Effect of the dipole potential of a bilayer lipid membrane on gramicidin channel dissociation kinetics

A technique of measuring of the light-induced transients of the gramicidin-mediated electric current across a membrane in the presence of a photosensitizer has been applied for the study of the effect of agents modifying the dipole potential of a bilayer lipid membrane (phloretin, 6-ketocholestanol, and RH421) on the processes of the gramicidin channel dissociation and formation. It is shown that phloretin, known to lower the dipole potential, decelerates the flash-induced decrease in the current, whereas 6-ketocholestanol and RH421, known to raise the dipole potential, accelerate the current decrease. It is revealed that the addition of phloretin leads to a decrease in the dissociation rate constant, whereas addition of either 6-ketocholestanol or RH421 causes an increase in this constant. Single-channel data show that phloretin brings about an increase in the lifetime of the gramicidin channels, whereas RH421 produces a more complicated effect. It is conclude that the dipole potential affects the process of channel dissociation, presumably via the influence on the movement of the dipoles of gramicidin molecules through the layer of the dipole potential drop near the membrane-water interface.     

Vasculopathy and insulin resistance in the JCR:LA-cp rat

The fluorescent dye FM1-43 labels nerve terminals in an activity-dependent fashion and has been found increasingly useful in exploring the exo- and endocytosis of synaptic vesicles and other cells by fluorescence methods. The dye distributes between the aqueous phase and the lipid membrane but the physical-chemical parameters characterizing the adsorption/partition equilibrium have not yet been determined. Fluorescence spectroscopy alone is not sufficient for a detailed elucidation of the adsorption mechanism since the method can be applied only in a rather narrow low-concentration window. In addition to fluorescence spectroscopy, we have therefore employed high sensitivity isothermal titration calorimetry (ITC) and deuterium magnetic resonance (2H-NMR). ITC allows the measurement of the adsorption isotherm up to 100 microM dye concentration whereas 2H-NMR provides information on the location of the dye with respect to the plane of the membrane. Dye adsorption/partition isotherms were measured for neutral and negatively-charged phospholipid vesicles. A non-linear dependence between the extent of adsorption and the free dye concentration was observed. Though the adsorption was mainly driven by the insertion of the non-polar part of the dye into the hydrophobic membrane interior, the adsorption equilibrium was further modulated by an electrostatic attraction/repulsion interaction of the cationic dye (z=+2) with the membrane surface. The Gouy-Chapman theory was employed to separate electrostatic and hydrophobic effects. After correcting for electrostatic effects, the dye-membrane interaction could be described by a simple partition equilibrium (Xb=Kcdye) with a partition constant of 103-104 M-1, a partition enthalpy of DeltaH=-2.0 kcal/mol and a free energy of binding of DeltaG=-7.8 kcal/mol. The insertion of FM1-43 into lipid membranes at room temperature is thus an entropy-driven reaction following the classical hydrophobic effect. Deuterium nuclear magnetic resonance provided insight into the structural changes of the lipid bilayer induced by the insertion of FM1-43. The dye disturbed the packing of the fatty acyl chains and decreased the fatty acyl chain order. FM1-43 also induced a conformational change in the phosphocholine headgroup. The -P-N+ dipole was parallel to the membrane surface in the absence of dye and was rotated with its positive end towards the water phase upon dye insertion. The extent of rotation was, however, much smaller than that induced by other cationic molecules of similar charge, suggesting an alignment of FM1-43 such that the POPC phosphate group is sandwiched by the two quaternary FM1-43 ammonium groups. In such an arrangement the two cationic charges counteract each other in a rotation of the -P-N+ dipole.     

Transfer RNA mimicry in a new group of positive-strand RNA plant viruses, the furoviruses: differential aminoacylation between the RNA components of one genome

The effects of the organic calcium channel blocker verapamil and the beta-receptor blocker propranolol on dipole (phi(d)) and surface (phi(s)) potentials of bilayer lipid membranes were studied. The boundary potentials (phi(b)= phi(d) + phi(s)) of black lipid membranes, monitored by conductance measurements in the presence of nonactin and by capacitive current measurements were compared with phi(s) calculated from the electrophoretic mobility of lipid vesicles. It was shown that the increase of boundary potential, induced by the adsorption of the positively charged propranolol, was caused solely by an increase in surface potential. Although phi(s) also increases due to the adsorption of verapamil, phi(b) diminishes. A sharp decrease of the dipole potential was shown to be responsible for this effect. From Langmuir adsorption isotherm the dissociation constant Kd of verapamil was estimated. The uncharged form of verapamil (Kd=(0.061+/-0.01) mM at pH 10.5) has a tenfold higher affinity to a neutral bilayer membrane than the positively charged form. The alteration of membrane dipole potential due to verapamil adsorption may have important implications for both membrane translocation and partitioning of small or hydrophobic ions and charged groups of membrane proteins.     

The adsorption of phloretin to lipid monolayers and bilayers cannot be explained by langmuir adsorption isotherms alone

Phloretin and its analogs adsorb to the surfaces of lipid monolayers and bilayers and decrease the dipole potential. This reduces the conductance for anions and increases that for cations on artificial and biological membranes. The relationship between the change in the dipole potential and the aqueous concentration of phloretin has been explained previously by a Langmuir adsorption isotherm and a weak and therefore negligible contribution of the dipole-dipole interactions in the lipid surface. We demonstrate here that the Langmuir adsorption isotherm alone is not able to properly describe the effects of dipole molecule binding to lipid surfaces--we found significant deviations between experimental data and the fit with the Langmuir adsorption isotherm. We present here an alternative theoretical treatment that takes into account the strong interaction between membrane (monolayer) dipole field and the dipole moment of the adsorbed molecule. This treatment provides a much better fit of the experimental results derived from the measurements of surface potentials of lipid monolayers in the presence of phloretin. Similarly, the theory provides a much better fit of the phloretin-induced changes in the dipole potential of lipid bilayers, as assessed by the transport kinetics of the lipophilic ion dipicrylamine.     

The location of fluorescence probes with charged groups in model membranes

The location of commonly used charged fluorescent membrane probes in membranes was determined in order to: (1) investigate the relationship between the structure of hydrophobic molecules and their depth within membranes; and (2) aid interpretation of experiments in which these fluorescent probes are used to examine membrane structure. Membrane depth was calculated using parallax analysis, a method in which the quenching induced by lipids carrying a nitroxide group at different locations in the membrane is compared. Shallow locations were found for xanthene dyes (fluorescein, eosin, Texas Red and rhodamine) both in free form and when attached either to the headgroup of phospholipids or long hydrocarbon chains. The exact structure of the xanthene and the nature of its linkage to lipid had only a modest effect on membrane location, which ranged between 19 and 24 A from the center of the bilayer in a charged state. Thus, the location of these fluorophores largely reflects their intrinsic properties rather than the nature of the groups to which they are attached. Furthermore, cationic and anionic xanthene derivatives had similar depths, indicating the type of charge does not have a large effect on depth. Consistent with this conclusion, shallow locations were also found for other hydrocarbon chain-linked cationic (acridine orange and styrylpyridinium) and anionic (coumarin, anilinonaphthalenesulfonic acid (ANS), and toluidinylnaphthalenesulfonic acid (TNS)) charged probes. These all located at 16-18 A from the bilayer center. We conclude that both anionic and cationic molecules that are otherwise hydrophobic predominantly occupy shallow locations within the polar headgroup region of the bilayer no matter how hydrophobic the molecule to which they are linked. This depth is significantly shallower than that occupied by most previously studied uncharged polar molecules that locate near the membrane surface. Consistent with this conclusion, a 2-4 A deeper location was found for xanthene probes with no net charge. In other experiments, methods to avoid chemical reactions that can distort the measurement of depth by fluorescence quenching were developed.     

Molecular and physicochemical aspects of local anesthetic-membrane interaction

Local anesthesia is achieved by the binding of anesthetic molecules to the sodium channel, a membrane protein responsible for the transport of the extracellular sodium to the cytosol. Local anesthetics (LA) bind to the sodium channel inhibiting sodium transport and, as a consequence, the action potential responsible for the nervous impulse. Most LA are relatively hydrophobic ionizable amines that undergo partitioning into lipid. Both activity and toxicity correlate positively with LA hydrophobicity. Effects of LA on the structural and dynamical properties of the membrane lipid region may be responsible for some of the toxic effects caused by these molecules. The present review focuses on research done on the interaction between both the charged and uncharged forms of LA and lipid systems-bilayers and micelles. LA have been found to alter phospholipid gel to liquid crystal phase transition temperature (Tc), to affect bilayer permeability, to influence molecular packing, and to inhibit the bilayer to hexagonal phase transition. Anesthetics in micellized form disrupt bilayers giving rise to lipid-LA mixed micelle-like aggregates. The question of LA location in the bilayer is also addressed. Special emphasis is placed on work focusing on the quantitative analysis of drug binding, as well as on the effects of binding on physicochemical properties of the LA, such as extent of ionization (pK shifts) and rates of chemical reactions. The understanding of these phenomena has contributed to the development of less toxic liposomal formulations capable of prolonging the duration of anesthesia.     

Annexin V and vesicle membrane electroporation

The method of membrane electroporation (ME) has been used as an analytical tool to quantify the effect of membrane curvature on transient electric pore formation, and on the adsorption of the protein annexin V (M(r)= 35,800) to the outer surface of unilamellar lipid vesicles (of radii 25 < or = a/nm < or = 200). Relaxation kinetic studies using optical membrane probes of the diphenylhexatriene type suggest that electric pore formation is induced by ionic interfacial polarization causing entrance of the (more polarizable) water into the lipid bilayer membrane yielding (hydrophobic and hydrophilic) pore states with a mean stationary pore radius rp = 0.35 (+/-0.05) nm. Extent and rate of ME, compared at the same induced transmembrane voltage, were found to decrease both with increasing vesicle radius and with increasing protein concentration. This 'inhibitory' effect of annexin V is apparently allosteric and saturates at about [ANT]sat = 4 microM annexin V for vesicles of a = 100 nm at 1 mM total lipid concentration, 0.13 mM total Ca2+ concentration and at T = 293 K. Data analysis in terms of Gibbs area-difference-elasticity energy suggests that the bound annexin V reduces the gradient of the lateral pressure across the membrane. At [ANT]sat, about 20% of the vesicle surface is covered by the bound protein, but it is only 0.01% of the surface of the outer lipid leaflet in which a part of the protein, perhaps the aromatic residue of the tryptophan (W 187), is inserted. Insertion leads to a denser packing of the lipid molecules in the outer membrane leaflet. As a consequence, the radius of the electropores in the remaining membrane part, not covered by annexin V decreases (rp/nm = 0.37, 0.36 and 0.27) with increasing adsorption of the protein ([ANT] = 0, 2 and 4 microM, respectively).     

Adsorption of Negatively Charged Azo Dyes onto Surfactant-Modified Sepiolite

The adsorption of reactive dyes on sepiolite has been investigated in a series of batch adsorption experiments. Three reactive dyes (Everzol Black B, Everzol Red 3BS, Everzol Yellow 3RS H/C) were used in bottle adsorption studies. While no significant adsorption capacity was obtained for natural sepiolite, high-adsorptive capacities were observed upon using sepiolite modified with quaternary amines. The electrokinetic measurements along with calculations using the cross-sectional area reveal that the quaternary amines adsorb close to bilayer coverage. A mechanism involving electrostatic attraction of the anionic groups of dye molecules onto oppositely charged amine-modified sepiolite surface is proposed to be responsible for the uptake of dyes. The adsorption data were fitted to the Langmuir isotherm. It is found that the modified sepiolite yields adsorption capacities (qe) of 169, 120, and 108 mg/g for Yellow, Black, and Red, respectively. These results are comparable to the adsorption capacity of the same dyes onto activated carbon.     

The effect of undecaprenol on bilayer lipid membranes

The influence of undecaprenol on phosphatidylcholine macrovesicular bilayer lipid membranes has been studied by electrophysiological techniques. The current-voltage characteristics, ionic transference numbers, the membrane conductance-temperature relationships and the membrane breakdown voltage were measured. The permeability coefficients for Na+ and Cl- ions, the activation energy of ion migration across the membrane, the membrane hydrophobic thickness and the membrane Young's modulus were determined. Undecaprenol increases membrane conductance, membrane capacitance, membrane ionic permeability and membrane elastic deformability, decreases the activation energy, membrane hydrophobic thickness and membrane electromechanical stability, and does not change membrane selectivity. The formation by undecaprenyl molecules of fluid microdomains modulating membrane hydrophobic thickness is postulated. The data suggest that the behaviour of undecaprenol in membranes is regulated by transmembrane electrical potential.     

Structure of the membrane-bound form of the pore-forming domain of colicin A: a partial proteolysis and mass spectrometry study

The ion-channel-forming thermolytic fragment (thA) of colicin A binds to negatively charged vesicles and provides an example of the insertion of a soluble protein into a lipid bilayer. The soluble structure is known and consists of a 10-helix bundle containing a hydrophobic helical hairpin. In this study, partial proteolysis and mass spectrometry were used to determine the accessible sites to proteolytic attack by trypsin and alpha-chymotrypsin in the thA fragment in its membrane-bound state. Electrospray mass spectrometry was quite an efficient method for the identification of the cleavage products, even with partially purified peptide mixtures and with only few controls by N-terminal sequencing. This work confirms that a major part of the peptide chain lies at the membrane surface and that even the hydrophobic hairpin is not protected by the lipid bilayer from proteolytic degradation. In the absence of a membrane potential, the hydrophobic hairpin in the colicin A membrane-bound form seems not fixed in a transmembrane orientation.     

Transport kinetics of hydrophobic ions in lipid bilayer membranes. Charge-pulse relaxation studies

A modified version of the charge-pulse relaxation technique with improved time resolution was applied to the study of transport kinetics of hydrophobic ions (tetraphenylborate, dipicrylamine) through lipid bilayer membranes. Besides a better time resolution the charge-pulse method has the additional advantage that the perturbation of the membrane can be kept small (voltage amplitudes between 1 and 10 mV). The results of the analysis support the model proposed earlier, according to which the overall transport takes place in three consecutive steps, adsorption of the ion from water to the interface, translocation to the opposite interface, and desorption into the aqueous phase. The translocation rate constant ki and the partition coefficient gamma of the hydrophobic ion between water and the membrane were measured for lecithins with different mono-unsaturated fatty acid residues. Increasing the chain length of the fatty acid from C16 to C24 resulted in a decrease of ki by a factor of about 9 in the case of tetraphenylborate and by a factor of about 17 in the case of dipicrylamine.     

Adsorption of haematoporphyrins on the planar bilayer membrane

Adsorption of haematoporphyrin derivatives with different hydrophobicities of peripheral groups on a planar bilayer lipid membrane (BLM) was studied in the dark and upon illumination by the visible light. Haematoporphyrin molecules were shown to adsorb on the BLM as anions. The adsorption changed the boundary potential at the membrane/water interface, in particular, it altered the potential in the diffuse part of the double layer outside the membrane and increased an additional unscreenable potential drop inside it. Illumination decreased the value of the negative potential drop due probably to the appearance of a positive charge in the haematoporphyrin macrocycle. The adsorption of haematoporphyrins affected the BLM conductivity induced by different ionophores, which can be explained by changes in membrane structure. Haematoporphyrin derivatives with higher hydrophobicities adsorbed deeper inside the membrane, caused greater changes in its structure and displayed a stronger photodynamic effect.     

Mechanism of alamethicin insertion into lipid bilayers

Alamethicin adsorbs on the membrane surface at low peptide concentrations. However, above a critical peptide-to-lipid ratio (P/L), a fraction of the peptide molecules insert in the membrane. This critical ratio is lipid dependent. For diphytanoyl phosphatidylcholine it is about 1/40. At even higher concentrations P/L > or = 1/15, all of the alamethicin inserts into the membrane and forms well-defined pores as detected by neutron in-plane scattering. A previous x-ray diffraction measurement showed that alamethicin adsorbed on the surface has the effect of thinning the bilayer in proportion to the peptide concentration. A theoretical study showed that the energy cost of membrane thinning can indeed lead to peptide insertion. This paper extends the previous studies to the high-concentration region P/L > 1/40. X-ray diffraction shows that the bilayer thickness increases with the peptide concentration for P/L > 1/23 as the insertion approaches 100%. The thickness change with the percentage of insertion is consistent with the assumption that the hydrocarbon region of the bilayer matches the hydrophobic region of the inserted peptide. The elastic energy of a lipid bilayer including both adsorption and insertion of peptide is discussed. The Gibbs free energy is calculated as a function of P/L and the percentage of insertion phi in a simplified one-dimensional model. The model exhibits an insertion phase transition in qualitative agreement with the data. We conclude that the membrane deformation energy is the major driving force for the alamethicin insertion transition.     

Effect of nitroglycerin and nicorandil on regional poststenotic quantitative coronary blood flow in coronary artery disease: a combined digital quantitative angiographic and intracoronary doppler study

The biophysical activity of lung surfactant depends, to a large extent, on the presence of the hydrophobic surfactant proteins B (SP-B) and C (SP-C). The role of these proteins in lipid adsorption and lipid squeeze-out under dynamic conditions simulating breathing is not yet clear. Therefore, the aim of this study was to investigate the interaction of spread hydrophobic surfactant proteins with phospholipids in a captive-bubble surfactometer during rapid cyclic area changes (6 cycles/min). We found that SP-B and SP-C facilitated the rapid transport of lipids into the air-water interface in a concentration-dependent manner (threshold concentration > or = 0.05:0.5 mol% SP-B/SP-C). Successive rapid cyclic area changes did not affect the concentration-dependent lipid adsorption process, suggesting that SP-B and SP-C remained associated with the surface film.     

Intramembrane molecular dipoles affect the membrane insertion and folding of a model amphiphilic peptide

The relationship between the dipole potential and the interaction of the mitochondrial amphipathic signal sequence known as p25 with model membranes has been studied using 1-(3-sulfonatopropyl)-4-[beta[2-(di-n-octyl-amino)-6-naphthyl]viny l] pyridinium betaine (di-8-ANEPPS) as a fluorescent probe. The dipole potential of phosphatidylcholine membranes was modified by incorporating into the bilayer the sterols phloretin and 6-ketocholestanol (KC), which decrease and increase the dipole potential, respectively. The results derived from the application of a dual-wavelength ratiometric fluorescence method for following the variation of the membrane dipole potential have shown that when p25 inserts into the lipidic bilayer, a decrease in the dipole potential takes place. The magnitude of this decrease depends on the initial value of the dipole potential, i.e., before interaction with the peptide. Thus, when KC was incorporated into the bilayer, the decrease caused by the membrane insertion of p25 was larger than that caused in PC membranes. Alternatively, in the presence of phloretin, the decrease in the potential caused by the peptide insertion was smaller. Complementary studies involving attenuated total reflectance-Fourier transform infrared spectroscopy of the peptide membrane interactions have shown that modification of the dipole potential affects the conformation of the peptide during the course of its interaction with the membrane. The presence of KC induces a higher amount of helicoidal structure. The presence of phloretin, however, does not appear to affect the secondary structure of the peptide. The differences observed in the dipole potential decreases caused by the presence of the peptide with the PC membranes and phloretin-PC membranes, therefore, must involve differences in the tertiary and, perhaps, quaternary conformations of p25.     

The formation and annealing of structural defects in lipid bilayer vesicles

It is shown that sonication of phospholipid-water dispersions below the crystalline leads to liquid crystalline phase transition temperature (Tc) produces bilayer vesicles with structural defects within the bilayer membrane, which permit rapid permeation of ions and catalyze vesicle-vesicle fusion. These structural defects are annihilated simply by annealing the vesicle suspension above Tc. The rate of annealing was found to be slow, of the order of an hour for T = 3 degrees C above Tc, but annealing is complete within 10 min for T = 10 degrees C above Tc. It is proposed that these structural defects are fault-dislocations in the bilayer structure, which arise from a population defect in the distribution of the lipid molecules between the outer and inner monolayers, when small bilayer fragments reassemble to form the small bilayer vesicles during the sonication procedure. Such a population defect can only be remedied by lipid transport via the inside in equilibrium outside flip-flop mechanism, which would account for the slow kinetics of annealing observed even at 3 degrees C above the phase transition.     

De novo design, synthesis, and characterization of a pore-forming small globular protein and its insertion into lipid bilayers

The question of how to design a water-soluble globular protein remains. We report here the synthesis of a native-like and pore-forming small globular protein (SGP, 69 amino acid residues). The protein was designed to have four helices: a Trp-containing short hydrophobic helix in the middle surrounded by three Tyr-containing long basic amphiphilic helices. Size-exclusion chromatography and CD measurements indicated that in buffer solution SGP is monomeric with a 50% helical structure. SGP did not completely denature even at high temperature (90 degrees C) and at relatively high Gu x HCl concentration so that the denaturant concentration at the midpoint of the transition is 5 M. Dye binding studies and fluorescence energy transfer experiments showed that SGP possesses a hydrophobic binding site and its Trp of the central helix is present at a relatively hydrophobic region and accepts the energy from Tyr(s) in other amphiphilic helices, indicating that SGP takes a stable globular-like structure in aqueous solution. From the depth-dependent fluorescent studies using egg PC liposomes containing n-doxyl fatty acids and brominated phospholipid as quenchers, it was found that the hydrophobic central alpha-helix is able to enter spontaneously into the lipid bilayers and the Trp in the central alpha-helix is located at about the middle of the alkyl chain in the outer layer of the phospholipid bilayer. The peptide is also able to increase the membrane permeability with two modes of current (basal current and single ion channel) in planar phospholipid bilayers, indicating the spontaneous insertion of the protein into the lipid bilayer (basal current) and then the formation of a uniform size of channel pore (14 pS). SGP is useful as a basic and starting model to find good amino acid sequences that fold to a desired protein structure and to search translocation mechanisms from aqueous solution into lipid bilayers.     

Molecular dynamics simulation of melittin in a dimyristoylphosphatidylcholine bilayer membrane

Molecular dynamics trajectories of melittin in an explicit dimyristoyl phosphatidylcholine (DMPC) bilayer are generated to study the details of lipid-protein interactions at the microscopic level. Melittin, a small amphipathic peptide found in bee venom, is known to have a pronounced effect on the lysis of membranes. The peptide is initially set parallel to the membrane-solution interfacial region in an alpha-helical conformation with unprotonated N-terminus. Solid-state nuclear magnetic resonance (NMR) and polarized attenuated total internal reflectance Fourier transform infrared (PATIR-FTIR) properties of melittin are calculated from the trajectory to characterize the orientation of the peptide relative to the bilayer. The residue Lys7 located in the hydrophobic moiety of the helix and residues Lys23, Arg24, Gln25, and Gln26 at the C-terminus hydrophilic form hydrogen bonds with water molecules and with the ester carbonyl groups of the lipids, suggesting their important contribution to the stability of the helix in the bilayer. Lipid acyl chains are closely packed around melittin, contributing to the stable association with the membrane. Calculated density profiles and order parameters of the lipid acyl chains averaged over the molecular dynamics trajectory indicate that melittin has effects on both layers of the membrane. The presence of melittin in the upper layer causes a local thinning of the bilayer that favors the penetration of water through the lower layer. The energetic factors involved in the association of melittin at the membrane surface are characterized using an implicit mean-field model in which the membrane and the surrounding solvent are represented as structureless continuum dielectric material. The results obtained by solving the Poisson-Bolztmann equation numerically are in qualitative agreement with the detailed dynamics. The influence of the protonation state of the N-terminus of melittin is examined. After 600 ps, the N-terminus of melittin is protonated and the trajectory is continued for 400 ps, which leads to an important penetration of water molecules into the bilayer. These observations provide insights into how melittin interacts with membranes and the mechanism by which it enhances their lysis.     

Fatty acid transport: difficult or easy?

Transport of unesterified fatty acids (FA) into cells has been viewed either as a simple diffusion process regulated mainly by lipid physical chemistry or as a more complex process involving protein catalysis. In this review FA transport in cell membranes is broken down into three essential steps: adsorption, transmembrane movement, and desorption. The physical properties of FA in aqueous, membrane, and protein environments relevant to transport mechanisms are discussed, with emphasis on recent information derived from NMR and fluorescence studies. Because of their low solubility in water and high hydrophobicity, FA bind rapidly and avidly to model membranes (phospholipid bilayers); if albumin is a donor, FA desorb rapidly to reach their equilibrium distribution between the membrane and albumin. The ionization properties of FA in a phospholipid bilayer result in a high population of the un-ionized form (approximately 50%) at pH 7.4, which diffuses across the lipid bilayer (flip-flops) rapidly (t(1/2) < 1 sec). Desorption of FA from a phospholipid surface is slower than transmembrane movement and dependent on the FA chain length and unsaturation, but is rapid for typical dietary FA. These physical properties of FA in model systems predict that proteins are not essential for transport of FA through membranes. The only putative FA transport protein to be purified and reconstituted into phospholipid bilayers, the mitochondrial uncoupling protein (UCP1), was shown to transport the FA anion in response to FA flip-flop. New experiments with cells have found that FA movement into cells acidifies the cytosol, as predicted by the flip-flop model.     

Electric field-induced reorganization of two-component supported bilayer membranes

Application of electric fields tangent to the plane of a confined patch of fluid bilayer membrane can create lateral concentration gradients of the lipids. A thermodynamic model of this steady-state behavior is developed for binary systems and tested with experiments in supported lipid bilayers. The model uses Flory's approximation for the entropy of mixing and allows for effects arising when the components have different molecular areas. In the special case of equal area molecules the concentration gradient reduces to a Fermi-Dirac distribution. The theory is extended to include effects from charged molecules in the membrane. Calculations show that surface charge on the supporting substrate substantially screens electrostatic interactions within the membrane. It also is shown that concentration profiles can be affected by other intermolecular interactions such as clustering. Qualitative agreement with this prediction is provided by comparing phosphatidylserine- and cardiolipin-containing membranes.