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Normal phase behaviour

BaAn" 03 (An = Th Am) all have the perovskite strueture and are obtained from the aetinide dioxide. In aeeord with normal redox behaviour, the Pa and U eompounds are only obtainable if O2 is rigorously exeluded, and the Am eompound if O2 is present. Aetinide dioxides also yield an extensive series of nonstoiehiometrie, mixed oxide phases in whieh a seeond oxide is ineorporated into the fluorite lattiee of the An02. The UO2/PUO2 system, for example, is of great importanee in the fuel of fast-breeder reaetors. [Pg.1269]

The qualitative analysis of retention behaviour in liquid chromatography has now become possible. Quantitative retention-prediction is, however, still difficult the prediction of retention time and the optimization of separation conditions based on physicochemical properties have not yet been completely successful. One reason is the lack of an ideal stationary phase material. The stationary phase material has to be stable as part of an instrument, and this is very difficult to achieve in normal-phase liquid chromatography because the moisture in organic solvents ages the silica gel. [Pg.131]

Abbreviations o-HSPh, or(/io-mercaptophenyl, Diastereomers of unknown stereochemistry are characterized by chromatographic behaviour I = faster eluting, 2 = slower eluting diastereomer in normal-phase chromatography. With / -mercaptoethanol in the assay medium. [Pg.311]

Calculation of the critical pressure required to cause a phase transformation at 0 K can also be obtained from first-principle calculations. Assiuning the various phases exhibit normal elastic behaviour the tangency rule can be applied to energy vs volume plots to yield values for the critical pressure that would generate a phase transformation ... [Pg.182]

Case (i) Phase Behaviour of Normal Substances, for which Vg V > Vs... [Pg.68]

Mixtures of water (main component), organic substances and gases such as O2 or CO2 are multiphase systems under normal conditions. Pressures above 221 bar and temperatures higher than 374 °C generally provide single-phase behaviour and facilitate very fast oxidation reactions. These advantages led to the attempt to turn SCWO into a commercially available industrial process for sewage disposal especially in the case of hazardous waste. [Pg.565]

Normally, food and chyme are phase-separated systems, but only the first steps have been taken towards understanding the phase behaviour of food polymers in food processing and practically nothing in food digestion. The effects of thermodynamic compatibility of mucopolysaccharides, food fibers and exopolysaccharides of different bacteria species on selection of microflora in the intestine and colon have not been studied yet. The mechanisms of bacterial colonization of the intestine and peristaltic transportation of chyme also remain unstudied. [Pg.38]

In ternary organic mobile phases with a constant concentration ratio of two solvents with great elution strengths, (px/tpi, the sum of the two concentrations, tpx =

retention behaviour in normal-phase ternary solvent systems often can be described by the equation formally identical with Eq. (1.15) [27,80], as is illustrated by Fig. 1.20 ... [Pg.60]

Besides the asymmetry between monolayers in cytomembranes, two of the more obvious differences between cubic phases and membranes are the unit cell size and the water activity. It has been argued that tire latter must control the topology of the cubic membranes [15], and hence tiiat the cubic membrane structures must be of the reversed type (in the accepted nomenclature of equilibrium phase behaviour discussed in Chapters 4 and 5 type II) rather than normal (type I). All known lipid-water and lipid-protein-water systems that exhibit phases in equilibrium with excess water are of the reversed type. Thus, water activity alone cannot determine the topology of cubic membranes. Cubic phases have recently been observed with very high water activity (75-90 wt.%), in mixtures of lipids [127], in lipid-protein systems [56], in lipid-poloxamer systems [128], and in lipid A and similar lipopolysaccharides [129,130]. [Pg.322]

Shalliker, R.A. Rizk, M. Stocksiek, C. Sweeney, A.P. Retention behaviour of basic solutes on zirconia-silica composite stationary phase supports in normal phase liquid chromatography. J. Liq. Chromatogr. Relat. Technol. 2002, 25 (4), 561-572. [Pg.1748]

The experimental results will be considered first of all. Comparing the values for K, found in the Zintl phases with the ones in the pure metals one notices that the AB phases show a normal paramagnetic behaviour. For the AB compounds K, is distinctly smaller than in the case of pure metals. Kj is even negative for NaTl. [Pg.126]

The difficulties encountered in LLC can be overcome by the use of chemically bonded stationary phases or bonded-phases. Most bonded phases consist of organochlorosilanes or organoalkoxysilanes reacted with micro-particulate silica gel to form a stable siloxane bond. The conditions can be controlled to yield monomeric phases or polymeric phases. The former provides better efficiency because of rapid mass transfer of solute, whereas the polymeric phases provides higher sample capacity. BPC can be used in solvent gradient mode since the stationary phase is bonded and will not strip. Both normal-phase BPC (polar stationary, non-polar mobile) and reversed-phase BPC (non-polar stationary, polar mobile) can be performed. The latter is ideal for substances which are insoluble or sparingly soluble in water, but soluble in alcohols. Since many compounds exhibit this behaviour, reversed phase BPC accounts for about 60% of published applications. The main disadvantage of silica bonded phases is that the pH must be kept between 2 to 7.5. However, bonded phases with polymer bases (polystyrene-divinylbenzene) can be used in the pH range of 0 to 14. [Pg.22]

Swart, R., Brouwer, S., Kraak, J. C., Poppe, H., Swelling behaviour and kinetic performance of polyacrylate stationary phases for reversed-phase and normal phase open-tubular liquid chromatography. /. Chromatogr. A1996, 732, 201-207. [Pg.299]

It has not proved possible to develop general analytical hard-core models for liquid crystals, just as for normal liquids. Instead, eomputer simulations have played an important role in extending our understanding of the phase behaviour of hard partieles. Frenkel and Mulder found that a system of hard ellipsoids can form a nematic phase for ratios L/D > 2.5 (rods) or L/D < 0.4 (discs) [73] however, such a system cannot form a smectic phase, as can be shown by a sealing... [Pg.2557]

The sequence in which reversed phases occur is much more complicated than that for the normal phases and is not yet understood in terms of surfactant molecular structures. The main reason is (probably) that there is no limitation on the radius of the inverse micelles such as that imposed by the length of the paraffin chain on normal micelles. Water could swell the micelles indefinitely (this does not happen because the size and shape of inverse micelles is controlled by limits on surfactant packing on a curved surface). Figure 21.12 (or something similar) is often employed to describe the general pattern of mesophase behaviour as a function of surfactant (water) concentration. In the description... [Pg.480]

C. Cagran, C. Brunner, A. Seifter, G. Pottlacher Liquid-phase behaviour of normal spectral emis-sivily at 684.5 nm of some selected metals. High Temp.-High Press. 34, 669 (2002) Dechema-Werkstoff-Tabelle Oxidierende Heifigase (Dechema, Frankfurt 1981)... [Pg.425]

Svoboda et al. [ 111 ] referred to the UCST as a virtual UCST. UCST behaviour was only observed in rapidly quenched samples where samples were cooled so quickly that they were maintained as mobile liquids below the normal phase separation/crystallisation temperature. In bulk samples, where cooling was restricted by the thermal conductivity of the sample, it is unlikely that such phenomena will be observed. [Pg.137]


See other pages where Normal phase behaviour is mentioned: [Pg.67]    [Pg.113]    [Pg.210]    [Pg.261]    [Pg.27]    [Pg.342]    [Pg.481]    [Pg.181]    [Pg.149]    [Pg.239]    [Pg.32]    [Pg.314]    [Pg.69]    [Pg.362]    [Pg.85]    [Pg.85]    [Pg.354]    [Pg.165]    [Pg.124]    [Pg.407]    [Pg.497]    [Pg.194]    [Pg.304]    [Pg.223]    [Pg.70]    [Pg.571]   
See also in sourсe #XX -- [ Pg.23 ]

See also in sourсe #XX -- [ Pg.23 ]




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Normal phase

Phase behaviour

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