Interactions between a membrane sialoglycoprotein and planar lipid bilayers

Summary Bilayer membranes formed from lipids dissolved in decane were exposed to glycophorin, a sialoglycoprotein which had been extracted from human red cell membranes. The interaction with the bilayer produced an increase in the steady state electrical conductance of the membrane proportional to the amount added. Fluctuations in membrane current when the electrical potential difference was constant were observed concommitantly with this increase in membrane conductance. The minimum size of the fluctuations corresponds to a conductance of 10^–10 mho. The increase in conductance as well as the current fluctuations persisted after extensive washout of the chamber containing the protein (cisside). Subsequent addition of lectins (wheat germ agglutinin and phytohemoagglutinin) to the cis-side produced rupture of the membranes, whilst these hemoagglutinins added to the trans-side failed to produce an effect. Measurements of changes in surface potential using K⁺ nonactin as a probe indicated that glycophorin induces a negative surface charge. At high protein concentrations, the magnitude of the induced surface potential became independent of glycophorin concentration. The maximum number of charges introduced onto the membrane under these conditions was 1.4×10⁵/m². Cis (but not trans)-side addition of neuraminidase abolished these charges, indicating that they can be ascribed to the sialic acid residues that the protein bears. These results suggest that glycophorin incorporates into bilayer membranes with its N-terminal end (where the sialic acid and carbohydrates are located) facing the cis-side. Spectrin reversibly lowered the glycophorin-induced membrane conductance when added to the trans-side. Cis-side additions failed to produce an effect. Trypsin present on the trans-side irreversibly lowered the membrane conductance. These results indicate that parts of the glycophorin molecule, probably the C-terminal end, are accessible to reagents in the solution bathing the trans-side of the membrane. Thus glycophorin spans the planar bilayer in much the same way as it spans the red cell membrane.     

Interactions of hexachlorocyclohexanes with lipid bilayers

Quenching of the fluorescence of a hydrophobic analogue of tryptophan incorporated into lipid bilayers has been used to measure partition coefficients for lindane and the α- and δ-isomers of hexachlorocyclohexane. Partition coefficients between water and lipid are comparable to those between water and octanol and exhibit a negative temperature coefficient. Binding to the lipid phase is limited by saturation of the aqueous phase rather than of the lipid phase. The binding of lindane has no detectable effect on membrane fluidity as measured by fluorescence polarisation of diphenylhexatriene, or on the permeability properties of the membrane, as measured by the leak of carboxyfluorescein.     

Fusion of liposomes with planar lipid bilayers

The fusion of liposomes with planar lipid bilayers was monitored by two different methods. (a) Liposomes consisting of phospholipids and cholesterol were added to the aqueous phase bathing the cholesterol-deficient planar lipid bilayers in the presence of nystatin. The resulting increase in the planar lipid bilayer's electrical conductance was considered indicative of fusion. (b) Transplanar lipid bilayer injection of ³⁵SO₄^2? trapped inside the liposomes.It is shown by both methods that fusion is specifically dependent on the presence of negatively charged phospholipids both in the liposomes and the planar lipid bilayers and on Ca²⁺ in the aqueous phase of the fusion system.     

Lipid-protein interaction. The incorporation of myelin proteolipid apoprotein into phosphatidylcholine bilayers

Bovine myelin proteolipid apoprotein (PLA), obtained in high yield and purity by a novel ultrafiltration procedure, has been used to study the perturbations produced by this protein on phosphatidylcholine bilayers, using infrared spectroscopy, nuclear magnetic resonance and fluorescence polarisation. PLA interacts with phospholipids in a similar manner to other intrinsic proteins. For bilayers in the fluid state, the fatty-acyl chain static order, as measured by deuterium NMR, is slightly increased in the presence of the protein, except at very high PLA concentrations. Phosphorus NMR reveals some perturbation of the phospholipid polar group by PLA, but to a smaller degree than occurs with other intrinsic proteins. An increase in static order above tc (the onset temperature for gel-to-fluid transition) is also detected by infrared spectroscopy. Studies using steady-state polarisation of diphenylhexatriene fluorescence indicate that the microviscosity of the bilayer increases as a function of the protein mole fraction. From these data an estimation of the average number of lipids perturbed per protein monomer has been made, and a figure of 37 phospholipid molecules determined. The data are compatible with a picture of a hydrophobic polypeptide, perturbing the phospholipids close to it, but allowing rapid (greater than 10(4) s-1) exchange with all the lipid molecules in the system.     

Conformation of brain proteolipid apoprotein

The conformation of brain proteolipid apoprotein (PLA) has been investigated using infrared spectroscopy and freeze-fracture electron microscopy. For this purpose, spectroscopic samples consisting of a mixture of liquid paraffin and wet protein have been prepared. These systems have allowed us to record the infrared spectra of PLA at neutral pH. The amide I and III regions reveal the existence of a predominantly -helical structure, as well as the presence of minor -strands and random coil forms. The effect of sonication and a non-denaturing detergent, (n-octyl--d-glucopyranoside), on the structure of the protein have also been investigated. Sonication produces an increase of the and unordered structures at the expense of the -helical conformation. These structural changes are enhanced in the presence of the non-ionic detergent n-octyl--d-glucopyranoside. Lipids protect the native protein structure from the effects of sonication. The aforementioned detergent changes the PLA conformation by increasing the -helical content at the expense of -sheet and random coil forms. Therefore the PLA structure seems to be similar to the structures of other proteins intrinsic to non-neural membranes. The effects investigated also suggest that PLA behaves in a conformationally flexible manner.     

Organization and dynamics of the proteolipid complexes formed by annexin V and lipids in planar supported lipid bilayers

The consequences of the binding of annexin V on its lateral mobility and that of lipids were investigated by means of experimental and simulated FRAP experiments. Experiments were carried out on planar supported bilayers (PC/PS 9:1 mol/mol mixtures) in the presence of 1 mM CaCl2 in the subphase. The probes C12-NBD-PS and fluorescein-labeled annexin V were used and the data compared with that previously obtained for C12-NBD-PC [Saurel, O., Cézanne, L., Milon, A., Tocanne, J. F., & Demange, P. (1998) Biochemistry 37, 1403-1410]. At complete coverage of the lipid bilayer by the protein (Cannexin = 80 nM), the lateral mobility of C12-NBD-PC was reduced by 40% while C12-NBD-PS and bound annexin V molecules were nearly immobilized (D < 10(-)11 cm2/s). At moderate protein concentration (20 nM < Cannexin < 80 nM), best fitting of the lipid and protein probe recoveries was achieved with one single diffusion coefficient and a mobile fraction close to 100%, indicating homogeneous lipid and protein populations. In contrast, at low protein concentration (Cannexin < 20 nM), C12-NBD-PS showed a two-component diffusion. The slow PS population at Cannexin < 20 nM and the single PS population at Cannexin > 20 nM moved at the same rate that bound annexin V (mobile fraction close to 100%), indicating strong PS/protein interactions. With the aid of computer simulations of the lateral motion of PC molecules, based on the 2-D crystalline networks formed by annexin V in contact with the lipid bilayer, these FRAP results may be accounted for by considering a rather simple model of a proteolipidic complex consisting of an extended 2-D crystalline protein network facing the lipid bilayer and stabilized by strong interactions between annexin V and PS molecules. In this model, immobilization of annexin V and PS molecules originates from their mutual interactions. The slowing down of PC molecules is due to various obstacles to their lateral diffusion which can be described as: the four PS molecules bound to the protein, the tryptophan 187 which presumably interacts with the lipids at the level of their polar headgroups and probably the three other hydrophobic amino acid residues located on the AB calcium-binding loops of the protein.     

Raman spectra of planar supported lipid bilayers

Raman scattering has been used to obtain high quality vibrational spectra of planar supported lipid bilayers (pslb's) at the silica/water interface without the use of resonance or surface enhancement. A total internal reflection geometry was used both to increase the bilayer signal and to suppress the water background. Polarization control permits the determination of four components of the Raman tensor, of which three are independent for a uniaxial film. Spectra are reported of the phospholipids DMPC, DPPC, and POPC, in the C-H stretching region and the fingerprint region. The temperature-dependent polarized spectra of POPC show only small changes over the range 14-41 degrees C. The corresponding spectra of DMPC and DPPC bilayers show large thermal changes consistent with a decreasing tilt angle from the surface normal and increasing chain ordering at lower temperatures. The thermal behavior of DMPC pslb's is similar to that of vesicles of the same lipid in bulk suspension. In contrast to calorimetry, which shows a sharp phase transition (L alpha-L beta') with decreasing temperature, the changes in the Raman spectra occur over a temperature range of ca. 10 degrees C commencing at the calorimetric phase transition temperature.     

Raman spectra of planar supported lipid bilayers

Raman scattering has been used to obtain high quality vibrational spectra of planar supported lipid bilayers (pslb's) at the silica/water interface without the use of resonance or surface enhancement. A total internal reflection geometry was used both to increase the bilayer signal and to suppress the water background. Polarization control permits the determination of four components of the Raman tensor, of which three are independent for a uniaxial film. Spectra are reported of the phospholipids DMPC, DPPC, and POPC, in the C-H stretching region and the fingerprint region. The temperature-dependent polarized spectra of POPC show only small changes over the range 14-41 °C. The corresponding spectra of DMPC and DPPC bilayers show large thermal changes consistent with a decreasing tilt angle from the surface normal and increasing chain ordering at lower temperatures. The thermal behavior of DMPC pslb's is similar to that of vesicles of the same lipid in bulk suspension. In contrast to calorimetry, which shows a sharp phase transition (L_α-L_β') with decreasing temperature, the changes in the Raman spectra occur over a temperature range of ca. 10 °C commencing at the calorimetric phase transition temperature.     

Colicin E1 in planar lipid bilayers

The channel formed by the C-terminal domain of colicin E1 in planar lipid bilayers has proven to be more complex than one might have guessed for such a simple system. The protein undergoes a pH-dependent rearrangement which transforms it from a water soluble form to a much different membrane bound form. There are at least two bound states which don't form a channel. The process by which the channel opens and closes is regulated by the pH and the transmembrane voltage. The voltage is probably sensed by at least 3 (and more likely 4 or more) lysine residues which must be driven through the field to open the channel. The process appears to be hindered by particular carboxyl groups when they are in the unprotonated state. The open channel has several substates and several superstates. Very large positive voltage catalyzes a transition of the open channel to an inactivated state, and may be able to drive the channel-forming region of the protein across the membrane. Little is known about the structure of any of these states, but the open channel is large enough to allow NAD to traverse the membrane and appears to be formed by one colicin molecule. This single polypeptide mimics many of the properties found in channels of mammalian cell membranes, but it may prove more relevant as a model for the transport of proteins across membranes. The comparative ease with which the protein can be manipulated chemically and genetically, along with the complexity of its behavior, promises to keep several laboratories busy for some time.     

NH2-terminal analysis of Wolfgram and Folch-Lees proteolipid proteins

Abstract— The NH₂-terminal amino acids of Wolfgram and Folch-Lees proteolipids of bovine and human CNS myelin were determined using the cyanate method (Starke & Smyth , 1963) followed by direct amino acid analysis of the products. Glycine predominated in every case and was recovered in amounts similar to the results described by Whikehart & Lees (1973), who used a dansylation technique followed by thin layer chromatography of the DNS-amino acids. In the present study substantial amounts of glutamic acid, serine, alanine and aspartic acid were also recovered, plus traces of other amino acids. Few differences were observed between Wolfgram and Folch-Lees proteolipids. The end group products of purified W1 proteolipid of bovine Wolfgram fraction, of diazometholysed Folch-Lees proteolipid, and of a sample of phosphatidyl serine had essentially the same composition. The similarity of these results, especially for both fractionated and unfractionated Wolfgram proteolipid, may be evidence that the observed products are derived from phosphoglycerides present in proteolipid rather than from the actual NH₂-terminals of the protein.     

Wave-guide spectroscopy on planar lipid bilayers doped with hydrophobic ions

Wave-guide spectroscopy exploits the light pipe properties of planar lipid bilayers by propagating a light wave along the plane of the bilayer. Applying this technique to the optical absorption of chromophore in the membrane, results in an enhanced sensitivity when compared to normal incidence spectroscopy. This gain factor is of the order of 100 per mm optical path along the bilayer, thus transforming the weak absorbances in lipid membranes into easily measurable quantities. Wave-guide spectroscopy has been used to measure the adsorption isotherm of hydrophobic dipicrylamine ions in a phosphatidylcholine membrane. The adsorption isotherm is linear for low aqueous concentrations, in the micromolar range however, it changes into a sublinear dependence. The addition of an inert alkali salt to the electrolyte favours the adsorption of hydrophobic ions. Current saturation is observed with the transition to the sublinear isotherm. When using the time constant for current relaxation as an indicator of changes in the magnitude of the surface potential, it does not seem to vary with the additional dipicrylamine which adsorbs in the presence of high concentrations of alkali salt in the electrolyte. A compensation of hydrophobic charge by the alkali ions from the inert electrolyte is proposed.     

Protein-mediated intermembrane contact facilitates fusion of lipid vesicles with planar bilayers

Fusion of phospholipid vesicles with planar bilayer membranes occurs provided there is an intermembrane contact, which can be mediated by phospholipid-binding proteins, even in the absence of calcium. The firm attachment phase is then followed by the osmotically-driven fusion. These results show that hydrophobic proteins (not necessarily Ca²⁺-binding proteins) may enhance fusion by promoting contact of membranes. Such proteins may operate synergistically with Ca²⁺ to reduce the threshold concentration of Ca²⁺ needed for fusion of biological membranes. Protein-mediated intermembrane contact resulting in fusion may play a crucial role in the regulation and catalysis of biological fusion events.     

Toad bladder amiloride-sensitive channels reconstituted into planar lipid bilayers

In the present study we used established methods to obtain apical membrane vesicles from the toad urinary bladder and incorporated these membrane fragments to solvent-free planar lipid bilayer membranes. This resulted in the appearance of a macroscopic conductance highly sensitive to the diuretic amiloride added to the cis side. The blockage is voltage dependent and well described by a model which assumes that the drug binds to sites in the channel lumen. This binding site is localized at about 15% of the electric field across the membrane. The apparent inhibition constant (K(0)) is equal to 0.98 microM. Ca2+, in the micromolar range on the cis side, is a potent blocker of this conductance. The effect of the divalent has a complex voltage dependence and is modulated by pH. At the unitary level we have found two distinct amiloride-blockable channels with conductances of 160 pS (more frequent) and 120 pS. In the absence of the drug the mean open time is around 0.5 sec for both channels and is not dependent on voltage. The channels are cation selective (PNa/PCl = 15) and poorly discriminate between Na+ and K+ (PNa/PK = 2). Amiloride decreases the lifetime in the open state of both channels and also the conductance of the 160-pS channel.     

Wave-guide spectroscopy and ion transport in planar lipid bilayers

The refractive indices of the bilayer-electrolyte system allow the membrane to operate as a light-guide. This system is then able to monitor, optically, the flow of ions across the bilayer. The light is coupled into and decoupled from a spherically bulged bilayer by means of optical, single mode fibers. The light wave travels along the curved bilayer for several millimeters. This light transmission depends critically on the angle of incidence between the fiber axis and the tangent to the film. Three transmission peaks were observed when the angle of incidence was varied between 0° and 90°. The transmitted light intensity can be modulated by the application of an electric potential upon the bilayer. The center peak, with maximum light transmission, appears at an angle of incidence which is defined by the launching geometry. A quadratic field dependence (independent of the polarity) is observed, which originates from changes in the shape of the torus transition region. The transmission of the satellite peaks, which appear just before and after the central peak, can also be modulated by an external potential. This modulation signal reflects a linear dependence on the polarity of the external voltage. The phase of the modulation signal changes its sign at each satellite peak. It is shown that this modulation signal originates from the bimolecular area of the lipid film. We present evidence that this transmission modulation occurs as a result of ion transport through the lipid film. This provides the basis for the use of wave-guide spectroscopy to investigate membrane ionic fluxes.     

Delta-endotoxins form cation-selective channels in planar lipid bilayers.

Delta-endotoxins CryIA(c) and CryIIIA, two members of a large family of toxic proteins from Bacillus thuringiensis, were each allowed to interact with planar lipid bilayers and were analyzed for their ability to form ion-conducting channels. Both of these toxins made clearly resolved channels in the membranes and exhibited several conductance states, which ranged from 200 pS to about 4000 pS (in 300 mM KCl). The channels formed by both toxins were highly cation-selective, but not ideally so. The permeability ratio of K+ to Cl- was about 25 for both channels. The ability of these proteins to form such channels may account for their toxic action on sensitive cells, and suggests that this family of toxins may act by a common mechanism.     

Interactions of alpha-helices with lipid bilayers: a review of simulation studies

Membrane proteins, of which the majority seem to contain one or more alpha-helix, constitute approx. 30% of most genomes. A complete understanding of the nature of helix/bilayer interactions is necessary for an understanding of the structural principles underlying membrane proteins. This review describes computer simulation studies of helix/bilayer interactions. Key experimental studies of the interactions of alpha-helices and lipid bilayers are briefly reviewed. Surface associated helices are found in some membrane-bound enzymes (e.g. prostaglandin synthase), and as stages in the mechanisms of antimicrobial peptides and of pore-forming bacterial toxins. Transmembrane alpha-helices are found in most integral membrane proteins, and also in channels formed by amphipathic peptides or by bacterial toxins. Mean field simulations, in which the lipid bilayer is approximated as a hydrophobic continuum, have been used in studies of membrane-active peptides (e.g. alamethicin, melittin, magainin and dermaseptin) and of simple membrane proteins (e.g. phage Pf1 coat protein). All atom molecular dynamics simulations of fully solvated bilayers with transmembrane helices have been applied to: the constituent helices of bacteriorhodopsin; peptide-16 (a simple model TM helix); and a number of pore-lining helices from ion channels. Surface associated helices (e.g. melittin and dermaseptin) have been simulated, as have alpha-helical bundles such as bacteriorhodopsin and alamethicin. From comparison of the results from the two classes of simulation, it emerges that a major theoretical challenge is to exploit the results of all atom simulations in order to improve the mean field approach.     

Reconstitution of vacuolar ion channels into planar lipid bilayers.

Vacuolar ion channels were characterized after reconstitution into planar lipid bilayers. (1) Channel activity was observed after incorporation of tonoplast-enriched microsomal membranes, purified tonoplast membranes or of solubilized tonoplast proteins. (2) Channels of varying single-channel conductances were detected after reconstitution. In symmetrical 100 mmol l-1 KCl, conductances between 1 and 110 pS were frequently measured; the largest number of independent reconstitution events was seen for single-channel conductances of 16-25 pS (28 experiments), 30-42 pS (26), 49-56 pS (15) and 64-81 pS (15). Channel current usually increased linearly with voltage. (3) In asymmetrical solutions, cation-, non-selective and, for the first time for the tonoplast, anion-selective channels were detected. Ca(2+)-dependent regulation of channel opening was not observed in our reconstitution system. (4) Permeability was also observed for Cl-, NO3-, SO4(2-) and phosphate. (5) After fractionation of tonoplast proteins by size exclusion chromatography, ion channel activity was recovered in specific fractions. (6) Some of these fractions catalyzed sulfate transport after reconstitution into liposomes. The results suggest that different channels are active at the tonoplast membrane at a larger number than has been concluded from previous work.