Probing the U-Shaped Conformation of Caveolin-1 in a Bilayer

Caveolin induces membrane curvature and drives the formation of caveolae that participate in many crucial cell functions such as endocytosis. The central portion of caveolin-1 contains two helices (H1 and H2) connected by a three-residue break with both N- and C-termini exposed to the cytoplasm. Although a U-shaped configuration is assumed based on its inaccessibility by extracellular matrix probes, caveolin structure in a bilayer remains elusive. This work aims to characterize the structure and dynamics of caveolin-1 (D82–S136; Cav1_82–136) in a DMPC bilayer using NMR, fluorescence emission measurements, and molecular dynamics simulations. The secondary structure of Cav1_82–136 from NMR chemical shift indexing analysis serves as a guideline for generating initial structural models. Fifty independent molecular dynamics simulations (100 ns each) are performed to identify its favorable conformation and orientation in the bilayer. A representative configuration was chosen from these multiple simulations and simulated for 1 μs to further explore its stability and dynamics. The results of these simulations mirror those from the tryptophan fluorescence measurements (i.e., Cav1_82–136 insertion depth in the bilayer), corroborate that Cav1_82–136 inserts in the membrane with U-shaped conformations, and show that the angle between H1 and H2 ranges from 35 to 69°, and the tilt angle of Cav1_82–136 is 27 ± 6°. The simulations also reveal that specific faces of H1 and H2 prefer to interact with each other and with lipid molecules, and these interactions stabilize the U-shaped conformation.     

Probing the caveolin-1 P132L mutant: critical insights into its oligomeric behavior and structure

Caveolin-1 is the most important protein found in caveolae, which are cell surface invaginations of the plasma membrane that act as signaling platforms. A single point mutation in the transmembrane domain of caveolin-1 (proline 132 to leucine) has deleterious effects on caveolae formation in vivo and has been implicated in various disease states, particularly aggressive breast cancers. Using a combination of gel filtration chromatography and analytical ultracentrifugation, we found that a fully functional construct of caveolin-1 (Cav1(62-178)) was a monomer in dodecylphosphocholine micelles. In contrast, the P132L mutant of Cav1(62-178) was dimeric. To explore the dimerization of the P132L mutant further, various truncated constructs (Cav1(82-178), Cav1(96-178), Cav1(62-136), Cav1(82-136), Cav1(96-136)) were prepared which revealed that oligomerization occurs in the transmembrane domain (residues 96-136) of caveolin-1. To characterize the mutant structurally, solution-state NMR experiments in lyso-myristoylphosphatidylglycerol were undertaken of the Cav1(96-136) P132L mutant. Chemical shift analysis revealed that, compared to the wild-type, helix 2 in the transmembrane domain was lengthened by four residues (wild-type, residues 111-129; mutant, residues 111-133), which corresponds to an extra turn in helix 2 of the mutant. Lastly, point mutations at position 132 of Cav1(62-178) (P132A, P132I, P132V, P132G, P132W, P132F) revealed that no other hydrophobic amino acid can preserve the monomeric state of Cav1(62-178), which indicates that proline 132 is critical in supporting proper caveolin-1 behavior.     

Irregular structure of the HIV fusion peptide in membranes demonstrated by solid-state NMR and MD simulations

To better understand peptide-induced membrane fusion at a molecular level, we set out to determine the structure of the fusogenic peptide FP23 from the HIV-1 protein gp41 when bound to a lipid bilayer. An established solid-state ¹⁹F nuclear magnetic resonance (NMR) approach was used to collect local orientational constraints from a series of CF₃-phenylglycine-labeled peptide analogues in macroscopically aligned membranes. Fusion assays showed that these ¹⁹F-labels did not significantly affect peptide function. The NMR spectra were characteristic of well-behaved samples, without any signs of heterogeneity or peptide aggregation at 1:300 in 1,2-dimyristoyl-sn-glycero-3-phosphatidylcholine (DMPC). We can conclude from these NMR data that FP23 has a well-defined (time-averaged) conformation and undergoes lateral diffusion in the bilayer plane, presumably as a monomer or small oligomer. Attempts to evaluate its conformation in terms of various secondary structures, however, showed that FP23 does not form any type of regular helix or β-strand. Therefore, all-atom molecular dynamics (MD) simulations were carried out using the orientational NMR constraints as pseudo-forces to drive the peptide into a stable alignment and structure. The resulting picture suggests that FP23 can adopt multiple β-turns and insert obliquely into the membrane. Such irregular conformation explains why the structure of the fusion peptide could not be reliably determined by any biophysical method so far.     

The structural properties of the transmembrane segment of the integral membrane protein phospholamban utilizing C CPMAS, H, and REDOR solid-state NMR spectroscopy

Solid-state NMR spectroscopic techniques were used to investigate the secondary structure of the transmembrane peptide phospholamban (TM-PLB), a sarcoplasmic Ca²⁺ regulator. ¹³C cross-polarization magic angle spinning spectra of ¹³C carbonyl-labeled Leu39 of TM-PLB exhibited two peaks in a pure 1-palmitoyl-2-oleoyl-phosphocholine (POPC) bilayer, each due to a different structural conformation of phospholamban as characterized by the corresponding ¹³C chemical shift. The addition of a negatively charged phospholipid (1-palmitoyl-2-oleoylphosphatidylglycerol (POPG)) to the POPC bilayer stabilized TM-PLB to an α-helical conformation as monitored by an enhancement of the α-helical carbonyl ¹³C resonance in the corresponding NMR spectrum. ¹³C-¹⁵N REDOR solid-state NMR spectroscopic experiments revealed the distance between the ¹³C carbonyl carbon of Leu39 and the ¹⁵N amide nitrogen of Leu42 to be 4.2 ± 0.2Å indicating an α-helical conformation of TM-PLB with a slight deviation from an ideal 3.6 amino acid per turn helix. Finally, the quadrupolar splittings of three ²H labeled leucines (Leu28, Leu39, and Leu51) incorporated in mechanically aligned DOPE/DOPC bilayers yielded an 11° ± 5° tilt of TM-PLB with respect to the bilayer normal. In addition to elucidating valuable TM-PLB secondary structure information, the solid-state NMR spectroscopic data indicates that the type of phospholipids and the water content play a crucial role in the secondary structure and folding of TM-PLB in a phospholipid bilayer.     

High-resolution structural profile of hylaseptin-4: Aggregation,membrane topology and pH dependence of overall membrane binding process

Hylaseptin-4 (HSP-4, GIGDILKNLAKAAGKAALHAVGESL-NH₂) is an antimicrobial peptide originally isolated from Hypsiboas punctatus tree frog. The peptide has been chemically synthetized for structural investigations by CD and NMR spectroscopies. CD experiments reveal the high helical content of HSP-4 in biomimetic media. Interestingly, the aggregation process seems to occur at high peptide concentrations either in aqueous solution or in presence of biomimetic membranes, indicating an increase in the propensity of the peptide for adopting a helical conformation. High-resolution NMR structures determined in presence of DPC-d₃₈ micelles show a highly ordered α-helix from amino acid residues I2 to S24 and a smooth bend near G14. A large separation between hydrophobic and hydrophilic residues occurs up to the A16 residue, from which a shift in the amphipathicity is noticed. Oriented solid-state NMR spectroscopy show a roughly parallel orientation of the helical structure along the POPC lipid bilayer surface, with an insertion of the hydrophobic N-terminus into the bilayer core. Moreover, a noticeable pH dependence of the aggregation process in both aqueous and in biomimetic membrane environments is attributed to a single histidine residue (H19). The protonation degree of the imidazole side-chain might help in modulating the peptide-peptide or peptide-lipid interactions. Finally, molecular dynamics simulations confirm the orientation and preferential helical conformation and in addition, show that HSP-4 tends to self-aggregate in order to stabilize its active conformation in aqueous or phospholipid bilayer environments.     

Colocalization between caveolin isoforms in the intestinal smooth muscle and interstitial cells of Cajal of the Cav1+/+ and Cav1−/− mouse

Confocal microscopic images were obtained from the immunohistochemical sections of jejeunum to determine the localization/colocalization between caveolin-1, caveolin-2 and caveolin-3 in intestinal smooth muscle cells (SMCs) and interstitial cells of Cajal (ICC) of Cav1^+/+ and Cav1^−/− mouse. Intestinal regions were segmented [inner circular muscle (icm), outer circular muscle (ocm), myenteric plexus region (mp), and longitudinal muscle (lm)] by LSM 5 and analyzed by ImageJ to show Pearson’s correlation (r _p) and overlap coefficient (r) of colocalization. In the intestine of Cav1^+/+, caveolin-1 (cav1) was colocalized with caveolin-2 (cav2) and caveolin-3 (cav3). Cav2 also was well colocalized with cav3. In the intestine of Cav1^−/−, cav1 and cav2 were absent in all images, but reduced cav3 was expressed in ocm. Caveolae were present in cell types with cav1 in Cav1^+/+, and present with cav3 in ocm of Cav1^−/−. C-kit occurred in deep muscular plexus (ICC-DMP) and myenteric plexus (ICC-MP), in both Cav1^+/+ and Cav1^−/−, and colocalized with cav1 and cav2 in the intestine of Cav1^+/+. Cav3 was absent/present at low immunoreactivity in ICC-DMP and ICC-MP of the intestines of Cav1^+/+ and Cav1^−/−. To conclude, cav1 is necessary for the expression of cav2 in SMC and ICC of intestine and facilitates, but is not necessary for the expression of cav3.     

Tilt and Azimuthal Angles of a Transmembrane Peptide: A Comparison between Molecular Dynamics Calculations and Solid-State NMR Data of Sarcolipin in Lipid Membranes

We report molecular dynamics simulations in the explicit membrane environment of a small membrane-embedded protein, sarcolipin, which regulates the sarcoplasmic reticulum Ca-ATPase activity in both cardiac and skeletal muscle. In its monomeric form, we found that sarcolipin adopts a helical conformation, with a computed average tilt angle of 28 ± 6° and azymuthal angles of 66 ± 22°, in reasonable accord with angles determined experimentally (23 ± 2° and 50 ± 4°, respectively) using solid-state NMR with separated-local-field experiments. The effects of time and spatial averaging on both ¹⁵N chemical shift anisotropy and ¹H/¹⁵N dipolar couplings have been analyzed using short-time averages of fast amide out-of-plane motions and following principal component dynamic trajectories. We found that it is possible to reproduce the regular oscillatory patterns observed for the anisotropic NMR parameters (i.e., PISA wheels) employing average amide vectors. This work highlights the role of molecular dynamics simulations as a tool for the analysis and interpretation of solid-state NMR data.     

On the Combined Analysis of H and N/H Solid-State NMR Data for Determination of Transmembrane Peptide Orientation and Dynamics

The dynamics of membrane-spanning peptides have a strong affect on the solid-state NMR observables. We present a combined analysis of ²H-alanine quadrupolar splittings together with ¹⁵N/¹H dipolar couplings and ¹⁵N chemical shifts, using two models to treat the dynamics, for the systematic evaluation of transmembrane peptides based on the GWALP23 sequence (acetyl-GGALW(LA)₆LWLAGA-amide). The results indicate that derivatives of GWALP23 incorporating diverse guest residues adopt a range of apparent tilt angles that span 5°–35° in lipid bilayer membranes. By comparing individual and combined analyses of specifically ²H- or ¹⁵N-labeled peptides incorporated in magnetically or mechanically aligned lipid bilayers, we examine the influence of data-set size/identity, and of explicitly modeled dynamics, on the deduced average orientations of the peptides. We conclude that peptides with small apparent tilt values (<∼10°) can be fitted by extensive families of solutions, which can be narrowed by incorporating additional ¹⁵N as well as ²H restraints. Conversely, peptides exhibiting larger tilt angles display more narrow distributions of tilt and rotation that can be fitted using smaller sets of experimental constraints or even with ²H or ¹⁵N data alone. Importantly, for peptides that tilt significantly more than 10° from the bilayer-normal, the contribution from rigid body dynamics can be approximated by a principal order parameter.     

Structure, Dynamics, and Ion Conductance of the Phospholamban Pentamer

A 52-residue membrane protein, phospholamban (PLN) is an inhibitor of an adenosine-5′-triphosphate-driven calcium pump, the Ca²⁺-ATPase. Although the inhibition of Ca²⁺-ATPase involves PLN monomers, in a lipid bilayer membrane, PLN monomers form stable pentamers of unknown biological function. The recent NMR structure of a PLN pentamer depicts cytoplasmic helices extending normal to the bilayer in what is known as the bellflower conformation. The structure shows transmembrane helices forming a hydrophobic pore 4 Å in diameter, which is reminiscent of earlier reports of possible ion conductance through PLN pentamers. However, recent FRET measurements suggested an alternative structure for the PLN pentamer, known as the pinwheel model, which features a narrower transmembrane pore and cytoplasmic helices that lie against the bilayer. Here, we report on structural dynamics and conductance properties of the PLN pentamers from all-atom (AA) and coarse-grained (CG) molecular dynamics simulations. Our AA simulations of the bellflower model demonstrate that in a lipid bilayer membrane or a detergent micelle, the cytoplasmic helices undergo large structural fluctuations, whereas the transmembrane pore shrinks and becomes asymmetric. Similar asymmetry of the transmembrane region was observed in the AA simulations of the pinwheel model; the cytoplasmic helices remained in contact with the bilayer. Using the CG approach, structural dynamics of both models were investigated on a microsecond timescale. The cytoplasmic helices of the CG bellflower model were observed to fall against the bilayer, whereas in the CG pinwheel model the conformation of the cytoplasmic helices remained stable. Using steered molecular dynamics simulations, we investigated the feasibility of ion conductance through the pore of the bellflower model. The resulting approximate potentials of mean force indicate that the PLN pentamer is unlikely to function as an ion channel.     

The transmembrane domain of caveolin-1 exhibits a helix–break–helix structure

Caveolin is an integral membrane protein that is found in high abundance in caveolae. Both the N- and C- termini lie on the same side of the membrane, and the transmembrane domain has been postulated to form an unusual intra-membrane horseshoe configuration. To probe the structure of the transmembrane domain, we have prepared a construct of caveolin-1 that encompasses residues 96–136 (the entire intact transmembrane domain). Caveolin-1(96–136) was over-expressed and isotopically labeled in E. coli, purified to homogeneity, and incorporated into lyso-myristoylphosphatidylglycerol micelles. Circular dichroism and NMR spectroscopy reveal that the transmembrane domain of caveolin-1 is primarily α-helical (57–65%). Furthermore, chemical shift indexing reveals that the transmembrane domain has a helix–break–helix structure which could be critical for the formation of the intra-membrane horseshoe conformation predicted for caveolin-1. The break in the helix spans residues 108 to 110, and alanine scanning mutagenesis was carried out to probe the structural significance of these residues. Our results indicate that mutation of glycine 108 to alanine does not disrupt the structure, but mutation of isoleucine 109 and proline 110 to alanine dramatically alters the helix–break–helix structure. To explore the structural determinants further, additional mutagenesis was performed. Glycine 108 can be substituted with other small side chain amino acids (i.e. alanine), leucine 109 can be substituted with other β-branched amino acids (i.e. valine), and proline 110 cannot be substituted without disrupting the helix–break–helix structure.     

Identification of structural transitions in bacterial fatty acid binding proteins that permit ligand entry and exit at membranes

Fatty acid (FA) transfer proteins extract FA from membranes and sequester them to facilitate their movement through the cytosol. Detailed structural information is available for these soluble protein–FA complexes, but the structure of the protein conformation responsible for FA exchange at the membrane is unknown. Staphylococcus aureus FakB1 is a prototypical bacterial FA transfer protein that binds palmitate within a narrow, buried tunnel. Here, we define the conformational change from a “closed” FakB1 state to an “open” state that associates with the membrane and provides a path for entry and egress of the FA. Using NMR spectroscopy, we identified a conformationally flexible dynamic region in FakB1, and X-ray crystallography of FakB1 mutants captured the conformation of the open state. In addition, molecular dynamics simulations show that the new amphipathic α-helix formed in the open state inserts below the phosphate plane of the bilayer to create a diffusion channel for the hydrophobic FA tail to access the hydrocarbon core and place the carboxyl group at the phosphate layer. The membrane binding and catalytic properties of site-directed mutants were consistent with the proposed membrane docked structure predicted by our molecular dynamics simulations. Finally, the structure of the bilayer-associated conformation of FakB1 has local similarities with mammalian FA binding proteins and provides a conceptual framework for how these proteins interact with the membrane to create a diffusion channel from the FA location in the bilayer to the protein interior.     

Interaction abolishment between mutant caveolin-1(Δ62-100) and ABCA1 reduces HDL-mediated cellular cholesterol efflux

Our previous study shows that caveolin-1 colocalizes and interacts with ATP-binding cassette transporter A1 (ABCA1), which is intimately involved in cellular cholesterol efflux. In this study, we further clarified the region of caveolin-1 that interacts with ABCA1. We also examined the interaction between mutant caveolin-1 and ABCA1 in HDL-mediated cholesterol efflux. We constructed a panel of mutant caveolin-1 proteins and co-transfected them into rat aortic endothelial and human embryonic kidney 293 (HEK293) cells. The co-immunoprecipitation shows that mutant oligomerization domain of caveolin-1, caveolin-1_Δ62–100, is required for the interaction of caveolin-1 with ABCA1. Caveolin-1_Δ62–100 did not colocalize with ABCA1 in the cholesterol-loaded cells after HDL incubation as observed by immunofluorescence confocal microscopy. Concomitantly, caveolin-1_Δ62–100 suppressed HDL-mediated cholesterol efflux. The results suggest that the region of caveolin-1 between amino acids 62 and 100 is an oligomerization domain as well as an attachment site for ABCA1 interaction that regulates HDL-mediated cholesterol efflux.     

Phase Separation in Binary Mixtures of Bipolar and Monopolar Lipid Dispersions Revealed by H NMR Spectroscopy, Small Angle X-Ray Scattering, and Molecular Theory

Binary mixtures of C₂₀BAS and POPC membranes were studied by solid-state ²H NMR spectroscopy and small angle x-ray scattering (SAXS) over a wide range of concentrations and at different temperatures. Three specifically deuterated C₂₀BAS derivatives—[1′,1′,20′,20′-²H₄]C₂₀BAS, [2′,2′,19′,19′-²H₄]C₂₀BAS, and [10′,11′-²H₂]C₂₀BAS—combined with protiated 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC), as well as membranes containing POPC-d₃₁ and fully protiated bolalipid, were used in NMR experiments to obtain structural information for the mixtures. The ²H NMR spectra of [10′,11′-²H₂]C₂₀BAS/POPC membrane dispersions reveal that the bolalipid is predominantly in the transmembrane conformation at high bolalipid concentrations (100, 90, and 70 mol %). At ≤50 mol % C₂₀BAS, smaller quadrupolar couplings appear in the spectra, indicating the presence of U-shaped conformers. The proportion of U-shaped bolalipids increases as the amount of POPC in the membrane increases; however, the transmembrane component remains the dominant bolalipid conformation in the membrane even at 45°C and 10 mol % C₂₀BAS, where it accounts for ∼50% of the bolalipid population. The large fraction of C₂₀BAS transmembrane conformers, regardless of the C₂₀BAS/POPC ratio, together with the findings from molecular mean-field theory calculations, suggests the coexistence of phase-separated bolalipid-rich domains and POPC-rich domains. A single lamellar repeat distance was observed in SAXS experiments corresponding to the average repeat spacing expected for C₂₀BAS- and POPC-rich domains. These observations are consistent with the presence of microphase-separated domains in the mixed membrane samples that arise from POPC-C₂₀BAS hydrophobic mismatch.     

Lipid-Linked Oligosaccharides in Membranes Sample Conformations That Facilitate Binding to Oligosaccharyltransferase

Lipid-linked oligosaccharides (LLOs) are the substrates of oligosaccharyltransferase (OST), the enzyme that catalyzes the en bloc transfer of the oligosaccharide onto the acceptor asparagine of nascent proteins during the process of N-glycosylation. To explore LLOs’ preferred location, orientation, structure, and dynamics in membrane bilayers of three different lipid types (dilauroylphosphatidylcholine, dimyristoylphosphatidylcholine, and dioleoylphosphatidylcholine), we have modeled and simulated both eukaryotic (Glc₃-Man₉-GlcNAc₂-PP-Dolichol) and bacterial (Glc₁-GalNAc₅-Bac₁-PP-Undecaprenol) LLOs, which are composed of an isoprenoid moiety and an oligosaccharide, linked by pyrophosphate. The simulations show no strong impact of different bilayer hydrophobic thicknesses on the overall orientation, structure, and dynamics of the isoprenoid moiety and the oligosaccharide. The pyrophosphate group stays in the bilayer head group region. The isoprenoid moiety shows high flexibility inside the bilayer hydrophobic core, suggesting its potential role as a tentacle to search for OST. The oligosaccharide conformation and dynamics are similar to those in solution, but there are preferred interactions between the oligosaccharide and the bilayer interface, which leads to LLO sugar orientations parallel to the bilayer surface. Molecular docking of the bacterial LLO to a bacterial OST suggests that such orientations can enhance binding of LLOs to OST.     

Lipid-Linked Oligosaccharides in Membranes Sample Conformations That Facilitate Binding to Oligosaccharyltransferase

Lipid-linked oligosaccharides (LLOs) are the substrates of oligosaccharyltransferase (OST), the enzyme that catalyzes the en bloc transfer of the oligosaccharide onto the acceptor asparagine of nascent proteins during the process of N-glycosylation. To explore LLOs’ preferred location, orientation, structure, and dynamics in membrane bilayers of three different lipid types (dilauroylphosphatidylcholine, dimyristoylphosphatidylcholine, and dioleoylphosphatidylcholine), we have modeled and simulated both eukaryotic (Glc₃-Man₉-GlcNAc₂-PP-Dolichol) and bacterial (Glc₁-GalNAc₅-Bac₁-PP-Undecaprenol) LLOs, which are composed of an isoprenoid moiety and an oligosaccharide, linked by pyrophosphate. The simulations show no strong impact of different bilayer hydrophobic thicknesses on the overall orientation, structure, and dynamics of the isoprenoid moiety and the oligosaccharide. The pyrophosphate group stays in the bilayer head group region. The isoprenoid moiety shows high flexibility inside the bilayer hydrophobic core, suggesting its potential role as a tentacle to search for OST. The oligosaccharide conformation and dynamics are similar to those in solution, but there are preferred interactions between the oligosaccharide and the bilayer interface, which leads to LLO sugar orientations parallel to the bilayer surface. Molecular docking of the bacterial LLO to a bacterial OST suggests that such orientations can enhance binding of LLOs to OST.     

NMR structure of a parallel-stranded DNA duplex at atomic resolution

DNA dodecamers have been designed with two cytosines on each end and intervening A and T stretches, such that the oligomers have fully complementary A:T base pairs when aligned in the parallel orientation. Spectroscopic (UV, CD and IR), NMR and molecular dynamics studies have shown that oligomers having the sequences d(CCATAATTTACC) and d(CCTATTAAATCC) form a parallel-stranded duplex when dissolved at 1:1 stoichiometry in aqueous solution. This is due to the C:C⁺ clamps on either end and extensive mismatches in the antiparallel orientation. The structure is stable at neutral and acidic pH. At higher temperatures, the duplex melts into single strands in a highly cooperative fashion. All adenine, cytosine and thymine nucleotides adopt the anti conformation with respect to the glycosidic bond. The A:T base pairs form reverse Watson–Crick base pairs. The duplex shows base stacking and NOEs between the base protons T(H6)/A(H8) and the sugar protons (H1′/H2′/H2″) of the preceding nucleotide, as has been observed in antiparallel duplexes. However, no NOEs are observed between base protons H2/H6/H8 of sequential nucleotides, though such NOEs are observed between T(CH₃) and A(H8). A three-dimensional structure of the parallel-stranded duplex at atomic resolution has been obtained using molecular dynamics simulations under NMR constraints. The simulated structures have torsional angles very similar to those found in B-DNA duplexes, but the base stacking and helicoid parameters are significantly different.     

Membrane interface composition drives the structure and the tilt of the single transmembrane helix protein PMP1: MD studies

PMP1, a regulatory subunit of the yeast plasma membrane H⁺-ATPase, is a single transmembrane helix protein. Its cytoplasmic C-terminus possesses several positively charged residues and interacts with phosphatidylserine lipids as shown through both ¹H- and ²H-NMR experiments. We used all-atom molecular dynamics simulations to obtain atomic-scale data on the effects of membrane interface lipid composition on PMP1 structure and tilt. PMP1 was embedded in two hydrated bilayers, differing in the composition of the interfacial region. The neutral bilayer is composed of POPC (1-palmitoyl-2-oleoyl-3-glycero-phosphatidylcholine) lipids and the negatively charged bilayer is composed of POPC and anionic POPS (1-palmitoyl-2-oleoyl-3-glycero-phosphatidylserine) lipids. Our results were consistent with NMR data obtained previously, such as a lipid sn-2 chain lying on the W28 aromatic ring and in the groove formed on one side of the PMP1 helix. In pure POPC, the transmembrane helix is two residues longer than the initial structure and the helix tilt remains constant at 6 ± 3°. By contrast, in mixed POPC-POPS, the initial helical structure of PMP1 is stable throughout the simulation time even though the C-terminal residues interact strongly with POPS headgroups, leading to a significant increase of the helix tilt within the membrane to 20 ± 5°.     

Membrane interactions and dynamics of a 21-mer cytotoxic peptide: A solid-state NMR study

We have investigated the membrane interactions and dynamics of a 21-mer cytotoxic model peptide that acts as an ion channel by solid-state NMR spectroscopy. To shed light on its mechanism of membrane perturbation, ³¹P and ²H NMR experiments were performed on 21-mer peptide-containing bicelles. ³¹P NMR results indicate that the 21-mer peptide stabilizes the bicelle structure and orientation in the magnetic field and perturbs the lipid polar head group conformation. On the other hand, ²H NMR spectra reveal that the 21-mer peptide orders the lipid acyl chains upon binding. ¹⁵N NMR experiments performed in DMPC bilayers stacked between glass plates also reveal that the 21-mer peptide remains at the bilayer surface. ¹⁵N NMR experiments in perpendicular DMPC bicelles indicate that the 21-mer peptide does not show a circular orientational distribution in the bicelle planar region. Finally, ¹³C NMR experiments were used to study the 21-mer peptide dynamics in DMPC multilamellar vesicles. By analyzing the ¹³CO spinning sidebands, the results show that the 21-mer peptide is immobilized upon membrane binding. In light of these results, we propose a model of membrane interaction for the 21-mer peptide where it lies at the bilayer surface and perturbs the lipid head group conformation.