transmission spectra or reflection-absorption spectra at different angles of incidence, the second order parameter of the absorption transition dipole moment in the chromophoric groups caii be determined. In the case of a reflection-absorption configuration, the underlying theory is similar to that of IRRAS, i.e. based upon calculation of the reflection and transmission coefficients in a stratified-layer system and extended to account for the anisotropic nature of monolayers ). [Pg.368]

This result suggests that the dissipation of kinetic energy in the stratified layers may vary in space and time as the total energy of the internal wave field varies in the Baltic Sea. [Pg.36]

With rising temperature the volume of the aqueous phase grows, the micelles swell until suddenly, at the so-called phase inversion temperature, the oil phase has the larger volume. This effect is explained by the polyoxyethylene chains dehydrating as the temperature rises. The hydrophilic/hydrophobic balance of the molecule is thereby altered and the solubility in the oil phase grows. When concentration is great enough, micelles are formed in the oil phase and water is solubilised. If the two phases do not exist as stratified layers but as emulsion a... [Pg.22]

Convective heat transfer across two immiscible stably stratified layers, bounded above by an isothermal plate and below by an adiabatic plate, and with the bottom layer heated internally, has been measured by Nguyen and Kulacki [206]. A similar problem was earlier studied by Schramm and Reineke [245]. [Pg.271]


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See also in sourсe #XX -- [ Pg.7 , Pg.8 , Pg.50 ]




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