Simulating induced interdigitation in membranes

In this study we introduce a mesoscopic lipid-water-alcohol model. Dissipative particle dynamics (DPD) simulations have been used to investigate the induced interdigitation of bilayers consisting of double-tail lipids by adding alcohol molecules to the bilayer. Our simulations nicely reproduce the experimental phase diagrams. We find that alcohol can induce an interdigitated structure where the common bilayer structure changes into monolayer in which the alcohol molecules screen the hydrophobic tails from the water phase. At low concentrations of alcohol the membrane has domains of the interdigitated phase that are in coexistence with the common membrane phase. We compute the effect of the chain length of the alcohol on the phase behavior of the membrane and show that the stability of the interdigitated phase depends on the length of the alcohol. We show that we can reproduce the experimental hydrophobic thickness of the bilayer for various combinations of lipids and alcohols. We use our model to clarify some of the experimental questions related to the structure of the interdigitated phase and put forward a simple model that explains the alcohol chain length dependence of the stability of this interdigitated phase.     

Interdigitated structure of phospholipid-alcohol systems studied by x-ray diffraction.

In the interdigitated structure of phosphatidylcholine/alcohol systems, the one-dimensional electron density profile in the direction normal to the membrane surface is generated from the x-ray diffraction pattern. The membrane thickness for these systems is expressed by the sum of the hydrocarbon chain lengths of phosphatidylcholine and alcohol molecules. For this study, various sets of phosphatidylcholines and 1-alcohols were used; a phosphatidylcholine has a carbon number from 14 to 18 in a hydrocarbon chain, and an alcohol has a carbon number from 1 (methanol) to 4 (1-butanol). Based upon the results, we propose a model for the interdigitated structure in which 1) two alcohol molecules occupy a volume whose surface is surrounded interstitially by the headgroups of phosphatidylcholine molecules, and 2) the methyl ends of both hydrocarbon chains in alcohol and phosphatidylcholine molecules face each other at the bottom of the volume.     

Differential scanning calorimetric studies of ethanol interactions with distearoylphosphatidylcholine: transition to the interdigitated phase

It is well established that ethanol and other amphipathic molecules induce the formation of a fully interdigitated gel phase in saturated like-chain phosphatidylcholines (PC's). We have previously shown that the induction of interdigitation in PC's by ethanol is dependent upon the alcohol concentration, the lipid chain length, and the temperature [Nambi, P., Rowe, E. S. & McIntosh, T. J. (1988) Biochemistry 27, 9175-9182]. In the present study, we have used high-sensitivity differential scanning calorimetry to investigate the transitions of distearoylphosphatidylcholine between the noninterdigitated and the interdigitated phases. The enthalpy of the L beta' to L beta I transition is approximately half that of the L beta' to P beta' transition which occurs in the absence of ethanol. The reversibility of these transitions has also been investigated by employing both heating and cooling scans in order to establish the most stable phases as a function of temperature and ethanol concentration. It has been demonstrated that the transition to the interdigitated phase is reversible as a function of temperature. Kinetic studies on the reverse transition (L beta I to L beta') demonstrate that this transition can be very slow, requiring weeks to reach completion. The rate depends upon temperature and ethanol concentration. The slow phase changes mean that the lipid can exist for long periods of time in a phase structure which is not the most stable state. The biological significance of this type of lipid behavior is the implication that the phase structure of biological membranes may depend not only on the most stable phase structure of the lipids present but also on the synthetic pathway or other kinetic variables.     

The structure and function of gramicidin A embedded in interdigitated bilayer

The effects of phase transition from normal to interdigitated lipid bilayer on the function and structure of membrane proteins were studied using linear gramicidin (gramicidin A) as a model. Interdigitated bilayer structure of dipalmitoylphosphatidylglycerol (DPPG) liposomes that was induced by atropine could not be changed notably by intercalating of gramicidin. The K+ transportation of gramicidin in both normal and interdigitated bilayer was assayed by measuring the membrane potential. Results showed that gramicidin in interdigitated bilayer exhibited lower transport capability. Intrinsic fluorescence spectrum of gramicidin in interdigitated bilayer blue-shifted 2.8 nm from the spectrum in normal bilayer, which means that interdigitation provides a more hydrophobic environment for gramicidin. Circular dichroism measurement results indicated that the conformation of gramicidin in interdigitated bilayer is not the typical beta6.3 helix as in the normal bilayer. The results suggested that the interdigitated lipid bilayer might largely affect the structure and function of membrane proteins.     

Alcohol induction of interdigitation in distearoylphosphatidylcholine: fluorescence studies of alcohol chain length requirements.

Although it is now well established that the fully interdigitated phase is induced in saturated like-chain phosphatidylcholines (PCs) by a variety of amphipathic molecules including alcohols, no systematic study of the properties of the inducing molecules has been reported. To elucidate the stereochemical features that lead to the alcohol induction of interdigitation in PCs, we have investigated the induction of interdigitation in distearoylphosphatidylcholine (DSPC) by a series of alcohols. Our previously established DPH (1,6-diphenyl-1,3,5-hexatriene) fluorescence intensity method has been expanded (P. Nambi, E. S. Rowe, and T. M. McIntosh (1988), Biochemistry 27:9175-9182) and used to determine which of the alcohols induce interdigitation and to determine the threshold concentrations for each. We have found that each of the n-alcohols up to heptanol and several branched alcohols are capable of inducing interdigitation in DSPC; octanol and nonanol do not appear to induce interdigitation by these criteria. The threshold concentrations for interdigitation for each of these alcohols up to heptanol were found to be correlated with the membrane: buffer partition coefficients. The mole fraction of bound alcohol at the threshold concentration was similar for each of the alcohols up to pentanol. These results are discussed in terms of a general mechanism of the formation of the interdigitated phase.     

Studies of the ethanol-induced interdigitated gel phase in phosphatidylcholines using the fluorophore 1,6-diphenyl-1,3,5-hexatriene

It is now well established that a number of amphiphilic molecules such as ethanol can induce the formation of the fully interdigitated gel phase in phosphatidylcholines. We have shown earlier that alcohols such as ethanol induce biphasic melting behavior in phosphatidylcholines [Rowe, E. S. (1983) Biochemistry 22, 3299-3305] but not in phosphatidylethanolamines [Rowe, E. S. (1985) Biochim. Biophys. Acta 813, 321-330]. Simon and McIntosh [(1984) Biochim. Biophys. Acta 773, 169-172] showed that the alcohol-induced biphasic melting behavior in phosphatidylcholines is a consequence of acyl chain interdigitation. In the present study we demonstrate the detection of the transition of DPPC and DSPC to the interdigitated phase in the presence of ethanol using the fluorescence properties of the commonly used fluorophore 1,6-diphenyl-1,3,5-hexatriene (DPH). By correlating fluorescence and X-ray diffraction results, we have demonstrated the use of fluorescence to study the phase transition from the noninterdigitated to the interdigitated phase. Using this method, we have investigated the temperature and ethanol concentration dependence of the induction of the interdigitated phase in DSPC and DPPC and shown that the induction of interdigitation by ethanol is temperature dependent, with higher temperature favoring interdigitation. The temperature-ethanol phase diagrams have been determined for DPPC and DSPC.     

Effect of hydrophobic mismatch on phase behavior of lipid membranes

We investigate the competing effects of hydrophobic mismatch and chain stretching on the morphology and evolution of domains in lipid membranes via Monte Carlo techniques. We model the membrane as a binary mixture of particles that differ in their preferred lengths, with the shorter particles mimicking unsaturated nonraft lipids and the longer particles mimicking saturated raft lipids. We find that phase separation can be induced upon increasing either the ratio J/kappa of the hydrophobic surface tension J to the compressibility modulus kappa. J/kappa determines the decay length for thickness changes. When this decay length is larger than the system size the membrane remains mixed. Furthermore, increasing the thickness relaxation time can induce transient phase separation.     

Studies of mixed-chain diacyl phosphatidylcholines with highly asymmetric acyl chains: a Fourier transform infrared spectroscopic study of interfacial hydration and hydrocarbon chain packing in the mixed interdigitated gel phase.

The mixed interdigitated gel phases of unlabeled, specifically 13C = O-labeled, and specifically chain-perdeuterated samples of 1-O-eicosanoyl, 2-O-lauroyl phosphatidylcholine and 1-O-decanoyl, 2-O-docosanoyl phosphatidylcholine were studied by infrared spectroscopy. Our results suggest that at the liquid-crystalline/gel phase transition temperatures of these lipids, there is a greater redistribution in the populations of free and hydrogen-bonded ester carbonyl groups than is commonly observed with symmetric chain n-saturated diacyl phosphatidylcholines. The formation of the mixed interdigitated gel phase coincides with the appearance of a marked asymmetry in the contours of the C = O stretching band, a process which becomes more pronounced as the temperature is reduced. This asymmetry is ascribed to the emergence of a predominant lipid population consisting of free sn1- and hydrogen-bonded (hydrated) sn2-ester carbonyl groups. This suggests that the region of the mixed interdigitated bilayer polar/apolar interface near to the sn1-ester carbonyl group is less hydrated than is the case with the noninterdigitated gel-phase bilayers formed by normal symmetric chain phosphatidylcholines. In the methylene deformation region of the spectrum, the unlabeled lipids exhibit a pronounced splitting of the CH2 scissoring bands. This splitting is significantly attenuated when the short chains are perdeuterated and collapses completely upon perdeuteration of the long chains, irrespective of whether the long (or short) chains are esterified to the sn1 or sn2 positions of the glycerol backbone. These results are consistent with a global hydrocarbon chain packing motif in which the zigzag planes of the hydrocarbon chains are perpendicular to each other and the sites occupied by long chains are twice as numerous as those occupied by short chains. The experimental support for this chain-packing motif enabled more detailed considerations of the possible ways in which these lipid molecules are assembled in the mixed interdigitated gel phase. Generally, our results are compatible with a previously proposed model in which the mixed interdigitated gel phase is an assembly of repeat units which consists of two phosphatidylcholine molecules forming a triple-chain structure with the long chains traversing the bilayer and with the methyl termini of the shorter chains opposed at the bilayer center. Our data also suggest that the packing format which is most consistent with our results and previously published work is one in which the hydrocarbon chains of each repeat unit are parallel to each other with the repeat units themselves being perpendicularly packed.     

山莨菪碱诱导DPPG／DPPC混合物形成交插凝胶相──荧光偏振研究

山莨菪碱诱导ＤＰＰＧ脂质体交插结构,其脂酰链末端插到对面分子层脂酰链第五个碳原子的位置,而生物膜中普遍存在的ＤＰＰＣ不能被山莨菪碱诱导形成交插相,但ＤＰＰＧ／ＤＰＰＣ混合物则能形成交插相,即伴随ＤＰＰＧ的交插,ＤＰＰＣ分子也发生交插。当ＤＰＰＧ／ＤＰＰＣ摩尔比为２：１或１：１时,其脂酰链末端插到对面分子层第八个碳原子的位置。当ＤＰＰＧ／ＤＰＰＣ摩尔比为１：２时,就不能发生交插而呈完全的非交插状态。同时,发现当体系中钠离子浓度达到４００ｍｍｏｌ／Ｌ时,山莨菪碱就不能再诱导ＤＰＰＧ形成交插凝胶相。     

Membrane hydrophobicity determines the activation free energy of passive lipid transport

The collective behavior of lipids with diverse chemical and physical features determines a membrane’s thermodynamic properties. Yet, the influence of lipid physicochemical properties on lipid dynamics, in particular interbilayer transport, remains underexplored. Here, we systematically investigate how the activation free energy of passive lipid transport depends on lipid chemistry and membrane phase. Through all-atom molecular dynamics simulations of 11 chemically distinct glycerophospholipids, we determine how lipid acyl chain length, unsaturation, and headgroup influence the free energy barriers for two elementary steps of lipid transport: lipid desorption, which is rate limiting, and lipid insertion into a membrane. Consistent with previous experimental measurements, we find that lipids with longer, saturated acyl chains have increased activation free energies compared to lipids with shorter, unsaturated chains. Lipids with different headgroups exhibit a range of activation free energies; however, no clear trend based solely on chemical structure can be identified, mirroring difficulties in the interpretation of previous experimental results. Compared to liquid-crystalline phase membranes, gel phase membranes exhibit substantially increased free energy barriers. Overall, we find that the activation free energy depends on a lipid’s local hydrophobic environment in a membrane and that the free energy barrier for lipid insertion depends on a membrane’s interfacial hydrophobicity. Both of these properties can be altered through changes in lipid acyl chain length, lipid headgroup, and membrane phase. Thus, the rate of lipid transport can be tuned through subtle changes in local membrane composition and order, suggesting an unappreciated role for nanoscale membrane domains in regulating cellular lipid dynamics.     

The influence of proteins and peptides on the phase properties of lipids

This paper reviews model membrane studies on the modulation of the macroscopic structure of lipids by lipid-protein interactions, with particular emphasis on the gramicidin molecule. This hydrophobic peptide has three main effects on lipid polymorphism: (1) in lysophosphatidylcholine it triggers a micellar to bilayer transition, (2) in phosphatidylethanolamine it lowers the bilayer to hexagonal H_II phase transition temperature and (3) in phosphatidylcholine and other bilayer preferring lipids it is able to induce the formation of an H_II phase. From experiments in which the gramicidin molecule was chemically modified it can be concluded that the tryptophan residues play a determining role in the peptide-induced changes in polymorphism. The experimental data lead to the proposal that gramicidin molecules have a tendency to self-associate, possibly mediated by tryptophan-tryptophan interactions and organize into tubular structures such as found in the H_II phase.     

On the propensity of phosphatidylglycerols to form interdigitated phases

We have determined the phase behavior of disaturated phosphatidylglycerols (PGs) of chain lengths n(CH2) = 14-18 at high pH and ionic strength using calorimetry, dilatometry, as well as x-ray diffraction. PGs with n(CH2) = 14 and 16 show thermotropic behavior similar to that of phosphatidylcholines (PCs). The area/lipid obtained in the gel phase is smaller than that reported for PCs despite the expected larger effective headgroup size. This can be explained by the tilting of the PG headgroup out of the bilayer plane, and we provide experimental evidence for a headgroup tilt transition. For distearoyl PG, we further find that the "usual" gel phase coexists with an interdigitated phase, which exhibits a transition from an orthorhombic into a hexagonal chain packing. The total amount of the interdigitated phase depends significantly on the temperature but is found to be largely independent of temperature equilibration time and different sample preparation protocols. Thus, the development of the interdigitated phase appears to be kinetically trapped. The formation of interdigitated phases in PGs at much smaller chain lengths than in PCs is of high relevance to interaction studies with antimicrobial peptides, as it provides a mechanism for the discrimination of membranes composed of different lipid species.     

Effect of alcohols on the phase transitions of dihexadecylphosphatidylcholine

We have systematically investigated the effect of short chain alcohols (methanol to n-propanol) on the phase transitions of 1,2-dihexadecylphosphatidylcholine (DHPC), a lipid that forms a stable interdigitated gel phase (L beta I) in aqueous solution. The temperature of the low-temperature L beta I to P beta' phase transition of DHPC was found to increase with alcohol concentration, showing that alcohol interacts preferentially with the interdigitated phase relative to the non-interdigitated gel. The main transition of DHPC exhibited a biphasic effect of alcohol concentration similar to that previously observed with DPPC (Rowe, E.S. (1983) Biochemistry 22,3299-3305). As alcohol concentration is increased the lower L beta I to P beta' and main P beta' to L alpha transitions of DHPC merge at the threshold concentration of the biphasic effect, so that above this concentration there is one phase transition from L beta I directly to L alpha. This is analogous to DPPC above its biphasic threshold. Similar to DPPC, the transition between L beta I and L alpha exhibits marked hysteresis.     

Effect of cholesterol on the formation of an interdigitated gel phase in lysophosphatidylcholine and phosphatidylcholine binary mixtures

We previously reported that 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) forms an interdigitated gel phase in the presence of 1-palmitoyl-sn-glycero-3-phosphocholine (16:0LPC) at concentrations below 30 mol%. In the present investigation, fluorescent probe 1,6-diphenyl-1,3,5-hexatriene (DPH), X-ray diffraction, and differential scanning calorimetry (DSC) were used to investigate the effect of cholesterol on the phase behavior of 16:0LPC/DPPC binary mixtures. At 25 degrees C, 30 mol% 16:0LPC significantly decreases the DPH fluorescence intensity during the transition of DPPC from the L(beta') phase to the L(betaI) phase. However, the addition of cholesterol to 16:0LPC/DPPC mixtures results in a substantial increase in fluorescence intensity. The changes in DPH fluorescence intensity reflect the probe's redistribution from an orientation parallel to the acyl chain to the center of the bilayer, suggesting a bilayer structure transition from interdigitation to noninterdigitation. The normal repeat period of small angle X-ray diffraction patterns can be restored and a reflection appears at 0.42 nm with a broad shoulder around 0.41 nm in wide angle X-ray diffraction patterns when 10 mol% cholesterol is incorporated into 30 mol% 16:0LPC/DPPC vesicles, indicating that the mixtures are in the gel phase (L(beta')). Moreover, DSC results demonstrate that 10 mol% cholesterol is sufficient to significantly decrease the main enthalpy, cooperativity and lipid chain melting of 30 mol% 16:0LPC/DPPC binary mixtures, which are L(betaI), indicating that the transition of the interdigitated phase is more sensitive to cholesterol than that of the noninterdigitated phase. Our data imply that the interdigitated gel phase induced by 16:0LPC is prevented in the presence of 10 mol% cholesterol, but unlike ethanol, an increasing concentration of 16:0LPC is not able to restore the interdigitation structure of the lipid mixtures.     

Dependence of lipid chain and head group packing of the inverted hexagonal phase on hydration

A model which positions the hydrophobic/hydrophilic boundary in phosphatidylethanolamine lipids at the first CH₂ group in the acyl or alkyl chain is used to calculate the surface area per lipid, the mean chain and head-group dimensions and diameters of the hydrophilic tubes of the inverted hexagonal phase of didodecylphosphatidylethanolamine. The calculated surface areas compare favorably with areas obtained for the lamellar liquid crystal phase of the same lipid using the same boundary. Placement of the boundary within the lipid structure permits a determination of the maximum headgroup packing at hydration levels down to complete dehydration. The headgroup dimensions are consistent with a 5 Å diam void at the center of a hydrophilic tube at zero hydration. The calculated mean fluid chain length is ~2 Å smaller than the mean chain length of the lamellar phase at comparable levels of hydration. Comparison of the calculated mean fluid chain length and distances between hydrophobic boundaries shows that the fluid chains are interdigitated between adjacent tubes, and not interdigitated in the central space between three tubes. At low hydration the chains interdigitate in both spaces. The number of lipids packed around a tube at low hydration is only a function of the headgroup geometry, whereas at high hydration, it is a function of the number of carbon atoms in the chains.     

Structural and thermodynamic determinants of chain-melting transition temperatures for phospholipid and glycolipids membranes

For optimum function, biological membranes need a fluid environment, which is afforded by the liquid-disordered phase of lipids with low chain-melting temperatures or the liquid-ordered phase that is formed by combining high chain-melting lipids with cholesterol. The dependence of chain-melting transition temperature on lipid chain structure is therefore of central importance. The currently available database, including sphingolipids and glycolipids, is summarised here by parameterising systematic dependences on molecular structure in terms of suitable thermodynamic models. Chain-length dependence, chain asymmetry of lipids forming partially interdigitated and mixed interdigitated gel phases, chain unsaturation, positional dependence of methyl branching, headgroup-attached and α-branched chains, and length of zwitterionic headgroups are all covered. This type of information is essential for biophysical approaches to functional lipidomics.     

Interdigitated lipid bilayers of long acyl chain species of cerebroside sulfate. A fatty acid spin label study

The metastable phase behavior of semi-synthetic species of cerebroside sulfate (CBS), with hydroxy and non-hydroxy fatty acids from 16 to 26 carbons in length, was compared in Li+ and K+ using differential scanning calorimetry. The structure of the metastable and various stable phases formed in the presence of these two cations was investigated using a fatty acid spin label, 16-doxylstearate. A number of stable phases with successively higher phase transition temperatures and enthalpies occur in the presence of K+ (see the preceding paper). Li+ prevents formation of the most stable phases with the highest transition temperatures and enthalpies for all species of CBS. However, it does not prevent a transition from the metastable phase to the first stable phase of the longer chain C24 and C26 species. Furthermore, it allows C24:0h-CBS to undergo a similar transition, in contrast to a high K+ concentration, which prevents it. The spin label has anisotropic motion in the metastable gel phase formed by all species of CBS on cooling from the liquid crystalline phase. The spectra resemble those in gel phase phospholipids. The spin label is partially insoluble in the most stable phases formed by all the lipids, including the unsaturated C24:1 species, preventing further elucidation of their structure using this technique. However, the spin label is soluble in the first stable phase formed on cooling by the longer chain C24:0 and C26:0-CBS in Li+ and K+ and by C24:0h-CBS in Li+, and is motionally restricted in this phase. The motional restriction is similar to that observed in the mixed interdigitated bilayers of asymmetric species of phosphatidylcholine and fully interdigitated bilayers formed by symmetric phospholipids. It strongly suggests that the highly asymmetric long chain species of CBS form a mixed interdigitated bilayer in their first stable gel phases while the metastable phase of these and the shorter chain lipids may be partially interdigitated. The metastable phase of C24:1-CBS is more disordered suggesting that it may not be interdigitated at all. Thus the results suggest that (i) the hydroxy fatty acid inhibits but does not prevent formation of a mixed interdigitated bilayer by long chain species of CBS, (ii) an increase in non-hydroxy fatty acid chain length from 24 to 26 carbons promotes it, and (iii) a cis double bond probably prevents any form of interdigitation. These results may be relevant to the physiological and pathological roles of these structural modifications of CBS.     

Effect of cholesterol on the ethanol-induced interdigitated gel phase in phosphatidylcholine: use of fluorophore pyrene-labeled phosphatidylcholine

It is now recognized that many amphiphilic molecules such as ethanol can induce the formation of the fully interdigitated gel phase (L beta I) in phosphatidylcholines (PC's). In the present study, we have developed a simple detection method for the L beta I phase using pyrene-labeled PC (PyrPC), which is a PC analogue with covalently coupled pyrene moiety at the end of one of its acyl chains. The intensity ratio of its fluorescence vibrational bands is a reflection of the polarity of the environment of the fluorophore. We have tested this fluorophore in several established interdigitated lipid systems, including 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (1,2-DPPC) in the presence of high concentrations of ethanol and 1,2-di-O-hexadecyl-sn-glycero-3-phosphocholine (DHPC) and 1,3-dipalmitoyl-sn-glycero-2-phosphocholine (1,3-DPPC) in the absence of any additives. We have found in each of these systems that the ratio of the intensities of band III (387.5 nm) to band I (376.5 nm) is sensitive to the lipid phase change from the noninterdigitated L beta' phase to the interdigitated L beta I phase. By comparison of the III/I ratios for PyrPC in the lipid systems with the III/I ratios for methylpyrene in organic solvents, it was shown that the polarity of the PyrPC environment in the L beta I phase is similar to that of pentanol or ethanol. Using this method, we investigated the effect of cholesterol on the ethanol induction of the interdigitated gel phase in 1,2-DPPC. We found that the ethanol induction of the interdigitated gel phase is prevented by the presence of 20 mol % cholesterol.     

Scanning calorimetric study of fully hydrated asymmetric phosphatidylcholines with one acyl chain twice as long as the other

The asymmetric C(18):C(10)PC molecules are known by X-ray diffraction to self-assemble, in excess water, into a lamellar structure known as the mixed interdigitated bilayer at T less than Tm. In this structure, the long C(18)-acyl chain is interdigitated fully across the entire hydrocarbon width of the bilayer, while the shorter C(10)-acyl chain, which is about half as long as the C(18)-acyl chain, packs end to end with a C(10)-acyl chain of another lipid molecule in the opposing bilayer leaflet. We have synthesized the following asymmetric phosphatidylcholines (PC's): C(16):C(9)PC, C(16):C(10)PC, C(18):C(10)PC, C(18):C(11)PC, C(20):C(11)PC, C(20):C(12)PC, C(22):C(12)PC, C(22):C(13)PC, C(8):C(18)PC, and C(10):C(22)PC. These 10 asymmetric phosphatidylcholines have a common characteristic; i.e., the length of the longer extended acyl chain is about twice as long as that of the shorter acyl chain. On the basis of the known lamellar structure of C(18):C(10)PC, we anticipate that these asymmetric phosphatidylcholines will also form mixed interdigitated bilayers. We have employed high-resolution differential scanning calorimetry (DSC) to investigate the thermotropic behavior of liposomes prepared from these asymmetric phosphatidylcholines. If our anticipation is correct, one would find that the thermodynamic data (Tm, delta H, or delta S) associated with the main thermal phase transitions of these asymmetric phosphatidylcholine dispersions will fit into a continuous curve as they are plotted as a function of the hydrocarbon width of the putative mixed interdigitated bilayer. Experimental data presented in this paper indeed bear this out. For comparison, a DSC study of multilamellar dispersions prepared from a series of saturated symmetric phosphatidylcholines has also been carried out.(ABSTRACT TRUNCATED AT 250 WORDS)     

Polymorphic phase behavior of lysophosphatidylethanolamine dispersions. A thermodynamic and spectroscopic characterization.

We have investigated the phase behavior of aqueous dispersions of a series of synthetic lysophosphatidylethanolamines as a function of the acyl chain length. Lysophosphatidylethanolamines exhibit phase polymorphism encompassing a well-ordered crystalline phase which may arise either from a metastable interdigitated lamellar gel phase or a metastable micellar phase. The time course of interconversion between these various phases have been outlined by observing the low temperature incubation time dependence of the calorimetric thermograms. We have determined differences in structure of these phases by Raman spectroscopy and 31P nuclear magnetic resonance spectroscopy. It appears that a principal contribution to this polymorphic phase behavior lies in the nature of headgroup hydration and headgroup-headgroup interactions.