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Solids, characteristic temperature melting

These ideas are best learned by using them yourself. Let us take an example from your own laboratory work. You have observed the heating of a variety of solid materials sulfur, wax, tin, lead, silver chloride, and copper. Each melts at a characteristic temperature. This fact led us to the generalization A solid melts to a liquid at a characteristic temperature. Your confidence in the generalization was bolstered by the additional information (communicated to you, not experienced) that this applies to hundreds of thousands of substances. ... [Pg.7]

The boiling points of different types of liquids vary widely. They are an important physical characteristic both of liquids and of the many solids that melt to become liquids and then boil at a certain characteristic temperature. [Pg.397]

Figure 22. The configurational entropy Sc per lattice site as calculated from the LCT for a constant pressure, high molar mass (M = 40001) F-S polymer melt as a function of the reduced temperature ST = (T — To)/Tq, defined relative to the ideal glass transition temperature To at which Sc extrapolates to zero. The specific entropy is normalized by its maximum value i = Sc T = Ta), as in Fig. 6. Solid and dashed curves refer to pressures of F = 1 atm (0.101325 MPa) and P = 240 atm (24.3 MPa), respectively. The characteristic temperatures of glass formation, the ideal glass transition temperature To, the glass transition temperature Tg, the crossover temperature Tj, and the Arrhenius temperature Ta are indicated in the figure. The inset presents the LCT estimates for the size z = 1/of the CRR in the same system as a function of the reduced temperature 5Ta = T — TaI/Ta. Solid and dashed curves in the inset correspond to pressures of P = 1 atm (0.101325 MPa) and F = 240 atm (24.3 MPa), respectively. (Used with permission from J. Dudowicz, K. F. Freed, and J. F. Douglas, Journal of Physical Chemistry B 109, 21350 (2005). Copyright 2005, American Chemical Society.)... Figure 22. The configurational entropy Sc per lattice site as calculated from the LCT for a constant pressure, high molar mass (M = 40001) F-S polymer melt as a function of the reduced temperature ST = (T — To)/Tq, defined relative to the ideal glass transition temperature To at which Sc extrapolates to zero. The specific entropy is normalized by its maximum value i = Sc T = Ta), as in Fig. 6. Solid and dashed curves refer to pressures of F = 1 atm (0.101325 MPa) and P = 240 atm (24.3 MPa), respectively. The characteristic temperatures of glass formation, the ideal glass transition temperature To, the glass transition temperature Tg, the crossover temperature Tj, and the Arrhenius temperature Ta are indicated in the figure. The inset presents the LCT estimates for the size z = 1/of the CRR in the same system as a function of the reduced temperature 5Ta = T — TaI/Ta. Solid and dashed curves in the inset correspond to pressures of P = 1 atm (0.101325 MPa) and F = 240 atm (24.3 MPa), respectively. (Used with permission from J. Dudowicz, K. F. Freed, and J. F. Douglas, Journal of Physical Chemistry B 109, 21350 (2005). Copyright 2005, American Chemical Society.)...
Differential Scanning Calorimetry (DSC) is a sensitive way of detecting phase transformations of a bulk material [85,86]. Monitoring the thermal behavior of a crystal or a powder as a function of its conversion to product can give important information. This technique can verify whether a reaction occurs in a purely solid phase or whether there may be liquid phases involved at a given temperature. Melting point depression can be monitored as product appears, and the characteristic melting of a new phase can be detected if one is formed. DSC can reveal whether or not a eutectic transition attributable to a mixture of phases is present. We have also used DSC in our lab to monitor the thermal stability of reactive crystals. [Pg.211]

For example, by employing a temperature of 250° C. and a rapid stream of fluorine, a very reactive osmium preparation was found to yield a high percentage of Osmium Oetafluoride, OsF8. This, being the most volatile of the products, is collected in a vessel cooled in a mixture of solid carbon dioxide and alcohol, under which conditions it yields a yellow, solid sublimate. It melts at 34-5° C. to a yellowish red liquid. Its vapour is colourless, has a characteristic odour and metallic taste it attacks the mucous membranes of the nose and eyes. In moist air the vapour yields a white cloud. [Pg.213]

Thermal Properties at Low Temperatures For solids, the Debye model developed with the aid of statistical mechanics and quantum theory gives a satisfactory representation of the specific heat with temperature. Procedures for calculating values of 0d, the Debye characteristic temperature, using either elastic constants, the compressibility, the melting point, or the temperature dependence of the expansion coefficient are outlined by Barron Cryogenic Systems, 2d ed., Oxford University Press, 1985, pp 24—29). [Pg.1131]

Colorless crystalliue solid with a characteristic odor sublimes at ambient temperature melts at 54°C (129°F) boils at 174 C (345 F) insoluble in water, soluble in organic solvents. [Pg.462]

Type I plasticizers are used to soften the binder polymer chains, allowing them to stretch or deflect under an applied force. These additives can be accurately described as modifiers or binder solvents. Tg is a symbol that stands for glass transition temperature. While crystalline solids have a distinct change from solid to liquid, the binder polymer in the dry tape is a noncrystalline solid, having a gentle transformation from solid to liquid. While crystalline solids freeze and melt, the polymer matrix softens more and more until it is considered a liquid. In order to describe the softening characteristics of a polymer (or glass), a temperature is calculated... [Pg.50]

The rheological properties and associated melt-processing characteristics of ethylene-co-styrene polymers, including solid-state DMS, melt strength, and pressure-volume-temperature (PVT) data, have been reported by Kaijala and coworkers (59,60). Rheological master curves were generated via time-temperature... [Pg.2790]


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See also in sourсe #XX -- [ Pg.194 ]




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