Asymmetrical Lipid Bilayer Structure for Biological Membranes

IT is generally accepted that the matrix of cellular membranes is a bimolecular leaflet of phospholipid molecules in which the phospholipids are oriented so that their polar heads reside on the outer surfaces of the bilayer, in contact with the aqueous environment, the interior of the sandwich being composed of hydrophobic lipid chains^1–5. To this basic structure proteins cholesterol, glycolipids and other molecules are usually inserted in such a way as to confer on the bilayer the functional properties appropriate for the particular membrane.     

Chloride Transport in Porous Lipid Bilayer Membranes

This paper describes dissipative Cl_- transport in "porous" lipid bilayer membranes, i.e., cholesterol-containing membranes exposed to 1–3 x 10^-7 M amphotericin B. P_DCl (cm·s^-1), the diffusional permeability coefficient for Cl^-, estimated from unidirectional ³⁶Cl^- fluxes at zero volume flow, varied linearly with the membrane conductance (Gm, Ω^-1·cm^-2) when the contributions of unstirred layers to the resistance to tracer diffusion were relatively small with respect to the membranes; in 0.05 M NaCl, P_DCl was 1.36 x 10^-4 cm·s^-1 when Gm was 0.02 Ω^-1·cm^-2. Net chloride fluxes were measured either in the presence of imposed concentration gradients or electrical potential differences. Under both sets of conditions: the values of P_DCl computed from zero volume flow experiments described net chloride fluxes; the net chloride fluxes accounted for ~90–95% of the membrane current density; and, the chloride flux ratio conformed to the Ussing independence relationship. Thus, it is likely that Cl^- traversed aqueous pores in these anion-permselective membranes via a simple diffusion process. The zero current membrane potentials measured when the aqueous phases contained asymmetrical NaCl solutions could be expressed in terms of the Goldman-Hodgkin-Katz constant field equation, assuming that the P_DNa/P_DCl ratio was 0.05. In symmetrical salt solutions, the current-voltage properties of these membranes were linear; in asymmetrical NaCl solutions, the membranes exhibited electrical rectification consistent with constant-field theory. It seems likely that the space charge density in these porous membranes is sufficiently low that the potential gradient within the membranes is approximately linear; and, that the pores are not electrically neutral, presumably because the Debye length within the membrane phase approximates the membrane thickness.     

Permeability of Lipid Bilayer Membranes to Organic Solutes

A sensitive fluorescence technique was used to measure transport of organic solutes through lipid bilayer membranes and to relate permeability to the functional groups of the solute, lipid composition of the membrane, and pH of the medium. Indole derivatives having ethanol, acetate, or ethylamine in the 3-position, representing neutral, acidic, and basic solutes, respectively, were the primary models. The results show: (a) Neutral solute permeability is not greatly affected by changes in lipid composition but presence or absence of cholesterol in the membranes could greatly alter permeability of the dissociable substrates. (b) Indole acetate permeability was reduced by introduction of phosphatidylserine into membranes to produce a net negative charge on the membranes. (c) Permeability response of dissociable solutes to variation in pH was in the direction predicted but not always of the magnitude expected from changes in the calculated concentrations of the undissociated solute in the bulk aqueous phase. Concentration gradients of amines across the membranes caused substantial diffusion potentials, suggesting that some transport of the cationic form of the amine may occur. It is suggested that factors such as interfacial charge and hydration structure, interfacial polar forces, and lipid organization and viscosity, in addition to the expected solubility-diffusion relations, may influence solute flux.     

Association of Model Neurotransmitters with Lipid Bilayer Membranes

Aimed at reproducing the results of electrophysiological studies of synaptic signal transduction, conventional models of neurotransmission are based on the specific binding of neurotransmitters to ligand-gated receptor ion channels. However, the complex kinetic behavior observed in synaptic transmission cannot be reproduced in a standard kinetic model without the ad hoc postulation of additional conformational channel states. On the other hand, if one invokes unspecific neurotransmitter adsorption to the bilayer—a process not considered in the established models—the electrophysiological data can be rationalized with only the standard set of three conformational receptor states that also depend on this indirect coupling of neurotransmitters via their membrane interaction. Experimental verification has been difficult because binding affinities of neurotransmitters to the lipid bilayer are low. We quantify this interaction with surface plasmon resonance to measure equilibrium dissociation constants in neurotransmitter membrane association. Neutron reflection measurements on artificial membranes, so-called sparsely tethered bilayer lipid membranes, reveal the structural aspects of neurotransmitters’ association with zwitterionic and anionic bilayers. We thus establish that serotonin interacts nonspecifically with the membrane at physiologically relevant concentrations, whereas γ-aminobutyric acid does not. Surface plasmon resonance shows that serotonin adsorbs with millimolar affinity, and neutron reflectometry shows that it penetrates the membrane deeply, whereas γ-aminobutyric is excluded from the bilayer.     

Transmembrane Lipid Migration in Planar Asymmetric Bilayer Membranes

Planar asymmetric bilayer membranes, formed by apposing a monolayer of the neutral lipid glyceroldioleate (GDO) with one of the negatively charged lipid oleyl acid phosphate (OAP), were used to measure the rate of transmembrane OAP migration. The assay for this lipid flip-flop was the interaction of Ca²⁺ ions with negatively charged lipids which causes membranes to break: when Ca²⁺ is added to the compartment limited initially by the neutral lipid, flip-flop of the charged lipid eventually results in membrane breakdown. At 22 ± 2°C, in the absence of an externally applied electric field, an upper limit to the half time of OAP flip-flop was measured as 18.7 h, with a tentative lower limit of 14.4 h.     

Analysis of the Torus Surrounding Planar Lipid Bilayer Membranes

The characteristics and behavior of the torus (annulus) surrounding planar lipid bilayer membranes formed across a cylindrical aperture are analyzed using equations for the shape and volume of the annulus derived by the methods of variational calculus. The analysis leads to the following results: (a) Design criteria for the aperture can be established. (b) The transition region between thin film and thick annulus can be defined quantitatively and its effect on the measurement of specific capacitance determined. (c) At fixed annulus volume the diameter of the thin membrane is a function of the thin film-annulus contact angle. This suggests a new method for examining changes in free energy of the thin film, and explains why the area of thin film increases reversibly when potentials are present across the film. (d) In the absence of buoyant forces, the equations for the shape and volume of the annulus consist of incomplete elliptic integrals of the first and second kinds; however, the shape of the annulus in the transition region can be described with good accuracy by an approximate equation of greater simplicity.     

Interaction of Horse Heart Cytochrome c with Lipid Bilayer Membranes: Effects on Redox Potentials

Cyclic voltammetry has been used to study the effects of interactions between horse cytochrome c and solid-supported planar lipid membranes, comprised of either egg phosphatidylcholine (PC) or PC plus 20 mol.% cardiolipin (CL), on the redox potential and the electrochemical electron transfer rate between the protein and a semiconductor electrode. Experiments were performed over a wide range of cytochrome c concentrations (0–440 M) at low (20 mM) and medium (160 mM) ionic strengths. Three types of electrochemical behavior were observed, which varied as a function of the experimental conditions. At very low cytochrome c concentration (0.1 M), and under conditions where electrostatic forces dominated the protein–lipid membrane interaction (i.e., low ionic strength with membranes containing CL), a redox potential (265 mV) and an electrochemical electron transfer rate constant (0.09s ^–1)were obtained which compare well with those measured in other laboratories using a variety of different chemical modifications of the working electrode. Two other electrochemical signals (not reported with chemically modified electrodes) were also observed to occur at higher cytochrome c concentrations with this membrane system, as well as with two other systems (membranes containing CL under medium ionic strength conditions, and PC only at low ionic strength). These involved positive shifts of the cytochrome c redox potential (by 40 and 60 mV) and large decreases in the electron transfer rate (to 0.03 and 0.003 s^–1). The observations can be rationalized in terms of a structural model of the cytochrome c–membrane interaction, in which association involves both electrostatic and hydrophobic forces and results in varying degrees of insertion of the protein into the hydrophobic interior of the membrane.     

Oligomeric Structure of Colicin Ia Channel in Lipid Bilayer Membranes

Colicin Ia is a soluble, harpoon-shaped bacteriocin which translocates across the periplasmic space of sensitive Escherichia coli cell by parasitizing an outer membrane receptor and forms voltage-gated ion channels in the inner membrane. This process leads to cell death, which has been thought to be caused by a single colicin Ia molecule. To directly visualize the three-dimensional structure of the channel, we generated two-dimensional crystals of colicin Ia inserted in lipid-bilayer membranes and determined a ∼17 three-dimensional model by electron crystallography. Supported by velocity sedimentation, chemical cross-linking and single-particle image analysis, the three-dimensional structure is a crown-shaped oligomer enclosing a ∼35 Å-wide extrabilayer vestibule. Our study suggests that lipid insertion instigates a global conformational change in colicin Ia and that more than one molecule participates in the channel architecture with the vestibule, possibly facilitating the known large scale peptide translocation upon channel opening.Colicin Ia is a pore-forming water-soluble bacterial toxin produced by some strains of Escherichia coli to kill other competing bacteria (1, 2). It belongs to a functionally and structurally similar group of proteins that also includes colicins A (3), E1 (4), and N (5). Each of these proteins consist of three domains with distinct properties; the receptor domain (R), which binds a specific outer membrane receptor on the target cell, and the translocation domain (T) at the N terminus, responsible for traversing the outer membrane and the periplasmic space to deliver the channel-forming domain (C) at the C terminus to the bacterial inner membrane. The bundle of 10 α-helices that compose the C domain changes its conformation to form a voltage-gated ion channel in the plasma membrane. Opening of the channel produces an efflux of ions that depletes the cellular energy resources and ultimately leads to cell death.The x-ray structure of full-length, soluble colicin Ia (69 kDa) has been determined (6). The monomeric molecule is mostly α-helical, with the R domain separated from the T and C domains by a pair of unusually long (∼160 Å) α-helices thought possibly to span the periplasmic space during channel formation (6). The C domain is characterized by two hydrophobic helices (VIII and IX; residues Ala-580—Ile-612) that is surrounded by the remaining eight largely amphipathic α-helices. The same structural motif for the C domain is conserved in other members of the colicin family and is also present in the channel-forming domains of diphtheria toxin, exotoxin A, and the Bcl family of pro- and anti-apoptotic proteins (7). This pair of helices, termed the hydrophobic hairpin, is instrumental in driving the initial membrane insertion event (8) that is followed by a series of large scale pH and voltage-dependent conformational changes in the C domain, resulting in the opening of the ion channel in the plasma membrane (9, 10). In the absence of a high resolution membrane-inserted structure of a channel-forming colicin, solid-state NMR (11, 12), streptavidin binding (8) and cross-linking of site-directed cysteine mutants (9) have suggested that the initial membrane-bound intermediate exists as a two-dimensional helical array of the eight amphipathic helices (I-VII and X) spread across the membrane surface, with the hydrophobic helices (VIII and IX) embedded in the bilayer. A recent electron paramagnetic resonance study using preparations of spin-labeled ColA proteoliposomes has supported a similar umbrella model where the eight amphipathic helices reside at the air-water interface for the closed-channel state (13). Biotin-labeled cysteine mutants have also been used to determine how much of the C domain (aside from the hydrophobic hairpin) crosses the plasma membrane (14, 15) for colicin Ia. A large region of the amphipathic sequence (helices II-V; residues Leu-474—Tyr-541) has been found to cross from the cis to the trans side of the membrane in planar lipid bilayer experiments, resulting in a four-transmembrane segment molecule that is thought to form the ion channel.Because the 12–13 residue α-helices of the C domain are well short of the ∼20 residues required to span the plasma membrane, it has been proposed that conformational changes causing helix extension take place during the channel formation process. ¹³C spin diffusion NMR has indicated that whereas the overall secondary structure of the C domain is preserved, most of the helices undergo “opening,” and modulation of the tertiary structure allows for the required extension of the helices to cross the plasma membrane and form the channel (16). The internal structure of the colicin Ia channel has been investigated by examining the effect of different nonelectrolyte molecules on the single-channel conductance in planar lipid bilayer membranes (17). It was determined that the diameter at the cis entrance (equivalent to the outside of the cell) is 18 Å, and the diameter at the trans entrance (inside the membrane) is 10 Å, with a 7 Å diameter constriction located in close proximity to the trans entrance of the channel. More recent studies (18) employing the substituted cysteine accessibility method to determine what residues line the open colicin Ia channel suggest an hourglass-shaped pore with the most constricted part near the cis rather than the trans side, as opposed to the conclusion of Krasilnikov et al. (17). Both studies point to a pore constriction inside the membrane, and as pointed out by Kienker et al. 18), there exist plausible explanations to reconcile some of the differing results. The large diameter of the colicin Ia channel coupled with the studies which indicate that each colicin Ia molecule contributes four transmembrane segments in the membrane integrated state (14) suggests that the ion channel is formed by a multimer of colicin Ia molecules. However, all of the past studies directed at determining the oligomeric state of any of the colicin channels indicate a monomeric structure. The question as to how a four-transmembrane monomeric protein can form an ion channel of sufficient diameter to allow the passage of ions as large as tetraethyl ammonium (19) has remained unanswered.In this work we have subjected colicin Ia incorporated into lipid bilayer membranes to structural and biochemical investigations. We show, based on cross-linking and velocity sedimentation experiments, single-particle analysis of electron micrographs and results from electron crystallographic analysis of two-dimensional crystals of colicin Ia that the protein forms oligomers upon insertion into the bilayer. The suggested architecture of this oligomer based on the ∼17 Å resolution three-dimensional model and the biological implications, are discussed.     

Nonlinear Electrical Effects in Lipid Bilayer Membranes: III. The Dissociation Field Effect

In the course of an analysis of nonlinear electrical effects in lipid bilayer membranes, the influence of the dissociation field (or Wien) effect on the membrane conductivity is investigated. It is shown that the theory of Onsager for the Wien effect in a macroscopic phase can be applied to a thin membrane when the proper boundary conditions at the membrane-solution interface are introduced. It is assumed that an activation energy is associated with the passage of the ion across the interface. The mathematical treatment of the model is restricted to the case for which cations and anions have identical properties except for the charge sign. The resulting differential equations for the ion concentration within the membrane are integrated numerically. The analysis shows that the influence of the Wien effect on the membrane conductivity is appreciable only if the energy barrier at the interface is sufficiently high, i.e. if the rate limiting step for the ion transport is the passage of the ion across the interface.     

Platinum-supported Bilayer Lipid Membranes modified by ferrocene and its derivatives

The biferrocene-containing Schiff base complexes (1) and (2) were synthesized and characterized by elemental analyses and spectral data. The Pt-supported Bilayer Lipid Membranes (BLMs) modified by ferrocene and its derivatives were studied by cyclic voltametry (CV) and the electrochemical properties of this system are reported. The oxidation mechanism of electrocatalysis of ascorbic acid on the Pt-supported BLMs is discussed.     

Coupling of Solute and Solvent Flows in Porous Lipid Bilayer Membranes

The present experiments were designed to evaluate coupling of water and nonelectrolyte flows in porous lipid bilayer membranes (i.e., in the presence of amphotericin B) in series with unstirred layers. Alterations in solute flux during osmosis, with respect to the flux in the absence of net water flow, could be related to two factors: first, changes in the diffusional component of solute flux referable to variations in solute concentrations at the membrane interfaces produced by osmotic flow through the unstirred layers; and second, coupling of solute and solvent flows within the membrane phase. Osmotic water flow in the same direction as solute flow increased substantially the net fluxes of glycerol and erythritol through the membranes, while osmotic flow in the opposite direction to glycerol flow reduced the net flux of that solute. The observed effects of osmotic water flow on the fluxes of these solutes were in reasonable agreement with predictions based on a model for coupling of solute and solvent flows within the membrane phase, and considerably in excess of the prediction for a diffusion process alone.     

Kinetic Analysis of Permeation of Mitochondria-Targeted Antioxidants Across Bilayer Lipid Membranes

Mitochondria-targeted antioxidants consisting of a quinone part conjugated with a lipophilic cation via a hydrocarbon linker were previously shown to prevent oxidative damage to mitochondria in vitro and in vivo. In the present work, we studied the permeation of a series of compounds of this type across a planar bilayer phospholipid membrane. For this purpose, relaxation of the electrical current after a voltage jump was measured. With respect to the characteristic time of the relaxation process reflecting the permeation rate, hydrophobic cations can be ranked in the following series: 10(plastoquinonyl) decylrhodamine 19 (SkQR1) > 10-(6'-plastoquinonyl) decyltriphenylphosphonium (SkQ1) > 10-(6'-methylplastoquinonyl) decyltriphenylphosphonium (SkQ3) > 10-(6'-ubiquinonyl) decyltriphenylphosphonium (MitoQ). Thus, the permeation rate increased with (1) an increase in the size of the hydrophobic cation and (2) an increase in hydrophobicity of the quinone moiety. SkQ1 containing plastoquinone was shown to be more permeable through the membrane compared to MitoQ containing ubiquinone, which might be the reason for more pronounced beneficial action of SkQ1 in vitro and in vivo. The above approach can be recommended for the search for new antioxidants or other compounds targeted to mitochondria.     

Measurement of Dipole Potential in Bilayer Lipid Membranes by Dielectric Spectroscopy

Planar bilayer lipid membranes formed from egg phosphatidylcholine in aqueous media containing the lipophilic anion, dipicrylamine (DPA), were studied by dielectric spectroscopy over a frequency range of 10 Hz–10 MHz. The membranes showed dielectric relaxation due to the translocation of DPA between the membrane interfaces. Incorporating either cholesterol or 6-ketocholestanol into the membranes increased the characteristic frequency of the relaxation, which is proportional to the translocation rate constant of DPA. The results suggested that the sterol dipoles induced positive potential changes within the membrane interior. The changes of the dipole potential were 70 mV for cholesterol and 150 mV for 6-ketocholestanol when the sterol mole fraction was 0.67. The opposite effect was caused by phloretin added to the aqueous media, and the maximum dipole potential change was ?90 mV at 100 μM.     

Controlling and Measuring Local Composition and Properties in Lipid Bilayer Membranes

Local composition, structure, morphology, and phase are interrelated in lipid bilayer membranes. This gives us the opportunity to control one or more of these properties by manipulating others. We investigate theserelationships with combinations of simultaneous two-color widefield fluorescence imaging, three-dimensional rendering of vesicle domains, andmanipulation of the vesicle morphology via optical trapping and micropipetteaspiration. We describe methods to modulate, to measure, and to probe thelocal structure of model membranes through control of membrane curvature inliposomes.     

Nonlinear Electrical Effects in Lipid Bilayer Membranes: II. Integration of the Generalized Nernst-Planck Equations

In this paper the ion transport across a thin lipid membrane is treated using a generalized form of the Nernst-Planck equations. An additional term is introduced into the flux equations to account for the image force acting on the ion. As the membrane thickness is of the same order of magnitude as the range of the image forces, the potential energy of the ion in the membrane is strongly dependent on position. The integration of the flux equations leads to a general expression for the integral membrane conductance lambda as a function of the voltage u. The ratio lambda(u)/lambda(0) (lambda(0) = membrane conductance in the limit u --> 0) depends on the dielectric constant and the thickness of the membrane, but is independent of the ionic radius. When the numerical values of the potential energy function, as calculated by the method of electrical images, are inserted into the expression for lambda(u)/lambda(0), a strongly non-linear current-voltage characteristic is obtained. The theoretical current-voltage curve agrees satisfactorily with the experimental data at a low ionic strength and at low voltages; at higher voltages the observed membrane conductance exceeds the predicted value.     

Chemical and Photochemical Modification of Colicin E1 and Gramicidin A in Bilayer Lipid Membranes

Chemical modification and photodynamic treatment of the colicin E1 channel-forming domain (P178) in vesicular and planar bilayer lipid membranes (BLMs) was used to elucidate the role of tryptophan residues in colicin E1 channel activity. Modification of colicin tryptophan residues by N-bromosuccinimide (NBS), as judged by the loss of tryptophan fluorescence, resulted in complete suppression of wild-type P178 channel activity in BLMs formed from fully saturated (diphytanoyl) phospholipids, both at the macroscopic-current and single-channel levels. The similar effect on both the tryptophan fluorescence and the electric current across BLM was observed also after NBS treatment of gramicidin channels. Of the single-tryptophan P178 mutants studied, W460 showed the highest sensitivity to NBS treatment, pointing to the importance of the water-exposed Trp460 in colicin channel activity. In line with previous work, the photodynamic treatment (illumination with visible light in the presence of a photosensitizer) led to suppression of P178 channel activity in diphytanoyl-phospholipid membranes concomitant with the damage to tryptophan residues detected here by a decrease in tryptophan fluorescence. The present work revealed novel effects: activation of P178 channels as a result of both NBS and photodynamic treatments was observed with BLMs formed from unsaturated (dioleoyl) phospholipids. These phenomena are ascribed to the effect of oxidative modification of double-bond-containing lipids on P178 channel formation. The pronounced stimulation of the colicin-mediated ionic current observed after both pretreatment with NBS and sensitized photomodification of the BLMs support the idea that distortion of membrane structure can facilitate channel formation.Abbreviations: AlP_cS₃, almininum trisulfophthalocyanine; BLM, bilayer lipid membrane; DOPC, dioleoylphosphatidylcholine; DOPG, dioleoylphosphatidyl-glycerol; DPhPG, diphytanoylphos-phatidylglycerol; DPhPg, diphytanoylphosphatidylcholine; gA, gramicidin A; NBS, N-bromosuccinimideThis revised version was published online in August 2005 with a corrected cover date.     

Lipid Bilayer Composition Can Influence the Orientation of Proteorhodopsin in Artificial Membranes

Artificial membrane systems allow researchers to study the structure and function of membrane proteins in a matrix that approximates their natural environment and to integrate these proteins in ex vivo devices such as electronic biosensors, thin-film protein arrays, or biofuel cells. Given that most membrane proteins have vectorial functions, both functional studies and applications require effective control over protein orientation within a lipid bilayer. In this work, we explored the role of the bilayer surface charge in determining transmembrane protein orientation and functionality during formation of proteoliposomes. We reconstituted a model vectorial ion pump, proteorhodopsin, in liposomes of opposite charges and varying charge densities and determined the resultant protein orientation. Antibody-binding assay and proteolysis of proteoliposomes showed physical evidence of preferential orientation, and functional assays verified the vectorial nature of ion transport in this system. Our results indicate that the manipulation of lipid composition can indeed control orientation of an asymmetrically charged membrane protein, proteorhodopsin, in liposomes.     

Lipid Bilayer Composition Can Influence the Orientation of Proteorhodopsin in Artificial Membranes

Artificial membrane systems allow researchers to study the structure and function of membrane proteins in a matrix that approximates their natural environment and to integrate these proteins in ex vivo devices such as electronic biosensors, thin-film protein arrays, or biofuel cells. Given that most membrane proteins have vectorial functions, both functional studies and applications require effective control over protein orientation within a lipid bilayer. In this work, we explored the role of the bilayer surface charge in determining transmembrane protein orientation and functionality during formation of proteoliposomes. We reconstituted a model vectorial ion pump, proteorhodopsin, in liposomes of opposite charges and varying charge densities and determined the resultant protein orientation. Antibody-binding assay and proteolysis of proteoliposomes showed physical evidence of preferential orientation, and functional assays verified the vectorial nature of ion transport in this system. Our results indicate that the manipulation of lipid composition can indeed control orientation of an asymmetrically charged membrane protein, proteorhodopsin, in liposomes.     

Chronopotentiometric Technique as a Method for Electrical Characterization of Bilayer Lipid Membranes

The basic electrical parameters of bilayer lipid membranes are capacitance and resistance. This article describes the application of chronopotentiometry to the research of lipid bilayers. Membranes were made from egg yolk phosphatidylcholine. The chronopotentiometric characteristic of the membranes depends on the current value. For low current values, no electroporation takes place and the voltage rises exponentially to a constant value. Based on these kinds of chronopotentiometric curves, a method of the membrane capacitance and the membrane resistance calculations are presented.