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Four phase interactions

If tire mean Aq is positive tlien tire majority of tire residues are hydrophilic. A description of tire collapsed phase of tire chain requires introducing tliree- and and four-body interaction tenns. Thus, tire total Hamiltonian is... [Pg.2660]

The most popular bonded phases are, without doubt, the reverse phases which consist solely of aliphatic hydrocarbon chains bonded to the silica. Reverse phases interact dispersively with solvent and solute molecules and, as a consequence, are employed with very polar solvents or aqueous solvent mixtures such as methanol/water and acetonitrile/water mixtures. The most commonly used reverse phase appears to be the brush type phase with aliphatic chains having four, eight or eighteen carbon atom chains attached. These types of reverse phase have been termed C4, C8 and Cl8 phases respectively. The C8... [Pg.76]

Steric repulsions come from two orbital-four electron interactions between two occupied orbitals. Facially selective reactions do occur in sterically unbiased systems, and these facial selectivities can be interpreted in terms of unsymmetrical K faces. Particular emphasis has been placed on the dissymmetrization of the orbital extension, i.e., orbital distortions [1, 2]. The orbital distortions are described in (Chapter Orbital Mixing Rules by Inagaki in this volume). Here, we review the effects of unsymmetrization of the orbitals due to phase environment in the vicinity of the reaction centers [3]. [Pg.130]

Now we consider thermodynamic properties of the system described by the Hamiltonian (2.4.5) it is a generalized Hamiltonian of the isotropic Ashkin-Teller model100,101 expressed in terms of interactions between pairs of spins lattice site nm of a square lattice. Hamiltonian (2.4.5) differs from the known one in that it includes not only the contribution from the four-spin interaction (the term with the coefficient J3), but also the anisotropic contribution (the term with the coefficient J2) which accounts for cross interactions of spins a m and s m between neighboring lattice sites. This term is so structured that it vanishes if there are no fluctuation interactions between cr- and s-subsystems. As a result, with sufficiently small coefficients J2, we arrive at a typical phase diagram of the isotropic Ashkin-Teller model,101 102 limited by the plausible values of coefficients in Eq. (2.4.6). At J, > J3, the phase transition line... [Pg.44]

Figure 7.6. Comparison of (a) experimental phase diagram for the Cu-Au system (Hansen 1958) with (b) predictions for the Cu-Au system calculated using the tetrahedron approximation but including asymmetric four-body interactions (de Fontaine and Kikuchi 1978). Figure 7.6. Comparison of (a) experimental phase diagram for the Cu-Au system (Hansen 1958) with (b) predictions for the Cu-Au system calculated using the tetrahedron approximation but including asymmetric four-body interactions (de Fontaine and Kikuchi 1978).
DSC traces of mixtures of cationic lipid (20 with DOPC (Fig. 34) indicate strong interaction between the components. Upon heating, the unpolymerized vesicle dispersion exhibits four phase transitions none of which corresponds to the pure... [Pg.35]

To describe the phase diagram of cuprates, where we observe four phase separations, we consider a Poole model with three different anisotropic interactions yi, y2, and y3 giving rise to three different intermediate phases with preferential volume VyI, Vy2 and Vys respectively. [Pg.149]

Figure 1 Schematic representation of a time-resolved coherent Raman experiment, (a) The excitation of the vibrational level is accomplished by a two-photon process the laser (L) and Stokes (S) photons are represented by vertical arrows. The wave vectors of the two pump fields determine the wave vector of the coherent excitation, kv. (b) At a later time the coherent probing process involving again two photons takes place the probe pulse and the anti-Stokes scattering are denoted by subscripts P and A, respectively. The scattering signal emitted under phase-matching conditions is a measure of the coherent excitation at the probing time, (c) Four-photon interaction scheme for the generation of coherent anti-Stokes Raman scattering of the vibrational transition. Figure 1 Schematic representation of a time-resolved coherent Raman experiment, (a) The excitation of the vibrational level is accomplished by a two-photon process the laser (L) and Stokes (S) photons are represented by vertical arrows. The wave vectors of the two pump fields determine the wave vector of the coherent excitation, kv. (b) At a later time the coherent probing process involving again two photons takes place the probe pulse and the anti-Stokes scattering are denoted by subscripts P and A, respectively. The scattering signal emitted under phase-matching conditions is a measure of the coherent excitation at the probing time, (c) Four-photon interaction scheme for the generation of coherent anti-Stokes Raman scattering of the vibrational transition.
Stable o/w creams prepared with ionic or nonionic emulsifying waxes are composed of (at least) four phases (Fig. 7.20) (f) dispersed oil phase, (2) crystalline gel phase, (3) crystalline hydrate phase, and (4) bulk aqueous phase containing a dilute solution of surfactant. The interaction of the surfactant and fatty alcohol components of emulsifying mixtures to form these stmctures (body) is critical. It is also time-dependent, giving the name self-bodying to these emulsions. The overall stability of a cream is dependent on the stability of the crystalline gel phase. [Pg.248]

Pseudoternary phase diagrams of the water-dodecane-SDS-pentanol and water-dodecane-SDS-hexanol systems have been investigated in detail. A great variety of new domains has been evidenced in the oil rich part of these diagrams including, one-, two-, three- and four-phase liquid regions. An interpretation of these diagrams is proposed it is shown that interactions between water domains play an important role in microemulsion stability. [Pg.105]

Extension of the model Hamiltonian to include higher-order interactions results in the Cu-Au phase diagram shown in fig. 6.24. In particular, the cluster expansion for the total energy in this case includes four-site interactions between those sites... [Pg.296]

The gas-phase interaction of the d fragment [Cp2ZrMe] with D2 to produce [Cp2ZrD] and CH3D showed a high second-order rate constant and collision efficiency consistent with a four-center transition state. " The lack of reversibility was attributed to greater Zr—bond strength. [Pg.290]


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Phase interaction

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