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INDEX phase diagram

Figure 10.18 Dynamic light scattering (DLS) of vesicle mixtures, (a) P-index phase diagram and (b) size distributions (from DLS) for DDAB-oleate mixtures, total concentration 1 mM in 0.2 M borate buffer at pH 8.5, 25.0 °C, scattering angle 90°. (From Thomas and Luisi, 2004.)... Figure 10.18 Dynamic light scattering (DLS) of vesicle mixtures, (a) P-index phase diagram and (b) size distributions (from DLS) for DDAB-oleate mixtures, total concentration 1 mM in 0.2 M borate buffer at pH 8.5, 25.0 °C, scattering angle 90°. (From Thomas and Luisi, 2004.)...
As an indication of the central role that phase diagrams now play in the whole of materials science, the cumulative index for the whole of the 18-volume book series. Materials Science and Technology (Cahn et al. 1991-1998) can be cited in evidence. There are 89 entries under the heading phase diagram , one of the most extensive of all listings in this 390-page index. [Pg.82]

The strength of the Cu-0 bond will be lower on the Cu(lll) face than on the Cu(100) and Cu(110).593 Indeed, the Cu-0 stretching frequency in UHV is lowest on the (111) face and only a disordered oxygen structure is observed.596 These results suggest that a specific Pourbaix pH -E phase diagram is needed to describe the behavior of each low-index face of Cu. [Pg.93]

W. G. Moffatt, The Handbook of Binary Phase Diagrams, General Electric Co., Schenectady, NY, 1977. Lxxiseleaf system in three volumes with regular updating. Contains excellent index to material contained in refs. 1-3. [Pg.471]

Figure 5.11 (T, a, A< ) phase diagrams for all low index surfaces of a-Pt02 (a) and P-PVO2... Figure 5.11 (T, a, A< ) phase diagrams for all low index surfaces of a-Pt02 (a) and P-PVO2...
Figure 14. The phase diagram of the gradient copolymer melt with the distribution functions g(x) = l — tanh(ciit(x —fo)) shown in the insert of this figure for ci = 3,/o = 0.5 (solid line), and/o — 0.3 (dashed line), x gives the position of ith monomer from the end of the chain in the units of the linear chain length. % is the Flory-Huggins interaction parameter, N is a polymerization index, and/ is the composition (/ = J0 g(x) dx). The Euler characteristic of the isotropic phase (I) is zero, and that of the hexagonal phase (H) is zero. For the bcc phase (B), XEuier = 4 per unit cell for the double gyroid phase (G), XEuier = -16 per unit cell and for the lamellar phases (LAM), XEuier = 0. Figure 14. The phase diagram of the gradient copolymer melt with the distribution functions g(x) = l — tanh(ciit(x —fo)) shown in the insert of this figure for ci = 3,/o = 0.5 (solid line), and/o — 0.3 (dashed line), x gives the position of ith monomer from the end of the chain in the units of the linear chain length. % is the Flory-Huggins interaction parameter, N is a polymerization index, and/ is the composition (/ = J0 g(x) dx). The Euler characteristic of the isotropic phase (I) is zero, and that of the hexagonal phase (H) is zero. For the bcc phase (B), XEuier = 4 per unit cell for the double gyroid phase (G), XEuier = -16 per unit cell and for the lamellar phases (LAM), XEuier = 0.
Fig. 13.3. The phase diagram of Ao.33A o.67Mn03 (A = divalent cation, A = rare earth) as a function of temperature and the global instability index of the idealized perovskite structure. The points show the observed transition temperatures in various compounds. FMM = ferromagnetic metal, PMI = paramagnetic insulator, FMI = ferromagnetic insulator (from Rao et al. 1998). Fig. 13.3. The phase diagram of Ao.33A o.67Mn03 (A = divalent cation, A = rare earth) as a function of temperature and the global instability index of the idealized perovskite structure. The points show the observed transition temperatures in various compounds. FMM = ferromagnetic metal, PMI = paramagnetic insulator, FMI = ferromagnetic insulator (from Rao et al. 1998).
The American Ceramic Society (ACerS) (ed) (1996) Cumulative Indexes of Phase Equilibria Diagrams - Phase Diagrams for Ceramists . Vol I-XII and Annuals 91-93, Westerville, Ohio... [Pg.150]

Fig. 17. Phase diagram for intermediately segregated (%N=20) symmetric diblock (f=0.5) films confined between identical walls calculated from self-consistent field theory. The film thickness D is normalized by the bulk lamellar period Xb, and the ordinate AN is a measure of the surface field (which has the functional form H(z)=Aj (+cos(ti z/ )) bVN /e for 0 Fig. 17. Phase diagram for intermediately segregated (%N=20) symmetric diblock (f=0.5) films confined between identical walls calculated from self-consistent field theory. The film thickness D is normalized by the bulk lamellar period Xb, and the ordinate AN is a measure of the surface field (which has the functional form H(z)=Aj (+cos(ti z/ )) bVN /e for 0<z< , and an analogous form at the other wall). The index v of the phases Lv denotes the number of A/B interfaces parallel to the walls. From Matsen [63]...
Fig. 2.1 shows the phase diagram. For clarity, the polymorphism of C3S and the distinction between a - and a L-C2S are omitted. Calcium oxide (CaO) has the sodium chloride structure, in which all ions are octahedrally coordinated the unit cell is cubic, with a = 0.48105 nm, space group Fm3m, Z = 4, = 3345 kgm (S5). The refractive index is 1.837 (W3). [Pg.33]

Koynova R, Caffrey M. An index of lipid phase diagrams. Chem. Phys. Lipids 2002 115 107-219. [Pg.855]

Among other things, it became established that the nature of the structure adopted by a given compound on crystallization would then exert a profound effect on the solid-state properties of that system. For a given material, the heat capacity, conductivity, volume, density, viscosity, surface tension, diffusivity, crystal hardness, crystal shape and color, refractive index, electrolytic conductivity, melting or sublimation properties, latent heat of fusion, heat of solution, solubility, dissolution rate, enthalpy of transitions, phase diagrams, stability, hygroscopicity, and rates of reactions were all affected by the nature of the crystal structure. [Pg.2935]

Figure 4. Comparison of the phase diagrams determined from the refractive index measurements with that obtained by the visual method. The weight fraction w is the concentration variable. Empty symbols are used, when the compositions are estimated from refractive index data (Cemim+BFJ in 1-butanol (A), 1-pentanol (y), 2-butanol (0), and 2-pentanol (<)), full symbols, when the data are obtained by the visual method observing the separation temperature in samples of different composition (Gemini+ in water ( ), 1-propanol (O). 1-butanol (A), 2-butanol (y), 1-pentanol (0), 2-pentanol (<), and 1-hexanol (>)). Figure 4. Comparison of the phase diagrams determined from the refractive index measurements with that obtained by the visual method. The weight fraction w is the concentration variable. Empty symbols are used, when the compositions are estimated from refractive index data (Cemim+BFJ in 1-butanol (A), 1-pentanol (y), 2-butanol (0), and 2-pentanol (<)), full symbols, when the data are obtained by the visual method observing the separation temperature in samples of different composition (Gemini+ in water ( ), 1-propanol (O). 1-butanol (A), 2-butanol (y), 1-pentanol (0), 2-pentanol (<), and 1-hexanol (>)).

See other pages where INDEX phase diagram is mentioned: [Pg.659]    [Pg.153]    [Pg.264]    [Pg.324]    [Pg.46]    [Pg.97]    [Pg.190]    [Pg.987]    [Pg.376]    [Pg.240]    [Pg.185]    [Pg.128]    [Pg.367]    [Pg.83]    [Pg.288]    [Pg.139]    [Pg.364]    [Pg.754]    [Pg.228]    [Pg.204]    [Pg.168]    [Pg.382]    [Pg.332]   


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Diagrams 212 INDEX

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