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Characteristic temperature Coexistence

As described in Section 14-1. when AR and ZlS have the same sign, the spontaneous direction of a process depends on T. For a phase change, enthalpy dominates AG at low temperature, and the formation of the more constrained phase is spontaneous, hi contrast, entropy dominates AG at high temperature, and the formation of the less constrained phase is spontaneous. At one characteristic temperature, A G = 0, and the phase change proceeds in both directions at the same rate. The two phases coexist, and the system is in a state of d Tiamic equilibrium. [Pg.1021]

The characteristic line of attack for the development of mesostructured materials is the use of the following standard synthesis conditions low temperatures, coexistence of inorganic and organic moieties, and extensive choice of precursors [61],... [Pg.124]

The triblock copolymer EO PO EOn is soluble in water and forms micelles above a critical polymer concentration and above a characteristic temperature. This was shown by Zhou and Chu [352,375,376]. These authors afiBmed that micelle formation is temperature dependent because the hydrophilic/hydropho-bic characteristics of these polymers can be easily modified by changing the temperature. They mentioned the presence of three temperature regions a uni-mer region, a micelle region and a transition region where unimers and micelles coexist. The micelles seem to be monodisperse in size, even if the polymer itself is polydisperse, their radii being independent of concentration but dependent on temperature [377],... [Pg.131]

Liquid/solid Equilibria. The solubility of crystalline polymers is normally considerably lower than that of amorphous polymers because they require an additional energy, namely, the heat of fusion, in order for the bulk polymer to mix with solvent. Fig. 6 shows as an example the behavior of semi crystalline polyethylene in two different solvents(20). The solvent xylene is favorable in the temperature range of interest (no liquid/liquid demixing) up to the melting temperature T. o of the pure polymer a saturated solution coexists with the crystalline polyethylene and the components are completely miscible once T has surpassed Tm,o- Nitrobenzene on the other hand, is thermod5mamically less favorable and exhibits liquid/liquid demixing in addition to the solid/liquid phase separation. In this case one observes the coexistence of three phases at a characteristic temperature (broken line in Fig. 6) and concentration. [Pg.1075]

On a global scale, the atmosphere serves as the major pathway for the transport and deposition of contaminants from emission sources to terrestrial and aquatic ecosystem receptors (22, 27). Once a contaminant is airborne, the processes of atmospheric di sion, transport, transformation, and deposition act to determine its fate. These processes are complex and the degree to which they influence the fate of a particular contaminant is dependent on its physico-chemical characteristics, the properties and concentrations of coexisting substances, and the prevailing meteorological conditions, including wind, precipitation, humidity, temperature, clouds, fog, and solar irradiation. [Pg.138]

The resulting overall picture of liquid water is that of a very dynamical macromolecular system, where clusters of different size and structure coexist in different subvolumes of the liquid and each has characteristic lifetimes and specific temperature dependences. In our opinion, if we would... [Pg.211]

Some of the methods of analysis of porosity are based on specific properties of porous and disperse materials, namely, thermoporometiy method is based on shifts of the temperature of phase transitions and permeametry methods are based on characteristics of mass transfer through porous media. Each method has its advantages, for example low cost of equipment and high performance. Each has its own range of optimal measurements. But, all the methods are really doomed for coexistence, and in many cases they supplement each other. [Pg.280]

Three-Phase Transformations in Binary Systems. Although this chapter focuses on the equilibrium between phases in binary component systems, we have already seen that in the case of a entectic point, phase transformations that occur over minute temperature fluctuations can be represented on phase diagrams as well. These transformations are known as three-phase transformations, becanse they involve three distinct phases that coexist at the transformation temperature. Then-characteristic shapes as they occnr in binary component phase diagrams are summarized in Table 2.3. Here, the Greek letters a, f), y, and so on, designate solid phases, and L designates the liquid phase. Subscripts differentiate between immiscible phases of different compositions. For example, Lj and Ljj are immiscible liquids, and a and a are allotropic solid phases (different crystal structures). [Pg.157]

These occur particularly in solution, but in the solid state also coexistence of the different stereochemistries is possible in either case, complicated magnetic behaviours as functions of concentration, preparative details and temperature arise. Complexes of (3-diketones, substituted alkylenediamines and salicylaldiamines are characteristic sources of these phenomena. [Pg.274]


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Characteristic temperature

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