Conformation and interactions of uteroglobin fragments 4–14 and 49–65 in aqueous solution containing surfactant micelles

The conformation of two fragments of rabbit uteroglobin is described. The peptides are PRFAHVIENLL and PQTTRENIMKLTEKIVK, corresponding to helices I and IV in the crystal structure. CD shows that both peptides interact with sodium dodecyl sulfate (SDS) micelles and change their conformation to an α-helix. The helical content estimated from the CD band at 222 nm is about 40% in each peptide. Surface tension measurements show that both peptides lower the critical micellar concentration (cmc) of SDS, with a more dramatic effect in the case of helix I. This peptide by itself acts as a surfactant, and is able to interact with SDS even below the observed cmc, forming β aggregates. Proton magnetic resonance (¹H-nmr) suggests that flexible helices are present. The longest helical stretches compatible with ¹H-nmr data extend from Phe⁶ to Leu¹⁴ for helix I and from Arg⁵³ to Ile⁶³ for helix IV. © 1993 John Wiley & Sons, Inc.     

Development of the multiple sequence approximation within the AGADIR model of α-helix formation: Comparison with Zimm-Bragg and Lifson-Roig formalisms

In this work we present the development of the multiple sequence approximation (AGADIRms) and the standard one-sequence approximation (AGADIRIs) within the framework of AGADIR's α-helix formation model. The extensive comparison between these new formulations and the original one [AGADIR; v. Muñoz and L. Serrano (1994),Nat. Struct. Biol., Vol. 1, pp. 399–409] indicates that the standard one-sequence approximation is virtually identical to the multiple sequence approximation, while the previously used residue partition function approximation [Muñoz and Serrano (1994); (1995), J. Mol. Biol., Vol. 245, pp. 275–296] is less precise. The calculations of the average helical content performed with AGADIR are precise for peptides of less than 30 residues and progressively diverge from the multiple sequence formulation for longer peptides. The helicity distribution of heteropolypeptides with less than 50% average helical content is also well described, while those of quasi-homopolymers with high helical content tend to be flattened. These inaccuracies lead to an underestimation of 0.017 kcal/mol for the mean-residue enthalpic contribution in AGADIR, as compared to AGADIRms and AGADIRIs. The other energy contributions to α-helix stability are not affected by the original statistical approximation. We also discuss the particularities of the model for α-helix formation utilized in AGADIR and compare it with the classical Zimm-Bragg and Lifson-Roig theories. Moreover, we develop the mathematical relationships between the basic AGADIR energy contributions and helix nucleation and elongation, which permit the quantitative comparison between formalisms. Remarkably, the comparison between AGADIRms and the Lifson-Roig formalism shows that, despite the differences on treating helix/coil cooperativity, both theories give virtually identical results when an equivalent set of parameters is used. This indicates that the helix/coil transition is a solid theory independent of the particularities of the model for α-helix formation. © 1997 John Wiley & Sons, Inc. Biopoly 41: 495–509, 1997.     

Correlation between computed conformational properties of cytochrome c peptides and their antigenicity in a T-lymphocyte proliferation assay

By means of conformational energy calculations, we previously showed that the antigenic strength of a series of oligopeptides (derived from the carboxyl terminal sequence of cytochrome c) in a T-lymphocyte proliferation assay depends on their ability to adopt the α-helix conformation. Using experimentally determined statistical weights (within the framework of the Zimm–Bragg theory for the helix–coil transition), here we present a simple free energy analysis of the ability of these peptides to adopt the α-helix conformation in water. The experimental statistical weights have been modified to include the effect of long-range charge–dipole interactions on helix stability. We find that there is a close correlation between the tendency of a peptide to adopt the α-helix conformation and its ability to stimulate antigen-primed T cells. The shortest peptide with a tendency to adopt the α-helix conformation is also the shortest one that exhibits antigenic activity. The rapid and simple method presented here can thus be used to predict relative antigenicities for different peptides derived from cytochrome c.     

A stone's throw and its launch window: timing precision and its implications for language and hominid brains

The Chou-Fasman conformational parameters, P, for amino acid residues in proteins are shown to be a linear function of intermolecular force and steric parameters. For α- helix, coil and turn parameters, steric effects are predominant; whereas for β-sheet parameters, intramolecular forces are predominant. Turn and coil parameters show little or no difference in their dependence which is different from that of α-helix and in some ways almost reciprocal. Factors which increase the probability of finding an amino acid residue in an α-helix usually decrease the probability of finding it in coil or turn. Values of P were calculated for several of the less common amino acids.     

1H-NMR analysis of CD3-ϵ reveals the presence of turn-helix structures around the ITAM motif in an otherwise random coil cytoplasmic tail

The conformation adopted in solution by the cytoplasmic tail of CD3-ϵ has been analyzed by ¹H-nmr. The cytoplasmic tail is mostly random coil except for the amino acids conforming the immunoreceptor tyrosine-based activation motif (ITAM), YxxL/IxxxxxxxY xxL. Although the N-terminal Y xxL sequence of the motif is poorly folded, adopting 6-residue turn-like conformations with the Tyr side chain in two different orientations, the C-terminal Y xxL sequence is placed in a more complex structure involving a set of nonclassical α-helix turns and β-turns that comprises 11 amino acids. This structure is not modified by phosphorylation of the tyrosine residue. The differences in the conformation adopted around the two tyrosines of the ITAM motif suggest that they may play different roles pertaining to either binding signal transducing proteins or, alternatively, proteins involved in other processes such as endoplasmic reticulum location. © 1997 John Wiley & Sons, Inc. Biopoly 42: 75–88, 1997     

Assignment of the helical structure in neuropeptide Y by HPLC studies of methionine replacement analogues and 1H-NMR spectroscopy

The HPLC retention behavior of three complete single methionine and methionine sulfoxide replacement sets of two 18-mer model peptides and neuropeptide Y (NPY) were investigated. All peptides were prepared by multiple solid-phase peptide synthesis. Plotting the retention time differences between methionine and methionine sulfoxide analogues vs the position of replacement shows that potentially α-helical peptides become helical on binding during reversed-phase high performance liquid chromatography. In the case of an amphipathic α-helix, the retention time differences change periodically with a 3–4 repeat pattern, which allow the location of amphipathic helical structures. Replacements in nonamphipathic α-helical domains cause local preferential binding areas and lead to sequence-dependent retention time profiles. Methionine replacement studies of NPY suggest an unstructured or extended conformation from Tyr¹ to Ala¹² connected to a well-defined amphipathic α-helix from Pro¹³ to Arg³⁵. The assignment is confirmed by comparison of nuclear Overhauser effects based two-dimensional ¹H-nmr spectroscopy and utilization of the C^αH shift index method in 50% trifluoroethanol/50% water. © 1996 John Wiley & Sons, Inc.     

Strategy for trapping intermediates in the folding of ribonuclease and for using 1H-nmr to determine their structures

The major unfolded form of ribonuclease A is known to show well-populated structural intermediates transiently during folding at 0°–10°C. We describe here how the exchange reaction between D₂O and peptide NH protons can be used to trap folding intermediates. The protons protected from exchange during folding can be characterized by ¹H-nmr after folding is complete. The feasibility of using ¹H-nmr to resolve a set of protected peptide protons is demonstrated by using a specially prepared sample of ribonuclease S in D₂O in which only the peptide protons of residues 7–14 are in the ¹H-form. All eight of these protected peptide protons are H-bonded. Resonance assignments made on isolated peptides containing these residues have been used to identify the protected protons. Other sets of protected protons trapped in the ¹H-form can also be isolated by differential exchange, using either ribonuclease A or S. Earlier model compound studies have indicated that H-bonded folding intermediates should be unstable in water unless stabilized by additional interactions. Nevertheless, peptides derived from ribonuclease A that contain residues 3–13 do show partial helix formation in water at low temperatures. We discuss the possibility that specific interactions between side chains can stabilize short α-helixes by nucleating the helix, and that specific interactions may also define the helix boundaries at early stages in folding.     

Potentiometric titration of poly-L-lysine: the coil-to-beta transition

We have performed potentiometric titrations of poly-L -lysine. From these data we have calculated the free energy and enthalpy changes for the folding of the random coil to the α-helix in 10% ethanol (?120 and ?120 cal/mole) and from the random coil to the β-structure in water (?140 and 870 cal/mole) and in 10% ethanol (?180 and 980 cal mole). Comparison of these values with each other and with values for the coil → α- helix transition in water (?78 and ?880 cal/mole) led to the following conclusions. The stabilization by ethanol of ethanol of the α-helix with respect to the coil is that predicted from the known free energy of transfer of the peptide group from water to 10% ethanol. Similar data to explain the enthalpy difference are not available. The thermodynamic functions for the transition from α-helix to β-structure, obtained by subtracting those for the coil → α-helix and coil → β-structure transitions, are explained from a consideration of the structural differences: non bonded interactions of the polypeptide backbone are less favorable in the β-structure than in the α-helix, causing an increase in the energy, while hydrophobic contacts between side chains raise the entropy of the β-structure as compared with the α-helix, so that the free energy difference between the two structures is small, but enthalpy and entropy differences are large. The observation of only small differences in the free energy and enthalpy changes for the transition from coil β-structure upon going from water to 10% ethanol is expected by considering both the free energy of transfer of the peptide group (as for the α-helix) and the free energy and enthalpy of transfer of the apolar part of the side chain involved in hydrophobic bond formation.     

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.     

Structures of peptides from α-amino acids methylated at the α-carbon,

The structural preferences of peptides (and depsipeptides) from the achiral MeAib and Hib residues, and the chiral Iva, (αMe) Val, (αMe) Leu, and (αMe) Phe residues, as determined by conformational energy computations, x-ray diffraction analyses, and ¹H-nmr and spectroscopic studies, are reviewed and compared with literature data on Aib-containing peptides. The results obtained indicate that helical structures are preferentially adopted by peptides rich in these α-amino acids methylated at the α-carbon. Intriguing experimental findings on the impact of the chirality of Iva, (αMe) Val, and (αMe) Phe residues on helix screw sense are illustrated. © 1993 John Wiley & Sons, Inc.     

Optical and other properties of a hydrocarbon-soluble polypeptide, poly-gamma-(N-dodecyl)-L-glutamate

The polypeptide poly-γ-(n-dodecyl)-L -glutamate (PDLG) is soluble in hydrocarbon solvents such as hexane, cyclohexane, and dodecane. The CD spectra of PLDG in these solvents are reported here. These spectra are typical α-helix spectra and show none of the wavelength shifts and magnitude changes displayed by partially helical proteins in membrane preparations. This observation rules out the possibility that the membrane protein CD spectra result from solvent effects. The PDLG helix is stable in dodecane up to at least 70 °C. However, it is easily disrupted by trifluoroacetic acid, with the helix–coil transition centered at 3% TFA in hexane. Viscosity measurements of PDLG in dry dichloroacetic acid exhibit polyelectrolyte effects which can be suppressed by addition of several percent water.     

Identification of an “α-helix-extended segment-α-helix” conformation of the sixth transmembrane domain in DMT1

DMT1 (divalent metal ion transporter 1) is one member of a family of proton-coupled transporters that facilitate the cellular absorption of divalent metal ions. A pair of mutation-sensitive and highly conserved histidines in the sixth transmembrane domain (TM6) of DMT1 was found to be important for proton-metal ion cotransport. In the present work, we investigate the structures and locations of the peptides from TM6 of DMT1 and its H267A and H272A mutants in SDS micelles by CD and NMR methods. The circular dichroism studies show that the α-helix is a predominant conformation for the wildtype peptide and H267A mutant in SDS micelles, whereas the helicity is evidently decreased for H272A mutant. The pH value has little effect on the α-helical contents of the three peptides. The NMR studies indicate that the wildtype peptide in SDS micelles forms an “α-helix-extended segment-α-helix” structure in which the His267 locates near the central part of the extended segment, while the His272 is involved in the α-helical folding. Both histidines are buried in SDS micelles as evidenced by their pK_a values. The structure of the wildtype peptide is evidently changed by the mutations of H267A and H272A. The H267A mutant forms an ordered structure consisting of an α-helix from the C-terminus to the central part and continuous turns in the residual part. The extended structure in the central part of the wildtype peptide is abolished by H267A mutation. The H272A mutation mainly induces unfolding of the short helix in the N-terminal side, while the short helix in the C-terminal side and unordered conformation in the central part remain. All the three peptides are embedded in SDS micelles, and the H267A mutant is inserted more deeply due to increasing hydrophobicity in the central part of the peptide. The specific “α-helix-extended segment-α-helix” structure of TM6 may have an important implication for the binding of the transporter to H⁺ and metal ions and the conformation change induced by the mutations of two highly conserved histidines may be correlated to the deficiency of the transport activity of DMT1.     

Addition of side-chain interactions to 3(10)-helix/coil and alpha-helix/3(10)-helix/coil theory.

An increasing number of experimental and theoretical studies have demonstrated the importance of the 3(10)-helix/ alpha-helix/coil equilibrium for the structure and folding of peptides and proteins. One way to perturb this equilibrium is to introduce side-chain interactions that stabilize or destabilize one helix. For example, an attractive i, i + 4 interaction, present only in the alpha-helix, will favor the alpha-helix over 3(10), while an i, i + 4 repulsion will favor the 3(10)-helix over alpha. To quantify the 3(10)/alpha/coil equilibrium, it is essential to use a helix/coil theory that considers the stability of every possible conformation of a peptide. We have previously developed models for the 3(10)-helix/coil and 3(10)-helix/alpha-helix/ coil equilibria. Here we extend this work by adding i, i + 3 and i, i + 4 side-chain interaction energies to the models. The theory is based on classifying residues into alpha-helical, 3(10)-helical, or nonhelical (coil) conformations. Statistical weights are assigned to residues in a helical conformation with an associated helical hydrogen bond, a helical conformation with no hydrogen bond, an N-cap position, a C-cap position, or the reference coil conformation plus i, i + 3 and i, i + 4 side-chain interactions. This work may provide a framework for quantitatively rationalizing experimental work on isolated 3(10)-helices and mixed 3(10)-/alpha-helices and for predicting the locations and stabilities of these structures in peptides and proteins. We conclude that strong i, i + 4 side-chain interactions favor alpha-helix formation, while the 3(10)-helix population is maximized when weaker i, i + 4 side-chain interactions are present.     

Secondary structure and position of the cell-penetrating peptide transportan in SDS micelles as determined by NMR

Transportan is a 27-residue peptide (GWTLN SAGYL LGKIN LKALA ALAKK IL-amide) which has the ability to penetrate into living cells carrying a hydrophilic load. Transportan is a chimeric peptide constructed from the 12 N-terminal residues of galanin in the N-terminus with the 14-residue sequence of mastoparan in the C-terminus and a connecting lysine. Circular dichroism studies of transportan and mastoparan show that both peptides have close to random coil secondary structure in water. Sodium dodecyl sulfate (SDS) micelles induce 60% helix in transportan and 75% helix in mastoparan. The 600 MHz (1)H NMR studies of secondary structure in SDS micelles confirm the helix in mastoparan and show that in transportan the helix is localized to the mastoparan part. The less structured N-terminus of transportan has a secondary structure similar to that of the same sequence in galanin [Ohman, A., et al. (1998) Biochemistry 37, 9169-9178]. The position of mastoparan and transportan relative to the SDS micelle surface was studied by adding spin-labeled 5-doxyl- or 12-doxyl-stearic acid or Mn2+ to the peptide/micelle system. The combined results show that the peptides are for the most part buried in the SDS micelles. Only the C-terminal parts of both peptides and the central segment connecting the two parts of transportan are clearly surface exposed. For mastoparan, the secondary chemical shifts of the amide protons were found to vary periodically and display a pattern almost identical to those reported for mastoparan in phospholipid bicelles [Vold, R., et al. (1997) J. Biomol. NMR 9, 329-335], indicating similar structures and interactions in the two membrane-mimicking environments.     

Helix-forming tendencies of nonpolar amino acids predicted by Monte Carlo simulated annealing

Monte Carlo simulated annealing is applied to the study of the α-helix-forming tendencies of seven nonpolar amino acids, Ala, Leu, Met, Phe, Ile, Val, and Gly. Homooligomers of 10 amino acids are used and the helix tendency is calculated by folding α-helicies from completely random initial conformations. The results of the simulation imply that Met, Ala, and Leu are helix formers and that Val, Ile, and Gly are helix breakers, while Phe comes in between the two groups. The differences between helix formers and breakers turned out to be large in agreement with the recent experiments with short peptides. It is argued from the energy distributions of the obtained conformations that the helix tendency is small for the helix breakers because of steric hindrance of side chains. Homoglycine is shown to favor a random coil conformation. The β-strand tendencies of the same homooligomers are also considered, and they are shown to agree with the frequencies of amino acids in β-sheet from the protein data base. © 1994 Wiley-Liss, Inc.     

Pressure-tuning FT-IR spectroscopic study on the helix–coil transition of Ala-rich oligopeptide in aqueous solution

We investigated the effect of pressure on the helix–coil transition of an Ala-rich peptide (AK16: YGAAKAAAAKAAAAKA-NH₂) in aqueous solution by FT-IR spectroscopy. The spectra of the amide I' region of AK16 in aqueous solution was decomposed into some component bands using a curve fitting method. The peak at around 1635 cm ^?1 corresponding to the solvent exposed α-helix conformer increases with increasing pressures, while the peak at around 1655 cm ^?1 corresponding to the random coil conformer decreases. From the pressure dependence of the band intensities, we determined the volume change from the α-helix to random coil conformers of AK16 to be + 10.5 ± 0.3 cm³/mol. The positive volume change is different from the negative volume change generally observed in the pressure denaturation of proteins.     

Secondary structure of proteins associated in thin films

The solid state secondary structure of myoglobin, RNase A, concanavalin A (Con A), poly(L -lysine), and two linear heterooligomeric peptides were examined by both far-uv CD spectroscopy¹ and by ir spectroscopy. The proteins associated from water solution on glass and mica surfaces into noncrystalline, amorphous films, as judged by transmission electron microscopy of carbon-platinum replicas of surface and cross-fractured layer. The association into the solid state induced insignificant changes in the amide CD spectra of all α-helical myoglobin, decreased the molar ellipticity of the α/β RNase A, and increased the molar ellipticity of all-β Con A with no change in the positions of the bands' maxima. High-temperature exposure of the films induced permanent changes in the conformation of all proteins, resulting in less α-helix and more β-sheet structure. The results suggest that the protein α-helices are less stable in films and that the secondary structure may rearrange into β-sheets at high temperature. Two heterooligomeric peptides and poly (L -lysine), all in solution at neutral pH with “random coil” conformation, formed films with variable degrees of their secondary structure in β-sheets or β-turns. The result corresponded to the protein-derived Chou-Fasman amino acid propensities, and depended on both temperature and solvent used. The ir and CD spectra correlations of the peptides in the solid state indicate that the CD spectrum of a “random” structure in films differs from random coil in solution. Formic acid treatment transformed the secondary structure of the protein and peptide films into a stable α-helix or β-sheet conformations. The results indicate that the proteins aggregate into a noncrystalline, glass-like state with preserved secondary structure. The solid state secondary structure may undergo further irreversible transformations induced by heat or solvent. © 1993 John Wiley & Sons, Inc.     

Conformational constraints of amino acid side chains in alpha-helices

The conformational freedom of amino acid side chains is strongly reduced when the side chains occur on an α-helix. A quantitative evaluation of this freedom has been carried out by means of conformational energy computations for all naturally occurring amino acids and for α-aminobutyric acid when they are placed in the middle of a right-handed poly(L-alanine) α-helix. One of the three possible rotameric states for rotation around the C^α ? C^β bond (viz. g⁺) is excluded completely on the helix because of steric hindrance, and the relative populations of the other two rotamers (t and g^?) are altered because of steric interactions and the reduction of hydrogen-bonding possibilities. The computed tendencies of the changes in distributions of rotamers, on going from an ensemble of all backbone conformations to the α-helix, agree with the observed tendencies in proteins. Minimum-energy side-chain conformations in an α-helix have been tabulated for use in conformational energy computations on polypeptides.     

Statistical mechanical treatment of α-helices and extended structures in proteins with inclusion of short- and medium-range interactions

A statistical mechanical model of protein conformation with medium-range interactions between theith and (i+k)^th residues (k<-4) is presented. Two two-state models, an α-helix-coil and an extended-structure-coil model, are formulated using the same form of the partition function, but the two models are applied independently to predict the locations of α-helical, extended, and coil segments; in the relatively few cases (<2%) where the predictions from the two models are in conflict, the prediction is scored as an incorrect one. Two independent sets of statistical weights (one set for each model) are derived to describe the interactions between the 20 amino acid residues for each range of interactionk; they are evaluated by minimizing an objective function so that the probability profiles for the α-helix or extended structure, respectively, in proteins computed from these statistical weights correlate optimally with the experimentally observed native conformations of these proteins. Examination of the resulting statistical weights shows that those for the interactions between hydrophobic residues and between a hydrophobic and a hydrophilic residue have reasonable magnitudes compared to what would be expected from the spatial arrangements of the side chains in the α-helix and the extended structure, and that those for the α-helix-coil model correlate well with experimentally determined values of the Zimm-Bragg parameterss and σ of the helix-coil transition theory. From the point of view of a method to predict the conformational states (i.e., α-helix, extended structure, and coil) of each residue, the statistical weights (as inall empirical prediction schemes) depend very much on the proteins used for the data base, since the presently available set of proteins of known structure is still too small for very high predictability; as a result, the correctness of the prediction is not very good for proteins not included in the data base. However, the correctness of the prediction, at least for the 37 proteins utilized as the data base in this study, is 91% and 87% for the α-helix-coil and the extended-structure-coil models, respectively; further, 79% of all the residues are predicted correctly when both the α-helix-coil and extended-structure-coil models are applied independently.     

Design,synthesis, and conformation of a model peptide of endothelin with cystine-stabilized α-helix motif

A model 16-peptide of endothelin-1 (MET-1), which has the minimized sequence homology to the corresponding pan of endothelin-1 (ET-1), was designed to confirm the cystine-stabilized α-helix motif. The model structure consists of an extended structure, a β-turn part, and an α-helix structure that is stabilized by two disulfide bonds. The α-helix segment was designed to emphasize the amphiphilic nature. In order to combine the extended structure and the α-helix segment, a D -Ala-Pro sequence was selected to fix the β-turn. The model endothelin 16-peptide amide was synthesized by solid-phase synthesis on a 4-methylbenzhydrylamine resin. Its conformation was examined by CD and two-dimensional (2D) ¹H-nmr measurements. MET-1 showed similar CD patterns to ET-1 in both buffer and 50% aqueous trifluoroethanol solution. The 2D nmr experiments in 50% aqueous ethylene glycol revealed that MET-1 closely resembles the conformation of ET-1 with an extended structure, an α-helix, and a β-turn unit in the same position of the sequence. Furthermore, model peptides without disulfide bond(s) could not assume a stable structure in aqueous solution, while they did have similar α-helical content in 50% trifluoroethanol with MET-1. When the two disulfide bridges were simultaneously formed, the peptide with the correct disulfide bonds (MET-1) was obtained in threefold excess to the isomer (apamin type. MET-2). These findings obtained by the modeling of ET-1 showed an important role for the stabilization of peptide conformation with disulfide bonds. © 1994 John Wiley & Sons, Inc.