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Critical volume locus

Figure 2. Critical pressure locus for Figure 3. Critical volume locus for CO2 — 1-hexene mixtures. CO2 — 1-hexene mixtures. Figure 2. Critical pressure locus for Figure 3. Critical volume locus for CO2 — 1-hexene mixtures. CO2 — 1-hexene mixtures.
Clarke and Vincent in these studies established the phase diagrams for the free polystyrene-microgel-ethyl benzene systems, two of which are displayed in Fig. 16.2a and b. In all cases, only the stability/instability boun ry is shown. These lines correspond to the locus of the critical volume fraction of free polymer required to induce flocculation (vj ) as a function of the volume fraction of the microgel particles (< 3). [Pg.356]

Figure 7.4 The Subcritical Fluid Cliromatography range. This occupies the volume in the phase diagram below the locus of critical temperatures, above and below the locus of critical pressures, and is composed mostly of the more volatile mobile-phase component. Reproduced by peimission of the American Chemical Society. Figure 7.4 The Subcritical Fluid Cliromatography range. This occupies the volume in the phase diagram below the locus of critical temperatures, above and below the locus of critical pressures, and is composed mostly of the more volatile mobile-phase component. Reproduced by peimission of the American Chemical Society.
Figure 2-10 shows a more nearly complete pressure-volume diagram.2 The dashed line shows the locus of all bubble points and dew points. The area within the dashed line indicates conditions for which liquid and gas coexist. Often this area is called the saturation envelope. The bubble-point line and dew-point line coincide at the critical point. Notice that the isotherm at the critical temperature shows a point of horizontal inflection as it passes through the critical pressure. [Pg.59]

The phase behaviour of blends of homopolymers containing block copolymers is governed by a competition between macrophase separation of the homopolymer and microphase separation of the block copolymers. The former occurs at a wavenumber q = 0, whereas the latter is characterized by q + 0. The locus of critical transitions at q, the so-called X line, is divided into q = 0 and q + 0 branches by the (isotropic) Lifshitz point. The Lifshitz point can be described using a simple Landau-Ginzburg free-energy functional for a scalar order parameter rp(r), which for ternary blends containing block copolymers is the total volume fraction of, say, A monomers. The free energy density can be written (Selke 1992)... [Pg.391]

Besides, the molecular comparisons also embrace several critical and vital aspects to expatiate molecular modeling in drug design, such as volume mapping, locus maps, vector maps and conformational mimicry, directionality, and field effects. [Pg.90]


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See also in sourсe #XX -- [ Pg.3 , Pg.5 , Pg.6 ]




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