α-Helical assembly of biologically active peptides and designed helix bundle protein

The formation of α-helical assembly by complexing biologically active peptides with de novo designed protein is described. The de novo designed protein described here is a cystinelinked 4-helix bundle protein constructed with 80 amino acid residues and forms a hydrophobic core region surrounded by 4 helices in an aqueous solution. The biologically active peptides, such as melittin and human growth hormone releasing factor, contain the sequences that are able to form amphiphilic helices. These peptides alone do not form the α-helix structure in a diluted solution with low ion strength. But on mixing with the designed helix bundle protein, the peptides are strongly bound to the protein with the induction of α-helical structure in the biologically active peptides. The content of induced α-helix is in accord with that estimated from the amphiphilic sequence. The results mean that a novel architecture composed of α-helices is formed. Fluorescent and temperature-scanning measurement revealed that the α-helical assembly is constructed with hydrophobic interaction. Also, it is shown by means of fluorescence depolarization that the assembly has a compact globular form corresponding to 1 : 1 complex. © 1994 John Wiley & Sons, Inc.     

Energetics of multihelix interactions in protein folding: application to myoglobin

Conformational-energy calculations have been carried out in order to determine favorable packing arrangements within a group of α-helices. The influence of side chains and of the number of interacting α-helices on the mode of packing was analyzed. In this work, our earlier methods for computing the packing energy of a pair of α-helices [Chou, K.-C., Némethy, G. & Scheraga, H. A. (1984) J. Am. Chem. Soc. 106 , 3161–3170] have been extended to treat the interactions among several helices. Also, new algorithms allow the matching of standard peptide geometry to x-ray coordinates of helical complexes and the analysis of interrelations between several helices. As a specific test case, the packing of three neighboring α-helices, viz., the A, G, and H helices of sperm whale myoglobin, was considered. Minimum-energy arrangements were computed for the separate A-H and the G-H α-helix pairs as well as for the A-G-H three-helix complex. For the packing of the nearly antiparallel G and H α-helices, the same optimal structure was obtained in two- and three-helix complexes, indicating that a single packing arrangement is specifically favored by interhelix interactions. For the pair of nearly perpendicular A and H α-helices, interactions are less specific, so that there is no unique optimal structure in the two-helix complex; in the three-helix complex, however, a specific mode of packing is favored even for the A-H pair. This result indicates that the presence of other nearby α-helices can influence the packing of a given α-helix pair. The computed arrangement of the A-G-H complex is very close to that of the crystallographically determined structure. These results can be used to make deductions about the likely sequence of events in protein folding, where, in this particular case, it appears that the G-H helix pair may form first and then induce proper orientation of the A helix.     

Effect of pressure on the secondary structure of coiled coil peptide GCN4-p1

It has recently been demonstrated that pressure induces folding of the α-helix of an alanine-based peptide (AK20), which is a monomer in water (Imamura and Kato, Proteins 2009;76:911–918). The present study focused on a coiled coil peptide GCN4-p1, the α-helices of which associate via a hydrophobic core, to examine whether the pressure stability of the α-helices depends on the hydrophobic core. Fourier transform infrared spectroscopy was used to investigate the effect of pressure on the secondary structures of GCN4-p1. The infrared spectra of GCN4-p1 shows the two amide I' peaks at ∼ 1650 and ∼ 1630 cm^− 1 stemming from the solvent-inaccessible α-helix and the solvent-accessible α-helix, respectively. The intensities of both the peaks increase with increasing pressure, whereas they decrease with increasing temperature. This indicates that pressure induces both the α-helices of GCN4-p1 to fold. The present result suggests that the positive volume change upon unfolding of an α-helix is a common characteristic of peptides. The pressure-induced stabilization of the α-helices is discussed in comparison with the pressure denaturation of proteins.     

Role of terminal dipole charges in aggregation of α-helix pair in the voltage gated K+ channel

The voltage sensor domain (VSD) of the potassium ion channel KvAP is comprised of four (S1–S4) α-helix proteins, which are encompassed by several charged residues. Apart from these charges, each peptide α-helix having two inherent equal and opposite terminal dipolar charges behave like a macrodipole. The activity of voltage gated ion channel is electrostatic, where all the charges (charged residues and dipolar terminal charges) interact with each other and with the transmembrane potential. There are evidences that the role of the charged residues dominate the stabilization of the conformation and the gating process of the ion channel, but the role of the terminal dipolar charges are never considered in such analysis. Here, using electrostatic theory, we have studied the role of the dipolar terminal charges in aggregation of the S3b–S4 helix pair of KvAP in the absence of any external field (V = 0). A system attains stability, when its potential energy reaches minimum values. We have shown that the presence of terminal dipole charges (1) change the total potential energy of the charges on S3b–S4, affecting the stabilization of the α-helix pair within the bilayer lipid membrane and (2) the C- and the N-termini of the α-helices favor a different dielectric medium for enhanced stability. Thus, the dipolar terminal charges play a significant role in the aggregation of the two neighboring α-helices.     

Conformational change in poly-L-lysine on reaction with polyacids

When solutions of poly-L -lysine and poly(acrylic acid) in salt solutions at neutral pH are mixed, complexes are formed. Optical rotatory dispersion studies of these complexes away from the equivalence point reveals the formation of α-helices. The α-helix content of the polylysine never rises above about 50%. On addition of 25% by volume of dioxane, the turbidity of the complex solutions disappears, and there is some enhancement of the α-helix content. Poly(phosphoric acid) behaves essentially in the same way as poly(acrylic acid). Poly(uridylic acid) forms complexes with polylysine but with no detectable formation of α-helix. The same is true of ribosomal RNA and native and denatured DNA. A number of other polyacid polybase systems involving basic proteins have been examined, but again no α-helix formation is induced. The results are related to the case of biological nucleoproitein complexes, and the conformational specificity of these systems is discussed. The effect of scattering on measured optical rotation has been investigated and is shown to be unimportant up to quite high levels.     

Secondary-structure analysis of alcohol-denatured proteins by vacuum-ultraviolet circular dichroism spectroscopy

To elucidate the structural characteristics of alcohol-denatured proteins, we measured the vacuum-ultraviolet circular dichroism (VUVCD) spectra of six proteins-myoglobin, human serum albumin, α-lactalbumin, thioredoxin, β-lactoglobulin, and α-chymotrypsinogen A-down to 170 nm in trifluoroethanol solutions (TFE: 0-50%) and down to 175 nm in methanol solutions (MeOH: 0-70%) at pH 2.0 and 25°C, using a synchrotron-radiation VUVCD spectrophotometer. The contents of α-helices, β-strands, turns, poly-L-proline type II helices (PPIIs), and unordered structures of these proteins were estimated using the SELCON3 program, including the numbers of α-helix and β-strand segments. Furthermore, the positions of α-helices and β-strands on amino acid sequences were predicted by combining these secondary-structure data with a neural-network method. All alcohol-denatured proteins showed higher α-helix contents (up to ~ 90%) compared with the native states, and they consisted of several long helical segments. The helix-forming ability was higher in TFE than in MeOH, whereas small amounts of β-strands without sheets were formed in the MeOH solution. The produced α-helices were transformed dominantly from the β-strands and unordered structures, and slightly from the turns. The content and mean length of α-helix segments decreased as the number of disulfide bonds in the proteins increased, suggesting that disulfide bonds suppress helix formation by alcohols. These results demonstrate that alcohol-denatured proteins constitute an ensemble of many long α-helices, a few β-strands and PPIIs, turns, and unordered structures, depending on the types of proteins and alcohols involved.     

Stabilizing effects of 2-methylalanine residues on β-turns and α-helices

¹³C-, ¹H-nmr, CD, and x-ray crystallography revealed β-turns of type III for Boc-Gly-L-Ala-Aib-OMe, Boc-L-Ala-Aib-L-Ala-OMe; the 3₁₀-helix for Boc-Aib-L-Ala-Aib-L-Ala-Aib-OMe; and antiparallel arranged α-helices for Boc-L-Ala-Aib-Ala-Aib-Ala-Glu(OBzl)-Ala-Aib-Ala-Aib-Ala-OMe. An N-terminal rigid α-helical segment is found in the polypeptide antibiotics alamethicin, suzukacillin, and trichotoxin. The α-helix dipole is essential for their voltage-dependent pore formation in lipid bilayer membranes, which is explained by a flip-flop gating mechanism based on dipole–dipole interactions of parallel and antiparallel arranged α-helices within oligomeric structures.     

Solid-phase synthesis of short α-helices stabilized by the hydrogen bond surrogate approach

Stabilized α-helices and nonpeptidic helix mimetics have emerged as powerful molecular scaffolds for the discovery of protein-protein interaction inhibitors. Protein-protein interactions often involve large contact areas, which are often difficult for small molecules to target with high specificity. The hypothesis behind the design of stabilized helices and helix mimetics is that these medium-sized molecules may pursue their targets with higher specificity because of a larger number of contacts. This protocol describes an optimized synthetic strategy for the preparation of stabilized α-helices that feature a carbon-carbon linkage in place of the characteristic N-terminal main-chain hydrogen bond of canonical helices. Formation of the carbon-carbon bond is enabled by a microwave-assisted ring-closing metathesis reaction between two terminal olefins on the peptide chain. The outlined strategy allows the synthesis and purification of a hydrogen bond surrogate (HBS) α-helix in ～ 1 week.     

Proline-induced constraints in alpha-helices

The disrupting effect of a prolyl residue on an α-helix has been analyzed by means of conformational energy computations. In the preferred, nearly α-helical conformations of Ac-Ala₄-Pro-NHMe and of Ac-Ala₇-Pro-Ala₇-NHMe, only the residue preceding Pro is not α-helical, while all other residues can occur in the α-helical A conformation; i.e., it is sufficient to introduce a conformational change of only one residue in order to accommodate proline in a distorted α-helix. Other low-energy conformations exist in which the conformational state of three residues preceding proline is altered considerably; on the other hand, another conformation in which these three residues retain the near-α-helical A-conformational state (with up to 26° changes of their dihedral angles ? and ψ, and a 48° change in one ω from those of the ideal α-helix) has a considerably higher energy. These conclusions are not altered by the substitution of other residues in the place of the Ala preceding Pro. The conformations of the peptide chain next to prolyl residues in or near an α-helix have been analyzed in 58 proteins of known structure, based on published atomic coordinates. Of 331 α-helices, 61 have a Pro at or next to their N-terminus, 21 have a Pro next to their C-terminus, and 30 contain a Pro inside the helix. Of the latter, 16 correspond to a break in the helix, 9 are located inside distorted first turns of the helix, and 5 are parts of irregular helices. Thus, the reported occurrence of prolyl residues next to or inside observed α-helices in proteins is consistent with the computed steric and energetic requirements of prolyl peptides.     

Helix sense of poly-γ-p-chlorobenzyl L-glutamate

Poly(γ-p-chlorobenzyl L -glulamate), for which theoretical calculations have shown only a small difference in energy between the left- and right-handed α-helices, has been synthesized and its screw sense determined by ORD in various solvents. In all solvents studied, a right-handed α-helix has been observed.     

Structural changes of IgG induced by heat treatment and by adsorption onto a hydrophobic Teflon surface studied by circular dichroism spectroscopy

Thermal denaturation of mouse monoclonal immunoglobulin G (isotype 1), as well as structural rearrangements resulting from adsorption on a hydrophobic Teflon surface, are studied by circular dichroism spectroscopy. Both heat-induced and adsorption-induced denaturation do not lead to complete unfolding into an extended polypeptide chain, but leave a significant part of the IgG molecule in a globular or corpuscular form. Heating dissolved IgG causes a decrease of the fractions of β-sheet and β-turn conformations, whereas those of random coil and, to a lesser extent, α-helix increase. Adsorption enhances the formation of α-helices and random coils, but the β-sheet content is strongly reduced. Heating adsorbed IgG results in a gradual break-down of the α-helix and β-turn contents, and a concomitant formation of β-sheet structures. Thus, the structural changes in IgG caused by heating and by adsorption, respectively, are very different. However, after heating, the structure of adsorbed IgG approaches the structure of thermally denatured IgG in solution.     

Structure of the leech protein saratin and characterization of its binding to collagen

The leech protein Saratin from Hirudo medicinalis prevents thrombocyte aggregation by interfering with the first binding step of the thrombocytes to collagen by binding to collagen. We solved the three-dimensional structure of the leech protein Saratin in solution and identified its collagen binding site by NMR titration experiments. The NMR structure of Saratin consists of one α-helix and a five-stranded β-sheet arranged in the topology ββαβββ. The C-terminal region, of about 20 amino acids in length, adopts no regular structure. NMR titration experiments with collagen peptides show that the collagen interaction of Saratin takes place in a kind of notch that is formed by the end of the α-helix and the β-sheet. NMR data-driven docking experiments to collagen model peptides were used to elucidate the putative binding mode of Saratin and collagen. Mainly, parts of the first and the end of the fifth β-strand, the loop connecting the α-helix and the third β-strand, and a short part of the loop connecting the fourth and fifth β-strand participate in binding.     

The structure of the ends of α-helices in globular proteins: effect of additional hydrogen bonds and implications for helix formation

We prepared a set of about 2000 α-helices from a relational database of high-resolution three-dimensional structures of globular proteins, and identified additional main chain i ← i+3 hydrogen bonds at the ends of the helices (i.e., where the hydrogen bonding potential is not fulfilled by canonical i ← i+4 hydrogen bonds). About one-third of α-helices have such additional hydrogen bonds at the N-terminus, and more than half do so at the C-terminus. Although many of these additional hydrogen bonds at the C-terminus are associated with Schellman loops, the majority are not. We compared the dihedral angles at the termini of α-helices having or lacking the additional hydrogen bonds. Significant differences were found, especially at the C-terminus, where the dihedral angles at positions C2 and C1 in the absence of additional hydrogen bonds deviate substantially from those occurring within the α-helix. Using a novel approach we show how the structure of the C-terminus of the α-helix can emerge from that of constituent overlapping α-turns and β-turns, which individually show a variation in dihedral angles at different positions. We have also considered the direction of propagation of the α-helix using this approach. If one assumes that helices start as a single α-turn and grow by successive addition of further α-turns, the paths for growth in the N → C and C → N directions differ in a way that suggests that extension in the C → N direction is favored.     

Evolutionary origin of a secondary structure: π-helices as cryptic but widespread insertional variations of α-helices that enhance protein functionality

Formally annotated π-helices are rare in protein structures but have been correlated with functional sites. Here, we analyze protein structures to show that π-helices are the same as structures known as α-bulges, α-aneurisms, π-bulges, and looping outs, and are evolutionarily derived by the insertion of a single residue into an α-helix. This newly discovered evolutionary origin explains both why π-helices are cryptic, being rarely annotated despite occurring in 15% of known proteins, and why they tend to be associated with function. An analysis of π-helices in the diverse ferritin-like superfamily illustrates their tendency to be conserved in protein families and identifies a putative π-helix-containing primordial precursor, a “missing link” intermediary form of the ribonucleotide reductase family, vestigial π-helices, and a novel function for π-helices that we term a “peristaltic-like shift.” This new understanding of π-helices paves the way for this generally overlooked motif to become a noteworthy feature that will aid in tracing the evolution of many protein families, guide investigations of protein and π-helix functionality, and contribute additional tools to the protein engineering toolkit.     

ω-Helices in Proteins

A modification of the α-helix, termed the ω-helix, has four residues in one turn of a helix. We searched the ω-helix in proteins by the HELFIT program which determines the helical parameters—pitch, residues per turn, radius, and handedness—and p = rmsd/(N ? 1)^1/2 estimating helical regularity, where “rmsd” is the root mean square deviation from the best fit helix and “N” is helix length. A total of 1,496 regular α-helices 6–9 residues long with p ≤ 0.10 Å were identified from 866 protein chains. The statistical analysis provides a strong evidence that the frequency distribution of helices versus n indicates the bimodality of typical α-helix and ω-helix. Sixty-two right handed ω-helices identified (7.2% of proteins) show non-planarity of the peptide groups. There is amino acid preference of Asp and Cys. These observations and analyses insist that the ω-helices occur really in proteins.     

Direct determination of the π-helix structure and helix transition behavior of poly(β-phenethyl l-aspartate) via synchrotron X-ray diffraction

The helix-sense inversions of poly(β-phenethyl l -aspartate) (2P) and diblock copolymers (2P-3P), with 2P and poly(β-phenylpropyl l -aspartate) (3P) blocks, were studied in their solid states using synchrotron wide-angle X-ray diffraction and small-angle X-ray scattering. The characteristic parameters of the π-helix structure of 2P were directly determined in situ after the helix transition at a high temperature. In the 2P-3P block copolymers, the main chains of the 3P blocks initially convert from right- to left-handed α-helices, and then the 2P blocks convert irreversibly from right-handed α-helices to left-handed π-helices. The chemical structures of the side chains of poly(l -aspartic acid ester)s significantly affect their helix transition behaviors.     

Theoretical studies on the interaction of proteins and nucleic acid: II. The binding of α-helix to B-DNA

Interactions between B-DNA and homopolymeric α-helices of glycine, alanine, serine, asparagine and aspartic acid have been studied theoretically. The complexation energy has been minimised taking into account the interactions between DNA and the polypeptides as well as the internal energy of the α-helix and the interaction energy of counterions with the complex. The results obtained indicate the important role of strong hydrogen bonds between the peptide side chains and nucleic acid phosphate groups, these bonds being much stronger than specific interactions with the base-pairs. The formation of these structural bonds depends on the size of the α-helix, which in turn determines whether bridging across the major groove is possible. The steric role of the methyl group of thymine in orienting the peptide helix and the role of DNA screening cations in complex stabilization are also significant.     

Non-native States of Bovine Beta-Lactoglobulin Induced by Acetonitrile: pH-Dependent Unfolding of the Two Genetic Variants A and B

Acetonitrile (ACN)-induced unfolding of the beta-lactoglobulin variants A and B was investigated at pH 2.0, 7.0 and 9.0. ACN caused α-helix induction at low concentrations but lead to major conformational alterations when the concentration was raised. ACN also induced a concentration-dependent increase in the surface hydrophobicity of both the variants. Induction of α-helical structure and exposure of hydrophobic patches were, however, somewhat more pronounced in case of variant B, whereas the loss of tertiary structure was more marked for variant A. Both protein aggregation and helix induction necessitated higher ACN concentrations at pH 2.0 than at 7.0 and 9.0, suggesting the greater stability of the variants at acidic pH.     

Exposure of thiol groups in the heat-induced denaturation of β-lactoglobulin

Protein aggregates can be stabilised by disulphide bridges. The whey protein β-lactoglobulin (β-lac) contains a disulphide bridge and a free cysteine that are shielded from the solvent by an α-helix. These groups are important in the thiol–disulphide exchange that occurs during aggregation and gelation of β-lac. Replica exchange molecular dynamics simulations show that the exposure mechanism is very different for the two buried groups. While melting of the α-helix enhances exposure of the free cysteine, it does not for the buried bridge. These findings shed light on the molecular mechanism of the first step of β-lac denaturation and aggregation.     

Vibrational frequencies and modes of alpha-helix

Dichroic properties of the far-infrared absorption bands of the right-handed α-helix of poly-L -alanine were measured. The normal vibration frequencies of this structure were calculated. The assignments of bands were made and the vibrational modes dis-cussed. The frequencies of the α-helix vibrations with various phase differences were calculated. The frequencies of accordionlike vibrations and Young's modulus of the α-helix were estimated. The vibrational frequency for the right-handed α-helices of poly-D -alanine and poly(L -α-amino-n-butyric acid) were calculated, and the results were used for the interpretation of the spectra of copoly-D ,L -alanines and poly(L -α-amino-n-butyric acid). For the latter compound the existence of the rotational isomers in the side chain was strongly suggested. The vibrational modes of the bands characteristic of the α-helix were discussed with regard to the results of the normal coordinate treatment.