Structure of reconstituted bacterial membrane efflux pump by cryo-electron tomography

Complexes of OprM and MexA, two proteins of the MexA-MexB-OprM multidrug efflux pump from Pseudomonasaeruginosa, an opportunistic Gram-negative bacterium, were reconstituted into proteoliposomes by detergent removal. Stacks of protein layers with a constant height of 21 nm, separated by lipid bilayers, were obtained at stoichiometry of 1:1 (w/w). Using cryo-electron microscopy and tomography, we showed that these protein layers were composed of MexA-OprM complexes self-assembled into regular arrays. Image processing of extracted sub-tomograms depicted the architecture of the bipartite complex sandwiched between two lipid bilayers, representing an environment close to that of the native whole pump (i.e. anchored between outer and inner membranes of P. aeruginosa). The MexA-OprM complex appeared as a cylindrical structure in which we were able to identify the OprM molecule and the MexA moiety. MexA molecules have a cylindrical shape prolonging the periplasmic helices of OprM, and widening near the lipid bilayer. The flared part is likely composed of two MexA domains adjacent to the lipid bilayer, although their precise organization was not reachable mainly due to their flexibility. Moreover, the intermembrane distance of 21 nm indicated that the height of the bipartite complex is larger than that of the tripartite AcrA-AcrB-TolC built-up model in which TolC and AcrB are docked into contact. We proposed a model of MexA-OprM taking into account features of previous models based on AcrA-AcrB-TolC and our structural results providing clues to a possible mechanism of tripartite system assembly.     

Atomic force microscopy imaging of the structure of the motor protein prestin reconstituted into an artificial lipid bilayer

Prestin is the motor protein of cochlear outer hair cells and is essential for mammalian hearing. The present study aimed to clarify the structure of prestin by atomic force microscopy (AFM). Prestin was purified from Chinese hamster ovary cells which had been modified to stably express prestin, and then reconstituted into an artificial lipid bilayer. Immunofluorescence staining with anti-prestin antibody showed that the cytoplasmic side of prestin was possibly face up in the reconstituted lipid bilayer. AFM observation indicated that the cytoplasmic surface of prestin was ring-like with a diameter of about 11 nm.     

Lateral pressure dependence of the phospholipid transmembrane diffusion rate in planar-supported lipid bilayers

The dependence of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) flip-flop kinetics on the lateral membrane pressure in a phospholipid bilayer was investigated by sum-frequency vibrational spectroscopy. Planar-supported lipid bilayers were prepared on fused silica supports using the Langmuir-Blodgett/Langmuir-Schaeffer technique, which allows precise control over the lateral surface pressure and packing density of the membrane. The lipid bilayer deposition pressure was varied from 28 to 42 mN/m. The kinetics of lipid flip-flop in these membranes was measured by sum-frequency vibrational spectroscopy at 37°C. An order-of-magnitude difference in the rate constant for lipid translocation (10.9 × 10⁻⁴ s⁻¹ to 1.03 × 10⁻⁴ s⁻¹) was measured for membranes prepared at 28 mN/m and 42 mN/m, respectively. This change in rate results from only a 7.4% change in the packing density of the lipids in the bilayer. From the observed kinetics, the area of activation for native phospholipid flip-flop in a protein-free DPPC planar-supported lipid bilayer was determined to be 73 ± 12 Å²/molecule at 37°C. Significance of the observed activation area and potential future applications of the technique to the study of phospholipid flip-flop are discussed.     

Membrane attach complex of complement (MAC): three-dimensional analysis of MAC-phospholipid vesicle recombinants

The three-dimensional structure of recombinants of the isolated membrane attack complex (MAC) of complement with single bilayer dioleoyllecithin (DOL) vesicles and with dimyristoyllecithin (DML) vesicles was determined. A total of four MAC-vesicle complexes were analyzed by imaging negatively stained specimens at various defined tilting angles under minimal dose conditions in the electron microscope and by computer-aided three-dimensional reconstruction. The information on electron micrographs obtained at 6 degrees angular increments from +60 degrees to -60 degrees was digitized by densitometric scanning, Fourier-transformed, corrected for imaging errors, cross-correlated, and synthesized to the three-dimensional image. All four MAC-vesicle recombinants showed stain penetration into the interior of the vesicle, indicating increased permeability of the bilayer to negative stain. The MAC appeared as a hollow structure of 16-nm height, 2.0-nm wall thickness, and a 3.0-nm torus at the free end with an outer and inner diameter of 20.0 nm and 10.0 nm. In MAC-DOL vesicles the hollow core of the MAC terminated at the membrane-binding site, and only small pores of up to 2.0-nm in diameter penetrated the bilayer. In one MAC-DML vesicle lipid discontinuities on the outer circumference of the MAC binding site mediated stain penetration. The second MAC-DML vesicle showed a channel of approximately 4.0 nm connecting the hollow core of the MAC across the bilayer with the vesicle interior. The results suggest the MAC may mediate increased membrane permeability by protein channel formation in addition to lipid reorientation.     

Structure and orientation study of fusion peptide FP23 of gp41 from HIV-1 alone or inserted into various lipid membrane models (mono-, bi- and multibi-layers) by FT-IR spectroscopies and Brewster angle microscopy

In the present work, we study the structure and the orientation of the 23 N-terminal peptide of the HIV-1 gp 41 protein (AVGIGALFLGFLGAAGSTMGARS) called FP23. The behaviour of FP23 was investigated alone at the air/water interface and inserted into various lipid model systems: in monolayer or multibilayers of a DOPC/cholesterol/DOPE/DOPG (6/5/3/2) and in a DMPC bilayer. PMIRRAS and polarized ATR spectroscopy coupled with Brewster angle microscopy and spectral simulations were used to precisely determine the structure and the orientation of the peptide in its environment as well as the lipid perturbations induced by the FP23 insertion. The infra-red results show the structural polymorphism of the FP23 and its ability to transit quasi irreversibly from an α-helix to antiparallel β-sheets. At the air/water interface, the transition is induced by compression of the peptide alone and is modulated by compression and lipid to peptide ratio (Ri) when FP23 is inserted into a lipid monolayer. In multibilayers and in a single bilayer, there is coexistence in quasi equal proportions of α-helix and antiparallel β-sheets of FP23 at low peptide content (Ri = 100, 200) while antiparallel β-sheets are predominant at high FP23 concentration (Ri = 50). In (multi)bilayer systems, evaluation of dichroic ratios and sprectral simulations show that both the α-helix and the antiparallel β-sheets are tilted at diluted FP23 concentrations (tilt angle of α-helix with respect to the normal of the interface = 36.5 ± 3.0° for FP23 in multibilayers of DOPC/Chol/DOPE/DOPG at Ri = 200 and 39.0 ± 5.0° in a single bilayer of DMPC at Ri = 100 and tilt angle of the β-sheets = 36.0 ± 2.0° for the β-sheets in multibilayers and 30.0 ± 2.0° in the lipid bilayer). In parallel, the FP23 induces an increase of the lipid chain disorder which shows both by an increase of the methylene stretching frequencies and an increase of the average C-C-C angle of the acyl chains. At high FP23 content (Ri = 50), the antiparallel β-sheets induce a complete disorganization of the lipid chains in (multi)bilayers.     

Interaction of gramicidin S and its aromatic amino-acid analog with phospholipid membranes

To investigate the mechanism of interaction of gramicidin S-like antimicrobial peptides with biological membranes, a series of five decameric cyclic cationic β-sheet-β-turn peptides with all possible combinations of aromatic D-amino acids, Cyclo(Val-Lys-Leu-D-Ar1-Pro-Val-Lys-Leu-D-Ar2-Pro) (Ar ≡ Phe, Tyr, Trp), were synthesized. Conformations of these cyclic peptides were comparable in aqueous solutions and lipid vesicles. Isothermal titration calorimetry measurements revealed entropy-driven binding of cyclic peptides to POPC and POPE/POPG lipid vesicles. Binding of peptides to both vesicle systems was endothermic—exceptions were peptides containing the Trp-Trp and Tyr-Trp pairs with exothermic binding to POPC vesicles. Application of one- and two-site binding (partitioning) models to binding isotherms of exothermic and endothermic binding processes, respectively, resulted in determination of peptide-lipid membrane binding constants (K_b). The K_b1 and K_b2 values for endothermic two-step binding processes corresponded to high and low binding affinities (K_b1 ≥ 100 K_b2). Conformational change of cyclic peptides in transferring from buffer to lipid bilayer surfaces was estimated using fluorescence resonance energy transfer between the Tyr-Trp pair in one of the peptide constructs. The cyclic peptide conformation expands upon adsorption on lipid bilayer surface and interacts more deeply with the outer monolayer causing bilayer deformation, which may lead to formation of nonspecific transient peptide-lipid porelike zones causing membrane lysis.     

Trp2313-His2315 of Factor VIII C2 Domain Is Involved in Membrane Binding: STRUCTURE OF A COMPLEX BETWEEN THE C2 DOMAIN AND AN INHIBITOR OF MEMBRANE BINDING*

Factor VIII (FVIII) plays a critical role in blood coagulation by forming the tenase complex with factor IXa and calcium ions on a membrane surface containing negatively charged phospholipids. The tenase complex activates factor X during blood coagulation. The carboxyl-terminal C2 domain of FVIII is the main membrane-binding and von Willebrand factor-binding region of the protein. Mutations of FVIII cause hemophilia A, whereas elevation of FVIII activity is a risk factor for thromboembolic diseases. The C2 domain-membrane interaction has been proposed as a target of intervention for regulation of blood coagulation. A number of molecules that interrupt FVIII or factor V (FV) binding to cell membranes have been identified through high throughput screening or structure-based design. We report crystal structures of the FVIII C2 domain under three new crystallization conditions, and a high resolution (1.15 Å) crystal structure of the FVIII C2 domain bound to a small molecular inhibitor. The latter structure shows that the inhibitor binds to the surface of an exposed β-strand of the C2 domain, Trp²³¹³-His²³¹⁵. This result indicates that the Trp²³¹³-His²³¹⁵ segment is an important constituent of the membrane-binding motif and provides a model to understand the molecular mechanism of the C2 domain membrane interaction.     

Signaling through C2 domains: More than one lipid target

C2 domains are membrane-binding modules that share a common overall fold: a single compact Greek-key motif organized as an eight-stranded anti-parallel β-sandwich consisting of a pair of four-stranded β-sheets. A myriad of studies have demonstrated that in spite of sharing the common structural β-sandwich core, slight variations in the residues located in the interconnecting loops confer C2 domains with functional abilities to respond to different Ca^2 + concentrations and lipids, and to signal through protein–protein interactions as well. This review summarizes the main structural and functional findings on Ca^2 + and lipid interactions by C2 domains, including the discovery of the phosphoinositide-binding site located in the β3–β4 strands. The wide variety of functions, together with the different Ca^2 + and lipid affinities of these domains, converts this superfamily into a crucial player in many functions in the cell and more to be discovered. This Article is Part of a Special Issue Entitled: Membrane Structure and Function: Relevance in the Cell's Physiology, Pathology and Therapy.     

Factor VIII Lacking the C2 Domain Retains Cofactor Activity in Vitro

Factor (F) VIII consists of a heavy chain (A1A2B domains) and light chain (A3C1C2 domains). The activated form of FVIII, FVIIIa, functions as a cofactor for FIXa in catalyzing the membrane-dependent activation of FX. Whereas the FVIII C2 domain is believed to anchor FVIIIa to the phospholipid surface, recent x-ray crystal structures of FVIII suggest that the C1 domain may also contribute to this function. We constructed a FVIII variant lacking the C2 domain (designated ΔC2) to characterize the contributions of the C1 domain to function. Binding affinity of the ΔC2 variant to phospholipid vesicles as measured by energy transfer was reduced ∼14-fold. However, the activity of ΔC2 as measured by FXa generation and one-stage clotting assays retained 76 and 36%, respectively, of the WT FVIII value. Modest reductions (∼4-fold) were observed in the functional affinity of ΔC2 FVIII for FIXa and rates of thrombin activation. On the other hand, deletion of C2 resulted in significant reductions in FVIIIa stability (∼3.6-fold). Thrombin generation assays showed peak thrombin and endogenous thrombin potential were reduced as much as ∼60-fold. These effects likely result from a combination of the intermolecular functional defects plus reduced protein stability. Together, these results indicate that FVIII domains other than C2, likely C1, make significant contributions to membrane-binding and membrane-dependent function.     

AFM study on the electric-field effects on supported bilayer lipid membranes

Electric-field induced changes in structure and conductivity of supported bilayer lipid membranes (SLM) have been studied at submicroscopic resolution using atomic force microscopy and electrochemical impedance spectroscopy. The SLMs are formed on gold surfaces modified with mixed self-assembled monolayers of a cholesterol-tether and 6-mercaptohexanol. At applied potentials of ≤−0.25 V versus standard hydrogen electrode, the conductance of the SLM increases and membrane areas of <150 nm in size are found to elevate from the surface up to 15 nm in height. To estimate the electric field experienced by the lipid membrane, electrowetting has been used to determine the point of zero charge of a 6-mercaptohexanol-modified surface (0.19 ± 0.13 V versus standard hydrogen electrode). The effects of electric fields on the structure and conductance of supported membranes are discussed.     

A method to determine dielectric constants in nonhomogeneous systems: application to biological membranes

Continuum electrostatic models have had quantitative success in describing electrostatic-mediated phenomena on atomistic scales; however, there continues to be significant disagreement about how to assign dielectric constants in mixed, nonhomogeneous systems. We introduce a method for determining a position-dependent dielectric profile from molecular dynamics simulations. In this method, the free energy of introducing a test charge is computed two ways: from a free energy perturbation calculation and from a numerical solution to Poisson's Equation. The dielectric profile of the system is then determined by minimizing the discrepancy between these two calculations simultaneously for multiple positions of the test charge. We apply this method to determine the dielectric profile of a lipid bilayer surrounded by water. We find good agreement with dielectric models for lipid bilayers obtained by other approaches. The free energy of transferring an ion from bulk water to the lipid bilayer computed from the atomistic simulations indicates that large errors are introduced when the bilayer is represented as a single slab of low dielectric embedded in the higher-dielectric solvent. Significant improvement results from introducing an additional layer of intermediate dielectric (∼3) on each side of the low dielectric core extending from ∼12 Å to 18 Å. A small dip in transfer free energy just outside the lipid headgroups indicates the presence of a very high dielectric. These results have implications for the design of implicit membrane models and our understanding of protein-membrane interactions.     

Leakage-free membrane fusion induced by the hydrolytic activity of PlcHR2, a novel phospholipase C/sphingomyelinase from Pseudomonas aeruginosa

PlcHR₂ is the paradigm member of a novel phospholipase C/phosphatase superfamily, with members in a variety of bacterial species. This paper describes the phospholipase C and sphingomyelinase activities of PlcHR₂ when the substrate is in the form of large unilamellar vesicles, and the subsequent effects of lipid hydrolysis on vesicle and bilayer stability, including vesicle fusion. PlcHR₂ cleaves phosphatidylcholine and sphingomyelin at equal rates, but is inactive on phospholipids that lack choline head groups. Calcium in the millimolar range does not modify in any significant way the hydrolytic activity of PlcHR₂ on choline-containing phospholipids. The catalytic activity of the enzyme induces vesicle fusion, as demonstrated by the concomitant observation of intervesicular total lipid mixing, inner monolayer-lipid mixing, and aqueous contents mixing. No release of vesicular contents is detected under these conditions. The presence of phosphatidylserine in the vesicle composition does not modify significantly PlcHR₂-induced liposome aggregation, as long as Ca²⁺ is present, but completely abolishes fusion, even in the presence of the cation. Each of the various enzyme-induced phenomena have their characteristic latency periods, that increase in the order lipid hydrolysis < vesicle aggregation < total lipid mixing < inner lipid mixing < contents mixing. Concomitant measurements of the threshold diacylglyceride + ceramide concentrations in the bilayer show that late events, e.g. lipid mixing, require a higher concentration of PlcHR₂ products than early ones, e.g. aggregation. When the above results are examined in the context of the membrane effects of other phospholipid phosphocholine hydrolases it can be concluded that aggregation is necessary, but not sufficient for membrane fusion to occur, that diacylglycerol is far more fusogenic than ceramide, and that vesicle membrane permeabilization occurs independently from vesicle fusion.     

Neutron diffraction analysis of cytochrome b5 reconstituted in deuterated lipid multilayers

Cytochrome b5 was reconstituted with a highly deuterated phospholipid to form ordered multilayers consisting of repeated centrosymmetric pairs of asymmetric lipid-protein bilayers. Lamellar neutron diffraction data were collected to approximately 29 A resolution, and have been interpreted using models for the interaction of the membrane-binding domain of cytochrome b5 with the lipid bilayer. A range of different models was examined, and those in which the protein penetrates well into the bilayer, possibly spanning it, are favored.     

Differences in the Transbilayer and Lateral Motions of Fluorescent Analogs of Phosphatidylcholine and Phosphatidylethanolamine in the Apical Plasma Membrane of Bovine Aortic Endothelial Cells

In the plasma membrane of various eucaryotic cell types, in particular blood platelets and erythrocytes, it is known that phospholipids are asymmetrically distributed between the two leaflets of the lipid bilayer and that this transverse asymmetry is controlled by an aminophospholipid translocase activity. In this respect, it was of interest to check whether there are differential transbilayer movements between amino- and neutral phospholipids in the apical plasma membrane of vascular endothelial cells which form the inner nonthrombogenic lining of the large blood vessel. In the first step we compared the transbilayer localization and also the rate of lateral motion of two fluorescent analogs of phosphatidylcholine and phosphatidylethanolamine, namely C6-NBD-PC and C6-NBD-PE, inserted into the apical plasma membrane of bovine aortic endothelial cells, in vitro. By the use of back-exchange experiments we have found that C6-NBD-PC could be removed from the cell membrane toward the culture medium regardless of the incubation conditions used, i.e., just after cell labeling at 0°C or even after further cell incubation for 1 h at 0 or 20°C. In contrast, C6-NBD-PE could be removed only when the cells were maintained at 0°C. After incubation for 1 h at 20°C, 85% of the probe molecules remained nonexchangeable, indicating probe translocation from the outer to the inner leaflet of the lipid bilayer. This "flip" process, which occurred at 20°C, was abolished when the endothelial cells were preincubated with N-ethylmaleimide, diamide, vanadate (VO^3-₄) and vanadyl (VO²⁺) ions, a set of substances which inhibit aminophospholipid translocase activity in various systems, and with a combination of sodium azide and 2-deoxyglucose which led to nearly complete ATP depletion in the cells. Fluorescence recovery after photobleaching experiments were also carried out to specify more precisely the localization and dynamics of the probes in the two leaflets of the plasma membrane lipid bilayer. They produced lateral diffusion coefficients D of 1.2 ± 0.05 × 10^-9 cm²/s for C6-NBD-PC and 2.8 ± 0.3 × 10^-9 cm²/s for C6-NBD-PE, when the two probes were located in the outer leaflet of the plasma membrane, just after cell labeling at 0°C. After cell incubation for one hour at 20°C, i.e., when C6-NBD-PC was still in the outer leaflet whereas C6-NBD-PE was translocated in the inner leaflet, D was observed to slightly increase for C6-NBD-PC (D = 1.9 ± 0.06 × 10^-9 cm²/s) and to greatly increase by at least a factor of 3 for C6-NBD-PE (D = 9.1 ± 0.9 × 10^-9 cm²/s). These results show that the plasma membrane of bovine aortic endothelial cells is equipped with a protein-dependent and energy-mediated phosphatidylethanolamine translocase activity and that the lateral diffusion rate of this phospholipid is much faster in the inner than in the outer leaflet of the lipid bilayer, thus indicating large differences in the fluidity of the two halves of this membrane.     

Structural Features of Membrane Fusion between Influenza Virus and Liposome as Revealed by Quick-Freezing Electron Microscopy

The structure of membrane fusion intermediates between the A/PR/8(H1N1) strain of influenza virus and a liposome composed of egg phosphatidylcholine, cholesterol, and glycophorin was studied using quick-freezing electron microscopy. Fusion by viral hemagglutinin protein was induced at pH 5.0 and 23°C. After a 19-s incubation under these conditions, small protrusions with a diameter of 10–20 nm were found on the fractured convex faces of the liposomal membranes, and small pits complementary to the protrusions were found on the concave faces. The protrusions and pits corresponded to fractured parts of outward bendings of the lipid bilayer or “microprotrusions of the lipid bilayer.” At the loci of the protrusions and pits, liposomal membranes had local contacts with viral membranes. In many cases both the protrusions and the pits were aligned in regular polygonal arrangements, which were thought to reflect the array of hemagglutinin spikes on the viral surface. These structures were induced only when the medium was acidic with the virus present. Based on these observations, it was concluded that the microprotrusions of the lipid bilayer are induced by hemagglutinin protein. Furthermore, morphological evidence for the formation of the “initial fusion pore” at the microprotrusion was obtained. The protrusion on the convex face sometimes had a tiny hole with a diameter of <4 nm in the center. The pits transformed into narrow membrane connections <10 nm in width, bridging viruses and liposomes. The structures of the fusion pore and fusion neck with larger sizes were also observed, indicating growth of the protrusions and pits to distinct fusion sites. We propose that the microprotrusion of the lipid bilayer is a fusion intermediate induced by hemagglutinin protein, and suggest that the extraordinarily high curvature of this membrane structure is a clue to the onset of fusion. The possible architecture of the fusion intermediate is discussed with regard to the localization of intramembrane particles at the microprotrusion.     

The properties of Bacillus cereus hemolysin II pores depend on environmental conditions

Hemolysin II (HlyII), one of several cytolytic proteins encoded by the opportunistic human pathogen Bacillus cereus, is a member of the family of oligomeric β-barrel pore-forming toxins. This work has studied the pore-forming properties of HlyII using a number of biochemical and biophysical approaches. According to electron microscopy, HlyII protein interacts with liposomes to form ordered heptamer-like macromolecular assemblies with an inner pore diameter of 1.5-2 nm and an outer diameter of 6-8 nm. This is consistent with inner pore diameter obtained from osmotic protection assay. According to the 3D model obtained, seven HlyII monomers might form a pore, the outer size of which has been estimated to be slightly larger than by the other method, with an inner diameter changing from 1 to 4 nm along the channel length. The hemolysis rate has been found to be temperature-dependent, with an explicit lag at lower temperatures. Temperature jump experiments have indicated the pore structures formed at 37 °C and 4 °C to be different. The channels formed by HlyII are anion-selective in lipid bilayers and show a rising conductance as the salt concentration increases. The results presented show for the first time that at high salt concentration HlyII pores demonstrate voltage-induced gating observed at low negative potentials. Taken together we have found that the membrane-binding properties of hemolysin II as well as the properties of its pores strongly depend on environmental conditions. The study of the properties together with structural modeling allows a better understanding of channel functioning.     

The Calcium-Dependent and Calcium-Independent Membrane Binding of Synaptotagmin 1: Two Modes of C2B Binding

The Ca²⁺-independent membrane interactions of the soluble C2 domains from synaptotagmin 1 (syt1) were characterized using a combination of site-directed spin labeling and vesicle sedimentation. The second C2 domain of syt1, C2B, binds to membranes containing phosphatidylserine and phosphatidylcholine in a Ca²⁺-independent manner with a lipid partition coefficient of approximately 3.0 × 10² M^− 1. A soluble fragment containing the first and second C2 domains of syt1, C2A and C2B, has a similar affinity, but C2A alone has no detectable affinity to phosphatidylcholine/phosphatidylserine bilayers in the absence of Ca²⁺. Although the Ca²⁺-independent membrane affinity of C2B is modest, it indicates that this domain will never be free in solution within the cell. Site-directed spin labeling was used to obtain bilayer depth restraints, and a simulated annealing routine was used to generate a model for the membrane docking of C2B in the absence of Ca²⁺. In this model, the polybasic strand of C2B forms the membrane binding surface for the domain; however, this face of C2B does not penetrate the bilayer but is localized within the aqueous double layer when C2B is bound. This double-layer location indicates that C2B interacts in a purely electrostatic manner with the bilayer interface. In the presence of Ca²⁺, the membrane affinity of C2B is increased approximately 20-fold, and the domain rotates so that the Ca²⁺-binding loops of C2B insert into the bilayer. This Ca²⁺-triggered conformational change may act as a switch to modulate the accessibility of the polybasic face of C2B and control interactions of syt1 with other components of the fusion machinery.     

Fluorescence quenching of cytochrome b5 in vesicles with an asymmetric transbilayer distribution of brominated phosphatidylcholine

Several fluorescence techniques have been used to estimate the depth, in the membrane, of the endogenous tryptophans of membrane-bound proteins. We reported recently the use of phosphatidylcholines specifically brominated at different positions of the sn-2 acyl chain for this purpose (Markello, T., Zlotnick, A., Everett, J., Tennyson, J., and Holloway, P. W. (1985) Biochemistry 24, 2895-2901). The membranes made from these brominated lipids will have the brominated lipid in both monolayers, and so the estimated depth of the fluorophore will be relative to either the inner or outer surface of the membrane, but will not distinguish between these two extremes. To differentiate between these two models vesicles have now been made with an asymmetric distribution of brominated lipid, by use of phosphatidylcholine exchange protein. The asymmetric vesicles were isolated by virtue of their density, and their asymmetry was established by addition of an amphipathic fluorescent carbazole compound. With these vesicles it was shown that the tryptophan in the membrane-binding domain of cytochrome b5 which is quenched by bromolipid is located 0.7 nm below the outer surface of the membrane vesicles, rather than 0.7 nm from the inner surface.     

Asymmetric dipping of bacteriophage M13 coat protein with increasing lipid bilayer thickness

Knowledge about the vertical movement of a protein with respect to the lipid bilayer plane is important to understand protein functionality in the biological membrane. In this work, the vertical displacement of bacteriophage M13 major coat protein in a lipid bilayer is used as a model system to study the molecular details of its anchoring mechanism in a homologue series of lipids with the same polar head group but different hydrophobic chain length. The major coat proteins were reconstituted into 14:1PC, 16:1PC, 18:1PC, 20:1PC, and 22:1PC bilayers, and the fluorescence spectra were measured of the intrinsic tryptophan at position 26 and BADAN attached to an introduced cysteine at position 46, located at the opposite ends of the transmembrane helix. The fluorescence maximum of tryptophan shifted for 700 cm^-1 on going from 14:1PC to 22:1PC, the corresponding shift of the fluorescence maximum of BADAN at position 46 was approximately 10 times less (∼ 70 cm^-1). Quenching of fluorescence with the spin label CAT 1 indicates that the tryptophan is becoming progressively inaccessible for the quencher with increasing bilayer thickness, whereas quenching of BADAN attached to the T46C mutant remained approximately unchanged. This supports the idea that the BADAN probe at position 46 remains at the same depth in the bilayer irrespective of its thickness and clearly indicates an asymmetrical nature of the protein dipping in the lipid bilayer. The anchoring strength at the C-terminal domain of the protein (provided by two phenylalanine residues together with four lysine residues) was estimated to be roughly 5 times larger than the anchoring strength of the N-terminal domain.     

Cryo-EM of the ATP11C flippase reconstituted in Nanodiscs shows a distended phospholipid bilayer inner membrane around transmembrane helix 2

ATP11C is a member of the P4-ATPase flippase family that mediates translocation of phosphatidylserine (PtdSer) across the lipid bilayer. In order to characterize the structure and function of ATP11C in a model natural lipid environment, we revisited and optimized a quick procedure for reconstituting ATP11C into Nanodiscs using methyl-β-cyclodextrin as a reagent for the detergent removal. ATP11C was efficiently reconstituted with the endogenous lipid, or the mixture of endogenous lipid and synthetic dioleoylphosphatidylcholine (DOPC)/dioleoylphosphatidylserine (DOPS), all of which retained the ATPase activity. We obtained 3.4 Å and 3.9 Å structures using single-particle cryo-electron microscopy (cryo-EM) of AlF- and BeF-stabilized ATP11C transport intermediates, respectively, in a bilayer containing DOPS. We show that the latter exhibited a distended inner membrane around ATP11C transmembrane helix 2, possibly reflecting the perturbation needed for phospholipid release to the lipid bilayer. Our structures of ATP11C in the lipid membrane indicate that the membrane boundary varies upon conformational changes of the enzyme and is no longer flat around the protein, a change that likely contributes to phospholipid translocation across the membrane leaflets.