ESR study of the interaction of cytotoxin II with model membranes

Cytotoxin II from the venom of the Central-Asian cobra Naja oxiana spin-labeled at Lys35 (SLCT II) was studied by ESR spectroscopy in aqueous solution and upon interaction with phospholipid vesicles from egg phosphatidylcholine or its mixture with dimyristoylphosphatidylglycerol (molar ratio 9:1). The distribution of SLCT II between the aqueous and lipid phases depended on the toxin and lipid concentrations and on the solution ionic strength. It was analyzed using the modified Gouy-Chapman equation that takes into account different charges of the cytotoxin in solution and in membrane. The analysis revealed two states of the cytotoxin-lipid complex. The first state corresponds to monomeric SLCT II hydrophobically interacting with the lipid membrane [a binding constant of (8 +/- 3) x 10(3) M-1] and carrying the charge of 4.4 +/- 0.3. On the basis of these parameters and the spatial structure of cytotoxin II in dodecylphosphocholine micelles, we concluded that the cytotoxin is mainly incorporated into the region of polar groups of the lipid bilayer. The second state of SLCT II is realized at high cytotoxin concentrations in the membrane and corresponds to the formation of toxin-lipid complexes that destruct the membrane bilayer structure.     

An ESR Study of the Cytotoxin II Interaction with Model Membranes

Cytotoxin II from the venom of the Central-Asian cobra Naja oxianaspin-labeled at Lys35 (SLCT II) was studied by ESR spectroscopy in aqueous solution and upon interaction with phospholipid vesicles from egg phosphatidylcholine or its mixture with dimyristoylphosphatidylglycerol (molar ratio 9 : 1). The distribution of SLCT II between the aqueous and lipid phases depended on the toxin and lipid concentrations and on the solution ionic strength. It was analyzed using the modified Gouy–Chapman theory that takes into account different charges of the cytotoxin in solution and in membrane. The analysis revealed two states of the cytotoxin–lipid complex. The first state corresponds to monomeric SLCT II hydrophobically interacting with the lipid membrane [a binding constant of (8 ± 3) × 10³M^–1] and carrying the charge of 4.4 ± 0.3. On the basis of these parameters and the spatial structure of cytotoxin II in dodecylphosphocholine micelles, we concluded that the cytotoxin is mainly incorporated into the region of polar groups of the lipid bilayer. The second state of SLCT II is realized at high cytotoxin concentrations in the membrane and corresponds to the formation of toxin–lipid complexes that disorganize the membrane bilayer structure.     

Changes in the membrane surface charge and the potentiation of phospholipase A2 as affected by the cytotoxin from the venom of the Central Asian cobra

The interaction of iodine labelled cytotoxin of the middle-asian cobra venom with erythrocyte membranes has been studied. The pretreatment of erythrocytes by cytotoxin results in the sensitivity to the lytic action of pure phospholipase A2 of the same venom. Using I-labelled serum albumin it has been proved that cytotoxin promotes the binding of acid proteins on the membrane such as phospholipase A2 interacted with it synergetically. In the course of study of cytotoxin effect on the time of adhesion hemispheres of artificial bilayer phospholipide membranes it has been established that due to the basic properties cytotoxin neutralizes the negative charge of the membrane surface. This effect of cytotoxin plays an important role in the potentiation of membrane action of phospholipase A2.     

Structure of an adsorbed dimyristoylphosphatidylcholine bilayer measured with specular reflection of neutrons.

Using specular reflection of neutrons, we investigate for the first time the structure of a single dimyristoylphosphatidylcholine bilayer adsorbed to a planar quartz surface in an aqueous environment. We demonstrate that the bilayer is strongly adsorbed to the quartz surface and is stable to phase state changes as well as exchange of the bulk aqueous phase. Our results show that the main phase transition is between the L alpha phase and the metastable L beta'* phase, with formation of the P beta' ripple phase prevented by lateral stress on the adsorbed bilayer. By performing contrast variation experiments, we are able to elucidate substantial detail in the interfacial structure. We measure a bilayer thickness of 43.0 +/- 1.5 A in the L alpha phase (T = 31 degrees C) and 46.0 +/- 1.5 A in the L beta'* phase (T = 20 degrees C). The polar head group is 8.0 +/- 1.5 A thick in the L alpha phase. The water layer between the quartz and bilayer is 30 +/- 10 A for the lipid in both the L alpha and L'* phase. Our results agree well with those previously reported from experiments using lipid vesicles and monolayers, thus establishing the feasibility of our experimental methods.     

Molecular-dynamic simulation of DPPC bilayer in different phase state: Hydration and electric field distribution in the presence of Be<Superscript>2+</Superscript> cations

New molecular-dynamic topology of phosphatidylcholine bilayer (DPPC) in total atomic OPLS force field was developed and used to study the structural characteristics of liquid-crystalline and gel state of lipid bilayer in the absence and in the presence of Na⁺ and Be²⁺ cations adsorbed at the interface and different in their affinity. The parameters of bilayer geometry, the amount of surface water, and the electrostatic potential distribution were estimated quantitatively from the simulation in both phase states. The azimuthal angle of hydrocarbon chains was found nearly the same in the region of each monolayer in gel state. The amount of surface water decreases upon bilayer “freezing” mainly by loss of water molecules not participating in H-bonds between lipid headgroups. The cation adsorption was shown to have a small effect on these H-bonded water molecules, whereas Be²⁺ appeared to retain surface water in the bilayer upon its freezing. The electric potential distribution in the normal direction to the membrane-water interface had a similar shape in any bilayer phase state regardless of the presence of the adsorbed cations. Analysis of the microscopic nature of the electric potential revealed a mutual compensation of the contributions of the main structural components of the system (lipids, water, and ions). The boundary potential increased by 116 mV for pure DPPC, by 212 mV in the presence of Na⁺, and by 133 mV in the presence of Be²⁺ upon the phase transition of bilayer to the gel state. The boundary potential difference in the presence of Na⁺ and Be²⁺ and its change at the bilayer phase transition are in a good agreement with the experimental data published earlier [Ermakov Yu.A., 1993].     

The dependence of Fluorescein-PE fluorescence intensity on lipid bilayer state. Evaluating the interaction between the probe and lipid molecules

The degree of dependence of a lipid bilayer's surface properties on its conformational state is still an unresolved question. Surface properties are functions of molecular organization in the complex interfacial region. In the past, they were frequently measured using fluorescence spectroscopy. Since a fluorescent probe provides information on its local environment, there is a need to estimate the effect caused by the probe itself. In this paper, we address this question by calculating how lipid head-group orientation effects the fluorescence intensity of Fluorescein-PE (a probe that is sensitive to surface potential). In the theoretical model assumed the lipid bilayer state and the interactions between the charged fluorescent probe and the surrounding lipid molecules was evaluated. The results of this theoretical analysis were compared with experimentally obtained data. A lipid bilayer formed from DPPC was chosen as the experimental system, since it exhibits all the major conformational states within a narrow temperature range of 30 degrees C-45 degrees C. Fluorescein-PE fluorescence intensity depends on local pH, which in turn is sensitive to local electrostatic potential in the probe's vicinity. This local electrostatic potential is generated by lipid head-group dipole orientation. We have shown that the effect of the probe on lipid bilayer properties is limited when the lipid bilayer is in the gel phase, whereas it is more pronounced when the membrane is liquid-crystalline. This implies that Fluorescein-PE is a good reporter of local electrostatic fields when the lipid bilayer is in the gel phase, and is a poor reporter when the membrane is in the liquid-crystalline state.     

Electric capacitance of bilayer lipid membranes from hydrogenated egg lecithin during phase transition from liquid crystalline state to gel

The electrical capacity of planar bilayer lipid membranes (BLM) from natural hydrogenated egg lecithin (HEL) in n-decane at a temperature of phase transition was measured. The temperature of phase transition was determined calorimetrically to be 51 degrees C. The data obtained revealed a phase separation of HEL in BLM into two fractions, one freezing at 42-44 degrees C and one that is converted to a liquid-crystal state at 51-59 degrees C. It was assumed that the first fraction is rich in dipalmitoyl lecithin, and the second fraction is rich in distearoyl lecithin. Freezing and the transition to the liquid-crystal state were accompanied by an increase and decrease in membrane thickness, respectively, in part due to a displacement of the solvent from the torus to the planar part of the bilayer. The displacement of the solvent is explained by changes in the disjoining pressure in BLM, which arises across the lipid bilayer due to van der Waals forces of attraction between water layers on both sides of the BLM.     

The inverted hexagonal phase is more sensitive to hydroperoxidation than the multilamellar phase in phosphatidylcholine and phosphatidylethanolamine aqueous dispersions.

The effect of phase behaviour (hexagonal II phase and lamellar phase) on the peroxidation of membrane phospholipids has been investigated in dilinoleoyl phosphatidylcholine (DLPC)/dilinoleoyl phosphatidylethanolamine (DLPE) aqueous dispersions. Peroxidation was initiated with a water-soluble radical inducer 2,2'-azobis (2-amidino-propane) dihydrochloride (AAPN). The phospholipid morphology was monitored by 31P-nuclear magnetic resonance (NMR). Phospholipid hydroperoxides (PCOOH and PEOOH) were determined by chemiluminescence high-performance liquid chromatography (CL-HPLC). In pH-induced phase transition systems, DLPE in the bilayer state was much less oxidized than in the hexagonal II state. In composition-induced phase transition systems, the formation of total hydroperoxides and the consumption of alpha-tocopherol in the hexagonal II phase were greater than in the bilayer phase. These data suggest that the hexagonal II phase is more sensitive to hydroperoxidation than the bilayer phase in phospholipid aqueous dispersions.     

Prodan as a membrane surface fluorescence probe: partitioning between water and phospholipid phases.

Fluorescence spectral features of 6-propionyl-2-dimethylaminonaphthalene (Prodan) in phospholipid vesicles of different phase states are investigated. Like the spectra of 6-lauroyl-2-dimethylaminonaphthalene (Laurdan), the steady-state excitation and emission spectra of Prodan are sensitive to the polarity of the environment, showing a relevant shift due to the dipolar relaxation phenomenon. Because of the different lengths of their acyl residues, the partitioning of the two probes between water and the membrane bilayer differs profoundly. To account for the contribution of Prodan fluorescence arising from water, we introduce a three-wavelength generalized polarization method that makes it possible to separate the spectral properties of Prodan in the lipid phase and in water, and to determine the probe partitioning between phospholipid and water and between the gel and the liquid-crystalline phases of phospholipids. In contrast to Laurdan, Prodan preferentially partitions in the liquid-crystalline phase with respect to the gel and is sensitive to the polar head pretransition, and its partition coefficient between the membrane and water depends on the phase state, i.e., on the packing of the bilayer. Prodan is sensitive to polarity variations occurring closer to the bilayer surface than those detected by Laurdan.     

Chlorophyll a in bilayer membranes. I. The thermal phase diagram with distearoylphosphatidylcholine

Several groups have introduced chlorophyll a into artificial bilayer membranes in an attempt to develop a model system for studying the behavior of chlorophyll in the photosynthetic membrane. In order to investigate the organization of chlorophyll in these model systems, mixed bilayer systems containing chlorophyll a and distearoylphosphatidylcholine under conditions of excess water have been studied by differential thermal analysis. The resulting data suggest a phase diagram for this system consisting of a double eutectic with formation of a thermodynamic compound of defined stoichiometry between chlorophyll a and phospholipid at temperatures below the liquidus. The phase diagram may be simulated to obtain thermodynamic parameters characteristic of the compound phase. It is apparent that the organization and intermolecular interactions of chlorophyll in a bilayer membrane can very widely depending on the temperature and composition of the system. In particular, phase separation can occur within the membrane over certain temperature ranges, resulting in an inhomogeneous system. Thus in interpreting the physical and spectroscopic properties of chlorophyll a in bilayer membranes, it is essential to consider the phase state of the membrane and the organization and environment of the chlorophyll in the particular phase.     

A calorimetric and spectroscopic comparison of the effects of lathosterol and cholesterol on the thermotropic phase behavior and organization of dipalmitoylphosphatidylcholine bilayer membranes

We performed differential scanning calorimetry (DSC) and Fourier transform infrared (FTIR) spectroscopic measurements to study the effects of lathosterol (Lath) on the thermotropic phase behavior and organization of dipalmitoylphosphatidylcholine (DPPC) bilayer membranes and compared our results with those previously reported for cholesterol (Chol)/DPPC binary mixtures. Lath is the penultimate intermediate in the biosynthesis of Chol in the Kandutsch-Russell pathway and differs from Chol only in the double bond position in ring B, which is between C7 and C8 in Lath and between C5 and C6 in Chol. Our DSC studies indicate that the incorporation of Lath is more effective than Chol in reducing the temperature and enthalpy of the DPPC pretransition. At lower sterol concentrations (≤10 mol %), incorporation of both Lath and Chol decreases the temperature, enthalpy, and cooperativity of the sharp component of the main phase transition of DPPC to a similar extent, but at higher sterol concentrations, Lath is more effective at decreasing the phase transition temperature, enthalpy, and cooperativity than Chol. These results indicate that at higher concentrations, Lath is more disruptive of DPPC gel-state bilayer packing than Chol is. Moreover, incorporation of Lath decreases the temperature of the broad component of the main phase transition of DPPC, whereas Chol increases it; this difference in the direction and magnitude of the temperature shift is accentuated at higher sterol concentrations. Although at sterol concentrations of ≤20 mol % Lath and Chol are almost equally effective at reducing the enthalpy and cooperativity of the broad component of the main phase transition, at higher sterol levels Lath is less effective than Chol in these regards and does not completely abolish the cooperative hydrocarbon chain melting phase transition at 50 mol %, as does Chol. These latter results indicate that Lath both is more disruptive with respect to the low-temperature state of the sterol-enriched domains of DPPC bilayers and has a lower lateral miscibility in DPPC bilayers than Chol. Our FTIR spectroscopic studies suggest that Lath incorporation produces a less tightly packed bilayer than does Chol at both low (gel state) and high (liquid-crystalline state) temperatures, which is characterized by increased H-bonding between water and the carbonyl groups of the fatty acyl chains in the DPPC bilayer. Overall, our studies indicate that Lath and Chol incorporation can have rather different effects on the thermotropic phase behavior and organization of DPPC bilayers and thus that the position of the double bond in ring B of a sterol molecule can have an appreciable effect on the physical properties of sterol molecules.     

Effect of bilayer cholesterol content on reconstituted human erythrocyte sugar transporter activity

The influence of altered bilayer cholesterol content on the catalytic activity of the human red cell hexose transporter was examined by reconstitution of the transport protein (band 4.5) into bilayers of large unilamellar vesicles formed from dipalmitoyl lecithin and varying amounts of cholesterol. The physical state of the bilayers was characterized by differential scanning calorimetry. The major findings are as follows: changes in bilayer phase behavior occur at membrane cholesterol levels of 15 to 20 mol % and 30 to 40 mol %; and the catalytic activity of the reconstituted transporter (Vmax/transporter) correlates with bilayer phase behavior. In crystalline bilayers, this is seen as an abrupt, stimulation of activity at 15 mol % cholesterol (which is reversed at 17.5 mol %) and a gradual acceleration of activity between 30 to 40 mol % cholesterol. In fluid bilayers (where activity is high), activity is unaffected by 10, 20, and 30 mol % cholesterol. However, 12.5 and 17.5 mol % cholesterol reduce activity by 100-fold. These studies demonstrate that small changes in bilayer cholesterol content result in drastic alterations in transporter activity. Transporter sensitivity to cholesterol is a complex rather than monotonic function of bilayer cholesterol content and appears to be primarily determined by bilayer composition rather than by bilayer "fluidity."     

Specific interactions of tryptophan with phosphatidylcholine and digalactosyldiacylglycerol in pure and mixed bilayers in the dry and hydrated state

Amphiphilic solutes play an important role in the desiccation tolerance of plant cells, because they can reversibly partition into cellular membranes during dehydration. Their effects on membrane stability depend on their chemical structure, but also on the lipid composition of the host membrane. We have shown recently that tryptophan destabilizes liposomes during freezing. The degree of destabilization depends on the presence of glycolipids in the membranes, but not on the phase preference (bilayer or non-bilayer) of the lipids in mixtures with the bilayer lipid phosphatidylcholine. Here, we have investigated the influence of tryptophan on the phase behavior and intermolecular interactions in dry and hydrated bilayers made from the phospholipid egg phosphatidylcholine and the plant chloroplast glycolipid digalactosyldiacylglycerol, or from a mixture (1:1) of these lipids, using Fourier-transform infrared spectroscopy. To distinguish effects of the hydrophobic ring structure of tryptophan from those of the amino acid moiety, we also performed experiments with the hydrophilic amino acid glycine. Our data show that there are specific interactions between tryptophan and either phospholipid or glycolipid in the dry state, as well as H-bonding interactions between the lipids and both solutes. In the rehydrated state, the H-bonding interactions between amino acids and lipids are mostly replaced by interactions between water and lipids, while the hydrophobic interactions between lipids and tryptophan mostly persist.     

Interaction of the P-type cardiotoxin with phospholipid membranes.

The cardiotoxin (cytotoxin II, or CTII) isolated from cobra snake (Naja oxiana) venom is a 60-residue basic membrane-active protein featuring three-finger beta sheet fold. To assess possible modes of CTII/membrane interaction 31P- and 1H-NMR spectroscopy was used to study binding of the toxin and its effect onto multilamellar vesicles (MLV) composed of either zwitterionic or anionic phospholipid, dipalmitoylglycerophosphocholine (Pam2Gro-PCho) or dipalmitoylglycerophosphoglycerol (Pam2Gro-PGro), respectively. The analysis of 1H-NMR linewidths of the toxin and 31P-NMR spectral lineshapes of the phospholipid as a function of temperature, lipid-to-protein ratios, and pH values showed that at least three distinct modes of CTII interaction with membranes exist: (a) nonpenetrating mode; in the gel state of the negatively charged MLV the toxin is bound to the surface electrostatically; the binding to Pam2Gro-PCho membranes was not observed; (b) penetrating mode; hydrophobic interactions develop due to penetration of the toxin into Pam2Gro-PGro membranes in the liquid-crystalline state; it is presumed that in this mode CTII is located at the membrane/water interface deepening the side-chains of hydrophobic residues at the tips of the loops 1-3 down to the boundary between the glycerol and acyl regions of the bilayer; (c) the penetrating mode gives way to isotropic phase, stoichiometrically well-defined CTII/phospholipid complexes at CTII/lipid ratio exceeding a threshold value which was found to depend at physiological pH values upon ionization of the imidazole ring of His31. Biological implications of the observed modes of the toxin-membrane interactions are discussed.     

Changes in single K(+) channel behavior induced by a lipid phase transition

We show that the activity of an ion channel is correlated with the phase state of the lipid bilayer hosting the channel. By measuring unitary conductance, dwell times, and open probability of the K⁺ channel KcsA as a function of temperature in lipid bilayers composed of POPE and POPG in different relative proportions, we obtain that all those properties show a trend inversion when the bilayer is in the transition region between the liquid-disordered and the solid-ordered phase. These data suggest that the physical properties of the lipid bilayer influence ion channel activity likely via a fine-tuning of its conformations. In a more general interpretative framework, we suggest that other parameters such as pH, ionic strength, and the action of amphiphilic drugs can affect the physical behavior of the lipid bilayer in a fashion similar to temperature changes resulting in functional changes of transmembrane proteins.     

Fourier transform infrared spectroscopic studies of the interaction of the antimicrobial peptide gramicidin S with lipid micelles and with lipid monolayer and bilayer membranes

We have utilized Fourier transform infrared spectroscopy to study the interaction of the antimicrobial peptide gramicidin S (GS) with lipid micelles and with lipid monolayer and bilayer membranes as a function of temperature and of the phase state of the lipid. Since the conformation of GS does not change under the experimental conditions employed in this study, we could utilize the dependence of the frequency of the amide I band of the central beta-sheet region of this peptide on the polarity and hydrogen-bonding potential of its environment to probe GS interaction with and location in these lipid model membrane systems. We find that the GS is completely or partially excluded from the gel states of all of the lipid bilayers examined in this study but strongly partitions into lipid micelles, monolayers, or bilayers in the liquid-crystalline state. Moreover, in general, the penetration of GS into zwitterionic and uncharged lipid bilayer coincides closely with the gel to liquid-crystalline phase transition of the lipid. However, GS begins to penetrate into the gel-state bilayers of anionic phospholipids prior to the actual chain-melting phase transition, while in cationic lipid bilayers, GS does not partition strongly into the liquid-crystalline bilayer until temperatures well above the chain-melting phase transition are reached. In the liquid-crystalline state, the polarity of the environment of GS indicates that this peptide is located primarily at the polar/apolar interfacial region of the bilayer near the glycerol backbone region of the lipid molecule. However, the depth of GS penetration into this interfacial region can vary somewhat depending on the structure and charge of the lipid molecule. In general, GS associates most strongly with and penetrates most deeply into more disordered bilayers with a negative surface charge, although the detailed chemical structure of the lipid molecule and physical organization of the lipid aggregate (micelle versus monolayer versus bilayer) also have minor effects on these processes.     

A possible role of rhodopsin in maintaining bilayer structure in the photoreceptor membrane

31P-NMR measurements demonstrate that at 37 degrees C, independent of the photolytic state of the photopigment rhodopsin, the lipids in the photo-receptormembrane are almost exclusively organised in a bilayer. In strong contrast, the 31P-NMR spectra of the extracted lipids are characteristic for the hexagonal HII phase and an isotropic phase. The isotropic phase is characterised by freeze-fracture electron microscopy as particles and pits on smooth surfaces, possibly indicating inverted micelles. These results suggest a structural role for rhodopsin in maintaining the photoreceptor membrane lipids in a bilayer configuration.     

Two phases of gramicidin photoinactivation in bilayer lipid membranes in the presence of a photosensitizer

The kinetics of the light-induced decrease in the gramicidin-mediated current across a bilayer lipid membrane in the presence of a photosensitizer has been shown to include a slow phase with a characteristic time of the order of 1 s and a fast phase. Based on the dependence of the slow phase relative amplitude and characteristic time on the gramicidin-mediated stationary conductance we concluded that the slow phase reflected the establishment of an equilibrium between gramicidin monomers and dimers in the membrane after the distortion of this equilibrium resulting from modification of a portion of gramicidin molecules by reactive oxygen species generated upon excitation of the photosensitizer. The dependence of the fast phase contribution to the overall kinetics on the stationary conductance allowed us to conclude that the fast phase is associated with transition of gramicidin dimers into a nonconducting state. The characteristic time of the fast phase measured with nanosecond laser excited pulses is 1.5 ms. The slow phase of the decrease in the gramicidin-mediated current was considerably decelerated in the presence of Rose Bengal. The results obtained indicate that adsorption of Rose Bengal on the bilayer interface leads to a reduction of the dipole potential drop at the membrane-solution boundary, similarly to the action of phloretin.     

Molecular dynamics simulations and 2H NMR study of the GalCer/DPPG lipid bilayer

Molecular dynamics simulations were performed on a two-component lipid bilayer system in the liquid crystalline phase at constant pressure and constant temperature. The lipid bilayers were composed of a mixture of neutral galactosylceramide (GalCer) and charged dipalmitoylphosphatidylglycerol (DPPG) lipid molecules. Two lipid bilayer systems were prepared with GalCer:DPPG ratio 9:1 (10%-DPPG system) and 3:1 (25%-DPPG system). The 10%-DPPG system represents a collapsed state lipid bilayer, with a narrow water space between the bilayers, and the 25%-DPPG system represents an expanded state with a fluid space of approximately 10 nm. The number of lipid molecules used in each simulation was 1024, and the length of the production run simulation was 10 ns. The simulations were validated by comparing the results with experimental data for several important aspects of the bilayer structure and dynamics. Deuterium order parameters obtained from (2)H NMR experiments for DPPG chains are in a very good agreement with those obtained from molecular dynamics simulations. The surface area per GalCer lipid molecule was estimated to be 0.608 +/- 0.011 nm(2). From the simulated electron density profiles, the bilayer thickness defined as the distance between the phosphorus peaks across the bilayer was calculated to be 4.21 nm. Both simulation systems revealed a tendency for cooperative bilayer undulations, as expected in the liquid crystalline phase. The interaction of water with the GalCer and DPPG oxygen atoms results in a strong water ordering in a spherical hydration shell and the formation of hydrogen bonds (H-bonds). Each GalCer lipid molecule makes 8.6 +/- 0.1 H-bonds with the surrounding water, whereas each DPPG lipid molecule makes 8.3 +/- 0.1 H-bonds. The number of water molecules per GalCer or DPPG in the hydration shell was estimated to be 10-11 from an analysis of the radial distribution functions. The formation of the intermolecular hydrogen bonds was observed between hydroxyl groups from the opposing GalCer sugar headgroups, giving an energy of adhesion in the range between -1.0 and -3.4 erg/cm(2). We suggest that this value is the contribution of the hydrogen-bond component to the net adhesion energy between GalCer bilayers in the liquid crystalline phase.     

Thiocyanate and bromide ions influence the bilayer structural parameters of phosphatidylcholine bilayers

The influence of monovalent cations and anions on the structural parameters of dipalmitoylphosphatidylcholine (DPPC) bilayers was examined at 25 degrees C using X-ray diffraction. It was shown that monovalent salts, in general, have little effect on lipid packing within the bilayer. However, fully hydrated DPPC bilayers in 1 M KSCN pack in an interdigitated acyl chain phase. This is the first observation of an ion-induced interdigitated bilayer phase in a zwitterionic lipid. In addition, gel state DPPC bilayers in 1 M KBr imbibe approx. 10 A more solvent than bilayers in water. The influence of these same salts on the phase transitions of DPPC bilayers was also examined using high-resolution differential scanning calorimetry. These results are discussed in terms of ion-induced changes in solvent and solvent/bilayer structure.