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System, crystal equilibria

The isolation of crystalline products having mixed polymorphic compositions (often referred to as concomitant polymorphism) remains a topic of interest, even though the phase rule predicts that a system at equilibrium consisting two components (solvent + solute) and three phases (solution + Form I + Form II) is uni variant. Hence, for crystallizations performed at a fixed pressure (typically atmospheric) the system becomes nonvariant and genuine equilibrium can exist at only one temperature. Therefore, concomitant products must be obtained under nonequilibrium conditions. Flexibility in molecular conformation was attributed to the concomitant polymorphs of a spirobicyclic dione [34] and of 3-acetylcoumarin [35],... [Pg.268]

These photographs show a supersaturated solution of sodium acetate and the effect of adding a crystal to it. Is either of these systems at equilibrium ... [Pg.324]

Another crystallization technique is used when the isolation of a highly water-soluble compound in its salt form is required from aqueous reaction mixtures. This technique takes advantage of the common-ion effect and is based on the le Chatelier s principle, which states that, if, to a system in equilibrium, a stress is applied, the system will react so as to relieve the stress. Thus, in aqueous solutions, the solubility of the compound in salt form can be reduced by adding large amoimts of a common ion which is more soluble than the salt of the compoimd. [Pg.250]

The Phase Rule—A Method of Classifying Al Systems in Equilibrium. We have so far discussed a number of examples of systems in equilibrium. These examples include, among others, a crystal or a liquid in equilibrium with its vapor (Chap. 4), a crystal and its liquid in equilibrium with its vapor at its melting point (Chap. 4), a solution... [Pg.506]

The a and crystals may be transformed into each other When the point representing the state of the system is included between the lines CF and EO, the system in equilibrium incloses the two kinds of crystals if the representative point is to the left of CF, the system is homogeneous and of form a it is homogeneous and of form j9 if the representative point is to the right of the line EG. [Pg.306]

This description has to be compared with that proposed by non-equilibrium thermodynamics in terms of only two states, corresponding to the melted and crystallized phases in the example we are discussing, from which only one may account for the linear domain, when the chemical potentials at the wells are not very different. This feature imposes serious limitations in the application of NET to activation processes since that condition is rarely encountered in experimental situations and has therefore restricted its use to only transport processes. The mesoscopic version of non-equilibrium thermodynamics, on the contrary, circumvents the difficulty offering a promising general scenario useful in the characterization of the wide class of activated processes, which appear frequently in systems outside equilibrium of different nature. [Pg.261]

Freezing involves different factors in the conversion of water into ice thermodynamic factors that define the position of the system under equilibrium conditions, and kinetic factors that describe the rates at which equilibrium might be approached. The freezing process includes two main stages the formation of ice crystals (nucleation), and the subsequent increase in crystal size (growth). [Pg.310]

The characteristic hexagonal pattern of an ice crystal arises from the tetrahedral arrangement of the four H-bonds in which each water molecule can participate. Ice crystals have extremely open structures with only four nearest neighbors around each molecule. When many water molecules are involved in a large system, their equilibrium configuration can only be solved by using a computer and this process can also account for the highly open ice structure. [Pg.57]

Short Cycle Time. Figure 4 shows the temperature of benzene in a vessel 50 mm in diameter. Several thermocouples were arranged from the near inside wall of the vessel to the center. When pressure was applied r idly, the temperatures rapidly rose and reached a certain value. This value was the equilibrium temperature of solid and liquid at that pressure. This fact shows that crystallization progresses uniformly and rapidly with an increase in pressure, and stops soon after the pressurization ceases. Meanwhile, the temperature begins to decrease from the outside. It was found that in many other mixture systems, crystallization progresses as rapidly as it does in benzene. [Pg.140]

The Wulff theorem can be derived from the equilibrium condition of an isolated system containing a single crystal, i.e. the minimum free energy condition of the system.Under equilibrium at a constant temperature, an infinitesimal change in Helmholtz free energy of the system, dF, is... [Pg.216]

The fraction of molecules that do not partake in the long ranged order is very small (Nevertheless, grain boundaries or defects may have great effect on bulk properties despite their low number). The crystal stractures developing in low molecular systems are equilibrium stractures. [Pg.72]

In this section the broad spectrum of melting of one-component macromolecular systems is described by means of several specific polymers. The description starts with polyethylene, the most analyzed polymer. It continues with two sections that present several special effects seen in the thermal analysis of polymers including some examples of detailed analyses by TMDSC, documenting the locally reversible melting and crystallization equilibrium within a globally metastable structure. Then illustrations of poly(oxymethylene) and PEEK are given as typical common polymeric materials. This is followed in the last section with the discussion of special effects seen in drawn polymers, as are commonly found in fibers and films. [Pg.610]


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See also in sourсe #XX -- [ Pg.89 ]




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