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Temperature of phase transition

MS2 NiSAl-91 < X < 2.1) Nii j,CUySi.93 (0.03 < y < 0.1) Investigation of structural, electronic, and magnetic properties by means of X-ray diffraction, densitometry, resistivity, susceptibility, and Ni Mossbauer spectroscopy as function of x temperature of phase transition from semimetalhc to metallic state as function of x different Ni sites with different (l/f l) and different angle between H and EFG axis effect of Cu impurities... [Pg.255]

Some of the methods of analysis of porosity are based on specific properties of porous and disperse materials, namely, thermoporometiy method is based on shifts of the temperature of phase transitions and permeametry methods are based on characteristics of mass transfer through porous media. Each method has its advantages, for example low cost of equipment and high performance. Each has its own range of optimal measurements. But, all the methods are really doomed for coexistence, and in many cases they supplement each other. [Pg.280]

The second term sums all the heats of phase transition divided by the temperatures of phase transition. [Pg.113]

The swelling ratio X and modulus G of networks A and B vary continuously with temperature, but in networks C-H (xMNa 0.0095) a phase transition takes place, and the dependence of X and G on T is discontinuous (Fig. 10). With increasing charge concentration on the chain, both the extent of the transition A and the critical temperature of phase transition (hence also yc) increase (similar changes as in Fig. 5 and 7). [Pg.189]

Our quantum chemical approach has been applied to explain the thermodynamics of the TKHS-like materials on the level of simple mean (molecular) field approximation [1,4] which, however, is not well adapted to provide for quantitative estimations of the critical temperature of phase transitions. To examine the... [Pg.583]

What is the temperature of phase transition in a LB multilayer of cadmium arachidate Is it reversible ... [Pg.661]

Figure 4. The curve plots of the concentration dependence of free energies f[ (dotted lines) and f2 (full curves) in the region of temperatures of phase transitions I—HI (<5Pt—> PtHx). The intersection and extremal points are marked with circles. r=kTT02/ 0. Figure 4. The curve plots of the concentration dependence of free energies f[ (dotted lines) and f2 (full curves) in the region of temperatures of phase transitions I—HI (<5Pt—> <I>PtHx). The intersection and extremal points are marked with circles. r=kTT02/ 0.
The derived formulae (16), (18) allow us to elucidate the character of temperature dependence of the configurational heat capacity of sc and fee phases of fullerite of stoichiometric composition over the region of temperatures of phase transition from one phase to another. [Pg.222]

Other polymer properties also are important in addition to molecular weight and viscosity. If the polymer comes out of solution in the reactor as solid particles, then we would like to have the desired particle size distribution. Polymers composed of several different monomers, or copolymers, must have the appropriate compositions and segments along the polymer chain. The color of the polymer is important in some applications, as is the temperature of phase transitions, among other properties. [Pg.131]

Table 1. Heats and temperatures of phase transition of crystalline VO2. Table 1. Heats and temperatures of phase transition of crystalline VO2.
The OOA was not designed for and does not apply to temperature dependencies of any kind in JT crystals. In particular, one cannot expect a reasonable estimate of the temperature of phase transitions in crystal lattice (structural), electron orbital, and/or spin system. This follows from the partitioning procedure that includes averaging over vibrational degrees of freedom. One can see the same reason from another perspective. The pseudo spin of a JT site, as the basic concept used in the OOA, operates in the basis of degenerate ground state wave functions. Excited vibronic states are beyond the pseudo spin setup. Therefore, in the OOA, by its very definition, temperature population of excited states does not make sense. [Pg.723]

As we mentioned in Section V, near the temperature of phase transition to the metaphase the solid state of alkyl- and alkoxybenzoic acids is unstable in relation to the formation of hydrogen-bonded open associates. The associates merge in polymer chains, which can include over 10 acid molecules. Let us treat how the statistical model described above can account for such a behavior of the associates. [Pg.518]

If step (2) results in an enhanced rate of transbilayer movement of the functional lipid because of the raised temperature, one would expect, upon bringing the pH back to 8 [step 3], to detect a new fast process accounting for the ester lipid that has moved from the interior to the exterior of the vesicles. This is in fact what the authors were able to monitor. By repetition of cycles (l>-(3), all the ester surfactant is eventually cleaved. By variation of the incubation time, a lifetime of the flip-flop process could be determined. The ti/2 data are reported in Table 3. Scrutiny of this table reveals that apart from the above-mentioned temperature of phase transition, the flip-flop process is also affected by the structure of the lipid backbone. For instance, dialkylammonium amphiphiles are much more mobile than those featuring a glycerolUke backbone increasing the length of the chain decreased the rate of... [Pg.125]

Fig. 12. Phase diagram of the PEIs 82a-i temperatures of phase transitions vs the number (n) of CH2 groups in the spacer... Fig. 12. Phase diagram of the PEIs 82a-i temperatures of phase transitions vs the number (n) of CH2 groups in the spacer...
Orthoscopic examination with crossed polars is carried out first of all to determine the isotropism or the anisotropism of a sample. The polarization colors, the defects and variation in molecular orientation, and the orientation pattern or texture of liquid crystals are observed in this examination. With a heating stage the temperature of phase transition is also determined. In addition, with use of a compensator, the determination of vibration directions of the ordinary and extraordinary rays, the determination of relative retardation and birefringence are possible. In this section, the optical basics for orthoscopic observations are briefly outlined. The description of textures frequently observed for polymeric liquid crystals is given in Section 4.1.4. [Pg.201]

Figure 10-3. Temperatures of phase transition of the epsilon form of n-alkylammonium bromides, illustrating the odd-even effect... Figure 10-3. Temperatures of phase transition of the epsilon form of n-alkylammonium bromides, illustrating the odd-even effect...
Figure 10-6. TGA and DSC scans of crystals of C18Br.H20, one n-alkylammonium bromide monohydrate. Temperatures of phase transitions as observed by DSC are indicated widi dotted Unes... Figure 10-6. TGA and DSC scans of crystals of C18Br.H20, one n-alkylammonium bromide monohydrate. Temperatures of phase transitions as observed by DSC are indicated widi dotted Unes...
Temperatures of phase transitions (melting point and transition... [Pg.247]

Equation (3.18) represents the temperature of phase transition from paraelectric phase, that exists at T > 7/(/), into ferroelectric phase at T < 7/(/). The same transition can be obtained at fixed temperature T, but at some critical thickness / , so that at / < Icr paraelectric phase emerges and at / > Icr the ferroelectric phase exists. The temperature dependence of critical thickness can be found from the condition Tfdcr) = T, that leads (with respect to Eq. (3.18)) to the expression... [Pg.98]

L and dependence on temperature and film thickness in Fig. 3.24. It follows from Fig. 3.24a, c, that at fixed temperature the average polarization L decreases for the film thinning (compare curves 1-5). Built-in field smears the temperature of phase transition and susceptibility maximum its influence increases with the films thinning (see Fig. 3.24b, d). Moreover, the order parameter behavior for the thinnest possible films resembles that for thin films of ordered ferroelectrics with the thickness less than critical one (compare the curves 5 in Fig. 3.24c, d with Fig. in the paper [54]). Built-in field induces order parameter in the film with maximal disorder, see dotted curves 5 in Fig. 3.24a, b. However hysteresis loops is absent on these curves so that the behavior resembles that of electret state. [Pg.136]

DMA damping curves of glass cloth treated either with 2.5 wt% solutions of MS or, 7-MPS (Fig. 4) displayed similar bimodality to that shown by GPC curves, though temperatures of phase transitions shown by the two silanes were different... [Pg.146]

Embryonic Tissue/Organ Temperature of Phase Transition (°C) Liquid Crystal in Diseases Ref. [Pg.645]


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Field-Induced Shifts of the Phase Transition Temperatures

Of phase transition

Phase transition temperature

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Temperature of transition

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