Changes In Bilayer Thickness Research Articles

The impact of transmembrane peptides on lipid bilayer structure and mechanics: A study of the transmembrane domain of the influenza A virus M2 protein

Transmembrane peptides play important roles in many biological processes by interacting with lipid membranes. This study investigates how the transmembrane domain of the influenza A virus M2 protein, M2TM, affects the structure and mechanics of model lipid bilayers. Atomic force microscopy (AFM) imaging revealed small decreases in bilayer thickness with increasing peptide concentrations. AFM-based force spectroscopy experiments complemented by theoretical model analysis demonstrated significant decreases in bilayer's Young's modulus (E) and lateral area compressibility modulus (KA). This suggests that M2TM disrupts the cohesive interactions between neighboring lipid molecules, leading to a decrease in both the bilayer's resistance to indentation (E) and its ability to resist lateral compression/expansion (KA). The large decreases in bilayer elastic parameters (i.e., E and KA) contrast with small changes in bilayer thickness, implying that bilayer mechanics are not solely dictated by bilayer thickness in the presence of transmembrane peptides. The observed significant reduction in bilayer mechanical properties suggests a softening effect on the bilayer, potentially facilitating membrane curvature generation, a crucial step for M2-mediated viral budding. In parallel, our Raman spectroscopy revealed small but statistically significant changes in hydrocarbon chain vibrational dynamics, indicative of minor disordering in lipid chain conformation. Our findings provide useful insights into the complex interplay between transmembrane peptides and lipid bilayers, highlighting the significance of peptide-lipid interactions in modulating membrane structure, mechanics, and molecular dynamics.

Physiological changes in bilayer thickness induced by cholesterol control GPCR rhodopsin function

We monitored the effect on function of the G-protein-coupled receptor (GPCR) rhodopsin from small, stepwise changes in bilayer thickness induced by cholesterol. Over a range of phosphatidylcholine bilayers with hydrophobic thickness from ≈21 Å to 38 Å, the metarhodopsin-I (MI)/metarhodopsin-II (MII) equilibrium was monitored with UV-visible spectroscopy while ordering of hydrocarbon chains was probed by 2H-NMR. Addition of cholesterol shifted equilibrium toward MII for bilayers thinner than the average length of hydrophobic transmembrane helices (27 Å) and to MI for thicker bilayers, while small bilayer thickness changes within the range of the protein hydrophobic thickness drastically up- or downregulated MII formation. The cholesterol-induced shifts toward MII for thinner membranes correlated with the cholesterol-induced increase of bilayer hydrophobic thickness measured by NMR, consistent with continuum elastic modeling. The energetic penalty of adding cholesterol to thick bilayers caused rhodopsin oligomerization and a shift toward MI. In membranes of physiological thickness, changes in bilayer mechanical properties induced by cholesterol potentiated the interplay between bilayer and protein thickness resulting in large swings of the MI-MII equilibrium. In membrane containing cholesterol, elastic deformations near the protein are a dominant energetic contribution to the functional equilibrium of the model GPCR rhodopsin.

Lipid Membrane Flexibility in Protic Ionic Liquids.

Here, we determine by neutron spin echo spectrometry (NSE) how the flexibility of egg lecithin vesicles depends on solvent composition in two protic ionic liquids (PILs) and their aqueous mixtures. In combination with small-angle neutron scattering (SANS), dynamic light scattering (DLS), and fluorescent probe microscopy, we show that the bending modulus is up to an order of magnitude lower than in water but with no change in bilayer thickness or nonpolar chain composition. This effect is attributed to the dynamic association and exchange of the IL cation between the membrane and bulk liquid, which has the same origin as the underlying amphiphilic nanostructure of the IL solvent itself. This provides a new mechanism by which to tune and control lipid membrane behavior.

Electrostatic interactions between cationic dendrimers and anionic model biomembrane

The electrostatic interactions between cationic poly(amidoamine) (PAMAM) dendrimers of different generations, G3, G4, and G6, with net anionic model biomembranes have been predicted by adopting an analytical model based on two dissimilar soft spheres. The influence of bilayer surface charge density, ionic strength, pH, temperature, membrane softness (modeled as changes in bilayer thickness), and dendrimer generation on the attractive interaction was investigated. The attraction was found to decrease with increasing salt concentration, dendrimer charge, and thickness (or softness) of the membrane. On the other hand, the attraction increased with the surface charge density of the membrane, and the size of dendrimer generation. In fact, the attraction was found to be much larger for large generations, like G6 dendrimer that have a higher charge, than it is with small ones like G3 and G4 dendrimers. These results have implications for the use of PAMAM dendrimers as potential gene transfection vectors.

Molecular Mechanism for Gramicidin Dimerization and Dissociation in Bilayers of Different Thickness

Membrane protein functions can be altered by subtle changes in the host lipid bilayer physical properties. Gramicidin channels have emerged as a powerful system for elucidating the underlying mechanisms of membrane protein function regulation through changes in bilayer properties, which are reflected in the thermodynamic equilibrium distribution between nonconducting gramicidin monomers and conducting bilayer-spanning dimers. To improve our understanding of how subtle changes in bilayer thickness alter the gramicidin monomer and dimer distributions, we performed extensive atomistic molecular dynamics simulations and fluorescence-quenching experiments on gramicidin A (gA). The free-energy calculations predicted a nonlinear coupling between the bilayer thickness and channel formation. The energetic barrier inhibiting gA channel formation was sharply increased in the thickest bilayer (1,2-dierucoyl-sn-glycero-3-phosphocholine). This prediction was corroborated by experimental results on gramicidin channel activity in bilayers of different thickness. To further explore the mechanism of channel formation, we performed extensive unbiased molecular dynamics simulations, which allowed us to observe spontaneous gA dimer formation in lipid bilayers. The simulations revealed structural rearrangements in the gA subunits and changes in lipid packing, as well as water reorganization, that occur during the dimerization process. Together, the simulations and experiments provide new, to our knowledge, insights into the process and mechanism of gramicidin channel formation, as a prototypical example of the bilayer regulation of membrane protein function.

A QCM-D study of the concentration- and time-dependent interactions of human LL37 with model mammalian lipid bilayers.

The human antimicrobial peptide LL37 is promising as an alternative to antibiotics due to its biophysical interactions with charged bacterial lipids. However, its clinical potential is limited due to its interactions with zwitterionic mammalian lipids leading to cytotoxicity. Mechanistic insight into the LL37 interactions with mammalian lipids may enable rational design of less toxic LL37-based therapeutics. To this end, we studied concentration- and time-dependent interactions of LL37 with zwitterionic model phosphatidylcholine (PC) bilayers with quartz crystal microbalance with dissipation (QCM-D). LL37 mass adsorption and PC bilayer viscoelasticity changes were monitored by measuring changes in frequency (Δf) and dissipation (ΔD), respectively. The Voigt-Kelvin viscoelastic model was applied to Δf and ΔD to study changes in bilayer thickness and density with LL37 concentration. At low concentrations (0.10-1.00 μM), LL37 adsorbed onto bilayers in a concentration-dependent manner. Further analyses of Δf, ΔD and thickness revealed that peptide saturation on the bilayers was a threshold for interactions observed above 2.00 μM, interactions that were rapid, multi-step, and reached equilibrium in a concentration- and time-dependent manner. Based on these data, we proposed a model of stable transmembrane pore formation at 2.00-10.0 μM, or transition from a primarily lipid to a primarily protein film with a transmembrane pore formation intermediate state at concentrations of LL37 > 10 μM. The concentration-dependent interactions between LL37 and PC bilayers correlated with the observed concentration-dependent biological activities of LL37 (antimicrobial, immunomodulatory and non-cytotoxic at 0.1-1.0 μM, hemolytic and some cytotoxicity at 2.0-13 μM and cytotoxic at >13 μM).

Capacitive Detection of Low-Enthalpy, Higher-Order Phase Transitions in Synthetic and Natural Composition Lipid Membranes.

In-plane lipid organization and phase separation in natural membranes play key roles in regulating many cellular processes. Highly cooperative, first-order phase transitions in model membranes consisting of few lipid components are well understood and readily detectable via calorimetry, densitometry, and fluorescence. However, far less is known about natural membranes containing numerous lipid species and high concentrations of cholesterol, for which thermotropic transitions are undetectable by the above-mentioned techniques. We demonstrate that membrane capacitance is highly sensitive to low-enthalpy thermotropic transitions taking place in complex lipid membranes. Specifically, we measured the electrical capacitance as a function of temperature for droplet interface bilayer model membranes of increasing compositional complexity, namely, (a) a single lipid species, (b) domain-forming ternary mixtures, and (c) natural brain total lipid extract (bTLE). We observed that, for single-species lipid bilayers and some ternary compositions, capacitance exhibited an abrupt, temperature-dependent change that coincided with the transition detected by other techniques. In addition, capacitance measurements revealed transitions in mixed-lipid membranes that were not detected by the other techniques. Most notably, capacitance measurements of bTLE bilayers indicated a transition at ∼38 °C not seen with any other method. Likewise, capacitance measurements detected transitions in some well-studied ternary mixtures that, while known to yield coexisting lipid phases, are not detected with calorimetry or densitometry. These results indicate that capacitance is exquisitely sensitive to low-enthalpy membrane transitions because of its sensitivity to changes in bilayer thickness that occur when lipids and excess solvent undergo subtle rearrangements near a phase transition. Our findings also suggest that heterogeneity confers stability to natural membranes that function near transition temperatures by preventing unwanted defects and macroscopic demixing associated with high-enthalpy transitions commonly found in simpler mixtures.

The Interaction of Melittin with Dimyristoyl Phosphatidylcholine-Dimyristoyl Phosphatidylserine Lipid Bilayer Membranes

Membrane-active peptides (MAPs), which interact directly with the lipid bilayer of a cell and include toxins and host defense peptides, display lipid composition-dependent activity. Phosphatidylserine (PS) lipids are anionic lipids that are found throughout the cellular membranes of most eukaryotic organisms where they serve as both a functional component and as a precursor to phosphatidylethanolamine lipids. The inner leaflet of the plasma membrane contains more PS than the outer one, and the asymmetry is actively maintained. Here, the impact of the MAP melittin on the structure of lipid bilayer vesicles made of a mixture of phosphatidylcholine and phosphatidylserine was studied. Small-angle neutron scattering of the MAP associated with selectively deuterium-labeled lipid bilayer vesicles revealed how the thickness and lipid composition of phosphatidylserine-containing vesicles change in response to melittin. The peptide thickens the lipid bilayer for concentrations up to P/L=1/500, but membrane thinning results when P/L=1/200. The thickness transition is accompanied by a large change in the distribution of DMPS between the leaflets of the bilayer. The change in composition is driven by electrostatic interactions, while the change in bilayer thickness is driven by changes in the interaction of the peptide with the headgroup region of the lipid bilayer. The results provide new information about lipid-specific interactions that take place in mixed composition lipid bilayer membranes.

The Water Permeability and Pore Entrance Structure of Aquaporin-4 Depend on Lipid Bilayer Thickness

Aquaporin-4 (AQP4), the primary water channel in glial cells of the mammalian brain, plays a critical role in water transport in the central nervous system. Previous experiments have shown that the water permeability of AQP4 depends on the cholesterol content in the lipid bilayer, but it was not clear whether changes in permeability were due to direct cholesterol-AQP4 interactions or to indirect effects caused by cholesterol-induced changes in bilayer elasticity or bilayer thickness. To determine the effects resulting only from bilayer thickness, here we use a combination of experiments and simulations to analyze AQP4 in cholesterol-free phospholipid bilayers with similar elastic properties but different hydrocarbon core thicknesses previously determined by x-ray diffraction. The channel (unit) water permeabilities of AQP4 measured by osmotic-gradient experiments were 3.5 ± 0.2 × 10−13 cm3/s (mean ± SE), 3.0 ± 0.3 × 10−13 cm3/s, 2.5 ± 0.2 × 10−13 cm3/s, and 0.9 ± 0.1 × 10−13 cm3/s in bilayers containing (C22:1)(C22:1)PC, (C20:1)(C20:1)PC, (C16:0)(C18:1)PC, and (C13:0)(C13:0)PC, respectively. Channel permeabilities obtained by molecular dynamics (MD) simulations were 3.3 ± 0.1 × 10−13 cm3/s and 2.5 ± 0.1 × 10−13 cm3/s in (C22:1)(C22:1)PC and (C14:0)(C14:0)PC bilayers, respectively. Both the osmotic-gradient and MD-simulation results indicated that AQP4 channel permeability decreased with decreasing bilayer hydrocarbon thickness. The MD simulations also suggested structural modifications in AQP4 in response to changes in bilayer thickness. Although the simulations showed no appreciable changes to the radius of the pore located in the hydrocarbon region of the bilayers, the simulations indicated that there were changes in both pore length and α-helix organization near the cytoplasmic vestibule of the channel. These structural changes, caused by mismatch between the hydrophobic length of AQP4 and the bilayer hydrocarbon thickness, could explain the observed differences in water permeability with changes in bilayer thickness.

Controlling GPCR Rhodopsin Function by Small, Physiologically Relevant Changes in Bilayer Hydrophobic Thickness

It was established previously that the G protein-coupled membrane receptor rhodopsin has transmembrane helices which match a hydrophobic bilayer thickness of 27±1 A. Here we demonstrate that small changes of bilayer thickness of ±2 A about that match point translate in the considerable changes of rhodopsin activation measured as the metarhodopsin I (MI)/metarhodopsin II (MII) equilibrium. We observed a biphasic behavior of the MI/MII equilibrium, with a sharp decline towards MI from 25-27 A followed by a rapid increase of MII from 27-29 A. Results are qualitatively identical for thickness changes induced by mixing of 16:0-16:1 PC and 18:0-18:1 PC, or 16:1-16:1 PC and 18:1-18:1 PC, or addition of 0-30 mol% cholesterol to 16:0-16:1 PC. The biphasic behavior was observed regardless of lipids used to alter bilayer hydrophobic thickness suggesting a relationship between small changes in hydrophobic thickness and rhodopsin function. It strongly favors an explanation based on a change of elastic stresses in lipid bilayers upon the transition from negative curvature in lipid monolayers near the protein below 27 A hydrophobic thickness to positive monolayer curvature above the match point. A continuum elastic model of the membrane, including the effect of lipid monolayer curvature near the protein, predicts membrane mediated clustering of rhodopsin and stabilization of the MI photointermediate at the matching point. Small, physiologically relevant changes in cholesterol content of bilayers with a thickness in the physiologically relevant range do drastically down- or up regulate the amount of MII which is the state that activates G protein.

Direct detection of the gel-fluid phase transition of a single supported phospholipid bilayer using quartz crystal microbalance with dissipation monitoring.

Supported phospholipid bilayers (SPBs) are valuable models for fundamental studies of biological membranes and their interaction with biologically relevant solutes or particles. Herein, we demonstrate the capability of the quartz crystal microbalance with dissipation monitoring (QCM-D) to directly detect the gel-fluid phase transition of a SPB. The approach involves comparison of the frequency response of a bare and a bilayer-coated QCM-D crystal during linear temperature variation. Phase transition results in a change of the resonance frequency that coincides directly with the accompanied change in bilayer thickness detected by ellipsometry. Experiments performed at different heating rates further demonstrate the use of dissipation monitoring to determine the phase transition temperature based on the temperature-induced viscosity changes of the ambient medium in the immediate environment of the bilayer. Unlike other methods, the proposed approach enables precise determination of the phase transition of a SPB without the need for thermal equilibration of the measurement chamber and, thus, has great potential for sensitive detection of structural and/or compositional changes of the bilayer.

Membrane Dependence of the Mechanosensitive Channel of Large Conductance

The mechanosensitive channels of large conductance (MscL) are bacterial membrane proteins that serve as last resort emergency release valves in case of severe osmotic down shock. The channels activate with applied bilayer tension, opening a large (ca. 3 nS) mostly unselective pore. Among the mechanosensitive channels, MscL is the most studied and often used as a model for how proteins sense membrane tension. In addition to sensing bilayer tension MscL channels are influenced by various changes in the bilayer environment. For example, their gating kinetics is shifted by changes in bilayer thickness and lipid head group type; and they can be gated without applied tension by asymmetric addition of lysophosphatidylcholine.We use coarse-grained Martini molecular dynamics model[1,2] in combination with experiments to systematically explore the lipid bilayer influence on MscL function. We characterize the dependence of MscL gating kinetics on bilayer properties by simulating MscL embedded in bilayers of different composition and with systematic addition of straight chain alcohols. Both bilayer bulk properties and local properties/deformation around the proteins are analysed in addition to MscL time to opening after applied tension (ko). Analyses of over a hundred channel opening simulations reveal a short initial lag phase followed by an exponentially distributed channel opening time. In-silico predictions in different channel environments are compared with experimental data determined using reconstituted MscL in a liposomal fluorescent efflux assay. The in-silico model correctly predicts known MscL behaviour, like longer ko in thicker bilayers. Surprisingly, the model predicts longer ko with the addition of alcohols, a finding which was later experimentally confirmed. [1] S.J. Marrink, H.J. Risselada, S. Yefimov, D.P. Tieleman, A.H. De Vries. J. Phys. Chem. B 111:7812-7824, 2007. [2] S. Yefimov, E. van der Giessen, P.R. Onck, S.J. Marrink. Biophys. J., 94:2994-3002, 2008.

Single Tryptophan and Tyrosine Comparisons in the N-Terminal and C-Terminal Interface Regions of Transmembrane GWALP Peptides

Hydrophobic membrane-spanning helices often are flanked by interfacial aromatic or charged residues. In this paper, we compare the consequences of single Trp → Tyr substitutions at each interface for the properties of a defined transmembrane helix in the absence of charged residues. The choice of molecular framework is critical for these single-residue experiments because the presence of "too many" aromatic residues (more than one at either membrane-water interface) introduces excess dynamic averaging of solid state NMR observables. To this end, we compare the outcomes when changing W(5) or W(19), or both of them, to tyrosine in the well-characterized transmembrane peptide acetyl-GGALW(5)(LA)6LW(19)LAGA-amide ("GWALP23"). By means of solid-state (2)H and (15)N NMR experiments, we find that Y(19)GW(5)ALP23 displays similar magnitudes of peptide helix tilt as Y(5)GW(19)ALP23 and responds similarly to changes in bilayer thickness, from DLPC to DMPC to DOPC. The presence of Y(19) changes the azimuthal rotation angle ρ (about the helix axis) to a similar extent as Y(5), but in the opposite direction. When tyrosines are substituted for both tryptophans to yield GY(5,19)ALP23, the helix tilt angle is again of comparable magnitude, and furthermore, the preferred azimuthal rotation angle ρ is relatively unchanged from that of GW(5,19)ALP23. The extent of dynamic averaging increases marginally when Tyr replaces Trp. Yet, importantly, all members of the peptide family having single Tyr or Trp residues near each interface exhibit only moderate and not highly extensive dynamic averaging. The results provide important benchmarks for evaluating conformational and dynamic control of membrane protein function.

Cyclic Compression and Decompression of a Lipid Bilayer

In this study, we measure transient thicknesses of a lipid bilayer during electrostatic compression and decompression and deduce non-equilibrium molecular interactions of the surfactants' tails within the layer. The bilayer under investigation (sorbitan monooleate) is single-tailed and self-assembles between a water drop and hafnium oxide in dodecane. We detect minute changes in bilayer thickness (∼0.01 Å/s) resulting from step changes in electrostatic pressure. The dynamic response of the bilayer consists of an elastic response followed by an inelastic dissipative behavior. We observe a distinct asymmetry between the inelastic responses: compression triggers a linear reduction in thickness over time, whereas decompression induces a logarithmic increase in thickness.

Bilayer Thickness Mismatch Controls Domain Size in Model Membranes

The observation of lateral phase separation in lipid bilayers has received considerable attention, especially in connection to lipid raft phenomena in cells. It is widely accepted that rafts play a central role in cellular processes, notably signal transduction. While micrometer-sized domains are observed with some model membrane mixtures, rafts much smaller than 100 nm-beyond the reach of optical microscopy-are now thought to exist, both in vitro and in vivo. We have used small-angle neutron scattering, a probe free technique, to measure the size of nanoscopic membrane domains in unilamellar vesicles with unprecedented accuracy. These experiments were performed using a four-component model system containing fixed proportions of cholesterol and the saturated phospholipid 1,2-distearoyl-sn-glycero-3-phosphocholine (DSPC), mixed with varying amounts of the unsaturated phospholipids 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) and 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC). We find that liquid domain size increases with the extent of acyl chain unsaturation (DOPC:POPC ratio). Furthermore, we find a direct correlation between domain size and the mismatch in bilayer thickness of the coexisting liquid-ordered and liquid-disordered phases, suggesting a dominant role for line tension in controlling domain size. While this result is expected from line tension theories, we provide the first experimental verification in free-floating bilayers. Importantly, we also find that changes in bilayer thickness, which accompany changes in the degree of lipid chain unsaturation, are entirely confined to the disordered phase. Together, these results suggest how the size of functional domains in homeothermic cells may be regulated through changes in lipid composition.

Determining Membrane Capacitance by Dynamic Control of Droplet Interface Bilayer Area

By making dynamic changes to the area of a droplet interface bilayer (DIB), we are able to measure the specific capacitance of lipid bilayers with improved accuracy and precision over existing methods. The dependence of membrane specific capacitance on the chain-length of the alkane oil present in the bilayer is similar to that observed in black lipid membranes. In contrast to conventional artificial bilayers, DIBs are not confined by an aperture, which enables us to determine that the dependence of whole bilayer capacitance on applied potential is predominantly a result of a spontaneous increase in bilayer area. This area change arises from the creation of new bilayer at the three phase interface and is driven by changes in surface tension with applied potential that can be described by the Young-Lippmann equation. By accounting for this area change, we are able to determine the proportion of the capacitance dependence that arises from a change in specific capacitance with applied potential. This method provides a new tool with which to investigate the vertical compression of the bilayer and understand the changes in bilayer thickness with applied potential. We find that, for 1,2-diphytanoyl-sn-glycero-3-phosphocholine membranes in hexadecane, specific bilayer capacitance varies by 0.6-1.5% over an applied potential of ±100 mV.

Enthalpy Drives Phase Separation in Model Membranes: Evidence from Molecular Dynamics Simulations of Non-Lipid Amphiphiles Vitamin-E, triton-X, and Benzyl Alcohol

Phase separation of lipid bilayers into liquid-ordered and liquid-disordered regions facilitates compartmentalization of membrane proteins, an important prerequisite for cellular biochemical signaling. In this study, we investigated the phase behavior of binary and ternary lipid mixtures under the influence of three non-lipid amphiphiles, Vitamin-E, Triton-X 100, and benzyl alcohol. Molecular dynamics (MD) simulations of these additives in fluid-phase lipid bilayers were performed to investigate their effect on membrane thickness and fluidity as readouts of enthalpic and entropic changes, respectively. Simulation results indicate that Vitamin-E increases bilayer thickness and lowers the fluidity, while Triton-X and benzyl alcohol each decrease bilayer thickness and increase fluidity. Experimentally, in both binary and ternary lipid mixtures, Vitamin-E induced ideal mixing of the lipids whereas Triton-X and benzyl alcohol either resulted in sustained phase separation or induced large-scale phase separation. Because changes in bilayer thickness determined by MD correlate better than fluidity with phase separation observed in model membranes we conclude that hydrophobic mismatch of different lipid types (enthalpic effect) dominate the effect of fluidity (entropic effect) as the key driving force for the phase separation behavior observed in lipid bilayers. Moreover, these non-lipid amphiphiles provide new tools to tune raft formation/disruption and to study raft-related cell membrane functions through modulation of non-raft membrane thickness.

Conformational plasticity of the influenza A M2 transmembrane helix in lipid bilayers under varying pH, drug binding, and membrane thickness

Membrane proteins change their conformations to respond to environmental cues, thus conformational plasticity is important for function. The influenza A M2 protein forms an acid-activated proton channel important for the virus lifecycle. Here we have used solid-state NMR spectroscopy to examine the conformational plasticity of membrane-bound transmembrane domain of M2 (M2TM). 13C and 15N chemical shifts indicate coupled conformational changes of several pore-facing residues due to changes in bilayer thickness, drug binding, and pH. The structural changes are attributed to the formation of a well-defined helical kink at G34 in the drug-bound state and in thick lipid bilayers, nonideal backbone conformation of the secondary-gate residue V27 in the presence of drug, and nonideal conformation of the proton-sensing residue H37 at high pH. The chemical shifts constrained the (ϕ, ψ) torsion angles for three “basis” states, the equilibrium among which explains the multiple resonances per site in the NMR spectra under different combinations of bilayer thickness, drug binding, and pH conditions. Thus, conformational plasticity is important for the proton conduction and inhibition of M2TM. The study illustrates the utility of NMR chemical shifts for probing the structural plasticity and folding of membrane proteins.

Retinoschisin (RS1) Interacts with Negatively Charged Lipid Bilayers in the Presence of Ca2+: An Atomic Force Microscopy Study

Retinoschisin (RS1) is a retina-specific secreted protein encoding a conserved discoidin domain sequence. As an adhesion molecule, RS1 preserves the retinal cell architecture and promotes visual signal transduction. In young males, loss-of-function mutations in the X-linked retinoschisis gene (RS1) cause X-linked retinoschisis, a form of progressive blindness. Neither the structure of RS1 nor the nature of its anchoring and organization on the plasma membranes is fully understood. The discoidin C2 domains of coagulation factors V and VIII are known to interact with extracellular phosphatidylserine (PS). In this study we have used atomic force microscopy (AFM) to study the interactions of murine retinoschisin (Rs1) with supported anionic lipid bilayers in the presence of Ca(2+). The bilayers consisting of a single lipid, PS, and mixtures of lipids with or without PS were used. Consistent with previous X-ray diffraction studies, AFM imaging showed two distinct domains in pure PS bilayers when Ca(2+) was present. Upon Rs1 adsorption, these PS and PS-containing mixed bilayers underwent fast and extensive reorganization. Protein localization was ascertained by immunolabeling. AFM imaging showed the Rs1 antibody bound exclusively to the calcium-rich ordered phase of the bilayers pointing to the sequestration of Rs1 within those domains. This was further supported by the increased mechanical strength of these domains after Rs1 binding. Besides, changes in bilayer thickness suggested that Rs1 was partially embedded into the bilayer. These findings support a model whereby the Rs1 protein binds to PS in the retinal cell plasma membranes in a calcium-dependent manner.

Lipid−Rhodopsin Hydrophobic Mismatch Alters Rhodopsin Helical Content

The ability of photoactivated rhodopsin to achieve the enzymatically active metarhodopsin II conformation is exquisitely sensitive to bilayer hydrophobic thickness. The sensitivity of rhodopsin to the lipid matrix has been explained by the hydrophobic matching theory, which predicts that lipid bilayers adjust elastically to the hydrophobic length of transmembrane helices. Here, we examined if bilayer thickness adjusts to the length of the protein or if the protein alters its conformation to adapt to the bilayer. Purified bovine rhodopsin was reconstituted into a series of mono-unsaturated phosphatidylcholines with 14-20 carbons per hydrocarbon chain. Changes of hydrocarbon chain length were measured by (2)H NMR, and protein helical content was quantified by synchrotron radiation circular dichroism and conventional circular dichroism. Experiments were conducted on dark-adapted rhodopsin, the photo-intermediates metarhodopsin I/II/III, and opsin. Changes of bilayer thickness upon rhodopsin incorporation and photoactivation were mostly absent. In contrast, the helical content of rhodopsin increased with membrane hydrophobic thickness. Helical content did not change measurably upon photoactivation. The increases of bilayer thickness and helicity of rhodopsin are accompanied by higher metarhodopsin II/metarhodopsin I ratios, faster rates of metarhodopsin II formation, an increase of tryptophan fluorescence, and higher temperatures of rhodopsin denaturation. The data suggest a surprising adaptability of this G protein-coupled membrane receptor to properties of the lipid matrix.