Conformational energy studies on N-methylated analogs of thyrotropin releasing hormone, enkephalin, and luteinizing hormone-releasing hormone

Empirical conformational energy calculations have been carried out for N-methyl derivatives of alanine and phenylalanine dipeptide models and N-methyl-substituted active analogs of three biologically active peptides, namely thyrotropin-releasing hormone (TRH), enkephalin (ENK), and luteinizing hormone-releasing hormone (LHRH). The isoenergetic contour maps and the local dipeptide minima obtained, when the peptide bond (ω) preceding the N-methylated residue is in the trans configuration show that (1) N-methylation constricts the conformational freedom of both the ith and (i + 1)th residues; (2), the lowest energy position for both residues occurs around ? = ?135° ± 5° and ψ = 75° ± 5°, and (3) the α_L conformational state is the second lowest energy state for the (i + 1)th residue, whereas for the ith residue the C₅ (extended) conformation is second lowest in energy. When the peptide bond (ω_i) is in the cis configuration the ith residue is energetically forbidden in the range ? = 0° to 180° and ψ = ?180° to +180°. Conformations of low energy for ω_i = 0° are found to be similar to those obtained for the trans peptide bond. In all the model systems (irrespective of cis or trans), the α_R conformational state is energetically very high. Significant deviations from planarity are found for the peptide bond when the amide hydrogen is replaced by a methyl group. Two low-energy conformers are found for [(N-Me)His²]TRH. These conformers differ only in the ? and ψ values at the (N-Me)His² residue. Among the different low-energy conformers found for each of the ENK analogs [D -Ala²,(N-Me)Phe⁴, Met⁵]ENK amide and [D -Ala²,(N-Me)Met⁵]ENK amide, one low-energy conformer was found to be common for both analogs with respect to the side-chain orientations. The stability of the low-energy structures is discussed in the light of the activity of other analogs. Two low-energy conformers were found for [(N-Me)Leu⁷]LHRH. These conformations differ in the types of bend around the positions 6 and 7 of LHRH. One bend type is eliminated when the active analog [D -Ala⁶,(M-Me)Leu⁷]LHRH is considered.     

Peptide-bond distortions and the curvature of alpha-helices

Solvent accessible peptide bonds in proteins exhibit a 1–3° compression of the OCN bond angle and a corresponding expansion of the NCCa bond angle, relative to buried peptide bonds. These changes are consistent with an increase in hydrogen bonding to the carbonyl oxygen accompanying solvent exposure (J. D. Dunitz and F. K. Winkler, (1975) Acta Cryst. B31 , 251–263). For amphiphilic structures such as α-helices, systematic differences in peptide-bond geometry between solvent-exposed and buried residues will generate significant curvature. A decrease of 4° in the OCN bond angle between hydrophilic and hydrophobic sides of an amphiphilic helix will lead to smooth bending, with a radius of curvature of about 70 Å. This curvature is in the range observed for α-helices in proteins. Helix curvature is estimated to have only a small effect on the magnitude and direction of the helical dipole moment.     

Crystal structure of cyclo(Pro-Gly)3: Li complex: A model for ion transport by cyclo(Pro-Gly)3

The crystal structure of cyclo(Pro-Gly)₃ (PG3) complex with LiSCN (C₂₂H₃₀N₇O₆SLi) has been solved by x-ray diffraction. The crystals belong to the space group R3 in the hexagonal setting with unit cell parameters of a = 12.581(1), c = 29.705(3) Å, V = 4072.0 ų, Z = 6, M_r = 527.53, D_c = 1.23 g/cm³. The crystal structure was solved by direct methods using the program SHELXS-86 and refined to an R value of 5.3% for 1645 reflections (I > 2σI). There are two conformers in the crystal structure. One conformer has three carbonyls on one side and three on the other side of the peptide plane. The other conformer has all six of the carbonyls on the same side of the peptide plane. Both of these conformers bind independently to a Li ion. Based on the conformers of the Li complex and other reported ion complexes formed by PG3, we propose a model for the transport of ions across the lipid membrane. The features of the model are as follows: (1) PG3 forms a hexameric stack in a lipid bilayer when complexing and transporting metal ions. (2) It undergoes a conformational flipping in order pass the ion along the channel. The energy required for the conformational change involved in the flipping of the PG3 molecule may be provided by the applied potential during ion transport. © 1994 John Wiley & Sons, Inc.     

Depth of α-synuclein in a bilayer determined by fluorescence, neutron reflectometry, and computation

α-Synuclein (α-syn) membrane interactions are implicated in the pathogenesis of Parkinson's disease. Fluorescence and neutron reflectometry (NR) measurements reveal that α-syn penetrates ～9–14 Å into the outer leaflet of the bilayer, with a substantial portion of the membrane-bound polypeptide extending into the aqueous solvent. For the first time, to our knowledge, we used NR to obtain direct quantitative evidence of α-syn-induced membrane thinning. To examine the effect of specific residues on membrane penetration depths, we used a series of W4-containing N-terminal peptides. We identified that the first 15 residues (P15) nearly recapitulate the features of the full-length protein (i.e., partition constants, molecular mobility, and insertion of the W4 side chain into the bilayer), and found that as few as the first four N-terminal residues are sufficient for vesicle binding. Although at least one imperfect amphipathic repeat sequence (KAKEGV) is required for α-helical formation, secondary structural formation has little effect on membrane affinity. To develop an N-terminal α-syn model for bilayer interactions, we performed molecular-dynamics simulations of the P15 peptide submerged in a bilayer. The simulation results are highly consistent with experimental data indicating a broad low-energy region (8.5–14.5 Å) for W4 insertion.     

Chain length dependent transition of 310- to α-helix of Boc-(Ala-Aib)n-OMe

An apolar synthetic octapeptide, Boc-(Ala-Aib)₄-OMe, was crystallized in the triclinic space group P1 with cell dimensions a = 11.558 Å, b = 11.643 Å, c = 9.650 Å, α = 120.220°, β = 107.000°, γ = 90.430°, V = 1055.889 ų, Z = 1, C₃₄H₆₀O₁₁N₈·H₂O. The calculated crystal density was 1.217 g/cm³ and the absorption coefficient ? was 6.1. All the intrahelical hydrogen bonds are of the 3₁₀ type, but the torsion angles, ? and ψ, of Ala(5) and Ala(7) deviate from the standard values. The distortion of the 3₁₀-helix at the C-terminal half is due to accommodation of the bulky Boc group of an adjacent peptide in the nacking. A water molecule is held between the N-terminal of one peptide and the C-terminal of the other. The oxygen atom of water forms hydrogen bonds with N (1) -H and N (2) -H, which are not involved in the intrahelical hydrogen bonds. The hydrogen atoms of water also formed hydrogen bonds with carbonyl oxygens of the adjacent peptide molecule. On the other hand, ¹H-nmr analysis revealed that the octapeptide took an α-helical structure in a CD₃CN solution. The longer peptides, Boc-(Ala-Aib)₆-OMe and Boc-(Ala-Aib)₈-OMe, were also shown to take an α-helical structure in a CD₃CN solution. An α-helical conformation of the hexadecapeptide in the solid state was suggested by x-ray analysis of the crystalline structure. Thus, the critical length for transition from the 3₁₀- to α-helix of Boc-(Ala-Aib)_n-OMe is 8. © 1993 John Wiley & Sons, Inc.     

Crystal structures of two cyclic pseudopentapeptides containing ψ[CH2S] and ψ[CH2SO] backbone surrogates

The solid state conformations of cyclo[Gly–Proψ[CH₂S]Gly–D –Phe–Pro] and cyclo[Gly–Proψ[CH₂–(S)–SO]Gly–D –Phe–Pro] have been characterized by X-ray diffraction analysis. Crystals of the sulfide trihydrate are orthorhombic, P2₁2₁2₁, with a = 10.156(3) Å, b = 11.704(3) Å, c = 21.913(4) Å, and Z = 4. Crystals of the sulfoxide are monoclinic, P2₁, with a = 10.662(1) Å, b = 8.552(3) Å, c = 12.947(2) Å, β = 94.28(2), and Z = 2. Unlike their all-amide parent, which adopts an all-trans backbone conformation and a type II β-turn encompassing Gly-Pro-Gly-D -Phe, both of these peptides contain a cis Gly¹-Pro² bond and form a novel turn structure, i.e., a type II′ β-turn consisting of Gly–D –Phe–Pro–Gly. The turn structure in each of these peptides is stabilized by an intramolecular H bond between the carbonyl oxygen of Gly¹ and the amide proton of D -Phe⁴. In the cyclic sulfoxide, the sulfinyl group is not involved in H bonding despite its strong potential as a hydrogen-bond acceptor. The crystal structure made it possible to establish the absolute configuration of the sulfinyl group in this peptide. The two crystal structures also helped identify a type II′ β-turn in the DMSO-d₆ solution conformers of these peptides. © 1993 John Wiley & Sons, Inc.     

Channel‐like crystal structure of cinchoninium L‐O‐phosphoserine salt dihydrate

Studies on the interactions between L ‐O‐ phosphoserine, as one of the simplest fragments of membrane components, and the Cinchona alkaloid cinchonine, in the crystalline state were performed. Cinchoninium L ‐O‐phosposerine salt dihydrate (PhSerCin) crystallizes in a monoclinic crystal system, space group P2₁, with unit cell parameters: a = 8.45400(10) Å, b = 7.17100(10) Å, c = 20.7760(4) Å, α = 90°, β = 98.7830(10)°, γ = 90°, Z = 2. The asymmetric unit consists of the cinchoninium cation linked by hydrogen bonds to a phosphoserine anion and two water molecules. Intermolecular hydrogen bonds connecting phosphoserine anions via water molecules form chains extended along the b axis. Two such chains symmetrically related by twofold screw axis create a “channel.” On both sides of this channel cinchonine cations are attached by hydrogen bonds in which the atoms N1, O12, and water molecules participate. This arrangement mimics the system of bilayer biological membrane. Chirality 2010. © 2009 Wiley‐Liss, Inc.     

Experimental conformational study of two peptides containing α-aminoisobutyric acid. Crystal structure of N-acetyl-α-aminoisobutyric acid methylamide

Some theoretical studies have predicted that the conformational freedom of the α-aminoisobutyric acid (H-Aib-OH) residue is restricted to the α-helical region of the Ramachandran map. In order to obtain conformational experimental data, two model peptide derivatives, MeCO-Aib-NHMe 1 and Bu^tCO-LPro-Aib-NHMe 2 , have been investigated. The Aib dipeptide 1 crystallizes in the monoclinic system (a = 12.71 Å, b = 10.19 Å, c = 7.29 Å, β = 110.02°, Cc space group) and its crystal structure was elucidated by x-ray diffraction analysis. The azimuthal angles depicting the molecular conformation (? = ?55.5°, ψ = ?39.3°) fall in the α-helical region of the Ramachandran map and molecules are hydrogen-bonded in a three-dimensional network. In CCl₄ solution, ir spectroscopy provides evidence for the occurrence of the so-called ₅ and C₇ conformers stabilized by the intramolecular i → i and i + 2 → i hydrogen bonds, respectively. The tripeptide 2 was studied in various solvents [CCl₄, CD₂Cl₂, CDCl₃, (CD₃)₂SO, and D₂O] by ir and pmr spectroscopies. It was shown to accommodate predominantly the βII folded state stabilized by the i + 3 → i hydrogen bond. All these experimental findings indicate that the Aib residue displays the same conformational behavior as the other natural chiral amino acid residues.     

Effect of glycophorin on lipid polymorphism: A 31P-NMR study

(1) The effect of glycophorin, a major intrinsic glycoprotein of the human erythrocyte membrane, on lipid polymorphism has been investigated by ³¹P-NMR (at 36.4 MHz) and by freeze-fracture electron microscopy. (2) Incorporation of glycophorin into vesicles of 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC) results in the formation of unilamellar vesicles (1000–5000 Å diameter) which exhibit ³¹P-NMR bilayer spectra over a wide range of temperature. A reduction in the chemical shift anisotropy (Δσ_csa^eff) and an increase in spectral linewidth in comparison to dioleoylphosphatidylcholine liposomes may suggest a decrease in phospholipid headgroup order. (3) 1,2-Dioleoyl-sn-glycero-3-phosphoethanolamine (DOPE), in the presence of excess water, undergoes a bilayer to hexagonal (H_II) phospholipid arrangement as the temperature is increased above 0°C. Incorporation of glycophorin into this system stabilizes the bilayer configuration, prohibiting the formation of the H_II phase. (4) Cosonication of glycophorin with DOPE in aqueous solution (pH 7.4) produces small, stable unilamellar vesicles (300–1000 Å diameter), unlike DOPE alone which is unstable and precipitates from solution. (5) The current study demonstrates the bilayer stabilizing capacity of an intrinsic membrane protein, glycophorin, most likely by means of a strong hydrophobic interaction between the membrane spanning portion of glycophorin and the hydrophobic region of the phospholipid.     

Interaction of an Amphiphilic Peptide with a Phospholipid Bilayer Surface by Molecular Dynamics Simulation Study

Abstract

Corticotropin-releasing factor (CRF) is the principal neuroregulator of adrenocorticotropic hormone (ACTH) secretion. Previous experiments have demonstrated that CRF binds avidly to the surface of single egg phosphatidylcholine vesicles and its amphiphilic secondary structure might play an important role in the function. In this study, the interaction of the residues 13–41 in human CRF with the surface of a DOPC bilayer was investigated by molecular dynamics (MD) simulation in order to understand the role of the membrane surface in the formation of the amphiphilic α helix as well as to determine the effects of the peptide on the lipid bilayer. The model used included 60 DOPC molecules, 1 helical peptide (CRF_13–41) on the bilayer surface, and explicit waters of solvation in the lipid polar head group regions, together with constant-volume periodic boundary conditions in three dimensions. The MD simulation was carried out for 510 ps. In addition, CRF_13–41, initially in a helical form, was simulated in vacuo as a control. The results indicate that while it was completely unstable in vacuo, the peptide helical form was generally maintained on the bilayer surface, but with distortions near the terminal ends. The peptide was confined to the bilayer headgroup/water region, similar to that reported from neutron diffraction measurement of tripeptides bound to the phosphatidylcholine bilayer surface (Ref 1). The amphiphilicity of the peptide matched that of the bilayer headgroup environment, with the hydrophilic side oriented toward water and the hydrophobic side making contact with the bilayer hydrocarbon core. These results support the hypothesis that the amphiphilic environment of a membrane surface is important in the induction of peptide amphiphilic α-helical secondary structure. Two major effects of the peptide on the lipids were found: the first CH₂ segment in the lipid chains was significantly disordered and the lipid headgroup distribution was broadened towards the water region.     

A fluorescence and CD study on the interaction of synthetic lipophilic hepatitis B virus preS(120–145) peptide analogues with phospholipid vesicles

The interaction of the immunogenic peptide of human hepatitis B virus (HBV) preS(120–145), including B and T epitopes, with phospholipid vesicles has been studied by fluorescence techniques and CD. In addition, interaction of three lipopeptides derived from preS(120–145) containing stearoyl, cholanoyl, and tripalmitoyl-S-glyceryl-cysteine (Pam₃C) SS moieties with dipalmitoylphosphatidylcholine (DPPC) has been investigated by polarization fluorescence spectroscopy. Fluorescence experiments showed an increase in fluorescence intensity and a blue shift of the maximum emission wavelength upon interaction of preS(120–145) with DPPC vesicles below the transition temperature (T_c), indicating that the tryptophan moiety enters a more hydrophobic environment. Moreover, fluorescence polarization experiments showed that the peptide decreased the membrane fluidity at the hydrophobic core, increasing the T_c of the lipid and decreasing the amplitude of the change of fluorescence polarization associated with the cooperative melting of 1,6-diphenyl-1,3,5-hexatriene labeled vesicles. The absence of leakage of vesicle-entrapped carboxyfluorescein indicates that the peptide did not promote vesicle lysis. Besides, the three lipopeptides derived from preS(120–145) showed a more pronounced rigidifying effect at the hydrophobic core of the bilayer, with a significative increase in the T_c. Stearoyl- and cholanoyl-preS(120–145) restricted the motion of lipids also at the polar surface, whereas Pam₃CSS-preS(120–145) did not alter the polar head group order. Finally, CD studies in 2,2,2-triflouroethanol or in presence of vesicles suggested that the bound peptide adopted amphiphilic α-helical and β-sheet structures, with an important contribution of the β-turn. It is concluded that preS(120–145) can interact with the lipid membrane through the formation of an amphipathic structure combination of β-sheet and α-helix aligned parallel to the membrane surface, involving the N-terminal residues, and penetrating only a short distance into the hydrophobic core. The C-terminal part, with a combination of β-turn and β-sheet structure, remains at the outer part of the bilayer, being potentially accessible to immunocompetent cells. Furthermore, coupling of an hydrophobic moiety to the N-terminal part of the peptide favors anchoring to the membrane, probably facilitating interaction of the peptide with the immunoglobulin receptor. These results are in agreement with the induction of immune response by preS(120–145) and with the enhanced immunogenicity found in general for lipid-conjugated immunopeptides. © 1996 John Wiley & Sons, Inc.     

Crystallization and preliminary crystallographic study of the pentamerizing domain from cartilage oligomeric matrix protein: A five-stranded α-helical bundle

Cartilage oligomeric matrix protein (COMP) is a pentameric glycoprotein of the thrombospondin family found in cartilage and tendon. Self-association of COMP is achieved through the formation of a five-stranded α-helical bundle that involves 64 N-terminal residues (from 20 to 83). The complex is further stabilized by the interchain disulfide bonds between cysteines 68 and 71. We have prepared, by expression in Escherichia coli, several peptides of different lengths from the N-terminal region of COMP and studied their amenability to crystallization. Crystals of the best quality were obtained with a peptide spanning COMP residues 28–72. This peptide forms disulfide linked pentamers with 87% of α-helical structure. Crystals were grown by the hanging drop vapor diffusion method, using polyethylene glycol 1500 as a precipitant. The crystals belong to space group P2₁ with unit cell dimensions a = 38.47 Å, b = 49.47 Å, c = 54.98 Å, β = 103.84° and contain one pentamer per asymmetric unit. They diffract strongly to at least 1.8 Å resolution.     

Effects of End Group and Aggregation on Helix Conformation: Crystal Structure of Ac-(Aib-Val-Ala-Leu)2-Aib- OMe

The role of end groups in determining stereochemistry and packing in hydrophobic helical peptides has been investigated using an α-aminosobutyric acid (Aib) containing model nonapeptide sequence. In contrast to the Boc-analogue, Ac-(Aib-Val-Ala-Leu)₂-Aib-OMe crystallizes with two independent molecules in a triclinic cell. The cell parameters are: space group P1, a=10.100(2)Å, b=15.194(4) Å, c=19.948(5) Å, α=63.12(2)°, β=88.03(2)°, γ=88.61(2)°, Z=2, R=7.96% for 5140 data where |F_o|>3σ(F). The two independent molecules alternate in infinite columns formed by head-to-tail hydrogen bonding. The helices in the two independent molecules are quite similar to each other but one molecule is rotated ≈?123° about its helix axis with respect to the other. All the helical columns pack parallel to each other in the crystal. Replacement of the bulky Boc group does not lead to any major changes in conformation. Packing characteristics are also similar to those observed for similar helical peptides.     

Structure of cytochrome c oxidase in deoxycholate-drived two-dimensional crystals.

The structure of the two-dimensional crystals of cytochrome oxidase prepared with deoxycholate has been investigated. The crystals have space group p12₁ and contain a monomer (two heme-two copper complex) in the asymmetric unit. They are in the form of sheets and contain no continuous bilayer; the entire surface of the molecule seems to be visible in negatively stained samples. The monomer is roughly 110 Å long and resembles a lopsided “Y”. The domains which form the arms of the Y are 55 Å in length and have a center to center separation of 40 Å. These domains are on the matrix side of the molecule and are thought to be buried in the bilayer of the inner mitochondrial membrane. The cytoplasmic side of the molecule is composed of the single large domain which is the stem of the Y. The overall structure matches that of cytochrome oxidase seen in the p22₁2₁ crystals derived by Triton X100 treatment of mitochondria.     

Observation of a sterically unfavorable side-chain conformation in a leucyl residue: Crystal and molecular structure of L-leucyl–L-leucine · DMSO solvate

The crystal structure of a dipeptide L -leucyl–L -leucine (C₁₂H₂₄N₂O₃) has been determined. The crystals are monoclinic, space group P2₁, with a = 5.434(4) Å, b = 15.712(7) Å, c = 11.275(2) Å, β = 100.41(1)°, and Z = 2. The crystals contain one molecule of dimethyl sulfoxide (DMSO) as solvent of crystallization for each dipeptide molecule. The structure has been solved by direct methods and refined to a final R index of 0.059 for 920 reflections (sinθ/λ ? 0.60 Å^?1) with I ? 2σ (I). The trans peptide unit shows substantial degree of non-planarity (Δω = 14°). The peptide backbone adopts an extended conformation with torsion angles of ψ₁ = 138(1)°, ω₁ = 166(1)°, ?₂ = ? 149.3(7)°, ψ₂₁ = 164.2(7)°, and ψ₂₂ = ? 15(1)°. For the first leucyl residue, the side-chain conformation is specified by the torsion angles ¹χ₁ = 176.7(7)°, ¹χ₂₁ = 62(1)°, ¹χ₂₂ = ? 177.4(8)°; the second leucyl residue adopts a Sterically unfavorable conformation with ²χ₁ = 61(1)°, ²χ₂₁ = 97(1)°, and ²χ₂₂ = ?151(1)°. The packing involves head-to-tail interaction of peptide molecules and segregation of polar and nonpolar regions. The DMSO molecule is strongly hydrogen bonded to the terminal NH group. © 1994 John Wiley & Sons, Inc.     

Determining the helical tilt angle and dynamic properties of the transmembrane domains of pinholin S2168 using mechanical alignment EPR spectroscopy

The lytic cycle of bacteriophage φ21 for the infected E. coli is initiated by pinholin S²¹, which determines the timing of host cell lysis through the function of pinholin (S²¹68) and antipinholin (S²¹71). The activity of pinholin or antipinholin directly depends on the function of two transmembrane domains (TMDs) within the membrane. For active pinholin, TMD1 externalizes and lies on the surface while TMD2 remains incorporated inside the membrane forming the lining of the small pinhole. In this study, spin labeled pinholin TMDs were incorporated separately into mechanically aligned POPC (1-palmitoyl-2-oleoyl-glycero-3-phosphocholine) lipid bilayers and investigated with electron paramagnetic resonance (EPR) spectroscopy to determine the topology of both TMD1 and TMD2 with respect to the lipid bilayer; the TOAC (2,2,6,6-tetramethyl-N-oxyl-4-amino-4-carboxylic acid) spin label was used here because it attaches to the backbone of a peptide and is very rigid. TMD2 was found to be nearly colinear with the bilayer normal (n) with a helical tilt angle of 16 ± 4° while TMD1 lies on or near the surface with a helical tilt angle of 84 ± 4°. The order parameters (~0.6 for both TMDs) obtained from our alignment study were reasonable, which indicates the samples incorporated inside the membrane were well aligned with respect to the magnetic field (B₀). The data obtained from this study supports previous findings on pinholin: TMD1 partially externalizes from the lipid bilayer and interacts with the membrane surface, whereas TMD2 remains buried in the lipid bilayer in the active conformation of pinholin S²¹68. In this study, the helical tilt angle of TMD1 was measured for the first time. For TMD2 our experimental data corroborates the findings of the previously reported helical tilt angle by the Ulrich group.     

Modeling of Peptides in Implicit Membrane-Mimetic Media

Abstract

Lipid bilayer plays a crucial role in folding of membrane peptides and their stabilization in the membrane-bound state. Correct treatment of the media effects is thus essential for realistic simulations of peptides in bilayers. Previously (Volynsky et al., 1999), we proposed an efficient solvation model which mimics heterogeneous membrane-water system. The model is based on combined employment of atomic solvation parameters for water and hydrocarbon, which approximate hydrated headgroups and acyl chains of lipids, respectively. In this study, the model is employed in non-restrained Monte Carlo simulations of several peptides: totally apolar 20-residue poly-L-Leu, hydrophobic peptide with polar edges, and strongly amphiphilic pep-tide. The principal goals are: to explore energy landscape of these peptides in membrane; to characterize the structures of low-energy states and their orientations with respect to the bilayer. Simulations were performed starting from different structures (unordered or helical) and orientations. It was found that the membrane environment significantly promotes an α-helical conformation for all the peptides, while their energetically favourable orientations are quite different. Thus, poly-Leu was immobilized inside the membrane, the hydrophobic peptide with polar termini adapted transbilayer orientation, whereas the amphiphilic peptide stayed on the lipid-water interface in peripherial orientation. Energy barriers between different states were characterized. The computational results were compared with the experimental structural data.     

Atomistic mechanisms of huntingtin N‐terminal fragment insertion on a phospholipid bilayer revealed by molecular dynamics simulations

The huntingtin protein is characterized by a segment of consecutive glutamines (Q_N) that is responsible for its fibrillation. As with other amyloid proteins, misfolding of huntingtin is related to Huntington's disease through pathways that can involve interactions with phospholipid membranes. Experimental results suggest that the N‐terminal 17‐amino‐acid sequence (htt^NT) positioned just before the Q_N region is important for the binding of huntingtin to membranes. Through all‐atom explicit solvent molecular dynamics simulations, we unveil the structure and dynamics of the htt^NTQ_N fragment on a phospholipid membrane at the atomic level. We observe that the insertion dynamics of this peptide can be described by four main steps—approach, reorganization, anchoring, and insertion—that are very diverse at the atomic level. On the membrane, the htt^NT peptide forms a stable α‐helix essentially parallel to the membrane with its nonpolar side‐chains—mainly Leu‐4, Leu‐7, Phe‐11 and Leu‐14—positioned in the hydrophobic core of the membrane. Salt‐bridges involving Glu‐5, Glu‐12, Lys‐6, and Lys‐15, as well as hydrogen bonds involving Thr‐3 and Ser‐13 with the phospholipids also stabilize the structure and orientation of the htt^NT peptide. These observations do not significantly change upon adding the Q_N region whose role is rather to provide, through its hydrogen bonds with the phospholipids' head group, a stable scaffold facilitating the partitioning of the htt^NT region in the membrane. Moreover, by staying accessible to the solvent, the amyloidogenic Q_N region could also play a key role for the oligomerization of htt^NTQ_N on phospholipid membranes. Proteins 2014; 82:1409–1427. © 2014 Wiley Periodicals, Inc.     

Rab7: Crystallization of intact and C-terminal truncated constructs complexed with GDP and GppNHp

The GTP/GDP conformational switch of members of the rab family of ras-related GTP-ases control specific intracellular vesicle transport pathways. We report the crystallization of the late-endosomal rab protein rab7, in both GTP and GDP conformations. X-ray data from crystals of rab7_1–207GppNHp (i.e., intact rab7, without C-terminal bound lipid, complexed with a non-hydrolysable GTP analog), rab7_1–197GppNHp and rab7_1–197GDP were collected to 1.9Å (0°C), 1.76Å (100°K) and 1.75Å (100°K) respectively. Rab7-GDP crystals diffract to at least 1.35Å. © 1997 Wiley-Liss, Inc.     

Dioxo-, oxothio- and dithio-tungsten(VI) and tungsten(V) complexes of the ligand N,N′-Dimethyl-N,N′-bis(2-mercaptophenyl)ethylenediamine

Synthesis of complexes cis,cis-W^VOXL (X=Cl, NCS), cis,trans-W^VOXL (X=Cl, OPh, SPh) and cis,trans-W^VIE₂L (E₂=O₂, OS, S₂) of the title ligand LH₂ are reported. cis,cis-W^VOCIL crystallises in space group P2₁/c with a=13.6541(9) Å, b=7.1555(11) Å, c=18.198(2) Å, β=95.294(6)°, V=1770.4(3) ų and Z=4 while the cis,trans isomer crystallises in space group P2₁/n with a=10.361(3) Å, b=14.141(4) Å, c=12.213(5) Å, β=102.56(3)°, V=1747(2) ų and Z=4. cis,trans-W^VIS₂L crystallises in space group P2₁/n with a=10.645(2) Å, b=13.929(2) Å, c=12.189(2) Å, β=103.14(2)°, V=1760(1) ų and Z=4. A short CH₃···Cl distance of 3.067(7) Å and an acute OWCl angle of 94.1(2)° are seen in cis,cis-W^VOClL, which converts to the cis,trans form on heating in MeCN. The latter isomer features a CH₃···Cl distance of 3.38(2) Å and an OWCl angle of 105.1(8)°. Electrochemical and EPR data are reported. In particular, cis,trans-W^VIE₂L may be reduced to [W^VE₂L]^–. EPR properties of these anions and those of complexes W^VOXL are discussed in the context of W^V centres in tungsten enzymes.