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Results for “Phase Transition”

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PubMed1982

Morphology of the intermediate stages in the lamellar to hexagonal lipid phase transition.

The addition of calcium to suspensions of egg phosphatidylcholine and cardiolipin converts multiwalled liposomes to the hexagonal (HII) phase (Rand, R.P., Sengupta, S. (1972) Biochim. Biophys. Acta 255:484-492). We have studied this lamellar to hexagonal phase transition by freeze-fracture, thin-section electron microscopy, and X-ray diffraction and have morphologically characterized the intermediate stages. The first step in the transition involves the invagination and fusion of bilayers, marked by the appearance of lipidic intramembrane particles and "crater-like" indentations, as the large liposomes are converted to smaller flattened and elongated vesicles. The next step is the formation of tightly packed hexagonal arrays of tubules, each tubule being about 11 to 15 nm in diameter. These tubules are filled with fluid and a lipid bilayer forms the wall of each cylinder. Finally this tubular bilayer phase is converted to the hexagonal (HII) phase, where the distance between tubes is 5.5 to 7.5 nm.

Cardiolipins↗

PubMed2004

Phase transition in tensionless surfaces.

We study the critical behavior of the Laplacian roughening model, which describes the growth of tensionless surfaces. This type of growth phenomena is very important, for instance, in biological membranes and in molecular beam epitaxy. We summarize previous analytical and numerical results and point out their contradictions and differences, thus making clear the context of our work. Our contribution, achieved through large-scale numerical simulations, is the confirmation that the model exhibits a single continuous phase transition: the transition takes place between a continuum massless (i.e., with infinite correlation length) bilaplacian behavior and a massive propagator (finite correlation length).

Models, Chemical↗

PubMed2005

Driving forces of phase transitions in surfactant and lipid systems.

In aqueous surfactant and lipid systems, different liquid crystalline phases are formed at different temperatures and water contents. The "natural" phase sequence implies that phases with higher curvature are formed at higher water contents. On the other hand, there are exceptions to this rule, such as the monoolein/water system. In this system an anomalous transition from lamellar to reverse cubic phase upon addition of water is observed. The calorimetric data presented here show that the hydration-induced transitions to phases with higher curvature are driven by enthalpy, while the transitions to phases with lower curvature are driven by entropy. It is shown that the driving forces of phase transitions can be determined from the appearance of the phase diagram using the approach based on van der Waals differential equation. From this approach it follows that the slope of the phase boundary should be positive with respect to water content if the phase diagram obeys the "natural" phase sequence. The increase of entropy, which drives the anomalous phase transitions, arises from the increase of disorder of the hydrocarbon chains.

Lipids↗

PubMed2003

Liquid-liquid phase transition in supercooled silicon.

Silicon in its liquid and amorphous forms occupies a unique position among amorphous materials. Obviously important in its own right, the amorphous form is structurally close to the group of 4-4, 3-5 and 2-6 amorphous semiconductors that have been found to have interesting pressure-induced semiconductor-to-metal phase transitions. On the other hand, its liquid form has much in common, thermodynamically, with water and other 'tetrahedral network' liquids that show density maxima. Proper study of the 'liquid-amorphous transition', documented for non-crystalline silicon by both experimental and computer simulation studies, may therefore also shed light on phase behaviour in these related materials. Here, we provide detailed and unambiguous simulation evidence that the transition in supercooled liquid silicon, in the Stillinger-Weber potential, is thermodynamically of first order and indeed occurs between two liquid states, as originally predicted by Aptekar. In addition we present evidence to support the relevance of spinodal divergences near such a transition, and the prediction that the transition marks a change in the liquid dynamic character from that of a fragile liquid to that of a strong liquid.

Computer Simulation↗

PubMed1976

Effect of the gel to liquid crystalline phase transition on the osmotic behaviour of phosphatidylcholine liposomes.

Aspects of osmotic properties of liposomes, prepared from synthetic lecithin, above, at and below the gel to liquid crystalline phase transition temperature are described. The experiments show that liposomal membranes with their lipids in the gel state are still permeable to water. The rate of water permeation changes drastically on passing the transition temperature. The water permeation has activation energies of 9.5 +/- 1.28 and 26.4 +/- 0.9 kcal/mol above and below the transition temperature, respectively, indicating that the diffusion processes take place by different mechanisms. With respect to the barrier properties of the liposomes in the vicinity of the transition temperature, the following conclusions can be made. (1) Studying the osmotic shrinkage of liposomes at a fixed temperature near the transition point, the experiments indicate that dimyristoyl phosphatidylcholine membranes are highly permeable to glucose under these conditions, where liquid and solid domains co-exist. Under the same conditions the osmotic experiments did not indicate a strong increase in glucose permeability of dipalmitoyl phosphatidylcholine membranes as compared to the situation above and below the transition temperature. (2) On the other hand, perturbations of the phase equilibrium by temperature varations resulted in a marked increase of the glucose permeation through dipalmitoyl phosphatidylcholine bilayers. Once a new phase equilibrium of liquid and solid regions is established the permeation rate of glucose is much less.

Binding Sites↗

PubMed2006

Phase transition in two-dimensional dipolar fluids at low densities.

Monte Carlo computer simulations of a quasi two-dimensional (2D) dipolar fluid at low and intermediate densities indicate that the structure of the fluid is well described by an ideal mixture of self-assembling clusters. A detailed analysis of the topology of the clusters, of their internal energy and of their size (or mass) distributions is used to obtain approximations to their partition functions. Within the scope of these approximations, the results of this work suggest that the 2D dipolar fluid undergoes a phase transition from a dilute phase characterized by a number of disconnected clusters to a condensed phase characterized by a network or spanning (macroscopic) cluster that includes most of the particles in the system.

Journal Article↗

PubMed2000

Synthesis, control of substitution pattern and phase transitions of 2,3-di-O-methylcellulose.

An improved heterogeneous procedure has been found for the regioselective introduction of trityl and 4-methoxytrityl groups at the primary positions of cellulose. The 6-O-tritylcelluloses produced were completely methylated by MeI-NaOH in Me2SO solution. The trityl groups were then completely removed to afford 2,3-di-O-methylcellulose without significant degradation of the polymer. 1H and 13C NMR spectroscopy and degradation analysis showed less than 5% deviation from the regular substitution pattern. Under optimum reaction conditions, almost perfectly regular cellulose derivatives could be obtained. Small changes in the substitution pattern had a strong effect on the phase transitions of the O-methylcelluloses in water. It was shown by DSC for the first time that perfect 2,3-di-O-methylcellulose does not undergo phase separation at elevated temperatures.

Magnetic Resonance Spectroscopy↗

PubMed2005

Lyotropic and thermotropic phase transitions in films of ionene-alkyl sulfate complexes.

Five [X,Y]-ionenes [(CH2)(X)N+(CH3)2(CH2)(Y)N+(CH3)2]nBr-(2n) were prepared (X = 3, 5; Y = 10, 12, 22). Using new preparation methods, dry, salt-free complexes with three n-alkyl sulfates (octyl, decyl, and dodecyl) were obtained. The ionenes and their complexes were characterized in methanol solution by light scattering, viscometry, and fluorescent probe studies. The solid materials were investigated by means of DSC, TG, and ATR-IR. Transparent films were formed from stoichiometric [3,10], [3,12], and [5,10]-ionene complexes with decyl and dodecyl sulfate. In the films, mesogenic phase transitions could be induced: dry films were optically isotropic; when exposed to elevated humidity, the films slowly became optically anisotropic because of a lyotropic transition to a hexagonal mesogenic phase. The relative humidity, at which the hexagonal phase developed, was distinct for each complex. The anisotropic phases were converted to isotropic in a thermotropic transition under controlled relative humidity at specific clearing temperatures, which were higher for dodecyl complexes than for decyl complexes. This thermotropic isotropic-anisotropic transition could be cycled several times, but partial hydrolysis of the alkyl sulfates reduced the reproducibility of transition points.

Journal Article↗

PubMed2006

Signatures of a noise-induced quantum phase transition in a mesoscopic metal ring.

We study a mesoscopic ring with an inline quantum dot threaded by an Aharonov-Bohm flux. Zero-point fluctuations of the electromagnetic environment capacitively coupled to the ring, with omega(s) spectral density, can suppress tunneling through the dot, resulting in a quantum phase transition from an unpolarized to a polarized phase. We show that robust signatures of such a transition can be found in the response of the persistent current in the ring to the external flux as well as to the bias between the dot and the arm. Particular attention is paid to the experimentally relevant cases of Ohmic (s = 1) and sub-Ohmic (s = 1/2) noise.

Journal Article↗

PubMed1992

Phenylbutazone action on dimiristoyl phosphatidylcholine liposome phase transition and 8-anilino-1-naphthalene sulfonate binding.

Phenylbutazone (PhB), a powerful anti-inflammatory drug, is able to modify the phase transition of phospholipid bilayers without changing its calorimetric enthalpy (delta Hcal), as can be shown by differential scanning calorimetry (DSC) experiments. Under PhB interaction, dimiristoyl phosphatidylcholine (DMPC) multilamellar liposomes (MLV) undergo lateral phase separation as a result of immiscibility in the bilayer plane. On the other hand, the binding of the anionic fluorescent probe 8-anilino-1-naphthalene sulfonate (ANS) to the surface of DMPC liposomes is altered by PhB. Even though the quantum efficacy of the probe fluorescence emission remains unaffected, the negative cooperativity of the binding process disappears, with the intrinsic dissociation constant showing only a minor variation. From these results it is concluded that PhB would be most likely located close to the lipid:water interface.

Anilino Naphthalenesulfonates↗

PubMed2004

Pressure-induced quantum phase transition in the spin-liquid TlCuCl3.

The condensation of magnetic quasiparticles into the nonmagnetic ground state has been used to explain novel magnetic ordering phenomena observed in quantum spin systems. We present neutron scattering results across the pressure-induced quantum phase transition and for the novel ordered phase of the magnetic insulator TlCuCl3, which are consistent with the theoretically predicted two degenerate gapless Goldstone modes, similar to the low-energy spin excitations in the field-induced case. These novel experimental findings complete the field-induced Bose-Einstein condensate picture and support the recently proposed field-pressure phase diagram common for quantum spin systems with an energy gap of singlet-triplet nature.

Journal Article↗

PubMed1983

The measurement of the kinetics of lipid phase transitions: a volume-perturbation kinetic calorimeter.

A volume-perturbation kinetic calorimeter to be used to study membrane phase transitions in lipid vesicles has been developed. In this instrument, the voltage-dependent extension of a stack of piezoelectric crystals is used to force the solution being studied to undergo a small adiabatic bidirectional volume change. This volume change induces a shift in the equilibrium position of the lipid gel to liquid-crystalline transition. The time course of the relaxation to the new equilibrium position is then monitored by observing the induced temperature and pressure changes as a function of time.

Calorimetry↗

PubMed1994

Interconversion of bilayer phase transition temperatures between phosphatidylethanolamines and phosphatidylcholines.

High-resolution differential scanning calorimetric studies were performed to investigate the thermotropic phase behavior of 31 molecular species of phosphatidylethanolamines in excess water. Upon reheating, the aqueous dispersions of these lipids undergo the gel to liquid-crystalline phase transitions at well defined temperatures (Tm). These Tm values were shown to relate to the structural parameters of the underlying lipid molecules in a characteristic manner. Based on these observations, an interconversion of the Tm values between saturated phosphatidylethanolamines and phosphatidylcholines is established quantitatively for the first time.

Calorimetry, Differential Scanning↗

PubMed1991

Phospholipid phase transitions: kinetics and structural mechanisms.

A brief review is given on the principles and methods used to investigate structural phase transitions in phospholipid supramolecular structures. The conceptual differences of approaches close to and far from equilibrium are addressed, and the consequences in terms of the limits of interpretation for different types of methods, in particular referring to jump-relaxation and steady-state techniques, are surveyed. With the emphasis on connecting dynamic and structural information, the results obtained so far from different techniques are reviewed, and the open questions addressed. The more recent advances by millisecond time-resolved X-ray diffraction with synchrotron radiation and their main results obtained for transitions triggered by IR-laser temperature jumps are summarized. As a major novel aspect in the field, the necessity of considering martensitic, diffusionless transformation mechanisms and the occurrence of intermediate structures is highlighted.

Kinetics↗

PubMed1992

Chain-length dependence of lipid bilayer properties near the liquid crystal to gel phase transition.

The temperature dependence of the mean orientational order parameter in the vicinity of the liquid crystal to gel phase transition is obtained from the first moment M1 of deuterium nuclear magnetic resonance spectra for bilayers of chain perdeuterated phosphatidylcholines with acyl chains of 12, 14, 16, and 18 carbons. The data clearly show an increasing temperature dependence of the orientational order parameter in the vicinity of the transition, with the effect becoming more pronounced with decreasing chain length. Assuming a linear relationship between the mean orientational order parameter and the extension of the acyl chain, estimates of the change in area of the membrane at the transition are shown to be consistent with those obtained from other measurements. It is shown that the transition may be modeled in terms of a Landau expansion of the free energy involving a small number of phenomenological parameters. From this it is shown that the behavior of these systems in the temperature range of interest is, in large part, controlled by the close proximity of a spinodal to the transition temperature.

Biophysical Phenomena↗

PubMed2003

Dynamics of a surface phase transition as monitored by in situ second harmonic generation.

The dynamics of the (2 x 2)-3CO <--> dilute phase transition involving CO adsorbed on Pt(111) microfacets has been monitored in situ in a CO-saturated acidic electrolyte using potential step-second harmonic generation techniques. Apparent time constants derived strictly from the optical data were found to be orders of magnitude slower for the forward process as compared to those of the reverse process. This behavior is consistent with the activated nature of CO electrooxidation, which requires the presence of a neighboring adsorbed oxygenated species, for example, hydroxyl, for the process to ensue.

Journal Article↗

PubMed2002

Phase transitions in the starch-water system studied by adiabatic scanning calorimetry.

We report high-precision measurements of phase transitions in the starch-water system by using for the first time adiabatic scanning calorimetry (ASC). Potato starch and nixtamalized corn flours were studied by this technique as a function of the moisture content. We calculated the percentage of gelatinized starch granules, as a function of the temperature, for both flours. For bi-phasic behavior in potato starch, at intermediate water contents, we propose an explanation based on previous hypotheses and on the experimental behavior as deduced from ASC measurements. ASC results suggest, in the case of nixtamalized corn flour, that uniform moisture is present in corn starch granules for all the considered moistures. A shift to higher temperatures of the peak temperature is observed when comparing the c(p)(T) curves with the classical DSC endotherms as measured for this flour. For both flours we estimated from the ASC results the melting temperatures of the starch granules, at zero moisture content, by using Flory's equation.

Calorimetry, Differential Scanning↗

PubMed2003

Exchange anisotropy and the dynamic phase transition in thin ferromagnetic Heisenberg films.

Monte Carlo simulations have been performed to investigate the dependence of the dynamic phase behavior on the bilinear exchange anisotropy of a classical Heisenberg spin system. The system under consideration is a planar thin ferromagnetic film with competing surface fields subject to a pulsed oscillatory external field. The results show that the films exhibit a single discontinuous dynamic phase transition (DPT) as a function of the anisotropy of the bilinear exchange interaction in the Hamiltonian. Furthermore, there is no evidence of stochastic resonance associated with the DPT. These results are in marked contrast to the continuous DPT observed in the same system as a function of temperature and applied field strength for a fixed bilinear exchange anisotropy.

Journal Article↗