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Temperature of transition

At temperatures below 850°C this effect of varying airrgas ratio tended to disappear and it was not apparent in tests at 750°C. From the data shown in Table 7.8 it can be seen that 850°C is about the temperature of transition from protective to semi-protective behaviour, so atmospheric effects would be at their greatest. [Pg.1028]

Proceeding from the nature of yield stress as a characteristic of strength of the structure formed by a filler, a situation can be imagined where the character of inter-molecular contacts will depend on temperature to a large extent, or at least, will sharply change at certain temperatures of transition. However, this is rather an exotic case, and although researchers have not observed it, it cannot be excluded. [Pg.77]

Figure 8. The temperature dependence of the heat capacity in the condensed state for adamantane [5] as measured by a scanning calorimeter. Tu, stands for temperature of transition from rigid crystal (fee) to plastic crystal (cubic) state of adamantane and Tfas stands for fusion temperature. Figure 8. The temperature dependence of the heat capacity in the condensed state for adamantane [5] as measured by a scanning calorimeter. Tu, stands for temperature of transition from rigid crystal (fee) to plastic crystal (cubic) state of adamantane and Tfas stands for fusion temperature.
At a certain temperature of transition Tt, the two forms will be in equilibrium, AG will be zero, and m = m2. But at other temperatures the two forms will not be in equilibrium, and if ax > a2 then because AG = Z rin (a2/fli), AG will be negative and polymorph 1 will change spontaneously to polymorph 2 and will therefore be considered the less stable form and vice versa. Studies of the two polymorphic forms of methylprednisolone show that significant differences occur in the apparent solubilities of polymorphic forms and that these may be temperature-related. [Pg.606]

Once we have determined the entropy and enthalpy of polymerization, we can calculate the free energy of the process at a variety of temperatures. The only time this is problematic is when we are working near the temperatures of transition as there are additional entropic and enthalpic effects due to crystallization. From the free energy of polymerization, we can predict the equilibrium constant of the reaction and then use this and Le Chatelier s principle to design our polymerization vessels to maximize the percent yield of our process. [Pg.72]

To this purpose, Fossheim et al. reported temperature sensitive liposomal Gd(III)-based probes (137-138). The composition of the liposomes was chosen in order to tune the temperature of transition between the gel-crystalline, where the liposome is water-impermeable, to the liquid-crystalline state, where water has free access to the interior of the liposome. This means that at temperatures below the transition, the relaxivity of the system is very low (paramagnetic contribution close to zero), whereas at higher temperature the Gd(III) complex ([GdDTPABMA(H20)] is the reference) is no longer silent... [Pg.218]

The equilibrium temperature of transition is coinci(ient with the critical temperature ... [Pg.111]

Coefficients a, B, and C in equation 5.175 have the usual meanings in the Landau expansion (see section 2.8.1) and for the (second-order) displacive transition of albite assume the values = 1.309 cal/(mole X K) and B, = 1.638 kcal/mole (Salje et al., 1985). is the critical temperature of transition = Bla = 1251 K). The corresponding coefficients of the ordering process are = 9.947 cal/(mole X K), B = -2.233 kcal/mole, = 10.42 kcal/(mole X K), and = 824.1 K. With all three coefficients being present in the Landau expansion relative to substitutional disorder it is obvious that Salje et al. (1985) consider this transition first-order. A is a T-dependent coupling coefficient between displacive and substitutional energy terms (Salje et al., 1985) ... [Pg.356]

According to Merkel and Blencoe (1982), the relationship among the amount of KAlSi30g, pressure, and temperature of transition is... [Pg.362]

DSCDifferential Scanning Calorimetry (Heats and temperatures of transitions and reactions). [Pg.179]

The heat of transition from form III to form II is 310 keal/mol and that from form II to form I is 979 kcal/mol. Whetstone (Ref 113) studied the initiation of transition between forms III and IV. The effect of foreign substances on the transition IV III was studied by Campbell and Campbell (Ref 81) who found that in the case of a solid solution of 8. to 10% of KNOj in AN the temperature of transition of form III into form IV is depressed by about 20°. Such solid solutions can be prepared either by fusion or by co-crystallization from aqueous solutions. Hendricks et al (Ref 40) found form III to be ortho rhombic and form V to exist up to -18° and not to -16°. Bowen (Ref 30) showed that there is also a metastable inversion occurring at about 50° as follows orthorhombic form (j3)(32. l°to -16°) tetragonal form (5)(125-2° to 84.2°). [Pg.311]

It is for this reason (that AG = 0) that we were able to calculate standard entropies of transition by simply dividing the enthalpies of transition by the Kelvin temperature of transition as we did on p 214. Entropies of reaction cannot be calculated this way the more general expression must be used. [Pg.286]

Table 10. Temperature of transitions, Tn Tg and Tcl, activation energy EJ p and relaxation time p of dipole polarization of smectic cholesterol-containing polymers128 129)... Table 10. Temperature of transitions, Tn Tg and Tcl, activation energy EJ p and relaxation time p of dipole polarization of smectic cholesterol-containing polymers128 129)...
The temperature of transition is small relative to the value of splitting of the Mn3+ 5E ground state. That is why we suppose that the transition from monoclinic to rhombohedral phase is a transition from static to dynamic JT effect. Because of the strong correlation in motion of different [Mn06] octahedra we suppose that there is a cooperative dynamical effect. [Pg.597]

The instrument software can be used to derive properties of the sample from the thermogram data. These may include specific heat capacity, temperature of transition, heat of transition, solid fat content and reaction kinetics constants. [Pg.737]

It has been the merit of Picken (1989, 1990) having modified the Maier-Saupe mean field theory successfully for application to LCPs. He derived the stability of the nematic mesophase from an anisotropic potential, thereby making use of a coupling constant that determines the strength of the orientation potential. He also incorporated influences of concentration and molecular weight in the Maier-Saupe model. Moreover, he used Ciferri s equation to take into account the temperature dependence of the persistence length. In this way he found a relationship between clearing temperature (i.e. the temperature of transition from the nematic to the isotropic phase) and concentration ... [Pg.638]

In Eq. (1.161), temperature T is the boiling point at pressure P. Table 1.4 shows enthalpies and temperature of transition for some species. [Pg.30]

The effect of various stoichiometry VO2 powders on temperature and heat of phase transition has not been reported so far. In this paper, the heats and the temperatures of transition from VO196 to VO207 in the crystalline state were measured from DSC scans. The results are listed in Table 1, indicating that the heats of the oxygen-deficient VO2 are less than those of the oxygen-rich VO2, and the VO2 02 has the maximum transition heat. The transition temperature is increased about 10°C from VOi 95 to VO2.07- Those results are not consistent with the results observed by determination of electrical resistivity of monocrystals reported in the literature, and the results in the literature are also contradictory [16,17]. The IR spectra of various size, crystalline state and stoichiometry VO2 are observed, showing the effects of size, crystalline state and stoichiometry [18]. [Pg.484]

The Solid- olid Phase Transition.—A phase transition in the solid was indicated, by the vapour pressure data, to be between 35° and room temperature, but because of the small change in slope of the log vs. IJT plot, it was not possible, precisely, to locate the transition point from this data. The nature of the transition was determined by X-ray powder photography and the temperature of transition obtained accurately with the aid of a polarizing microscope. [Pg.252]

Te temperature of transition to superconducting state 6 index expressing departure from stoichiometry... [Pg.62]

Many enthalpies of fusion and enthalpies of solid-state transitions are obtained from enthalpy measurements. Here the enthalpies are given directly by the difference in enthalpy at the transition temperature. Normally, the enthalpy above and below can be smoothly extended to the temperature of transition, although the transition temperature may not be clearly obtainable from the enthalpy data. [Pg.14]

The temperature of transition is that reported by Naylor (9), the large uncertainty has been assigned since at 1424 K the... [Pg.698]


See other pages where Temperature of transition is mentioned: [Pg.234]    [Pg.19]    [Pg.201]    [Pg.794]    [Pg.795]    [Pg.702]    [Pg.433]    [Pg.344]    [Pg.489]    [Pg.108]    [Pg.213]    [Pg.15]    [Pg.550]    [Pg.593]    [Pg.120]    [Pg.170]    [Pg.47]    [Pg.193]    [Pg.55]    [Pg.55]    [Pg.311]    [Pg.350]    [Pg.21]    [Pg.476]    [Pg.722]   
See also in sourсe #XX -- [ Pg.148 ]

See also in sourсe #XX -- [ Pg.406 ]




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An example of a static (low temperature) FTIR measurement, the BR to K transition

Calculation of glass transition temperature

Characterisation of amorphous solids the glass transition temperature

Coefficient of thermal expansion glass transition temperatures

Comment on the Temperature Dependence of Radiationless Transition

Compositional dependence of glass transition temperature

Dependence of Multiphonon Transitions on Interaction Strength and Temperature

Dependence of glass transition temperature

Depression of glass transition temperature

Determination of Glass Transition Temperature by DTA or DSC

Determination of Phase Transition Temperatures

Determination of glass transition temperature

Determination of the glass transition temperature, Tg

Effect of Cure Conversion on Glass Transition Temperature (Tg)

Effect of Curing Conditions on the Glass-Transition Temperature

Effect of glass transition temperature

Effect of ions on the glass transition temperature

Effect of the glass transition temperature

Effects of molecular weight on glass transition temperature

Features of Temperature Transitions

Field-Induced Shifts of the Phase Transition Temperatures

Flow temperatures of transition from anisotropic to isotropic state

Glass Transition Temperature and Thermal Stability of Phosphorus-Containing Siliconized Epoxy Resin

Glass Transition Temperatures of Polytriazole Resins

Glass transition temperature of Blend

Glass transition temperature of PVC

Glass transition temperature of block copolymers

Glass transition temperature of epoxy resins

Glass transition temperature of poly

Glass transition temperature of polyethylene

Glass transition temperature of polyurethane

Glass transition temperature of the blend

Glass transition temperature, of polymer

Glass transition temperatures kinetics of phenol release

Glass transition temperatures of copolymers

High temperature properties of transition metals

Influence of Chemical Structure on Glass Transition Temperature

Measurement of Glass Transition Temperature and other Transitions

Measurement of glass transition temperature

Methods of Determining Glass Transition Temperature

Prediction of Discontinuous Volume Phase Transition with Respect to Temperature

Reductions of the transition temperatures

Relationship between glass transition temperature and melting point of polymers

Temperature and pressure dependence of relaxation near the glass transition

Temperature dependence of non-radiative transitions

Temperatures of phase transition

The Effect of Glass Transition Temperature on Adhesives and Sealants

Variation of glass transition temperature with

Vitrification of liquids above glass transition temperature

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