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Glass-formers

Glass former is sihca unless otherwise noted. See Table 1. [Pg.302]

Halide Glasses. Fluoride glasses are the most important of the haUde glasses. The only primary fluoride glass former is beryUium fluoride,... [Pg.330]

These are normally of pure platinum wound on a ceramic or glass former and encapsulated in a ceramic or glass shell, having an operating range of -250°C to +750°C,... [Pg.305]

NFS spectra of the molecular glass former ferrocene/dibutylphthalate (FC/DBP) recorded at 170 and 202 K are shown in Fig. 9.12a [31]. It is clear that the pattern of the dynamical beats changes drastically within this relatively narrow temperature range. The analysis of these and other NFS spectra between 100 and 200 K provides/factors, the temperature dependence of which is shown in Fig. 9.12b [31]. Up to about 150 K,/(T) follows the high-temperature approximation of the Debye model (straight line within the log scale in Fig. 9.12b), yielding a Debye tempera-ture 6x) = 41 K. For higher temperatures, a square-root term / v/(r, - T)/T,... [Pg.490]

Fig. 9.32 (a) Time evolution of the SRPAC signal (in log scale) for several temperatures obtained from the molecular glass former DBP doped with Fe-enriched ferrocene, (b) The relaxation rate X (in log scale) as a function of inverse temperature 1,000 obtained from analyzing the SRPAC... [Pg.515]

Silica, the universal glass former, generally makes up 60%-70% of the total mass of glass only in very few cases does the amount of silica exceed 70%. [Pg.153]

Figure 2 Sketch of typical temperature dependencies of the viscosity r of glass-forming systems. The viscosimetric Tg of a material is defined by the viscosity reaching 1013 Poise. Strong glass formers show an Arrhenius temperature dependence, whereas fragile glass formers follow reasonably well a Vogel-Fulcher (VF) law predicting a diverging viscosity at some temperature T0. Figure 2 Sketch of typical temperature dependencies of the viscosity r of glass-forming systems. The viscosimetric Tg of a material is defined by the viscosity reaching 1013 Poise. Strong glass formers show an Arrhenius temperature dependence, whereas fragile glass formers follow reasonably well a Vogel-Fulcher (VF) law predicting a diverging viscosity at some temperature T0.
Polymers are very good glass formers, with a few notable exceptions. For some polymers, such as atactic polypropylene or random copolymers like... [Pg.6]

III. Test of the Adam-Gibbs Relaxation Model for Glass Formers Based on the Heat-Capacity Data of 1,3,5-Tri-a-Naphthylbenzene. [Pg.156]


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See also in sourсe #XX -- [ Pg.118 ]

See also in sourсe #XX -- [ Pg.118 ]

See also in sourсe #XX -- [ Pg.22 , Pg.23 , Pg.26 , Pg.36 , Pg.37 , Pg.40 , Pg.42 , Pg.55 , Pg.118 , Pg.293 , Pg.500 , Pg.506 , Pg.535 ]

See also in sourсe #XX -- [ Pg.298 ]

See also in sourсe #XX -- [ Pg.49 ]

See also in sourсe #XX -- [ Pg.49 ]

See also in sourсe #XX -- [ Pg.59 , Pg.65 , Pg.70 ]




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