Construction of a DOPC/PSM/cholesterol phase diagram based on the fluorescence properties of trans-parinaric acid

Cell membranes have a nonhomogenous lateral organization. Most information about such nonhomogenous mixing has been obtained from model membrane studies where defined lipid mixtures have been characterized. Various experimental approaches have been used to determine binary and ternary phase diagrams for systems under equilibrium conditions. Such phase diagrams are the most useful tools for understanding the lateral organization in cellular membranes. Here we have used the fluorescence properties of trans-parinaric acid (tPA) for phase diagram determination. The fluorescence intensity, anisotropy, and fluorescence lifetimes of tPA were measured in bilayers composed of one to three lipid components. All of these parameters could be used to determine the presence of liquid-ordered and gel phases in the samples. However, the clearest information about the phase state of the lipid bilayers was obtained from the fluorescence lifetimes of tPA. This is due to the fact that an intermediate-length lifetime was found in samples that contain a liquid-ordered phase and a long lifetime was found in samples that contained a gel phase, whereas tPA in the liquid-disordered phase has a markedly shorter fluorescence lifetime. On the basis of the measured fluorescence parameters, a phase diagram for the 1,2-dioleoyl-sn-glycero-3-phosphocholine/N-palmitoyl sphingomyelin/cholesterol system at 23 °C was prepared with a 5 mol % resolution. We conclude that tPA is a good fluorophore for probing the phase behavior of complex lipid mixtures, especially because multilamellar vesicles can be used. The determined phase diagram shows a clear resemblance to the microscopically determined phase diagram for the same system. However, there are also significant differences that likely are due to tPA's sensitivity to the presence of submicroscopic liquid-ordered and gel phase domains.     

Interactions of surfactants and fatty acids with lipids

The recent studies on the interaction of surfactants and fatty acids with lipids are inspired by the want of knowledge from several research fields of highest activity: identification of membrane rafts; membrane protein crystallization; formation of non-lamellar phases in membranes; membrane fusion. Detailed phase diagrams for lipid–surfactant and lipid–fatty acid mixtures, obtained in the last few years, reveal complicated mesomorphic and polymorphic behavior, including miscibility gaps and compound formation. Surfactant-induced non-lamellar to lamellar transitions in lipids and specific temperature-driven bilayer–micelle transitions represent extensions of the general three-stage model of membrane solubilization. Further research is required to construct phase diagrams as to delineate the principles of lipid–surfactant and lipid–fatty acid interactions for the variety of membrane lipid classes.     

Multicomponent membranes on solid substrates: Interfaces for protein binding

Even though lipid membranes deposited on a solid support are now used for more than 20 years as a model system for cellular membranes, their potential has, as yet, not been fully exploited. Only in recent years, the composition of solid supported membranes became more and more complex, which is a prerequisite for the elucidation of biologically relevant protein adsorption processes. Multicomponent bilayers resemble the heterogeneity of the biological membrane, which is composed of hundreds of different lipids varying in their headgroup and acyl chain composition. The development of a multitude of elaborated surface sensitive techniques allows to study the phase behavior of these membranes and their interaction with proteins, some of which will be highlighted in this review.     

PREPARATION OF EVOH MICROPOROUS MEMBRANES via THERMALLY INDUCED PHASE SEPARATION USING BINARY SOLVENTS

Microporous ethylene-vinyl alcohol copolymer （EVOH） flat membranes and hollow-fiber membranes with 38 mol% ethylene content were prepared via thermally induced phase separation （TIPS） using the mixture of 1,4-butanediol and poly（ethylene glycol）（PEG400） as diluents. Effects of the ratio of 1,4-butanediol to PEG400 on the phase diagrams, phase separation mechanism and membrane morphology were studied by small angle light scattering （SALS） measurements, differential scanning calorimetry （DSC）, and scanning ele~：tron microscopy （SEM）. It was found that by varying the composition of the binary solvent, the phase diagrams and membrane morphology can be controlled successfully. Moreover, the phase diagrams showed that broader regions of Liquid-Liquid （L-L） phase separation were obtained, as well as closer distances between L-L phase separation lines and Solid-Liquid （S-L） phase separation lines, Interconnected structures observed both in the flat membrane and hollow fiber membrane consist with the above results.     

Calculation of phase diagrams of ternary M-Ga-Sb (M = In,Al) systems by convex hull approach

The ternary semiconductor phase diagrams of M-Ga-Sb (M = In, Al) are calculated by means of the convex hull approach. The software package TernAPI is tested as an effective tool for these purposes. The new facilities and advantages of this package are proven. It enables one to construct ternary phase diagrams based on thermodynamic properties of all phases existing in systems. The changes in phase region shapes and phase transformations with temperature can be studied by means of the TernAPI package. Selection of reliable thermodynamic models of solutions is of crucial importance for correct calculations of phase equilibria. It is shown that an adequate phase diagram can be constructed when a polynomial model of liquid solutions in the Al-Ga-Sb system is used.     

Optimization and Calculation of the EuCl<Subscript>3</Subscript>–MCl (M = Na,K, Rb,Cs) Phase Diagrams

By using the CALPHAD technique, an optimization of the binary EuCl₃–MCl (M = Na, K, Rb, Cs) systems has been carried out. To describe the Gibbs energies of liquid phases in these systems the new modified quasi-chemical model was used in the pair-approximation for short-range ordering. From the measured phase equilibrium data and the experimental thermo-chemical properties, the EuCl₃–MCl phase diagrams were optimized and calculated. A set of thermodynamic functions has been optimized based on an interactive computer-assisted analysis. The calculated phase diagrams and thermodynamic data are self-consistent.     

Nonuniform lipid distribution in membranes

The noniform lateral and transbilayer lipid arrangement existing in two-component lipid bilayers are reviewed.

The lateral lipid organization is considered on the basis of the temperature-composition phase diagrams of the lipid binaries. A comparative analysis of the phase diagrams of synthetic phospholipid mixtures is carried out. The various types of the phase diagrams observed are set in a continuous row determined by the increase of the lipid lateral immiscibility. A special emphasis is laid on the appearance of peculiar points in the phase diagrams--triple, critical, and isoconcentration points. Two basic statistical-mechanical methods for simulation of phase diagrams--Bragg-Williams (regular solutions, mean field) and quasichemical--are compared. Stability criteria indicating the regions of lateral phase separation are also given. The main advantage of the quasichemical method is that it also allows the short-range order in the lipid arrangement to be determined.

The physical interactions contributing to an equilibrium lipid asymmetry in mixed lipid bilayers are pointed out. The most important among them are: (i) electrostatic forces induced by differences in the membrane electric double layers; (ii) nonideal lateral mixing of the lipids; (iii) packing restrictions important in curved bilayers.

A unified electrostatic model is presented to calculate the surface charge asymmetry created by any factors affecting the electric double layers of the bilayer (external electric potential, overlapping electric double layers in parallel membranes or in vescicles, etc.).

The transmembrane asymmetry strongly depends on the degree of c corrections may increase up two-three times the asymmetry induced by factors of the order of 1–3 kT. A typical nonideality effect, which may be used in an experimental verification, is the appearance of an extremum in the dependence of the asymmetry on the mole fraction of the components.

As previously shown in other reviews on membrane organization, the packing restrictions are of importance in highly curved bilayers, e.g., in small unilamellar vesicles.

The experimental data on the asymmetry of two-component small unilamellar vesicles are summarized and some general conclusions are formulated.

With a view toward the native membranes, some inferences are drawn about (i) the state of thermodynamic equilibrium and (ii) the lipid organization in multicomponent membranes.     

Quantitative effect of nonionic surfactant partitioning on the hydrophile-lipophile balance temperature

Phase behaviors of water/nonionic surfactants/isooctane systems are determined experimentally in temperature-global surfactant concentration diagrams. The surfactants are monodistributed polyoxyethylene glycol n-dodecyl ether. They are used as model mixtures of two, three, or five compounds or as constituents of a commercial surfactant. It is found that the phase diagrams of these systems are bent gradually toward the highest temperatures as the global surfactant concentration decreases. Each phase diagram is well-characterized by the curve of the HLB (hydrophile-lipophile balance) temperature versus the global surfactant concentration. For any fixed global surfactant concentration, this temperature is the middle temperature of the three-phase region; it can be calculated from an additive rule of the HLB temperatures of the surfactants weighted by their mole fractions at the water/oil interface. These mole fractions are determined through the pseudophase model using surfactant partitioning. Calculations require the knowledge of the critical micelle concentration, the partition coefficient between water and oil, and the HLB temperature of each surfactant of the mixture. This treatment can be used to correctly predict the variation of the HLB temperatures of the surfactant mixtures studied versus the global surfactant concentration. Furthermore, these calculations show that the observed curvature of the phase diagrams at the lowest global concentrations is due to the most favorable partitioning toward the oil of the lowest ethoxylated surfactant molecules.     

超临界CO_2诱导相转化法制备聚苯乙烯膜及膜体系的相图计算

以甲苯为溶剂,利用超临界CO_2诱导相转化法制备了多孔非对称聚苯乙烯膜.通过扫描电镜对膜结构进行了表征,探讨了不同温度、压力和铸膜液中聚苯乙烯浓度对膜形态、孔径分布及膜孔隙率的影响;同时,基于Tompa扩展的Flory-Huggins聚合物溶液理论计算了聚苯乙烯/超临界CO_2/甲苯铸膜体系的三元相图.研究表明,在温度为35~65℃、压力为8~16 MPa及聚合物质量分数为15%~35%条件下,制备的聚苯乙烯膜截面呈胞腔状孔结构,孔隙率为53.54%~84.67%,且孔隙率随温度、压力和聚苯乙烯浓度均呈现出先增大后减小的趋势.相图计算结果表明,温度对体系双节线位置的改变影响较小,而压力对其影响相对较大.     

A molecular theory including hard rod interactions of liquid crystalline phases exhibited by highly polar compounds

We extend our molecular mean field model of highly polar compounds to include hard rod interactions to develop a hybrid model. The latter interactions are restricted to second virial terms, following a method developed by Koda and Kimura. This allows us to calculate pressure-temperature phase diagrams. Depending on the model parameters used, the phase diagrams exhibit the following features: nematic-nematic phase transition, bounded SmA_d region, double reentrance, reentrant nematic lake surrounded by the smectic A phase (the reentrant nematic lake merging with the main nematic sea) as well as the possibility of quadruple reentrance. We compare the calculated phase diagrams with the available experimental data.     

A molecular theory including hard rod interactions of liquid crystalline phases exhibited by highly polar compounds

We extend our molecular mean field model of highly polar compounds to include hard rod interactions to develop a hybrid model. The latter interactions are restricted to second virial terms, following a method developed by Koda and Kimura. This allows us to calculate pressure-temperature phase diagrams. Depending on the model parameters used, the phase diagrams exhibit the following features: nematic-nematic phase transition, bounded SmA_d region, double reentrance, reentrant nematic lake surrounded by the smectic A phase (the reentrant nematic lake merging with the main nematic sea) as well as the possibility of quadruple reentrance. We compare the calculated phase diagrams with the available experimental data.     

A simple statistical mechanical theory for the mutual solubility of fluid mixtures of water and organic solvents under high pressure

A simple statistical mechanical theory is presented to explain phase diagrams of fluid mixtures with both a lower critical solution temperature and an upper critical solution temperature under pressure. By postulating a temperature dependence for the interaction free energy parameter of the constituent molecules and a pressure dependence for the excess volume, phase diagrams with both lower critical solution temperature, and upper critical solution temperature and their pressure dependence can be reproduced by quadratic surfaces in temperature-concentration-pressure space. The topological aspects of the observed phase diagrams in this space have been related to our theoretical model, and the thermodynamical meaning of the topologies has been interpreted based on our model. Experimental data for the mutual solubility of water and 2-butanol under pressure and that of water and 3-methylpyridine with added salts have been analyzed quantitatively and theoretical parameters are determined.     

Induced smectic phases in phase diagrams of binary nematic liquid crystal mixtures

To elucidate induced smectic A and smectic B phases in binary nematic liquid crystal mixtures, a generalized thermodynamic model has been developed in the framework of a combined Flory-Huggins free energy for isotropic mixing, Maier-Saupe free energy for orientational ordering, McMillan free energy for smectic ordering, Chandrasekhar-Clark free energy for hexagonal ordering, and phase field free energy for crystal solidification. Although nematic constituents have no smectic phase, the complexation between these constituent liquid crystal molecules in their mixture resulted in a more stable ordered phase such as smectic A or B phases. Various phase transitions of crystal-smectic, smectic-nematic, and nematic-isotropic phases have been determined by minimizing the above combined free energies with respect to each order parameter of these mesophases. By changing the strengths of anisotropic interaction and hexagonal interaction parameters, the present model captures the induced smectic A or smectic B phases of the binary nematic mixtures. Of particular importance is the fact that the calculated phase diagrams show remarkable agreement with the experimental phase diagrams of binary nematic liquid crystal mixtures involving induced smectic A or induced smectic B phase.     

Diagramme d’equilibre liquide-solide de systemes binaires pyridine+n-alcanes

Solid-liquid phase diagrams have been determined for binary systems of pyridine withn-alkanes. These diagrams show the existence of large regions of partial miscibility. A general quasi chemical theory in terms of group surface interactions [1] has been applied to compute these solid-liquid phase diagrams.     

Energetics of cholesterol transfer between lipid bilayers

It is believed that natural biological membranes contain domains of lipid ordered phase enriched in cholesterol and sphingomyelin. Although the existence of these domains, called lipid rafts, is still not firmly established for natural membranes, direct microscopic observations and phase diagrams obtained from the study of three-component mixtures containing saturated phospholipids, unsaturated phospholipids, and cholesterol demonstrate the existence of lipid rafts in synthetic membranes. The presence of the domains or rafts in these membranes is often ascribed to the preferential interactions between cholesterol and saturated phospholipids, for example, between cholesterol and sphingomyelin. In this work, we calculate, using molecular dynamics computer simulation technique, the free energy of cholesterol transfer from the bilayer containing unsaturated phosphatidylcholine lipid molecules to the bilayer containing sphingomyelin molecules and find that the affinity of cholesterol to sphingomyelin is higher. Our calculations of the free-energy components, energy and entropy, show that cholesterol transfer is exothermic and promoted by the favorable change in the lipid-lipid interactions near cholesterol and not by the favorable energy of cholesterol-sphingomyelin interaction, as assumed previously.     

Theoretical studies of O-O bond formation in photosystem II

The most critical part of dioxygen evolution in photosystem II is the O-O bond formation step. In order to reach an efficient mechanism, nature uses a unique oxygen-evolving complex (OEC) having four manganese and one calcium center. Even though the structure of the OEC has become much more clear during recent years, it has still been difficult to find a transition state (TS) for O-O bond formation with a sufficiently low barrier. However, about a year ago, a quite surprising type of TS was found. With the latest X-ray ligand assignment, the local barrier for this TS is only 5.1 kcal/mol. It can be described as an attack by an oxygen radical, held by a dangling manganese, on a bridging oxo ligand in the Mn3Ca cube. In the present short Article, energy diagrams describing the entire process of dioxygen formation will be presented. An important conclusion drawn from these diagrams is that the major features of dioxygen formation remain the same irrespective of which one of the experimentally suggested structures the diagram is built on. Compared to earlier presentations of the same type, a slightly different approach has been used for setting up the diagrams. Results from a recent experimental study of the pressure dependence of oxygen release have been used to define the final energy levels. The loss of energy in the electron transfer from Tyrz to P680 has also been incorporated into the diagrams. A good agreement with experimental observations is demonstrated.     

Phase diagrams of diastereomeric pairs in inclusion resolution

In the development and understanding of the resolution of diastereomeric salts, phase diagrams are of great importance. This study constitutes the first example of phase diagrams of diastereomeric complexes formed from simple chiral compounds, as used in inclusion resolutions. Simple melting diagrams and DSC thermograms could not be used, because of the decomposition of the complex caused by the escape of the guest from the inclusion complex upon heating. A ternary solution phase diagram was constructed from the diastereomeric inclusion complexes of phenethylamine with a taddol. Solid solution behavior was found and confirmed by powder diffraction and X-ray studies. The limited scope of inclusion resolutions, as already indicated by our earlier studies, was confirmed by these results.     

Determining scaling in known phase diagrams of nonionic microemulsions to aid constructing unknown

Microemulsions based on nonionic surfactants of the ethylene oxide alkyl ether type C_mE_n, have been studied thoroughly for around 30 years. Thanks to the considerable amount of published data available on these systems, it is possible to observe trends to make predictions of phase diagrams not yet determined. Strey and Kahlweit, and subsequently Sottmann and Strey, with coworkers have studied and published phase diagrams for systems with a fixed ratio of oil to water, varying the surfactant, the so-called Kahlweit fish-cut diagrams. Some properties of the phase diagrams can be scaled to become general and not system dependent. Here are shown two examples of scaling data from phase diagrams and the use of trends to determine phase diagrams, both inside and outside a dataset. The trends of microemulsions with fixed ratio of surfactant to oil, the so-called Lund-cut diagrams, are also investigated. The trends are used to determine a new phase diagram and this is compared with previously unpublished experimental data on C₁₂E₅-Octadecane-Water system. The scalings and trends make it possible to get good estimations of many of the important properties of the phase diagrams, both temperatures and surfactant concentrations of interest, by investigating one sample in the 3-phase region of the balanced fish-cut diagram.     

Inorganic membranes for hydrogen production and purification: a critical review and perspective

Hydrogen as a high-quality and clean energy carrier has attracted renewed and ever-increasing attention around the world in recent years, mainly due to developments in fuel cells and environmental pressures including climate change issues. In thermochemical processes for hydrogen production from fossil fuels, separation and purification is a critical technology. Where water-gas shift reaction is involved for converting the carbon monoxide to hydrogen, membrane reactors show great promises for shifting the equilibrium. Membranes are also important to the subsequent purification of hydrogen. For hydrogen production and purification, there are generally two classes of membranes both being inorganic: dense phase metal and metal alloys, and porous ceramic membranes. Porous ceramic membranes are normally prepared by sol-gel or hydrothermal methods, and have high stability and durability in high temperature, harsh impurity and hydrothermal environments. In particular, microporous membranes show promises in water gas shift reaction at higher temperatures. In this article, we review the recent advances in both dense phase metal and porous ceramic membranes, and compare their separation properties and performance in membrane reactor systems. The preparation, characterization and permeation of the various membranes will be presented and discussed. We also aim to examine the critical issues in these membranes with respect to the technical and economical advantages and disadvantages. Discussions will also be made on the relevance and importance of membrane technology to the new generation of zero-emission power technologies.