Selective aromatic interactions in beta-hairpin peptides

To probe the selectivity possible in hydrophobic clusters, we have compared the cross-strand interactions of phenylalanine (Phe) and cyclohexylalanine (Cha) in a beta-hairpin peptide. We have found a preference for self-association among the aromatic residues, which provides 0.55 kcal/mol in stability relative to Cha-Cha cross-strand pair. NMR analysis of the Phe-Phe cross-strand pair indicates that it interacts in an edge-face interaction, despite the fact that it is highly solvent-exposed. The interaction geometry as well as the enthalpic and entropic values for the peptide containing the Phe-Phe cross-strand pair suggest that the preference for self-association arises from inherent differences in the nature of aromatic and aliphatic interactions in water.     

Aromatic-aromatic interactions in crystal structures of helical peptide scaffolds containing projecting phenylalanine residues

Aromatic-aromatic interactions between phenylalanine side chains in peptides have been probed by the structure determination in crystals of three peptides: Boc-Val-Ala-Phe-Aib-Val-Ala-Phe-Aib-OMe, I; Boc-Val-Ala-Phe-Aib-Val-Ala-Phe-Aib-Val-Ala-Phe-Aib-OMe, II; Boc-Aib-Ala-Phe-Aib-Phe-Ala-Val-Aib-OMe, III. X-ray diffraction studies reveal that all three peptides adopt helical conformations in the solid state with the Phe side chains projecting outward. Interhelix association in the crystals is promoted by Phe-Phe interactions. A total of 15 unique aromatic pairs have been characterized in the three independent crystal structures. In peptides I and II, the aromatic side chains lie on the same face of the helix at i/i + 4 positions resulting in both intrahelix and interhelix aromatic interactions. In peptide III, the Phe side chains are placed on the opposite faces of the helix, resulting in exclusive intermolecular aromatic interactions. The distances between the centroids of aromatic pair ranges from 5.11 to 6.86 A, while the distance of closest approach of ring carbon atoms ranges from 3.27 to 4.59 A. Examples of T-shaped and parallel-displaced arrangements of aromatic pairs are observed, in addition to several examples of inclined arrangements. The results support the view that the interaction potential for a pair of aromatic rings is relatively broad and rugged with several minima of similar energies, separated by small activation barriers.     

Experimental evaluation of CH-π interactions in a protein core

CH-π stacks up! Using the protein α(2) D as a model system, we estimate that a CH-π contact between cyclohexylalanine (Cha) and phenylalanine (F) contributes approximately -0.7?kcal mol(-1) to the protein stability. The stacking F-Cha pairs are sequestered in the core of the protein, where water interference does not exist (see figure). Therefore, the observed energetic gain should represent the inherent magnitude and upper limit of the CH-π interactions.     

Enantioselective molecular recognition between beta-sheets

This communication asks whether homochiral or heterochiral interaction is preferred between enantiomeric beta-sheets and finds that homochiral pairing is strongly preferred. Interactions between beta-sheets occur widely among proteins through pairing of the hydrogen-bonding edges. Although the hydrogen-bonding edges of both l- and d-beta-sheets put forth the same pattern of hydrogen-bond donor and acceptor groups, the side chains point in opposite directions. Homochiral pairing of beta-sheets generates structures in which the pleats and side chains of adjacent beta-strands are parallel to each other, while heterochiral pairing of beta-sheets generates structures in which the pleats and side chains are antiparallel. To test which pairing is preferred, we have prepared and studied the interactions of beta-sheets 1a-d, which comprise all l-amino acids, and beta-sheets 2a-c, which comprise all d-amino acids. Previous studies in our laboratory have established that these compounds form well-defined dimers in organic solvents. In the current study, 1H NMR experiments establish that when the l-beta-sheets (1) are mixed with the enantiomeric d-beta-sheets (2), homochiral beta-sheet dimers predominate, and only small quantities of heterochiral beta-sheet dimers form. Ratios of homochiral and heterochiral dimers ranging from 95.8:4.2 to 98.5:1.5 are measured in CDCl3 at 253 K, which correspond to statistically corrected free-energy differences of 3.1-4.2 kcal/mol (0.6-0.8 kcal/mol per interacting residue). Possible explanations for the high enantioselectivity of molecular recognition between beta-sheets include favorable nonbonded contacts between the adjacent beta-strands of the homochiral beta-sheets and poor fit of the heterochiral beta-strands, which should twist in opposite directions.     

In silico assembly of Alzheimer's Abeta16-22 peptide into beta-sheets

Recent studies suggest that soluble oligomers of amyloid-forming peptides have toxic effects in cell cultures. In this study, the folding of three Alzheimer's A beta(16-22) peptides have been simulated with the activation-relaxation technique and a generic energy model. Starting from randomly chosen states, the predicted lowest energy structure superposes within 1 A rms deviation from its conformation within the fibrils. This antiparallel structure is found to be in equilibrium with several out-of-register antiparallel beta-sheets and mixed parallel-antiparallel beta-sheets, indicating that full structural order in the fibrils requires larger aggregates. Folding involves the formation of dimers followed by the addition of a monomer and proceeds through a generalized mechanism between disordered and native alignments of beta-strands.     

Site-specific relaxation kinetics of a tryptophan zipper hairpin peptide using temperature-jump IR spectroscopy and isotopic labeling

Two antiparallel beta-strands connected by a turn make beta-hairpins an ideal model system to analyze the interactions and dynamics of beta-sheets. Site-specific conformational dynamics were studied by temperature-jump IR spectroscopy and isotopic labeling in a model based on the tryptophan zipper peptide, Trpzip2, developed by Cochran et al. (Proc. Natl. Acad. Sci. U.S.A. 2001, 98, 5578). The modified Trpzip2C peptides have nearly identical equilibrium spectral behavior as Trpzip2 showing that they also form well-characterized beta-hairpin conformations in aqueous solution. Selective introduction of 13C=O groups on opposite strands lead to distinguishable cross-strand coupling of the labeled residues as monitored in the amide I' band. These frequency patterns reflect theoretical predictions, and the coupled 13C=O band loses intensity with increase in temperature and unfolding of the hairpin. Thermal relaxation kinetics were analyzed for unlabeled and cross-strand isotopically labeled variants. T-jumps of approximately 10 degrees C induce relaxation times of a few microseconds that decrease with increase of the peptide temperature. Differences in kinetic behavior for the loss of beta-strand and gain of disordered structure can be used to distinguish localized structure dynamics by comparison of nonlabeled and labeled amide I' components. Analysis of the data supports multistate dynamic and equilibrium behavior, but because of this process it is not possible to clearly define a folding and unfolding rate. Nonetheless, site-specific relaxation kinetics could be seen to be consistent with a hydrophobic collapse hypothesis for hairpin folding.     

NMR analysis of aromatic interactions in designed peptide beta-hairpins

Designed octapeptide beta-hairpins containing a central (D)Pro-Gly segment have been used as a scaffold to place the aromatic residues Tyr and Trp at various positions on the antiparallel beta-strands. Using a set of five peptide hairpins, aromatic interactions have been probed across antiparallel beta-sheets, in the non-hydrogen bonding position (Ac-L-Y-V-(D)P-G-L-Y/W-V-OMe: peptides 1 and 2), diagonally across the strands (Boc-Y/W-L-V-(D)P-G-W-L-V-OMe: peptides 3 and 6), and along the strands at positions i and i + 2 (Boc-L-L-V-(D)P-G-Y-L-W-OMe: peptide 4). Two peptides served as controls (Boc-L-L-V-(D)P-G-Y-W-V-OMe: peptide 5; Boc-L-Y-V-(D)P-G-L-L-V-OMe: peptide 7) for aromatic interactions. All studies have been carried out using solution NMR methods in CDCl(3) + 10% DMSO-d(6) and have been additionally examined in CD(3)OH for peptides 1 and 2. Inter-ring proton-proton nuclear Overhauser effects (NOEs) and upfield shifted aromatic proton resonances have provided firm evidence for specific aromatic interactions. Calculated NMR structures for peptides 1 and 2, containing aromatic pairs at facing non-hydrogen bonded positions, revealed that T-shaped arrangements of the interacting pairs of rings are favored, with ring current effects leading to extremely upfield chemical shifts and temperature dependences for specific aromatic protons. Anomalous far-UV CD spectra appeared to be a characteristic feature in peptides where the two aromatic residues are spatially proximal. The observation of the close approach of aromatic rings in organic solvents suggests that interactions of an electrostatic nature may be favored. This situation may be compared to the case of aqueous solutions, where clustering of aromatic residues is driven by solvophobic (hydrophobic) forces.     

Context-dependence of the contribution of disulfide bonds to beta-hairpin stability

Incorporation of disulfide bonds to stabilize protein and peptide structures is not always a successful strategy. To advance current knowledge on the contribution of disulfide bonds to beta-hairpin stability, a previously reported beta-hairpin-forming peptide was taken as a template to design a series of Cys-containing peptides. The conformational behavior of these peptides in their oxidized, disulfide-cyclized peptides, and reduced, linear peptides, was investigated on the basis of NMR parameters: NOEs, and 1H and 13C chemical shifts. We found that the effect of disulfide bonds on beta-hairpin stability depends on its location within the beta-hairpin structure, being very small or even destabilizing when connecting two hydrogen-bonded facing residues. When the disulfide bond is linking non-hydrogen-bonded facing residues, we estimated that its contribution to the free-energy change of beta-hairpin folding is approximately -1.0 kcal mol(-1). This value is larger than those reported for most beta-hairpin-stabilizing cross-strand side-chain-side-chain interactions, except for some aromatic-aromatic interactions, in particular the Trp-Trp one, and the cation-pi interaction between Trp and the non-natural methylated Arg/Lys. As disulfide bonds are frequently used to stabilize peptide conformations, our conclusions can be useful for peptide, peptidomimetic, and protein design, and may even extend to other chemical cross-links.     

Contributions of NH...O and CH...O hydrogen bonds to the stability of beta-sheets in proteins

Ab initio quantum calculations are applied to both the parallel and the antiparallel arrangements of the beta-sheets of proteins. The energies of the NH...O and CH...O hydrogen bonds present in the beta-sheet are evaluated separately from one another by appropriate modifications of the model systems. The bond energies of these two sorts of hydrogen bonds are found to be very nearly equal in the parallel beta-sheet. The NH...O bonds are stronger than CH...O in the antiparallel geometry but only by a relatively small margin. Moreover, the former NH...O bonds are weakened when placed next to one another, as occurs in the antiparallel beta-sheet. As a result, there is little energetic distinction between the NH...O and CH...O bonds in the full antiparallel beta-sheet, just as in the parallel structure.     

Experimental evidence for the reorganization of beta-strands within aggregates of the Abeta(16-22) peptide

Amyloidogenic deposits that accumulate in brain tissue with the progression of Alzheimer's disease contain large amounts of the amyloid beta-peptide. A small fragment of this peptide, comprising residues 16-22 (Abeta(16-22)), forms beta-sheets in isolation, which then aggregate into amyloid fibrils. Here, using isotope edited infrared spectroscopy to probe the secondary structure of the peptide with residue level specificity, we are able to show conclusively that the beta-sheets formed are antiparallel and, following an anneal cycle or prolonged incubation, are in register with the central residue (Phe19) in alignment across all strands. The alignment of strands proceeds via a rapid interchange from one sheet to another. This realignment of the peptide strands into a more favorable registry may have important implications for therapeutics since previous work has shown that well aligned beta-sheets form more stable amyloid fibrils.     

Hybrid peptide hairpins containing alpha- and omega-amino acids: conformational analysis of decapeptides with unsubstituted beta-, gamma-, and delta-residues at positions 3 and 8

The effects of inserting unsubstituted omega-amino acids into the strand segments of model beta-hairpin peptides was investigated by using four synthetic decapeptides, Boc-Leu-Val-Xxx-Val-D-Pro-Gly-Leu-Xxx-Val-Val-OMe: peptide 1 (Xxx=Gly), peptide 2 (Xxx=betaGly=betahGly=homoglycine, beta-glycine), peptide 3 (Xxx=gammaAbu=gamma-aminobutyric acid), peptide 4 (Xxx=deltaAva=delta-aminovaleric acid). 1H NMR studies (500 MHz, methanol) reveal several critical cross-strand NOEs, providing evidence for beta-hairpin conformations in peptides 2-4. In peptide 3, the NMR results support the formation of the nucleating turn, however, evidence for cross-strand registry is not detected. Single-crystal X-ray diffraction studies of peptide 3 reveal a beta-hairpin conformation for both molecules in the crystallographic asymmetric unit, stabilized by four cross-strand hydrogen bonds, with the gammaAbu residues accommodated within the strands. The D-Pro-Gly segment in both molecules (A,B) adopts a type II' beta-turn conformation. The circular dichroism spectrum for peptide 3 is characterized by a negative CD band at 229 nm, whereas for peptides 2 and 4, the negative band is centered at 225 nm, suggesting a correlation between the orientation of the amide units in the strand segments and the observed CD pattern.     

Molecular conformation and packing of peptide beta hairpins in the solid state: structures of two synthetic octapeptides containing 1-aminocycloalkane-1-carboxylic acid residues at the i+2 position of the beta turn

Peptide beta-hairpin formation is facilitated by centrally positioned D-Pro-Xxx segments. The synthetic peptides Boc-Leu-Phe-Val-D-Pro-Ac(6)c-Leu-Phe-Val-OMe (1) and Boc-Leu-Phe-Val-D-Pro-Ac(8)c-Leu-Phe-Val-OMe (2) were synthesized in order to explore the role of bulky 1-aminocycloalkane-1-carboxylic acid residues (Ac(n)c, where n is the number of carbon atoms in the ring), at the i+2 position of the nucleating beta turn in peptide beta hairpins. Peptides 1 and 2 crystallize in the monoclinic space group P2(1) with two molecules in the asymmetric unit. The crystal structures of 1 and 2 provide conformational parameters for four peptide hairpin molecules. In all cases, the central segments adopts a type II' beta-turn conformation, and three of the four possible cross-strand hydrogen bonds are observed. Fraying of the hairpins at the termini is accompanied by the observation of NHpi interaction between the Leu(1)NH group and Phe(7) aromatic group. Cross strand stabilizing interactions between the facing residues Phe(2) and Phe(7) are suggested by the observed orientation of aromatic rings. Anomalous far-UV CD spectra observed in solution suggest that close proximity of the Phe rings is maintained even in isolated molecules. In both peptides 1 and 2, the asymmetric unit consists of approximately orthogonal hairpins, precluding the formation of a planar beta-sheet arrangement in the solid state. Solvent molecules, one dioxane and one water in 1, three water molecules in 2, mediate peptide association. A comparison of molecular conformation and packing motifs in available beta-hairpin structures permits delineation of common features. The crystal structures of beta-hairpin peptides provide a means of visualizing different modes of beta-sheet packing, which may be relevant in developing models for aggregates of polypeptides implicated in disease situations.     

The self‐assembled of cyclic D,L‐α‐peptide systems: Insights into the structure and energetics

Cyclic D,L ‐α‐peptides are able to self‐assemble to nanotubes, although the inherent reason of the stability of this kind of nanotube as well as the intrinsic driving force of self‐assembly of the cyclic D ,L ‐α‐peptides still remain elusive. In this work, using several computational approaches, we investigated the structural and energy characteristics of a series of cyclo[(‐L ‐Phe‐D ‐Ala‐)₄] and cyclo[(‐L ‐Ala‐D ‐Ala‐)₄] oligomers. The results reveal that the thermodynamic stability, cooperativity, and self‐assembly patterns of cyclic D ,L ‐α‐peptide nanotubes are mainly determined by the interactions between cross‐strand side chains instead of those between backbones. For cyclo[(‐L ‐Phe‐D ‐Ala‐)₄] oligomers, the steric interaction between cross‐strand side chains, especially the electrostatic repulsion between the phenyls in Phe residues, brings anticooperative effect into parallel stacking mode, which is responsible for the preference of self‐assembling nanotube in antiparallel vs. parallel stacking orientation. Based on our results, a novel self‐assembling mechanism is put forward—it is the L ‐L antiparallel dimer of cyclo[(‐L ‐Phe‐D ‐Ala‐)₄], instead of the commonly presumed monomer, that acts as the basic building block in self assembly. It explains why these cyclic peptides uniquely self‐assemble to form antiparallel nanotubes. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2010     

Vibrational circular dichroism studies of molecular conformation and association of dipeptides

Vibrational circular dichroism (VCD) and infrared (IR) absorption spectra in the NH stretching region have been measured for the dipeptides, R′COAANHR′'(R′ = Me and tertBu; AA = Ala, Leu, Val and Phe; R′' = Me, isoBu and neoPe). Analyses of the VCD and absorption spectra indicated that the VCD bands for the NH stretching are quite sensitive to the state of hydrogen bonding as well as the local conformation of oligopeptides. VCD spectra exhibit a negative VCD band at 3420-3405 cm⁻¹ due to the C₅ conformer with an intramolecularly hydrogen-bonded five-membered ring. The intermolecularly hydrogen-bonded NH stretching vibration exhibits a characteristic negative—positive couplet from the high wavenumber side due to the antiparallel C₅C₅ dimer formation. Hydrogen-bonded oligomers beyond the dimer formed in highly concentrated solutions give rise to an additional negative VCD band on the lower wavenumber side of the hydrogen-bonded absorption band.     

Structures, photoluminescence, and reversible vapoluminescence properties of neutral platinum(II) complexes containing extended pi-conjugated cyclometalated ligands

Reacting K2PtCl4 with the tridentate R-C(wedge)N(wedge)C-H2 ligands 2,6-di-(2'-naphthyl)-4-R-pyridine (R = H, 1a; Ph, 1b; 4-BrC6H4, 1c; 3,5-F2C6H3, 1d) in glacial acetic acid, followed by heating in dimethyl sulfoxide (DMSO), gave complexes [(R-C(wedge)N(wedge)C)Pt(DMSO)] (2a-d). In the crystal structures of 2a-c, the molecules are paired in a head-to-tail orientation with Pt...Pt separations >6.3 A, and there are extensive close C-H...pi (d = 2.656-2.891 A), pi...pi (d = 3.322-3.399 A), and C-H...O=S (d = 2.265-2.643 A) contacts. [(Ph-C(wedge)N(wedge)C)Pt(PPh3)] (3) was prepared by reacting 2b with PPh3. Reactions of 2a-d with bis(diphenylphosphino)methane (dppm) gave [(R-C(wedge)N(wedge)C)2Pt2(mu-dppm)] (4a-d). Both head-to-head (syn) and head-to-tail (anti) conformations were found for 4a.6CHCl3.C5H12, whereas only one conformation was observed for 4b.2CHCl3 (syn), 4c.3CH2Cl2 (syn), and 4d.2CHCl3 (anti). In the crystal structures of 4a-d, there are close intramolecular Pt...Pt contacts of 3.272-3.441 A in the syn conformers, and long intramolecular Pt...Pt separations of 5.681-5.714 A in the anti conformers. There are weak C-H...X (d = 2.497-3.134 A) and X...X (X = Cl or Br; d = 2.973-3.655 A) interactions between molecules 4a-d and occluded CHCl3/CH2Cl2 molecules, and their solvent channels are of varying diameters (approximately 9-28 A). Complexes 2a-d, 3, and 4a-d are photoluminescent in the solid state, with emission maxima at 602-643 nm. Upon exposure to volatile organic compounds, 4a shows a fast and reversible vapoluminescent response, which is most intense with volatile halogenated solvents (except CCl4). Powder X-ray diffraction analysis of desolvated 4a revealed a more condensed molecular packing of syn and anti complexes than crystal 4a.6CHCl3.C5H12.     

Structure and stability of beta-pleated sheets

Beside alpha-helices, beta-sheets are the most common secondary structure elements of proteins. In this article, the question of structure and stability of parallel and antiparallel sheets of various lengths is addressed. All data obtained are compared to a selected set of protein structures. In antiparallel beta-sheets, one of the two possible H-bonded structures (containing 14 atoms in the H-bonded pseudoring) is energetically more favored and also more abundant in proteins than the other one (with 10 atoms involved in the pseudoring). Parallel beta-sheets and their subunits are energetically less stable and indeed found to occur more rarely in proteins. Antiparallel hairpins are disfavored compared to beta-sheets formed by sequentially separated strands. Agreement between theory and experimental data indicates that characterization of structural building blocks at an appropriately accurate level of theory is a useful tool to get insight into fundamentals of protein structure.     

Tuning stability of coiled-coil heterotrimers by selection of steric matching partners

Coiled-coil trimers of differing stability have been designed by judicious choice of hydrophobic core side chain identity. Steric matching of two alanines with one large side chain at three core positions affords stable heterotrimers. Use of either cyclohexylalanine (Cha) or phenylalanine (Phe) as the large side chain is effective, and unfolding free energies can be varied by over 3 kcal/mol by mixing Cha- and Phe-containing subunits.     

Homochiral oligopeptides generated by induced "mirror symmetry breaking" lattice-controlled polymerizations in racemic crystals of phenylalanine N-carboxyanhydride

The formation of diastereoisomeric libraries of oligopeptides through the heterogeneous polymerization of racemic crystals of phenylalanine N-carboxyanhydride (PheNCA) is reported. The diastereoisomeric compositions of the oligopeptides formed on polymerization of (R,S) crystals incorporating the deuterium-tagged S enantiomer were determined by MALDI-TOF mass spectrometry. The racemic mixtures of the oligopeptides longer than pentamers are represented primarily by diastereoisomers of homochiral sequence and with peptides containing only one heterochiral repeating unit. A mechanism comprising the following three sequential steps to account for this unusual observation is proposed: 1) formation of dimers and trimers at a partially damaged liquid/solid interface, 2) chain propagation that takes place within the bulk of the crystal through a lattice-controlled "zipper-like" mechanism between homochiral molecules arranged in a head-to-tail motif to yield crystalline antiparallel beta-sheets of alternating oligopeptide chains of homochiral sequence of opposite handedness, and 3) enantiomeric cross-inhibition that results in chain termination. Induced desymmetrization of the racemic mixtures of the formed peptides was achieved by the polymerization of the mixed quasi-racemic crystals of (R)-PheNCA, ((S)-PheNCA), and (S)-ThieNCA (3-(2-thienyl)-alanine N-carboxyanhydride) of various compositions. These experiments resulted in the formation of nonracemic libraries of oligopeptides composed of homochiral chains of (R)-Phe and copolymers of randomly distributed (S)-Phe and (S)-Thie sequences. From these findings, we propose a stochastic model for the generation of libraries of nonracemic mixtures of oligopeptides from the polymerization of host (R,S)-PheNCA with racemic mixtures of other guest NCA amino acids dissolved in limited quantities in the crystal.     

Nucleation of beta-hairpin structures with cis amide bonds in E-vinylogous proline-containing peptides

Synthesis and conformational studies of peptides containing the E-vinylogous prolines 1 (VPro1) and 2 (VPro2), Boc-Ala-Val-VPro1-Xaa-Leu-OMe (3, Xaa = Gly; 4, Xaa = Phe), Boc-Ala-Val-VPro2-Xaa-Leu-OMe (5, Xaa = Gly; 6, Xaa = Phe), Boc-Leu-Ile-Val-VPro1-Xaa-Leu-OMe (7, Xaa = Gly; 8, Xaa = Phe), and Boc-Leu-Ile-Val-VPro2-Xaa-Leu-OMe (9, Xaa = Gly; 10, Xaa = Phe), were carried out. It has been shown that both VPro1 and VPro2 lead to the formation of 12-membered intramolecularly hydrogen bonded structures very similar to type VI beta-turns with a cis Xaa-VPro amide bond in the major conformers in all the peptides 3-10, resulting in the nucleation of beta-hairpin type structures in these molecules in CDCl(3).