Planar bilayer membranes from pure lipids.

Planar lipid bilayer membranes are formed from mixtures of pure lipids in the absence of non-biological solvents. The solventless bilayers are characterized by a large specific capacitance (586-957 nF/cm2) comparable to that of cell membranes but considerably greater than that of conventional lipid/decane bilayers. Hydrocarbon solvents, such as n-alkanes or squalene, thicken the bilayer. Membrane dielectric thickness is used as an indicator of bilayer lipid composition. For membranes made from pure monoglyceride/triglyceride mixtures the thickness of the solventless lipid bilayer is independent of both the chain length (11-22 carbons) and mol fraction (0.1-0.9) of triglyceride in the bulk mixture. In contrast, the thickness of the bilayer (2.0-3.3 nm) depends strongly upon the length (16-24 carbons) of the monoglyceride component. Molecular volume considerations lead to the conclusion that the bulk lipid mixture disproportionates to yield bilayer membranes composed of nearly pure monoglyceride. The dielectric thickness of the monoglyceride bilayer is consistent with the notion that the lipid fatty acyl chains are fluid.     

Large amplitude photo-voltage transients of bilayer lipid membranes in the presence of chlorophyllin

Large amplitude electrical voltage transients result from the flash illumination of bilayer lipid membranes (BLM) in the presence of chlorophyllin, electron acceptors [FeCl₃ or (NH₄)₂ Ce(NO₃)₆] and an electron donor (FeCl₂). The BLM were prepared from lecithin and oxidized cholesterol, or spinach chloroplast extracts. The photo-voltage waveforms observed may be resolved into three components, which have characteristic times of approximately the flash duration (8 sec), 1 msec, and the BLM resistance-capacitance discharge time. These components are thus comparable to the Components A, B, and D previously reported for BLM and thin lipid membranes (TLM) of the spinach chloroplast extracts in the presence of electron acceptors. Component C of the chloroplast-BLM is extinguished by near trace quantities (1 g/l) of chlorophyllin. Higher concentrations (1 to 20 mg/l) reduce the BLM resistance and stability but under some conditions the Component A response exceeds 200 mV. The inferred peak photo-current exceeds 10 mA/cm². Membrane resistance and stability data suggest that the chlorophyllin bonds within and disrupts the adjacent interface (monolayer), but that it does not permeate the BLM.     

Cyanine dye structural and voltage-induced variations in photo-voltages of bilayer membranes

Summary Flash illumination alters the voltage across bilayer lipid membranes in the presence of certain cyanine dyes. The waveforms of the photo-voltage vary systematically with dye structure and imposed transmembrane voltage. Experimental results are reported for 27 positively charged cyanine dyes, primarily oxazole derivatives, using lecithin/oxidized cholesterol bilayer membranes and 10-mm sodium chloride solutions. Several dyes do not induce any photo-voltages. Examples are 3,3 diethyl 9 ethyl 2,2 oxacarbocyanine iodide, 3,3 diethyl 2 oxa 2 thiacyanine iodide, and 3,3 dimethyl 2,2 indocarbocyanine iodide. Several dyes, when added to one side of the membranes, induce monophasic waveforms. Examples are 3,3 dimethyl 2,2 oxacarbocyanine chloride, and 3,4,3,4 tetramethyl 2,2 oxazalinocarbocyanine iodide. Other dyes induce a photo-voltage only if transmembrane voltages are imposed. These waveforms are biphasic with some dyes (3,3 diethyl 2,2 oxacarbocyanine iodide, for example) and monophasic with other dyes (3,3 dibutyl 2,2 oxacarbocyanine iodide, for example).The photo-voltage waveforms are explained by models that consider the movement of charged dye molecules within the membrane, following optical excitation. The dye movements are probably induced through charge rearrangements in the dye associated with long-lived triplet states, isomerization, or through excimer formation. These results provide information on the location and orientation of the dye molecules within bilayer membranes. The variations which occur in the waveforms with applied voltage indicate that these membranes are fluid in the direction perpendicular to the membrane plane.     

Voltage transients in neuronal dendritic trees.

An analytical method is outlined for calculating the passive voltage transient at each point in an extensively branched neuron model for arbitrary current injection at a single branch. The method is based on a convolution formula that employs the transient response function, the voltage response to an instantaneous pulse of current. For branching that satisfies Rall's equivalent cylinder constraint, the response function is determined explicitly. Voltage transients, for a brief current injected at a branch terminal, are evaluated at several locations to illustrate the attenuation and delay characteristics of passive spread. A comparison with the same transient input terminal input, the fraction of input charge dissipated by various branches in the neuron model is illustrated. These fractions are independent of the input time course. For transient synaptic conductance change at a single branch terminal, a numerical example demonstrates the nonlinear effect of reduced synaptic driving potential. The branch terminal synaptic input is compared with the same synaptic conductance input applied to the soma on the basis of excitatory postsynaptic potential amplitude at the soma and charge delivered to the soma.     

Galactocerebroside-phospholipid interactions in bilayer membranes.

Differential scanning calorimetry (DSC) and x-ray diffraction have been used to study the interaction of hydrated N-palmitoylgalactosylsphingosine (NPGS) and dipalmitoylphosphatidylcholine (DPPC). For mixtures containing less than 23 mol% NPGS, complete miscibility of NPGS into hydrated DPPC bilayers is observed in both the bilayer gel and liquid-crystal phases. X-ray diffraction data demonstrate insignificant differences in the DPPC-bilayer gel-phase parameters on incorporation of up to 23 mol% NPGS. At greater than 23 mol% NPGS, additional high-temperature transitions occur, indicating phase separation of cerebroside. For these cerebroside concentrations, at 20 degrees C, x-ray diffraction shows two lamellar phases, hydrated DPPC-NPGS gel bilayers (d = 64 A) containing 23 mol% NPGS, and NPGS "crystal" bilayers (d = 55 A). On heating to temperatures greater than 45 degrees C, the mixed DPPC-NPGS bilayer phase undergoes chain melting, and on further increasing the temperature progressively more NPGS is incorporated into the liquid-crystal DPPC-NPGS bilayer phase. At temperatures greater than 82 degrees C (the transition temperature of hydrated NPGS), complete lipid miscibility is observed at all DPPC/NPGS molar ratios.     

Dynamically stabilized pores in bilayer membranes.

Zhelev and Needham have recently created large, quasistable pores in artificial lipid bilayer vesicles. Initially created by electroporation, the pores remain open for up to several seconds before quickly snapping shut. This result is surprising, in light of the large line tension for holes in bilayer membranes and the rapid time scale for closure of large pores. We show how pores can be dynamically stabilized via a new feedback mechanism. We also explain quantitatively the observed sudden pore closure as a tangent bifurcation. Finally, we show how Zhelev and Needham's experiment can be used to measure accurately the pore line tension, an important material parameter. For their stearoyloleoylphosphatidylcholine/cholesterol mixture we obtain a line tension of 2.6 x 10(-6) dyn.     

Ionic transport in lipid bilayer membranes.

The current-voltage relationships of model bilayer membranes have been measured in various phospholipid systems, under the influence of both a gradient of potential and an ionic concentration, in order to describe the ion translocation through hydrated transient defects (water channels) across the bilayer formed because of lipid structure fluctuations and induced by temperature. The results have been analyzed in the light of a statistical rate theory for the transport process across a lipid bilayer, recently proposed by Skinner et al. (1993). In order to take into account the observed I-V curves and in particular the deviation from an ohmic behavior observed at high potential values, the original model has been modified, and a new version has been proposed by introducing an additional kinetic process. In this way, a very good agreement with the experimental values has been obtained for all of the systems we have investigated (dimyristoylphosphatidyl ethanolamine bilayers and mixed systems composed by dimyristoylphosphatidyl ethanolamine/dimyristoylphosphatidylcholine mixtures and dimyristoylphosphatidyl ethanolamine/phosphatidic acid dipalmitoyl mixtures). The rate constants governing the reactions at the bilayer interfaces have been evaluated for K+ and Cl- ions, as a function of temperature, from 5 to 35 degrees C and bulk ionic concentrations from 0.02 to 0.2 M. Finally, a comparison between the original model of Skinner and the modified version is presented, and the advantages of this new formulation are briefly discussed.     

Phospholipid exchange between bilayer membranes.

The mode of interaction of aqueous dispersions of phospholipid vesicles is investigated. The vesicles (average diameter 950 A) are prepared from total lipid extracts of Escherichia coli composed of phosphatidylethanolamine, phosphatidylglycerol and cardiolipin. One type of vesicle contains trans-delta 9-octadecenoate, the other type trans-delta 9-hexadecenoate as predominant acyl chain component. The vesicles show order in equilibrium disorder transitions at transition temperatures, Tt = 42 degrees C and Tt = 29 degrees C, respectively. A mixture of these vesicles is incubated at 45 degrees C and lipid transfer is studied as a function of time using the phase transition as an indicator. The system reveals the following properties: Lipids are transferred between the two vesicle types giving rise to a vesicle population where both lipid components are homogeneously mixed. Lipid transfer is asymmetric, i.e. trans-delta 9-hexadecenoate-containing lipid molecules appear more rapidly in the trans-delta 9-octadecenoate-containing vesicles than vice versa. At a given molar ratio of the two types of vesicles the rate of lipid transfer is independent of the total vesicle concentration. It is concluded that lipid exchange through the water phase by way of single molecules or micelles is the mode of communication of these negatively charged lipid vesicles.     

Calcium-induced changes in bilayer membranes from oxidized cholesterol

Elastic properties of oxidized cholesterol bilayers in n-octane and membrane solvent free were studied by measuring Young modulus E perpendicular in the direction perpendicular to the membrane plane as a function of concentration of calcium ions. Interaction between calcium ions and solvent free bilayers resulted in a significant increases of Young modulus E perpendicular in the concentration range 20-40 mmol/l Ca2+. It is suggested that the hardening of the membrane is caused by some structural changes in the hydrophobic region of the membrane.     

Polarity-dependent voltage-gated porin channels from Escherichia coli in lipid bilayer membranes.

A porin preparation from Escherichia coli 0111:B4 consisting of Omp F and Omp C (with Omp F in excess) was purified by salt extraction procedures and investigated in bilayer lipid membranes formed according to the Montal-Mueller technique. The porin preparation was added to the KCl electrolyte compartment of the Montal-Mueller cell which was connected to the voltage source. As the porin incorporated into the membrane, asymmetric, voltage-gated ion channels were formed. Transmembrane voltages greater than +50 mV (measured with respect to the side of porin addition) caused channel closing, while negative voltages, on the other hand, had no effect on channel behaviour but did increase the rate of porin incorporation at higher voltages. With porin added to both compartments voltage gating no longer occurred. Single-channel conductances corresponded to effective pore diameters of 1.5 nm for opening events and 1.18 nm for channel closing events. The number of charges involved in gating was approximately 2.     

Formation of planar bilayer membranes from lipid monolayers. A critique.

The formation of planar bilayer membranes from lipid monolayers as described by Montal and Mueller (Proc. Natl. Acad. Sci. 1972. 69:3561) is analyzed. Bilayers absolutely free of alkane solvents or other nonpolar hydrocarbons can be formed on polytetrafluoroethylene (PTFE) (e.g. Teflon) septa only if certain boundary conditions are satisfied. Measurements have been made of the contact angles between monolayer-coated water and PTFE in the presence and absence of alkane solvents. The measurement suggest that the boundary conditions for formation of stable bilayers can be satisfied only when a nonpolar solvent is present. We conclude that the bilayer must be surrounded by a torus of alkane solvent, petroleum jelly, or silicone grease depending upon the details of technique used to form the bilayer. The non-polar solvent used in the formation of the bilayer may or may not be present in the bilayer depending upon the water solubility and size of the solvent molecule relative to the size of the alkyl chain of the lipid. Detailed sketches describing the formation of bilayers from monolayers are presented.     

Voltage jump/capacitance relaxation studies of bilayer structure and dynamics. Studies on oxidized cholesterol membranes.

A voltage-jump technique for the study of the time course of small, voltage-induced changes in the structure of single bilayers is presented, and a method is introduced whereby electromechanical (electrostrictive) phenomena can be separated from dielectric relaxations. As no foreign molecules need be introduced into the bilayers, the question about probe artifacts is eliminated. The time constants and amplitudes of dielectric relaxations in oxidized cholesterol bilayers at 21 degrees C, along with their tentative identification are: (a) tau = 3.3 msec, deltaC/Co = 0.8% and tau = 0.7 msec, deltaC/Co = 0.6%: reorientation in the plane of the membrane of domains or clusters of dipoles. (b) tau = 155 musec, deltaC/Co = 1.5-3%: rotational reorientation of individual molecules. (c) tau = 18 musec, deltaC/Co - 1.4%: small amplitude reorientations individual dipoles about an axis lying in the plane of the membrane. Electrostictive effects with time constants between about 2 and 50 msec were also detected. A temperature study of both the dielectric and electrostrictive phenomena is reported. The application of the technique to other membrane compositions and to a variety of BLM problems is discussed.     

Fusion of synaptic vesicle membranes with planar bilayer membranes.

The interaction of synaptic vesicles with horizontal bilayer lipid membranes (BLMs) was investigated as a model system for neurotransmitter release. High concentrations (200 mM) of the fluorescent dye, calcein, were trapped within synaptic vesicles by freezing and thawing. In the presence of divalent ions (usually 15 mM CaCl2), these frozen and thawed synaptic vesicles (FTSVs) adhere to squalene-based phosphatidylserine-phosphatidylethanolamine BLMs whereupon they spontaneously release their contents which is visible by fluorescence microscopy as bright flashes. The highest rate of release was obtained in KCl solutions. Release was virtually eliminated in isotonic glucose, but could be elicited by perfusion with KCl or by addition of urea. The fusion and lysis of adhering FTSVs appears to be the consequence of stress resulting from entry of permeable external solute (KCl, urea) and accompanying water. An analysis of flash diameters in experiments where Co+2, which quenches calcein fluorescence, was present on one or both sides of the BLM, indicates that more than half of the flashes represent fusion events, i.e., release of vesicle contents on the trans side of the BLM. A population of small, barely visible FTSVs bind to BLMs at calcium ion concentrations of 100 microM. Although fusion of these small FTSVs to BLMs could not be demonstrated, fusion with giant lipid vesicles was obvious and dramatic, albeit infrequent. Addition of FTSVs or synaptic vesicles to BLMs in the presence of 100 microM-15 mM Ca2+ produced large increases in BLM conductance. The results presented demonstrate that synaptic vesicles are capable of fusing with model lipid membranes in the presence of Ca+2 ion which, at the lower limit, may begin to approach physiological concentrations.     

Biological membranes as bilayer couples. III. Compensatory shape changes induced in membranes

We have previously proposed the hypothesis that asymmetric membranes behave like bilayer couples: the two layers of the bilayer membrane can respond differently to a particular perturbation. Such a perturbation, for example, can result in the expansion of one layer relative to the other, thereby producing a curvature of that membrane. In experiments with erythrocytes and lymphocytes, we now demonstrate that different membrane perturbations which have opposite effects on membrane curvature can compensate and neutralize one another, as expected from the bilayer couple hypothesis. This provides a rational basis, for example, for understanding the effects of amphipathic drugs on a variety of cellular phenomena which involve shape changes of membranes.     

Pressure effects on alamethicin conductance in bilayer membranes.

We report here the first observations of the effects of elevated hydrostatic pressure on the kinetics of bilayer membrane conductance induced by the pore-forming antibiotic, alamethicin. Bacterial phosphatidylethanolamine-squalene bilayer membranes were formed by the apposition of lipid monolayers in a vessel capable of sustaining hydrostatic pressures in the range, 0.1-100 MPa (1-1,000 atm). Principal observations were (a) the lifetimes of discrete conductance states were lengthened with increasing pressure, (b) both the onset and decay of alamethicin conductance accompanying application and removal of supra-threshold voltage pulses were slowed with increasing pressure, (c) the onset of alamethicin conductance at elevated pressure became distinctly sigmoidal, suggesting an electrically silent intermediate state of channel assembly, (d) the magnitudes of the discrete conductance levels observed did not change with pressure, and, (e) the voltage threshold for the onset of alamethicin conductance was not altered by pressure. Apparent activation volumes for both the formation and decay of conducting states were positive and of comparable magnitude, namely, approximately 100 A3/event. Observation d indicates that channel geometry and the kinetics of ion transport through open channels were not affected by pressure in the range employed. The remaining observations indicate that, while the relative positions of free-energy minima characterizing individual conducting states at a given voltage were not modified by pressure, the heights of intervening potential maxima were increased by its application.     

The structure of melittin in lipid bilayer membranes.

0.15 M inorganic phosphate dramatically increased the alpha-helix content of melittin in aqueous solution. When melittin interacted with egg yolk phosphatidylcholine liposomes in the absence of inorganic phosphate, it was converted to an alpha-helix rich form, as postulated by Dawson et al. (Dawson, C.R., Drake, A.F. Helliwell, J. and Hider, R.C. (1978) Biochim. Biophys. Acta 510, 75--86).