Structure and dynamics of micelle-bound human alpha-synuclein

Misfolding of the protein alpha-synuclein (aS), which associates with presynaptic vesicles, has been implicated in the molecular chain of events leading to Parkinson's disease. Here, the structure and dynamics of micelle-bound aS are reported. Val3-Val37 and Lys45-Thr92 form curved alpha-helices, connected by a well ordered, extended linker in an unexpected anti-parallel arrangement, followed by another short extended region (Gly93-Lys97), overlapping the recently identified chaperone-mediated autophagy recognition motif and a highly mobile tail (Asp98-Ala140). Helix curvature is significantly less than predicted based on the native micelle shape, indicating a deformation of the micelle by aS. Structural and dynamic parameters show a reduced helical content for Ala30-Val37. A dynamic variation in interhelical distance on the microsecond timescale is complemented by enhanced sub-nanosecond timescale dynamics, particularly in the remarkably glycine-rich segments of the helices. These unusually rich dynamics may serve to mitigate the effect of aS binding on membrane fluidity. The well ordered conformation of the helix-helix connector indicates a defined interaction with lipidic surfaces, suggesting that, when bound to larger diameter synaptic vesicles, it can act as a switch between this structure and a previously proposed uninterrupted helix.     

Helix periodicity, topology, and dynamics of membrane-associated alpha-synuclein

The protein alpha-Synuclein (aS) is a synaptic vesicle-associated regulator of synaptic strength and dopamine homeostasis with a pathological role in Parkinson's disease. The normal function of aS depends on a membrane-associated conformation that is adopted upon binding to negatively charged lipid surfaces. Previously we found that the membrane-binding domain of aS is helical and suggested that it may exhibit an unusual structural periodicity. Here we present a study of the periodicity, topology, and dynamics of detergent micelle-bound aS using paramagnetic spin labels embedded in the micelle or attached to the protein. We show that the helical region of aS completes three full turns every 11 residues, demonstrating the proposed 11/3 periodicity. We also find that the membrane-binding domain is partially buried in the micelle surface and bends toward the hydrophobic interior, but does not traverse the micelle. Deeper submersion of certain regions within the micelle, including the unique lysine-free sixth 11-residue repeat, is observed and may be functionally important. There are no long-range tertiary contacts within this domain, indicating a highly extended configuration. The backbone dynamics of the micelle-bound region are relatively uniform with a slight decrease in flexibility observed toward the C-terminal end. These results clarify the topological features of aS bound to membrane-mimicking detergent micelles, with implications for aS function and pathology.     

NMR solution structure of the glucagon antagonist [desHis1, desPhe6, Glu9]glucagon amide in the presence of perdeuterated dodecylphosphocholine micelles

Glucagon, a 29-residue peptide hormone, plays an important role in glucose homeostasis and in diabetes mellitus. Several glucagon antagonists and agonists have been developed, but limited structural information is available to clarify the basis of their biological activity. The solution structure of the potent glucagon antagonist, [desHis1, desPhe6, Glu9]glucagon amide, was determined by homonuclear 2D NMR spectroscopy at pH 6.0 and 37 degrees C in perdeuterated dodecylphosphocholine micelles. The overall backbone root-mean-square deviation (rmsd) for the structured portion (residues 7-29, glucagon numbering) of the micelle-bound 27-residue peptide is 1.36 A for the 15 lowest-energy structures, after restrained molecular dynamics simulation. The structure consists of four regions (segment backbone rmsd in A): an unstructured N-terminal segment between residues 2 and 5 (1.68), an irregular helix between residues 7 and 14 (0.79), a hinge region between residues 15 and 18 (0.54), and a well-defined alpha-helix between residues 19 and 29 (0.33). The two helices form an L-shaped structure with an angle of about 90 degrees between the helix axes. There is an extended hydrophobic cluster, which runs along the inner surface of the L-structure and incorporates the side chains of the hydrophobic residues of each of the amphipathic helices. The outer surface contains the hydrophilic side chains, with two salt bridges (D15-R18 and R17-D21) implied from close approach of the charged groups. This result is the first clear indication of an overall tertiary fold for a glucagon analogue in the micelle-bound state. The relationship of the two helical structural elements may have important implications for the biological activity of the glucagon antagonist.     

Effect of Pseudorepeat Rearrangement on α-Synuclein Misfolding, Vesicle Binding, and Micelle Binding

The pathological and physiological hallmarks of the protein α-synuclein (aS) are its misfolding into cytotoxic aggregates and its binding to synaptic vesicles, respectively. Both events are mediated by seven 11-residue amphiphilic pseudorepeats and, most generally, involve a transition from intrinsically unstructured conformations to structured conformations. Based on aS interactions with aggregation-inhibiting small molecules, an aS variant termed shuffled α-synuclein (SaS), wherein the first six pseudorepeats had been rearranged, was introduced. Here, the effects of this rearrangement on misfolding, vesicle binding, and micelle binding are examined in reference to aS and β-synuclein to study the sequence characteristics underlying these processes. Fibrillization correlates with the distinct clustering of residues with high β-sheet propensities, while vesicle affinities depend on the mode of pseudorepeat interchange and loss. In the presence of micelles, the pseudorepeat region of SaS adopts an essentially continuous helix, whereas aS and β-synuclein encounter a distinct helix break, indicating that a more homogeneous distribution of surfactant affinities in SaS prevented the formation of an extensive helix break in the micelle-bound state. By demonstrating the importance of the distribution of β-sheet propensities and by revealing inhomogeneous aS surfactant affinities, the present study provides novel insights into two central themes of synuclein biology.     

Conserved core of amyloid fibrils of wild type and A30P mutant α-synuclein

The major component of neural inclusions that are the pathological hallmark of Parkinson's disease are amyloid fibrils of the protein α-synuclein (aS). Here we investigated if the disease-related mutation A30P not only modulates the kinetics of aS aggregation, but also alters the structure of amyloid fibrils. To this end we optimized the method of quenched hydrogen/deuterium exchange coupled to NMR spectroscopy and performed two-dimensional proton-detected high-resolution magic angle spinning experiments. The combined data indicate that the A30P mutation does not cause changes in the number, location and overall arrangement of β-strands in amyloid fibrils of aS. At the same time, several residues within the fibrillar core retain nano-second dynamics. We conclude that the increased pathogenicity related to the familial A30P mutation is unlikely to be caused by a mutation-induced change in the conformation of aS aggregates.     

Structure and dynamics of micelle-bound neuropeptide Y: comparison with unligated NPY and implications for receptor selection

The biological importance of the neuropeptide Y (NPY) has steered a number of investigations about its solution structure over the last 20 years. Here, we focus on the comparison of the structure and dynamics of NPY free in solution to when bound to a membrane mimetic, dodecylphosphocholine (DPC) micelles, as studied by 2D (1)H NMR spectroscopy. Both, free in solution and in the micelle-bound form, the N-terminal segment (Tyr1-Glu15) is shown to extend like a flexible tail in solution. This is not compatible with the PP-fold model for NPY that postulates backfolding of the flexible N terminus onto the C-terminal helix. The correlation time (tau(c)) of NPY in aqueous solution, 5.5 (+/-1.0) ns at 32 degrees C, is only consistent with its existence in a dimeric form. Exchange contributions especially enhancing transverse relaxation rates (R(2)) of residues located on one side of the C-terminal helix of the molecule are supposed to originate from dimerization of the NPY molecule. The dimerization interface was directly probed by looking at (15)N-labeled NPY/spin-labeled [TOAC34]-[(14)N]-NPY heterodimers and revealed both parallel and anti-parallel alignment of the helices. The NMR-derived three-dimensional structure of micelle-bound NPY at 37 degrees C and pH 6.0 is similar but not identical to that free in solution. The final set of 17 lowest-energy DYANA structures is particularly well defined in the region of residues 21-31, with a mean pairwise RMSD of 0.23 A for the backbone heavy atoms and 0.85 A for all heavy atoms. The combination of NMR relaxation data and CD measurements clearly demonstrates that the alpha-helical region Ala18-Thr32 is more stable, and the C-terminal tetrapeptide becomes structured only in the presence of the phosphocholine micelles. The position of NPY relative to the DPC micelle surface was probed by adding micelle integrating spin labels. Together with information from (1)H,(2)H exchange rates, we conclude that the interaction of NPY with the micelle is promoted by the amphiphilic alpha-helical segment of residues Tyr21-Thr32. NPY is located at the lipid-water interface with its C-terminal helix parallel to the membrane surface and penetrates the hydrophobic interior only via insertions of a few long aliphatic or aromatic side-chains. From these data we can demonstrate that the dimer interface of neuropeptide Y is similar to the interface of the monomer binding to DPC-micelles. We speculate that binding of the NPY monomer to the membrane is an essential key step preceeding receptor binding, thereby pre-orientating the C-terminal tetrapeptide and possibly inducing the bio-active conformation.     

Characterization of conformational and dynamic properties of natively unfolded human and mouse alpha-synuclein ensembles by NMR: implication for aggregation

Conversion of human α-synuclein (aS) from the free soluble state to the insoluble fibrillar state has been implicated in the etiology of Parkinson's disease. Human aS is highly homologous in amino acid sequence to mouse aS, which contains seven substitutions including the A53T that has been linked to familial Parkinson's disease, and including five substitutions in the C-terminal region. It has been shown that the rate of fibrillation is highly dependent on the exact sequence of the protein, and mouse aS is reported to aggregate more rapidly than human aS in vitro. Nuclear magnetic resonance experiments of mouse and human aS at supercooled temperatures (263 K) are used to understand the effect of sequence on conformational fluctuations in the disordered ensembles and to relate these to differences in propensities to aggregate. We show that both aS are natively unfolded at low temperature with different propensities to secondary structure, backbone dynamics and long-range contacts across the protein. Mouse aS exhibits a higher propensity to helical conformation around the C-terminal substitutions as well as the loss of transient long-range contacts from the C- to the N-terminal end and hydrophobic central regions of the protein relative to human aS. Lack of back-folding from the C-terminal end of mouse aS exposes the N-terminal region, which is shown, by ¹⁵N relaxation experiments, to be very restricted in mobility relative to human aS. We propose that the restricted mobility in the N-terminal region may arise from transient interchain interactions, suggesting that the N-terminal KTK(E/Q)GV repeats may serve as initiation sites for aggregation in mouse aS. These transient interchain interactions coupled with a non-Aβ amyloid component (NAC) region that is both more exposed and has a higher propensity to β structure may accelerate the rate of fibril formation of aS.     

Binding of retinol induces changes in rat cellular retinol-binding protein II conformation and backbone dynamics

The structure and backbone dynamics of rat holo cellular retinol-binding protein II (holo-CRBP II) in solution has been determined by multidimensional NMR. The final structure ensemble was based on 3980 distance and 30 dihedral angle restraints, and was calculated using metric matrix distance geometry with pairwise Gaussian metrization followed by simulated annealing. The average RMS deviation of the backbone atoms for the final 25 structures relative to their mean coordinates is 0.85(+/-0.09) A. Comparison of the solution structure of holo-CRBP II with apo-CRBP II indicates that the protein undergoes conformational changes not previously observed in crystalline CRBP II, affecting residues 28-35 of the helix-turn-helix, residues 37-38 of the subsequent linker, as well as the beta-hairpin C-D, E-F and G-H loops. The bound retinol is completely buried inside the binding cavity and oriented as in the crystal structure. The order parameters derived from the (15)N T(1), T(2) and steady-state NOE parameters show that the backbone dynamics of holo-CRBP II is restricted throughout the polypeptide. The T(2) derived apparent backbone exchange rate and amide (1)H exchange rate both indicate that the microsecond to second timescale conformational exchange occurring in the portal region of the apo form has been suppressed in the holo form.     

(1)H/(15)N heteronuclear NMR spectroscopy shows four dynamic domains for phospholamban reconstituted in dodecylphosphocholine micelles

We report the backbone dynamics of monomeric phospholamban in dodecylphosphocholine micelles using (1)H/(15)N heteronuclear NMR spectroscopy. Phospholamban is a 52-amino acid membrane protein that regulates Ca-ATPase in cardiac muscle. Phospholamban comprises three structural domains: a transmembrane domain from residues 22 to 52, a connecting loop from 17 to 21, and a cytoplasmic domain from 1 to 16 that is organized in an "L"-shaped structure where the transmembrane and the cytoplasmic domain form an angle of approximately 80 degrees (Zamoon et al., 2003; Mascioni et al., 2002). T(1), T(2), and (1)H/(15)N nuclear Overhauser effect values measured for the amide backbone resonances were interpreted using the model-free approach of Lipari and Szabo. The results point to the existence of four dynamic domains, revealing the overall plasticity of the cytoplasmic helix, the flexible loop, and part of the transmembrane domain (residues 22-30). In addition, using Carr-Purcell-Meiboom-Gill-based experiments, we have characterized phospholamban dynamics in the micros-ms timescale. We found that the majority of the residues in the cytoplasmic domain, the flexible loop, and the first ten residues of the transmembrane domain undergo dynamics in the micros-ms range, whereas minimal dynamics were detected for the transmembrane domain. Hydrogen/deuterium exchange factors measured at different temperatures support the existence of slow motion in both the loop and the cytoplasmic helix. We propose that these dynamic properties are critical factors in the biomolecular recognition of phospholamban by Ca-ATPase and other interacting proteins such as protein kinase A and protein phosphatase 1.     

NMR analysis of the conformational properties of the trapped on-pathway folding intermediate of the bacterial immunity protein Im7

Previous work shows that the transiently populated, on-pathway intermediate in Im7 folding contains three of the four native alpha-helices docked around a core stabilised by native and non-native interactions. To determine the structure and dynamic properties of this species in more detail, we have used protein engineering to trap the intermediate at equilibrium and analysed the resulting proteins using NMR spectroscopy and small angle X-ray scattering. Four variants were created. In L53AI54A, two hydrophobic residues within helix III are truncated, preventing helix III from docking stably onto the developing hydrophobic core. In two other variants, the six residues encompassing the native helix III were replaced with three (H3G3) or six (H3G6) glycine residues. In the fourth variant, YY, two native tyrosine residues (Tyr55 and Tyr56) were re-introduced into H3G6 to examine their role in determining the properties of the intermediate ensemble. All four variants show variable peak intensities and broad peak widths, consistent with these proteins being conformationally dynamic. Chemical shift analyses demonstrated that L53AI54A and YY contain native-like secondary structure in helices I and IV, while helix II is partly formed and helix III is absent. Lack of NOEs and rapid NH exchange for L53AI54A, combined with detailed analysis of the backbone dynamics, indicated that the hydrophobic core of this variant is not uniquely structured, but fluctuates on the NMR timescale. The results demonstrate that though much of the native-like secondary structure of Im7 is present in the variants, their hydrophobic cores remain relatively fluid. The comparison of H3G3/H3G6 and L53AI54A/YY suggests that Tyr55 and/or Tyr56 interact with the three-helix core, leading other residues in this region of the protein to dock with the core as folding progresses. In this respect, the three-helix bundle acts as a template for formation of helix III and the creation of the native fold.     

Effect of the A30P mutation on the structural dynamics of micelle-bound αSynuclein released in water: a molecular dynamics study

Atomistic molecular dynamics simulation has been used to probe the effect of the A30P mutation on the structural dynamics of micelle-bound, helical αSynuclein when released in an aqueous environment. On the timescales simulated, the effect of the mutation on the secondary structure is restricted to local changes close to the mutation site in the N-terminal helical domain. The changes are transient, and all residues except Lys23 recover their initial structure. The local behavior due to the mutation gives rise to a global difference in the A30P mutant in the form of a permanent kink in the N-terminal helical domain.     

Solution structure and backbone dynamics of Calsensin, an invertebrate neuronal calcium-binding protein

Calsensin is an EF-hand calcium-binding protein expressed by a subset of peripheral sensory neurons that fasciculate into a single tract in the leech central nervous system. Calsensin is a 9-kD protein with two EF-hand calcium-binding motifs. Using multidimensional NMR spectroscopy we have determined the solution structure and backbone dynamics of calcium-bound Calsensin. Calsensin consists of four helices forming a unicornate-type four-helix bundle. The residues in the third helix undergo slow conformational exchange indicating that the motion of this helix is associated with calciumbinding. The backbone dynamics of the protein as measured by (15)N relaxation rates and heteronuclear NOEs correlate well with the three-dimensional structure. Furthermore, comparison of the structure of Calsensin with other members of the EF-hand calcium-binding protein family provides insight into plausible mechanisms of calcium and target protein binding.     

NMR solution structure and dynamics of an exchangeable apolipoprotein,Locusta migratoria apolipophorin III

We report here the NMR structure and backbone dynamics of an exchangeable apolipoprotein, apoLp-III, from the insect Locusta migratoria. The NMR structure adopts an up-and-down elongated five-helix bundle, which is similar to the x-ray crystal structure of this protein. A short helix, helix 4', is observed that is perpendicular to the bundle and fully solvent-exposed. NMR experimental parameters confirm the existence of this short helix, which is proposed to serve as a recognition helix for apoLp-III binding to lipoprotein surfaces. The L. migratoria apoLp-III helix bundle displays several characteristic structural features that regulate the reversible lipoprotein binding activity of apoLp-III. The buried hydrophilic residues and exposed hydrophobic residues readily adjust the marginal stability of apoLp-III, facilitating the helix bundle opening. Specifically, upon lipoprotein binding the locations and orientations of the buried hydrophilic residues modulate the apoLp-III helix bundle to adopt a possible opening at the hinge that is opposite the recognition short helix, helix 4'. The backbone dynamics provide additional support to the recognition role of helix 4' and this preferred conformational adaptation of apoLp-III upon lipid binding. In this case, the lipid-bound open conformation contains two lobes linked by hinge loops. One lobe contains helices 2 and 3, and the other lobe contains helices 1, 4, and 5. This preferred bundle opening is different from the original proposal on the basis of the x-ray crystal structure of this protein (Breiter, D. R., Kanost, M. R., Benning, M. M., Wesenberg, G., Law, J. H., Wells, M. A., Rayment, I., and Holden, H. M. (1991) Biochemistry 30, 603-608), but it efficiently uses helix 4' as the recognition short helix. The buried interhelical H-bonds are found to be mainly located between the two lobes, potentially providing a specific driving force for the helix bundle recovery of apoLp-III from the lipid-bound open conformation. Finally, we compare the NMR structures of Manduca sexta apoLp-III and L. migratoria apoLp-III and present a united scheme for the structural basis of the reversible lipoprotein binding activity of apoLp-III.     

Impact of N-terminal acetylation of α-synuclein on its random coil and lipid binding properties

N-Terminal acetylation of α-synuclein (aS), a protein implicated in the etiology of Parkinson's disease, is common in mammals. The impact of this modification on the protein's structure and dynamics in free solution and on its membrane binding properties has been evaluated by high-resolution nuclear magnetic resonance and circular dichroism (CD) spectroscopy. While no tetrameric form of acetylated aS could be isolated, N-terminal acetylation resulted in chemical shift perturbations of the first 12 residues of the protein that progressively decreased with the distance from the N-terminus. The directions of the chemical shift changes and small changes in backbone (3)J(HH) couplings are consistent with an increase in the α-helicity of the first six residues of aS, although a high degree of dynamic conformational disorder remains and the helical structure is sampled <20% of the time. Chemical shift and (3)J(HH) data for the intact protein are virtually indistinguishable from those recorded for the corresponding N-terminally acetylated and nonacetylated 15-residue synthetic peptides. An increase in α-helicity at the N-terminus of aS is supported by CD data on the acetylated peptide and by weak medium-range nuclear Overhauser effect contacts indicative of α-helical character. The remainder of the protein has chemical shift values that are very close to random coil values and indistinguishable between the two forms of the protein. No significant differences in the fibrillation kinetics were observed between acetylated and nonacetylated aS. However, the lipid binding properties of aS are strongly impacted by acetylation and exhibit distinct behavior for the first 12 residues, indicative of an initiation role for the N-terminal residues in an "initiation-elongation" process of binding to the membrane.     

Effects of Parkinson's disease-linked mutations on the structure of lipid-associated alpha-synuclein

Alpha-synuclein (alphaS) is a lipid-binding synaptic protein of unknown function that is found in an aggregated amyloid fibril form in the intraneuronal Lewy body deposits that are a defining characteristic of Parkinson's disease (PD). Although intrinsically unstructured when free in solution, alphaS adopts a highly helical conformation in association with lipid membranes or membrane mimetic detergent micelles. Two mutations in the alphaS gene have been linked to early onset autosomal dominant hereditary forms of PD, and have been shown to affect the aggregation kinetics of the protein in vitro. We have used high-resolution NMR spectroscopy, circular dichroism, and limited proteolysis to investigate the effects of these PD-linked mutations on the helical structure adopted by alphaS in the lipid or detergent micelle-bound form. We show that neither the A53T nor the A30P mutation has a significant effect on the structure of the folded protein, although the A30P mutation may cause a minor perturbation in the helical structure around the site of the mutation. The A30P, but not the A53T, mutation also appears to decrease the affinity of the protein for lipid surfaces, possibly by perturbing the nascent helical structure of the free protein. The potential implications of these results for the role of alphaS in PD are discussed.     

Solution structure and backbone dynamics of long-[Arg(3)]insulin-like growth factor-I

Long-[Arg(3)]insulin-like growth factor-I (IGF-I) is a potent analog of insulin-like growth factor-I that has been modified by a Glu(3) --> Arg mutation and a 13-amino acid extension appended to the N terminus. We have determined the solution structure of (15)N-labeled Long-[Arg(3)]-IGF-I using high resolution NMR and restrained molecular dynamics techniques to a precision of 0.82 +/- 0.28 A root mean square deviation for the backbone heavy atoms in the three alpha-helices and 3.5 +/- 0.9 A root mean square deviation for all backbone heavy atoms excluding the 8 N-terminal residues and the 8 C-terminal eight residues. Overall, the structure of the IGF-I domain is consistent with earlier studies of IGF-I with some minor changes remote from the N terminus. The major variations in the structure, compared with IGF-I, occur at the N terminus with a substantial reorientation of the N-terminal three residues of the IGF-I domain. These results are interpreted in terms of the lower binding affinity for insulin-like growth factor-binding proteins. The backbone dynamics of Long-[Arg(3)]IGF-I were investigated using (15)N nuclear spin relaxation and the heteronuclear nuclear Overhauser enhancement (NOE). There is a considerable degree of flexibility in Long-[Arg(3)]IGF-I, even in the alpha-helices, as indicated by an average ((1)H)(15)N NOE of 0.55 for the regions. The largest heteronuclear NOEs are observed in the helical regions, lower heteronuclear NOEs are observed in the C-domain loop separating helix 1 from helix 2, and negative heteronuclear NOEs are observed in the N-terminal extension and at the C terminus. Despite these data indicating conformational flexibility for the N-terminal extension, slow amide proton exchange was observed for some residues in this region, suggesting some transitory structure does exist, possibly a molten helix. A certain degree of flexibility may be necessary in all insulin-like growth factors to enable association with various receptors and binding proteins.     

Exendin-4 and glucagon-like-peptide-1: NMR structural comparisons in the solution and micelle-associated states.

Exendin-4, a 39 amino acid peptide originally isolated from the oral secretions of the lizard Heloderma suspectum, has been shown to share certain activities with glucagon-like-peptide-1 (GLP-1), a 30 amino acid peptide. We have determined the structuring preferences of exendin-4 and GLP-1 by NMR in both the solution and dodecylphosphocholine (DPC) micelle-associated states. Based on both chemical shift deviations and the pattern of intermediate range NOEs, both peptides display significant helicity from residue 7 to residue 28 with greater fraying at the N-terminus. Thornton and Gorenstein [(1994) Biochemistry 33, 3532-3539] reported that the presence of a flexible, helix-destabilizing, glycine at residue 16 in GLP-1 was an important feature for membrane and receptor binding. Exendin-4 has a helix-favoring glutamate as residue 16. In the micelle-associated state, NMR data indicate that GLP-1 is less helical than exendin-4 due to the presence of Gly16; chemical shift deviations along the peptide sequence suggest that Gly16 serves as an N-cap for a second, more persistent, helix. In 30 vol-% trifluoroethanol (TFE), a single continuous helix is evident in a significant fraction of the GLP-1 conformers present. Exendin-4 has a more regular and less fluxional helix in both media and displays stable tertiary structure in the solution state. In the micelle-bound state of exendin-4, a single helix (residues 11-27) is observed with residues 31-39 completely disordered and undergoing rapid segmental motion. In aqueous fluoroalcohol or aqueous glycol, the Leu21-Pro38 span of exendin-4 forms a compact tertiary fold (the Trp-cage) which shields the side chain of Trp25 from solvent exposure and produces ring current shifts as large as 3 ppm. This tertiary structure is partially populated in water and fully populated in aqueous TFE. The Leu21-Pro38 segment of exendin-4 may be the smallest protein-like folding unit observed to date. When the Trp-cage forms, fraying of the exendin-4 helix occurs exclusively from the N-terminus; backbone NHs for the C-terminal residues of the helix display H/D exchange protection factors as large as 10(5) at 9 degrees C. In contrast, no tertiary structure is evident when exendin-4 binds to DPC micelles. An energetically favorable insertion of the tryptophan ring into the DPC micelle is suggested as the basis for this change. With the exception of exendin-4 in media containing fluoro alcohol cosolvents, NMR structure ensembles generated from the NOE data do not fully reflect the conformational averaging present in these systems. Secondary structure definition from chemical shift deviations may be the most appropriate treatment for peptides that lack tertiary structure.     

Structure and dynamics of an amphiphilic peptide in a lipid bilayer: a molecular dynamics study

A molecular dynamics simulation of a simple model membrane system composed of a single amphiphilic helical peptide (ace-K2GL16K2A-amide) in a fully hydrated 1,2-dimyristoyl-sn-glycero-3-phosphocholine bilayer was performed for a total of 1060 ps. The secondary structure of the peptide and its stability were described in terms of average dihedral angles, phi and psi, and the C alpha torsion angles formed by backbone atoms; by the average translation per residue along the helix axis; and by the intramolecular peptide hydrogen bonds. The results indicated that residues 6 through 15 remain in a stable right-handed alpha-helical conformation, whereas both termini exhibit substantial fluctuations. A change in the backbone dihedral angles for residues 16 and 17 is accompanied by the loss of two intramolecular hydrogen bonds, leading to a local but long-lived disruption of the helix. The dynamics of the peptide was characterized in terms of local and global helix motions. The local motions of the N-H bond angles were described in terms of the autocorrelation functions of P2[cos thetaNH(t, t + tau)] and reflected the different degrees of local peptide order as well as a variation in time scale for local motions. The chi1 and chi2 dihedral angles of the leucine side chains underwent frequent transitions between potential minima. No connection between the side-chain positions and their mobility was observed, however. In contrast, the lysine side chains displayed little mobility during the simulation. The global peptide motions were characterized by the tilting and bending motions of the helix. Although the peptide was initially aligned parallel to the bilayer normal, during the simulation it was observed to tilt away from the normal, reaching an angle of approximately 25 degrees by the end of the simulation. In addition, a slight bend of the helix was detected. Finally, the solvation of the peptide backbone and side-chain atoms was also investigated.     

NMR structural studies of the myristoylated N-terminus of ADP ribosylation factor 6 (Arf6)

Arf proteins are guanine nucleotide binding proteins that are implicated in endocytotic pathways and vesicle trafficking. The two widely studied isoforms of Arf proteins (Arf1 and Arf6) have different cellular functions and localizations but similar structures. Arf proteins have an N-terminal helix with a covalently bound myristoyl group. Except structural models, there are no three dimensional structures of the myristoylated N-terminal peptide or the intact myristoylated Arf proteins. However, understanding the role of both the myristoyl group and the N-terminal helix based on the details of their molecular structures is of great interest. In the solution structure of myristoylated N-terminal peptide of Arf6 described here, the myristoyl group folds toward the N-terminus to interact with the hydrophobic residues in particular, the phenyl ring. Also, the structure of the dodecylphosphocholine (DPC) micelle-bound of the peptide together with paramagnetic studies showed that the myristoyl group is inserted into the micelle while residues V4-G10 interact with the surface of the micelle. The structural differences between the unbound and micelle-bound myristoylated N-terminal peptide of Arf6 involves the myristoyl group and the side chains of the hydrophobic residues.