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Supercooled liquid state

Liquid solvents in this picture may be considered as islands in the northern hemisphere, because the state of molecules in a liquid solvent is quite definitely closer to the COSMO state than to the vacuum. The only exception may be alkane solvents, which are located somewhere close to the equator due to their fully nonpolar character. Solids may be considered as sunken islands and their depths below sea level may be considered as AG s. As discussed before, the methods to explore this depth are rather limited, but we can be quite sure that in general the depth below sea level will be much smaller than the distance of the islands from the North Pole or from each other. We now explore the methods to go from the sea level position of any island to the North Pole or vice versa. Given such a method we will be able to transfer a compound from any liquid or supercooled liquid state to any other such state. [Pg.293]

FIG. 31 Schematic diagram illustrating the transition between a supercooled liquid state (rubber) and an amorphous solid state (glass). The glass transition event is typically caused by a decrease in water content and/or temperature. The reversibility of the transition, as indicated by the dotted arrow, is material dependent (see text for further discussion of the reversibility of the transition). [Pg.66]

Table 3.5 includes results of applying this method to liquids. These results were obtained using the program MPBPVP referred to above. The values for the supercooled liquid state that Table 3.6 presents in parentheses were found in the same manner. [Pg.78]

Once the melt is completed, the sample is shock-cooled by removal from the calorimeter vessel and placement on the isothermal calorimeter block. This cools the sample sufficiently rapidly that most materials will be "trapped" in their metastable supercooled liquid state. A rescan of the sample over the same temperature span will show the cold recrystallization of the material followed by the melt. For maximum time efficiency and sensitivity, a fast scanning rate is recommended. [Pg.118]

In these experiments the DDT would almost certainly be in the supercooled liquid state, which persists for a surprisingly long time in much more concentrated suspensions than those used. The vapor pressures quoted from Balson (5) and the later, higher figures of Dickinson (10) refer to crystalline DDT. The supercooled liquid would be expected (since the solubility of the solid in best solvents corresponds to about one-ninth on a mole fraction basis) to have about nine times the vapor pressure at room temperature of the crystals. There is little discrepancy left. In view of the facts that all measurements had to be made at less than 1 p.p.m. concentration, that DDT loss had to be obtained by difference, and that adsorption on vessel walls is difficult to allow for, this work leaves me with no anxiety for the validity of classical physicochemical theory. Distillation from supercooled droplets on a glass plate to growing crystals has been demonstrated by Feichtmeir (12). [Pg.136]

Table I lists two materials evaporating from the crystalline solid. There is nothing very inhibitory about the solid state. Ice evaporates much faster than lubricating oil and naphthalene much more rapidly than glycerol. However, when we have a substance which can exist for sufficient time in the supercooled liquid state (e.g,impure DDT in thin films), it is significantly more volatile and more soluble in this form. As a rough rule, a crystalline substance becomes about one-third to one-fourth as volatile and as soluble as the supercooled liquid for each 50 °C. below the melting point. Table I lists two materials evaporating from the crystalline solid. There is nothing very inhibitory about the solid state. Ice evaporates much faster than lubricating oil and naphthalene much more rapidly than glycerol. However, when we have a substance which can exist for sufficient time in the supercooled liquid state (e.g,impure DDT in thin films), it is significantly more volatile and more soluble in this form. As a rough rule, a crystalline substance becomes about one-third to one-fourth as volatile and as soluble as the supercooled liquid for each 50 °C. below the melting point.
In the supercooled liquid state, BMGs have very high yield strength and a high elastic-strain limit (often exceeding 2 percent, compared with crystalline materials that are almost always less than 1 percent), which makes them very springy. However,... [Pg.48]

Spectroscopic methods, such as FT-infrared (FTIR) and Raman spectroscopy detect changes in molecular vibrational characteristics in noncrystalline solid and supercooled liquid states. Various nuclear magnetic resonance (NMR) techniques and electron spin resonance (ESR) spectroscopy, however, are more commonly used, detecting transition-related changes in molecular rotation and diffusion (Champion et al. 2000). These methods have been used for studies of the amorphous state of a number of sugars in dehydrated and freeze-concentrated systems (Roudaut et al. 2004). [Pg.73]

According to equation (8), the solubility of a substance would be proportional to the activity of the undissolved solid, and inversely proportional to its activity coefficient. Although the activity of a substance in its standard state is dehned as unity, the activity of the undissolved solid must depend on reference state. A hypothetical, supercooled liquid state of solute at the temperature of interest is commonly taken as the standard state, making the activity coefficient a more complicated term. The activity coefficient will depend on the nature of both the solute and solvent, as well as on the temperature of the solution. [Pg.6]

As discussed above, the absolute activity of the solid depends on the chosen reference or standard state, and the usual practice is to take the supercooled liquid state of the pure solute at the temperature of solution as the standard state of unit activity. At temperatures lower than the melting point, the liquid state of the solute is less stable than its solid state, making the activity of the corresponding solid less than one. [Pg.6]

Kind, R., Liechti. O.. Korner. N.. Hulliger. J.. Dolinsek, J., and Blinc. R.. Deuteron-magnetic-resonance study of the cluster formation in the liquid and supercooled-liquid state of 2-cyclooctylamino-5-nitropyridine. Phys. Rev. (1992). [Pg.79]

Calorimetric studies on embryos by DSC showed an endothermic event attributable to a glass transition between — 60 and — 65°C. Thus, at storage conditions (5°C), the systems were well above the glass-transition temperature, with most of their solutes in solution or in supercooled liquid state. At such a high proportion of water, metabolic activity and deteriorative reactions involved in the short life span of this seed are not precluded by mobility restrictions. The nonstored seeds presented the relative lowest values of freezable water and they were selected for the studies on cryoconservation. [Pg.560]

The present survey jointly reports on data on the thermal conductivities k(7) of methanol, ethanol and 1-propyl alcohol in the glass and supercooled liquid states. The data were measured under equilibrium vapor pressure in the temperature interval from 2 K - 160 K. [Pg.351]

During these studies It was found that the rate-determining step of the cyclopolymerization of RDMA In the solid and supercooled liquid states Is the Intramolecular cycllzatlon reaction (5.7.15). This conclusion has been deduced because only an un-... [Pg.108]

Similarly, ionic liquids bearing a hydroxyl functionality - which leads to unfavorable intermolecular hydrogen bondings - can be used as a liquid at low temperamre. Salts 30-33 are easily synthesized from 1-methylimidazole and 2-chloroethanol they are solid at room temperature. However, because of a weak tendency to crystallize, they enter into a metastable supercooled liquid state when cooled and can therefore be used as solvents at low temperature. The glass transition temperatures are very low, between -72°C (30) and -111°C (33, Table 2.5). The influence of the anion on the glass transition temperatures, as opposed to the melting points, is not clear, as the chlorine salt 33 is a metastable liquid at lower temperature than the hexafluorophosphate and tetrafluoroborate salts 30 and 31. ... [Pg.20]

Bartos, J., Sausa, O., Kristiak, J., Blochowicz, T., and Rossler, E., Free-volumemicroslructure of glycerol and its supercooled liquid-state dynamics, J. Phys. Condens. Matter, 13,11473-11484 (2001). [Pg.416]

Chatterji, A. Desai, D. Miller, D.A. Sandhu, H.K. Shah, N.H. A Process for Controlled Crystallization of an Active Pharmaceutical Ingredient from Supercooled Liquid State by Hot Melt Extrusion World InteUeetnal Property Organization, W02012110469. 2012. [Pg.1149]


See other pages where Supercooled liquid state is mentioned: [Pg.130]    [Pg.74]    [Pg.78]    [Pg.54]    [Pg.298]    [Pg.218]    [Pg.42]    [Pg.65]    [Pg.68]    [Pg.107]    [Pg.174]    [Pg.126]    [Pg.166]    [Pg.25]    [Pg.252]    [Pg.129]    [Pg.208]    [Pg.28]    [Pg.72]    [Pg.471]    [Pg.32]    [Pg.90]    [Pg.254]    [Pg.42]    [Pg.94]    [Pg.107]    [Pg.130]    [Pg.251]    [Pg.66]    [Pg.67]    [Pg.72]    [Pg.234]   
See also in sourсe #XX -- [ Pg.66 ]

See also in sourсe #XX -- [ Pg.435 ]

See also in sourсe #XX -- [ Pg.411 , Pg.412 ]




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Liquids supercooling

Liquids, supercooled

Supercooled

Supercooled state

Supercooling

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