On the position of the hydro-phobic/philic boundary in lipid bilayers

Cisplatin-Membrane Interactions and Their Influence on Platinum Complexes Activity and Toxicity

Cisplatin and other platinum(II) analogs are widely used in clinical practice as anti-cancer drugs for a wide range of tumors. The primary mechanism by which they exert their action is through the formation of adducts with genomic DNA. However, multiple cellular targets by platinum(II) complexes have been described. In particular, the early events occurring at the plasma membrane (PM), i.e., platinum-membrane interactions seem to be involved in the uptake, cytotoxicity and cell-resistance to cisplatin. In fact, PM influences signaling events, and cisplatin-induced changes on membrane organization and fluidity were shown to activate apoptotic pathways. This review critically discusses the sequence of events caused by lipid membrane-platinum interactions, with emphasis on the mechanisms that lead to changes in the biophysical properties of the membranes (e.g., fluidity and permeability), and how these correlate with sensitivity and resistance phenotypes of cells to platinum(II) complexes.

High-density reconstitution of functional water channels into vesicular and planar block copolymer membranes

The exquisite selectivity and unique transport properties of membrane proteins can be harnessed for a variety of engineering and biomedical applications if suitable membranes can be produced. Amphiphilic block copolymers (BCPs), developed as stable lipid analogs, form membranes that functionally incorporate membrane proteins and are ideal for such applications. While high protein density and planar membrane morphology are most desirable, BCP–membrane protein aggregates have so far been limited to low protein densities in either vesicular or bilayer morphologies. Here, we used dialysis to reproducibly form planar and vesicular BCP membranes with a high density of reconstituted aquaporin-0 (AQP0) water channels. We show that AQP0 retains its biological activity when incorporated at high density in BCP membranes, and that the morphology of the BCP–protein aggregates can be controlled by adjusting the amount of incorporated AQP0. We also show that BCPs can be used to form two-dimensional crystals of AQP0.

Life as a nanoscale phenomenon

The nanoscale is not just the middle ground between molecular and macroscopic but a dimension that is specifically geared to the gathering, processing, and transmission of chemical-based information. Herein we consider the living cell as an integrated self-regulating complex chemical system run principally by nanoscale miniaturization, and propose that this specific level of dimensional constraint is critical for the emergence and sustainability of cellular life in its minimal form. We address key aspects of the structure and function of the cell interface and internal metabolic processing that are coextensive with the up-scaling of molecular components to globular nanoobjects (integral membrane proteins, enzymes, and receptors, etc) and higher-order architectures such as microtubules, ribosomes, and molecular motors. Future developments in nanoscience could provide the basis for artificial life.

New insights into water–phospholipid model membrane interactions

Modulating the relative humidity (RH) of the ambient gas phase of a phospholipid/water sample for modifying the activity of phospholipid-sorbed water [humidity-controlled osmotic stress methods, J. Chem. Phys. 92 (1990) 4519 and J. Phys. Chem. 96 (1992) 446] has opened a new field of research of paramount importance. New types of phase transitions, occurring at specific values of this activity, have been then disclosed. Hence, it is become recognized that this activity, like the temperature T, is an intensive parameter of the thermodynamical state of these samples. This state can be therefore changed (phase transition) either, by modulating T at a given water activity (a given hydration level), or, by modulating the water activity, at a given T. The underlying mechanisms of these two types of transition differ, especially when they appear as disorderings of fatty chains. In lyotropic transitions, this disordering follows from two thermodynamical laws. First, acting on the activity (the chemical potential) of water external to a phospholipid/water sample, a transbilayer gradient of water chemical potential is created, leading to a transbilayer flux of water (Fick's law). Second, water molecules present within the hydrocarbon region of this phospholipid bilayer interact with phospholipid molecules through their chemical potential (Gibbs-Duhem relation): the conformational state of fatty chains (the thermodynamical state of the phospholipid molecules) changes. This process is slow, as revealed by osmotic stress time-resolved experiments. In thermal chain-melting transitions, the first rapid step is the disordering of fatty chains of a fraction of phospholipid molecules. It occurs a few degrees before the main transition temperature, T(m), during the pretransition and the sub-main transition. The second step, less rapid, is the redistribution of water molecules between the different parts of the sample, as revealed by T-jump time-resolved experiments. Finally, in lyotropic and thermal transitions, hydration and conformation are linked but the order of anteriority of their change, in each case, is probably not the same. In this review, first, the interactions of phospholipid submolecular fragments and water molecules, in the interfacial and hydrocarbon regions of phospholipid/water multibilayer stacks, will be described. Second, the coupling of the conformational states of phospholipid and water molecules, during thermal and lyotropic transitions, will be demonstrated through examples.

Conformation of alamethicin in oriented phospholipid bilayers determined by (15)N solid-state nuclear magnetic resonance

The conformation of the 20-residue antibiotic ionophore alamethicin in macroscopically oriented phospholipid bilayers has been studied using (15)N solid-state nuclear magnetic resonance (NMR) spectroscopy in combination with molecular modeling and molecular dynamics simulations. Differently (15)N-labeled variants of alamethicin and an analog with three of the alpha-amino-isobutyric acid residues replaced by alanines have been investigated to establish experimental structural constraints and determine the orientation of alamethicin in hydrated phospholipid (dimyristoylphosphatidylcholine) bilayers and to investigate the potential for a major kink in the region of the central Pro(14) residue. From the anisotropic (15)N chemical shifts and (1)H-(15)N dipolar couplings determined for alamethicin with (15)N-labeling on the Ala(6), Val(9), and Val(15) residues and incorporated into phospholipid bilayer with a peptide:lipid molar ratio of 1:8, we deduce that alamethicin has a largely linear alpha-helical structure spanning the membrane with the molecular axis tilted by 10-20 degrees relative to the bilayer normal. In particular, we find compatibility with a straight alpha-helix tilted by 17 degrees and a slightly kinked molecular dynamics structure tilted by 11 degrees relative to the bilayer normal. In contrast, the structural constraints derived by solid-state NMR appear not to be compatible with any of several model structures crossing the membrane with vanishing tilt angle or the earlier reported x-ray diffraction structure (Fox and Richards, Nature. 300:325-330, 1982). The solid-state NMR-compatible structures may support the formation of a left-handed and parallel multimeric ion channel.

Helix tilt of the M2 transmembrane peptide from influenza A virus: an intrinsic property

Solid-state NMR has been used to study the influence of lipid bilayer hydrophobic thickness on the tilt of a peptide (M2-TMP) representing the transmembrane portion of the M2 protein from influenza A. Using anisotropic (15)N chemical shifts as orientational constraints, single-site isotopically labeled M2-TMPs were studied in hydrated dioleoylphosphatidylcholine (DOPC) and dimyristoylphosphatidylcholine (DMPC) lipid bilayers oriented between thin glass plates. These chemical shifts provide orientational information for the molecular frame with respect to the magnetic field in the laboratory frame. When modeled as a uniform ideal alpha-helix, M2-TMP has a tilt of 37(+/-3) degrees in DMPC and 33(+/-3) degrees in DOPC with respect to the bilayer normal in these lipid environments. The difference in helix tilt between the two environments appears to be small. This lack of a substantial change in tilt further suggests that significant interactions occur between the helices, as in an oligomeric state, to prevent a change in tilt in thicker lipid bilayers.

Phospholipid acyl chain rotational dynamics are independent of headgroup structure in unilamellar vesicles containing binary mixtures of dioleoyl-phosphatidylcholine and dioleoyl-phosphatidylethanolamine

We have examined relationships between phospholipid headgroup structure and acyl chain dynamics, and their respective roles in modulating the physical properties of biological membranes. Fluorescence lifetime and anisotropy measurements were used to assess structural changes involving the lipid acyl chains in homogeneous populations of small and large unilamellar vesicles containing binary mixtures of dioleoyl-phosphatidylcholine (PC) and dioleoyl-phosphatidylethanolamine (PE) in the liquid-crystalline (Lalpha) phase. These measurements involve three different fluorescent lipid analogs containing diphenylhexatriene (DPH) linked to either a trimethylamine moiety (i.e., TMA-DPH) or the sn-1 position of monostearoyl-phospholipids containing PC or PE headgroups (i.e., DPH-PC and DPH-PE). The average lifetimes, rotational correlation times, and order parameters associated with DPH-PC and DPH-PE are virtually identical, and are not affected by alterations in the PE content of the membrane. These results suggest that the average cross-sectional areas of the phospholipid acyl chains of DOPE and DOPC relative to the membrane normal are similar in these unilamellar vesicles. Since PC headgroups are larger than those of PE, differences in the relative orientation of the phosphocholine and phosphoethanolamine moieties relative to the membrane surface probably function to maintain optimal van der Waals contact interactions between acyl chains. On the other hand, the average lifetime associated with TMA-DPH, whose chromophoric group is near the membrane surface, increases with increasing PE content. The position of TMA-DPH relative to the membrane surface does not change, since the rotational dynamics of TMA-DPH are independent of the PE concentration. Therefore, alterations in the average lifetime of TMA-DPH results from polarity differences near the membrane surface at the level of the glycerol backbone. These results are discussed in terms of how differences in the average conformation of the glycerol backbones or phospholipid headgroups of PE and PC have the potential to regulate membrane function.

Fourier transform infrared spectroscopy as a probe for the study of the hydration of lipid self-assemblies. II. Water binding versus phase transitions

The gradual hydration of phospholipid films can be effectively probed by Fourier transform infrared (FTIR) spectroscopy (cf. part I of this series). The hydration-induced changes observed for lipid IR-absorption bands are probably composed of contributions arising from the effects of both the direct binding of water molecules and the thereby caused conformational changes and phase transitions in the lipid molecules and assemblies, respectively. In this article, an attempt is made to attribute some of the more indicative spectroscopic results to these molecular and supermolecular processes with a view to separating their individual contributions to the relevant spectroscopic data. This is done by considering a series of suitable PLs consisting of the palmitoyl and oleoyl lecithins, DPPC, DOPC, POPC, and OPPC, and one cephalin, DOPE. This choice of PCs and DOPE means that at room temperature and different degrees of hydration, several phase states including lamellar gel and liquid crystalline as well as certain nonlamellar phases are covered. The separation of the water-binding and phase-transition contributions to the FTIR-spectroscopic data, we believe, is clearly demonstrated by interpreting the hydration-dependent wavenumber shifts of the nu C=O band of the PCs. Carbonyl groups are affected to a more significant degree for lipids arrayed in the L alpha phase than in the gel phase. A number of spectral features reveal the lyotropically triggered chain-melting transition as well as other structural rearrangements of PCs. This is discussed in detail and demonstrates the excellent sensitivity of the FTIR methodology for the study of such systems.

Hydration of the dienic lipid dioctadecadienoylphosphatidylcholine in the lamellar phase--an infrared linear dichroism and x-ray study on headgroup orientation, water ordering, and bilayer dimensions

In the phospholipid 1,2-bis(2,4-octadecadienoyl)-sn-glycero-3-phosphorylcholine (DODPC) in each of the fatty acid chains, a rigid diene group is inserted in a position near the polar/apolar boundary that is exceptionally sensitive for membrane stability. DODPC transforms upon gradual dehydration from the liquid-crystalline to a metastable gel state, which rearranges into two subgel phases at low and intermediate degrees of hydration. The molecular dimensions of the respective bilayers were determined by means of x-ray diffraction. Infrared linear dichroism of selected vibrations of the phosphate and trimethylammonium groups and of the nu13(OH) band of water adsorbed onto the lipid was used to study the molecular order in the polar part of the bilayers in macroscopically oriented samples. The dense packing of the tilted acyl chains in the subgel causes the in-plane orientation of the phosphatidylcholine headgroups with direct interactions between the phosphate and trimethylammonium groups, and a strong orientation of adsorbed water molecules. In the more disordered gel, the thickness of the polar part of the bilayer increases and the lateral interactions between the lipid headgroups weaken. The higher order in the headgroup region of the subgels correlates with shorter decay lengths of the repulsive forces acting between opposite membrane surfaces. This result can be understood if the work to dehydrate the lipid is determined to a certain degree by the work to break up the lipid-water interactions without compensation by adequate lipid-lipid contacts. Almost similar area compressibility moduli are found in the liquid-crystalline and solid phases. Obviously, the lipid avoids lateral stress by the structural rearrangement.

Is the high propensity of ethanolamine plasmalogens to form non-lamellar lipid structures manifested in the properties of biomembranes?

Plasmalogens are glycerophospholipids characterized by an alk-1'-enylether bond in position sn-1 and an acyl bond in position sn-2. These ubiquitous etherlipids exhibit a different molecular structure as compared to diacyl phospholipids. The most peculiar change is a perpendicular orientation of the sn-2 acyl chain at all segments to the membrane surface. This extended conformation results in an effectively longer aliphatic chain in plasmalogen than in the diacyl analog. Moreover, the lack of the carbonyl oxygen in position sn-1 affects the hydrophilicity of the headgroup and allows stronger intermolecular hydrogen-bonding between the headgroups of the lipid. These properties favour the formation of non-lamellar structures which are expressed in the high affinity of ethanolamine plasmalogen to adopt the inverse hexagonal phase. Such structures may be involved in membrane processes, either temporarily, like in membrane fusion or locally, e.g. to affect the activity of membrane-bound proteins. The predominant distribution of ethanolamine plasmalogens in some cellular membranes like nerve tissues or plasma membranes and their distinctly different properties in model membranes as compared to diacyl phospholipids impose the question, whether these differences are also manifested in the heterogeneous environment of biological membranes. The integration of biophysical studies and biochemical findings clearly indicated that the high propensity of ethanolamine plasmalogen to form non-lamellar structures is reflected in several physiological functions. So far it seems to be evident that ethanolamine plasmalogens play an important role in maintaining the balance between bilayer and non-lamellar phases which is crucial for proper cell function. Furthermore, they are the major phospholipid component of inverse hexagonal phase inclusions in native retina and are able to mediate membrane fusion as demonstrated between neurotransmitter vesicles and presynaptic membranes.

Definition of lipid membrane structural parameters from neutronographic experiments with the help of the strip function model

Neutron diffraction is an effective method for investigating model and biological membranes. Yet, to obtain accurate structural information it is necessary to use deuterium labels and much time is needed to acquire experimental data as there are a large number of diffraction reflections to register. This paper offers a way to define the hydrophobic boundary position in lipid membranes with high accuracy and for this purpose it is sufficient to take into consideration three structural factors. The method is based on modeling the density of the neutron diffraction amplitude rho(x) in the direction of the bilayer plane normal by means of a strip function, but it also takes into consideration the fact that the multiplication of the strip function amplitude rho i by the step width zi-zi-1 makes the sum of neutron scattering amplitudes of the atoms included in the step region. On the basis of the analysis of a large number of experimental data for different membranes, the effectiveness of this method in the determination of the position of hydrophilic/hydrophobic boundary is demonstrated, including the case of various rho(x) modifications in the region of polar heads and also the different phase states of membranes. However, it is shown in the present paper that the strip function model is not an adequate instrument for the determination of other structural parameters of membranes.

Chemical hydrolysis of phospholipids

Hydrolysis kinetics of phospholipids in liposomes composed of dimyristoylphosphatidylcholine (DMPC), dipalmitoylphosphatidylcholine/cholesterol (DPPC/CHOL) 10/4 (molar ratio) and egg phosphatidylcholine (EPC) at pH 4.0 and different temperatures could be described by Arrhenius curves without breaks. However, the Arrhenius curves for the hydrolysis of liposomal DPPC and distearoylphosphatidylcholine (DSPC) under the same conditions were biphasic. A break was observed in the curves extending over a broad range before and after the known Tm of each of these phospholipids in liposomes (42 and 56 degrees C, respectively). The activation energy (Ea) for the hydrolysis of liposomal DPPC and DSPC below the Tm was substantially larger than the Ea for liposomal DMPC, DPPC/CHOL 10/4, and EPC and decreased when DPPC was mixed with CHOL in a 10/4 molar ratio. Hardly any influence of the presence of alpha-tocopherol, cryoprotectants (glucose, trehalose, sucrose, and propylene glycol), and the major hydrolysis products lysophospholipids and fatty acids or of the absence of sodium chloride on the hydrolysis kinetics of DPPC at pH 4.0 and 30 degrees C was observed. Changes in fatty acid chains and size did not influence the hydrolysis rate constant (kobs) of liposomal phospholipids at pH 4.0 and 30 degrees C either. The only effects of uncharged compounds on the kobs of liposomal DPPC at pH 4.0 and 30 degrees C were found upon mixing with a high concentration of the detergent Triton X-100 or palmitic acid.(ABSTRACT TRUNCATED AT 250 WORDS)

Thermal transitions in dimyristoylphosphatidylcholine foam bilayers

Thermal transitions in the system dimyristoylphosphatidylcholine/water/ethanol/sodium chloride were studied in the temperature range 10-31 degrees C. The water-ethanol dispersions were investigated by differential scanning calorimetry and the foam bilayers by the microinterferometric method for investigation of thin liquid films. Calorimetry showed that an increase in ethanol content (up to 47.5 vol.%-the concentration used in the experiments with foam bilayers) did not significantly influence the temperature of the main phase transition and led to the disappearance of the pretransition. The microinterferometric study of the foam bilayer thickness showed that there were two thermal transitions-at 13 and 23 degrees C. An Arrhenius type dependence was obtained for the critical concentration of dimyristoylphosphatidyl-choline (DMPC) in the solution, which was necessary for the formation of the foam bilayer. A steep change in the slope of the linearized Arrhenius dependence was found at 23 degrees C. Values of the binding energy of a DMPC molecule in the foam bilayers were calculated using the hole-nucleation theory of stability and permeability of bilayers. It was proved that the phase transition at 23 degrees C was due to melting of the hydrocarbon tails of phospholipid molecules. The low-temperature phase transition was assumed to be due to a change in the tilt of the hydrocarbon tails. These experiments demonstrate for the first time the occurrence of phase transitions in foam bilayers.

Chemical stability of liposomes: implications for their physical stability

In the first part of this article, chemical and physical stability of aqueous liposome dispersions have been addressed. Chemical stability of phospholipids has been considered in two parts: oxidation and hydrolysis. Major attention has been paid to hydrolysis kinetics of phospholipids as a function of pH, temperature, buffer concentration and ionic strength. Furthermore, the effect of chain length, head group, state of aggregation, addition of cholesterol and presence of charge on the hydrolysis kinetics of phospholipids has been dealt with. In the second part physical stability of chemically degraded liposome dispersions has been evaluated. In the final part quality control assays for liposome dispersions is presented and a HPLC method with a refractive index detector for the analysis of phospholipids from aqueous liposome dispersions is described.

Polarity of lipid bilayers. A fluorescence investigation

Through steady-state and time-resolved fluorescence experiments, the polarity of the bilayers of egg phosphatidylcholine vesicles was studied by means of the solvatochromic 2-anthroyl fluorophore which we have recently introduced for investigating the environmental micropolarity of membranes and which was incorporated synthetically in phosphatidylcholine molecules (anthroyl-PC) in the form of 8-(2-anthroyl)octanoic acid. Fluorescence quenching experiments carried out with N,N-dimethylaniline and 12-doxylstearic acid as quenchers showed that the 2-anthroyl chromophore was located in depth in the hydrophobic region of the lipid bilayer corresponding to the C9-C16 segment of the acyl chains. Steady-state fluorescence spectroscopy revealed a nonstructured and red-shifted (lambda em(max) = 464 nm) spectrum for the probe in egg-PC bilayers, which greatly differed from the structured and blue (lambda em(max) = 404 nm) spectrum the fluorophore was shown to display in n-hexane. While the fluorescence decays of the fluorophore in organic solvents were monoexponential, three exponentials were required to account for the fluorescence decays of anthroyl-PC in egg-PC vesicles, with average characteristic times of 1.5 ns, 5.5 ns, and 20 ns. These lifetime values were independent of the emission wavelength used. Addition of cholesterol to the lipid did not alter these tau values. One just observed an increase in the fractional population of the 1.5-ns short-living species detrimental to the population of the 20-ns long-living ones. These observations enabled time-resolved fluorescence spectroscopy measurements to be achieved in the case of the 1/1 (mol/mol) egg-PC/cholesterol mixture. Three distinct decay associated spectra (DAS) were recorded, with maximum emission wavelengths, respectively, of 410 nm, 440 nm, and 477 nm for the 1.5-ns, 6-ns, and 20-ns lifetimes found in this system. On account of the properties and the polarity scale previously established for the 2-anthroyl chromophore in organic solvents, these data strongly suggest the occurrence of three distinct excited states for anthroyl-PC in egg-PC bilayers, corresponding to three environments for the 2-anthroyl chromophore, differing in polarity. The lifetime of 1.5 ns and the corresponding structured and blue (lambda em(max) = 410 nm) DAS account for a hydrophobic environment, with an apparent dielectric constant of 2, which is that expected for the hydrophobic core of the lipid bilayer.(ABSTRACT TRUNCATED AT 400 WORDS)

Effect of the unsaturation of phospholipid acyl chains on leucine transport of Lactococcus lactis and membrane permeability

The effect of the degree of unsaturation of the phospholipid acyl chains on the branched-chain amino acid transport system of Lactococcus lactis was investigated by the use of a membrane fusion technique. Transport activity was analyzed in hybrid membranes composed of equimolar mixtures of synthetic unsaturated phosphatidylethanolamine (PE) and phosphatidylcholine (PC) in which the number of cis double bonds in the 18-carbon acyl chains was varied. The accumulation level and initial rate of both counterflow and protonmotive-force driven transport of leucine decreased with increasing number of double bonds. The reduction in transport activity with increasing number of double bonds correlated with an increase in the passive permeability of the membranes to leucine. The membrane fluidity was hardly affected by the double bond content. It is concluded that the degree of lipid acyl chain unsaturation is a minor determinant of the activity of the branched chain amino acid transport system, but effects strongly the passive permeability of the membrane.

Structure of a fluid dioleoylphosphatidylcholine bilayer determined by joint refinement of x-ray and neutron diffraction data. III. Complete structure

We present in this paper the complete structure of 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC) in the L alpha phase (66% RH, 23 degrees C) obtained by the joint refinement of neutron and x-ray lamellar diffraction data. The structural details obtained have previously required a large number of neutron diffraction experiments, using numerous specifically-deuterated phospholipid isomorphs (Büldt et al., 1978. Nature (Lond.). 271:182-184). The joint-refinement approach minimizes specific deuteration by utilizing independent neutron and x-ray data sets. The method yields a quasimolecular structure consisting of a series of multiatomic fragments that are each represented by one or several Gaussian distributions whose positions and widths can be determined to within 0.06 to 0.52 A exclusive of the methylene region. The image of DOPC at 66% RH (5.36 +/- 0.08 waters per lipid) is consistent with many aspects of bilayer structure previously determined by structural and spectroscopic studies. The most striking feature of the structure is the large amount of transbilayer thermal motion suggested by the widths and overlaps of the Gaussian envelopes of the quasimolecular fragments. We discuss the "dynamic bilayer thickness" which describes the minimum effective thickness of the hydrocarbon permeability barrier in terms of the thermal motion of the water. A gradient of thermal motion exists that increases in either direction away from the glycerol backbone which is the most constrained portion of the bilayer. The steric interactions between headgroups of apposed bilayers, expected at the hydration level of our experiments, are clearly revealed. A useful consequence of the quasimolecular structure is that average boundaries within bilayers calculated using composition and volumetric data and ad hoc assumptions can be related to the positions of the principal structural groups. Several measures of "bilayer thickness" in common use can be identified as the positions of the cholines for Luzzati's d1 (Luzzati and Husson. 1962. J. Cell Biol. 12:207-219) and the glycerols for Small's dL (Small. 1967. J. Lipid Res. 8:551-556). We do not know if these relations will be true at other hydrations or for other lipids. Of particular interest is the fact that the position of the carbonyl groups marks the average hydrocarbon/headgroup boundary. It must be emphasized, however, that this region of the bilayer must be generally characterized as one of tumultuous chemical heterogeneity because of the thermal motion of the bilayer.

Incorporation of phosphonic acid diesters into lipid model membranes. Part II. X-ray and neutron diffraction studies

Mixtures of egg phosphatidylcholine and phosphonic acid diethyl or dibutyl esters of the general type RP(O)(OR')2 with R = hexane or dodecane were studied at room temperature in the fluid lamellar state by X-ray and by neutron diffraction. Generally a molar ratio of lipid and ester of 1:0.5 was used. Additionally an equimolar lipid/ester mixture of hexane phosphonic acid diethyl ester was studied. Depending on the ester used and its concentration a single L alpha-phase was observed above a certain water content which changes to an L alpha + water two phase system at high water concentration. Despite the large amounts of the amphiphilic ester molecules incorporated in the membrane and their high molecular asymmetry, the mixtures qualitatively show the typical hydration and swelling behaviour of non-charged lipid membranes. However, the incorporation of the esters induces a higher hydration capacity, a lateral extension and a decrease in membrane thickness. The position of the ester molecules and their orientation in the membrane were determined by neutron diffraction using partially deuterated esters. The esters were found to be located with their phosphonic moiety near or in the lipid/water interface. The lamellar structure contradicts this location of the cone-shaped ester molecules which should increase the tendency to form hexagonal structures. However, the experimental findings can be understood if one considers a partial interdigitation of the last hydrocarbon groups of the lipid chains accompanied by a larger disorder in the hydrophobic centre of the membrane. In the case of hexane phosphonic acid dibutyl ester, a vertical translocation of the ester takes place below a certain water content where it is distributed between two locations at the lipid water interface and the centre of the membrane.

Hydrophobic membrane thickness and lipid-protein interactions of the leucine transport system of Lactococcus lactis

The effect of the phospholipid acyl chain carbon number on the activity of the branched-chain amino acid transport system of Lactococcus lactis has been investigated. Major fatty acids identified in a total lipid extract of L. lactis membranes are palmitic acid (16:0), oleic acid (18:1) and the cyclopropane-ring containing lactobacillic acid (19 delta). L. lactis membrane vesicles were fused with liposomes prepared from equimolar mixtures of synthetic phosphatidylethanolamine (PE) and phosphatidylcholine (PC) with cis mono-unsaturated acyl chains. The activity of the branched-chain amino acid carrier is determined by the bulk properties of the membrane (Driessen, A.J.M., Zheng, T., In 't Veld, G., Op den Kamp, J.A.F. and Konings, W.N. (1988) Biochemistry 27, 865-872). PE acts as an activator and PC is ineffective. Counterflow and protonmotive-force driven transport of leucine is sensitive to changes in the acyl chain carbon number of both phospholipids and maximal with dioleoyl-PE/dioleoyl-PC. Above the gel to liquid-crystalline phase transition temperature of the lipid species, membrane fluidity decreased with increasing acyl chain carbon number. Our data suggest that the carbon number of the acyl chains of PE and PC determine to a large extent the activity of the transport system. This might be relevant for the interaction of PE with the transport protein. Variations in the acyl chain composition of PC exert a more general effect on transport activity. The acyl chain composition of phospholipids determines the membrane thickness (Lewis, B.A. and Engelman, D.M. (1983) J. Mol. Biol. 166, 211-217). We therefore propose that the degree of matching between the lipid-bilayer and the hydrophobic thickness of the branched-chain amino acid carrier is an important parameter in lipid-protein interactions.

Resolution of phospholipid conformational heterogeneity in model membranes by spin-label EPR and frequency-domain fluorescence spectroscopy

We have utilized both fluorescent and nitroxide derivatives of stearic acid as probes of membrane structural heterogeneity in phospholipid vesicles under physiological conditions, as well as conditions of varying ionic strengths and temperatures where spectral heterogeneity has been previously observed and attributed to multiple ionization states of the probes. To identify the source of this spectral heterogeneity, we have utilized complimentary measurements of the relaxation properties (lifetimes) and motion of both (a) spin labeled and anthroyloxy derivatives of stearic acid (i.e., SASL and AS) and (b) a diphenylhexatriene derivative of phosphatidylcholine (DPH-PC) in single component membranes containing dimyristoylphosphatidylcholine (DMPC). We use an 15N stearic-acid spin label for optimal sensitivity to membrane heterogeneity. The lifetime and dynamics of the fluorescent phospholipid analogue DPH-PC (with no ionizable groups over this pH range) were compared with those of AS, allowing us to discriminate between changes in membrane structure and the ionization of the label. The quantum yield and rotational dynamics of DPH-PC are independent of pH, indicating that changes in pH do not affect the conformation of the host phospholipids. However, both EPR spectra of SASL and the lifetime or dynamics of AS are affected profoundly by changes in solution pH. The apparent pKa's of these two probes in DMPC membranes were determined to be near pH 6.3, implying that at physiological pH and ionic strength these stearic-acid labels exist predominantly as a single ionized population in membranes. Therefore, the observed temperature- and ionic-strength-dependent alterations in the spectra of SASL as well as the lifetime or dynamics of AS in DMPC membranes at neutral pH are due to changes in membrane structure rather than the ionization of the probes. The possibility that ionic gradients across biological membranes induce alterations in phospholipid structures, thereby modulating lipid-protein interactions is discussed.

Effects of small organic molecules on phospholipid phase transitions

Small organic molecules are known to exhibit a wide spectrum of physiological or pharmacological effects and many of them are thought to be membrane associated. Therefore a great number of studies is devoted to the interaction between these molecules and phospholipid model membranes. Results obtained for molecular species of varying hydrophobic/hydrophilic balances will be described. It will be shown that, in general, these different molecules induce similar effects on phospholipid phase transitions, although they are located differently in the membrane. Detailed studies of these interactions will help to understand these processes on a molecular level.

Stabilization of non-bilayer structures by the etherlipid ethanolamine plasmalogen

The thermotropic phase behavior of mixtures between diradylphosphatidylethanolamines and diacylphosphatidylcholine was studied using polarized light microscopy, 31P-NMR spectroscopy and synchrotron X-ray diffraction. Multilamellar liposomes composed of alkenylacylphosphatidylethanolamine (ethanolamine plasmalogen) undergo a phase transition from a lamellar to an inverse hexagonal lipid structure at 30 degrees C, which is about 20 degrees C and 30 degrees C lower as compared to its alkylacyl- and diacyl-analog, respectively. These results indicate a higher affinity to non-bilayer structures for the ether lipids. In the presence of the bilayer stabilizing phospholipid, palmitoyloleoylphosphatidylcholine, the transition is shifted to higher temperature without any significant changes in the overall structural parameters as revealed by X-ray diffraction experiments. Again, ethanolamine plasmalogen stabilizes the inverted hexagonal phase to the highest extent, i.e. even in the presence of 40 mol% palmitoyloleoylphosphatidylcholine a pure inverse hexagonal phase is formed at 60 degrees C. Such a result was not reported so far for a diacylphosphatidylethanolamine. This property of ethanolamine plasmalogen might be predominantly explained by an optimized packing of the hydrocarbon chains in the corners and interface region of the hexagonal tubes, owing to a different conformation of the sn-2 chain, which was deduced from 2H-NMR experiments (Malthaner, M., Hermetter, A., Paltauf, F. and Seelig, J. (1987) Biochim. Biophys. Acta 900, 191-197). Data obtained by time resolved X-ray diffraction show a coexistence of lamellar and inverse hexagonal structures in the phase transition region, but do not indicate the existence of non-lamellar intermediates or disorder within the sensitivity limits of the method.

Adsorption to dipalmitoylphosphatidylcholine membranes in gel and fluid state: pentachlorophenolate, dipicrylamine, and tetraphenylborate

We measured the dependence of electrophoretic mobility of dipalmitoylphosphatidylcholine (DPPC) vesicles on the aqueous concentration of negatively charged ions of pentachlorophenol (PCP), dipicrylamine (DPA), and tetraphenylborate (TPhB). The objective was to determine how the physical state of hydrocarbon chains of lipids affects adsorption of lipophilic ions. The studies were done at 25 and 42 degrees C to determine adsorption properties of DPPC membrane in the gel and fluid state, respectively. From the analysis of zeta-potential isotherms in terms of Langmuir-Stern-Grahame model we obtained the association constant, K, the area of the adsorption site, Ps, and the linear partition coefficient, beta.

RESULTS

K, (x 10(4)M-1): K(gel): PCP (0.49 +/- 0.28), DPA (25 +/- 10), TPhB (31 +/- 10); K(fluid): PCP (4.5 +/- 0.9), DPA (74 +/- 21), TPhB (59 +/- 14); Ps, (nm2): Ps(gel): PCP (5.4 +/- 2.3), DPA (5.9 +/- 2), TPhB (5.0 +/- 1.7); Ps(fluid): PCP (4.5 +/- 0.4), DPA (5.2 +/- 0.4), TPhB (4.1 +/- 0.2); beta, (x 10(-5) m): beta(gel): PCP (0.15 +/- 0.09), DPA (7.1 +/- 0.3), TPhB (10 +/- 7); beta(fluid): PCP (1.7 +/- 0.3), DPA (24 +/- 7), TPhB (24 +/- 6). It was interesting to find that the adsorption site area for PCP, DPA, and TPhB were very similar for both the gel and fluid membranes; also, the areas were independent of the size and molecular structure of the adsorbing species. Using a simple discrete charge model the adsorption site areas for all species were consistent with a dielectric constant of 8-10 and with an ion adsorption depth of 0.4-0.6 nm below the water/dielectric interface. The delta delta G0 = delta G0(gel) - delta G0(fluid) was found to be about twice as large for PCP than for DPA and TPhB. This indicates that PCP will be significantly more adsorbed in the fluid and disordered regions of biomembranes, whereas the distribution of DPA and TPhB is expected to be relatively more even.

Relationships between lipid membrane area, hydrophobic thickness, and acyl-chain orientational order. The effects of cholesterol

A microscopic interaction model for a fully hydrated lipid bilayer membrane containing cholesterol is used to calculate, as a function of temperature and composition, the membrane area, the membrane hydrophobic thickness, and the average acyl-chain orientational order parameter, S. The order parameter, S, is related to the first moment, M1, of the quadrupolar magnetic resonance spectrum which can be measured for lipids with perdeuterated chains. On the basis of these model calculations as well as recent experimental measurements of M1 using magnetic resonance and of membrane area using micromechanical measurements, a discussion of the possible relationships between membrane area, hydrophobic thickness, and moments of nuclear magnetic resonance spectra is presented. It is pointed out that S under certain circumstances may be useful for estimating the hydrophobic membrane thickness. This is particularly advantageous for multicomponent membranes where structural data are difficult to obtain by using diffraction techniques. The usefulness of the suggested relationships is demonstrated for cholesterol-containing bilayers.