Alanine-based Peptides Research Articles

Effect of Thioxopeptide Bonds on α-Helix Structure and Stability

Thioxoamide (thioamide) bonds are nearly isosteric substitutions for amides but have altered hydrogen-bonding and photophysical properties. They are thus well-suited backbone modifications for physicochemical studies on peptides and proteins. The effect of thioxoamides on protein structure and stability has not been subject to detailed experimental investigations up to date. We used alanine-based model peptides to test the influence of single thioxoamide bonds on alpha-helix structure and stability. The results from circular dichroism measurements show that thioxoamides are strongly helix-destabilizing. The effect of an oxo-to-thioxoamide backbone substitution is of similar magnitude as an alanine-to-glycine substitution resulting in a helix destabilization of about 7 kJ/mol. NMR characterization of a helical peptide with a thioxopeptide bond near the N-terminus indicates that the thioxopeptide moiety is tolerated in helical structures. The thioxoamide group is engaged in an i, i+4 hydrogen bond, arguing against the formation of a 3(10)-helical structure as suggested for the N-termini of alpha-helices in general and for thioxopeptides in particular.

Stabilizing Helical Polyalanine Peptides with Negative Polarity or Charge: Capping with Cysteine

Alanine-based peptides are widely known for their propensity to form helices, whether in the gas phase or in aqueous solution. Interactions of substituent groups or peptides with the helical macrodipole may either encourage or discourage the formation or stability of a helix, depending upon the placement of these groups. We report the first study of the inductive stabilization of a number of peptides through electronegative or anionic N-terminal residue capping. Using Charmm27/CMAP equilibrium and replica-exchange (REX) molecular dynamics (MD) simulations with Generalized Born implicit solvation methods, we find that the N-terminal cysteine capping of alanine peptides strongly enhances the helicity, even allowing the helical moiety to remain at temperatures beyond the denaturing temperature. Though the overall number of hydrogen bonds is enhanced, this stabilization seems to occur indirectly through interaction with the helical macrodipole rather than as a direct result of hydrogen bonding involving the cysteine, though the nature of the hydrogen bonding changes.

Conformational Properties of a Peptide Model for Unfolded α-Helices

Models of protein folding often hypothesize that the first step is local secondary structure formation. The assumption is that unfolded polypeptide chains possess an intrinsic propensity to form these local secondary structures. On the basis of this idea, it is tempting to model the local conformational properties of unfolded proteins using well-established residue secondary structure propensities, in particular, alpha-helix forming propensities. We have used spectroscopic methods to investigate the conformational behavior of a host-guest series of peptides designed to model unfolded alpha-helices. A suitable peptide model for unfolded alpha-helices was determined from studies of the length dependence of the conformational properties of alanine-based peptides. The chosen host peptide possessed a small, detectable, alpha-helix content. Substituting various representative guest residues into the central position of the host peptide at times changed the conformational behavior dramatically, and often in ways that could not be predicted from known alpha-helix forming propensities. The data presented can be used to rationalize some of these propensities. However, it is clear that secondary structure propensities cannot be used to predict the local conformational properties of unfolded proteins.

Acidic‐basic properties of three alanine‐based peptides containing acidic and basic side chains: Comparison between theory and experiment

The purpose of this work was to evaluate the effect of the nature of the ionizable end groups, and the solvent, on their acid-base properties in alanine-based peptides. Hence, the acid-base properties of three alanine-based peptides: Ac-KK-(A)(7)-KK-NH(2) (KAK), Ac-OO-(A)(7)-DD-NH(2) (OAD), Ac-KK-(A)(7)-EE-NH(2) (KAE), where A, D, E, K, and O denote alanine, aspartic acid, glutamic acid, lysine, and ornithine, respectively, were determined in water and in methanol by potentiometry. With the availability of these data, the ability of two theoretical methods to simulate pH-metric titration of those peptides was assessed: (i) the electrostatically driven Monte Carlo method with the ECEPP/3 force field and the Poisson-Boltzmann approach to compute solvation energy (EDMC/PB/pH), and (ii) the molecular dynamics method with the AMBER force field and the Generalized Born model (MD/GB/pH). For OAD and KAE, pK(a1) and pK(a2) correspond to the acidic side chains. For all three compounds in both solvents, the pK(a1) value is remarkably lower than the pK(a) of a compound modeling the respective isolated side chain, which can be explained by the influence of the electrostatic field from positively charged ornithine or lysine side chains. The experimental titration curves are reproduced well by the MD/GB/pH approach, the agreement being better if restraints derived from NMR measurements are incorporated in the conformational search. Poorer agreement is achieved by the EDMC/PB/pH method.

Influence of charge and size of terminal amino‐acid residues on local conformational states and shape of alanine‐based peptides

We present results of conformational studies by Circular dichroism and NMR spectroscopy, differential scanning calorimetry, and molecular dynamics, of three alanine-based peptides: Ac-KK-(A)(7)-KK-NH(2) (KAK), Ac-OO-(A)(7)-DD-NH(2) (OAD), and Ac-KK-(A)(7)-EE-NH(2) (KAE), where A, K, O, D, and E, denote alanine, lysine, ornithine, aspartic acid, and glutamic acid residues, respectively. For OAD and KAE, canonical MD simulations with time-averaged NMR-derived restraints demonstrate the presence of an ensemble of structures with a variety of conformational states (polyproline II, alpha-helical, alpha', and extended, turn); for KAK the conformational states are predominantly polyproline II and extended. The OAD peptide exhibits a bent shape with its ends close to each other, whereas KAK and KAE are more extended. The bent shape was also observed in our earlier study of the Ac-XX-(A)(7)-OO-NH(2) (XAO) peptide, where X denotes the diaminobutyric acid residue; therefore, the shape seems to depend on the size of the charged side chains at the ends of the alanine sequence and not on their kind. This suggests that the bent shape of the alanine sequence is formed to enable screening of this nonpolar sequence from the solvent by sufficiently short charged side chains. As in our previous study of the XAO peptide, no long polyproline II segments were observed.

The Reversal by Sulfate of the Denaturant Activity of Guanidinium

Guanidinium (Gdm+) chloride is a powerful protein denaturant, whereas the sulfate dianion (SO42-) is a strong stabilizer of folded protein states; Gdm2SO4 is effectively neutral in its effects on protein stability. While the "neutralizing" effects of protein-stabilizing solutes on the activity of denaturants can be broadly interpreted in terms of additive effects of the solutes, recent experimental and simulation studies support a role for hetero-ion interactions in the effect of sulfate on Gdm+ denaturation [Mason, P. E.; et al. J. Phys. Chem. B 2005, 109, 24185-24196]. Here we describe an experimental strategy for testing this mechanism that involves spectroscopic analysis of the separate effects of alkali metal sulfates (Na2SO4, Rb2SO4), GdmCl, and Gdm2SO4 on the folded populations of several peptides chosen to dissect specific noncovalent contributions to the conformational stability of proteins [alanine-based helical peptides stabilized by hydrogen bonds, tryptophan zipper (trpzip) peptides stabilized largely by cross-strand indole-indole interactions]. While the trpzip peptides are highly sensitive to GdmCl denaturation, they are unaffected by NaCl, Na2SO4, or Gdm2SO4, indicating that the reversal of the denaturant activity of Gdm+ by sulfate in this case is not due to competing stabilizing (sulfate) and destabilizing (Gdm+) interactions. Gdm2SO4 was found to retain considerable denaturant activity against alanine-based alpha-helical peptides. The differences in the effects of Gdm2SO4 on the two peptide types can be understood in terms of the different mechanisms of Gdm+ denaturation of trpzip peptides and helical peptides, respectively, and the specific nature of Gdm+ and SO42- ionic "clustering" that differentially affects the ability of Gdm+ to make the molecular interactions with the peptides that underlie its denaturant activity.

The Effect of Charge-Charge Interactions on the Kinetics of α-Helix Formation

The formation of the monomeric α-helix represents one of the simplest scenarios in protein folding; however, our current understanding of the folding dynamics of the α-helix motif is mainly based on studies of alanine-rich model peptides. To examine the effect of peptide sequence on the folding kinetics of α-helices, we studied the relaxation kinetics of a 21-residue helical peptide, Conantokin-T (Con-T), using time-resolved infrared spectroscopy in conjunction with a laser-induced temperature jump technique. Con-T is a neuroactive peptide containing a large number of charged residues that is found in the venom of the piscivorous cone snail Conus tulipa. The temperature-jump relaxation kinetics of Con-T is distinctly slower than that of previously studied alanine-based peptides, suggesting that the folding time of α-helices is sequence-dependent. Furthermore, it appears that the slower folding of Con-T can be attributed to the fact that its helical conformation is stabilized by charge-charge interactions or salt bridges. Although this finding contradicts an earlier molecular dynamics simulation, it also has implications for existing models of protein folding.

Infrared Study of the Effect of Hydration on the Amide I Band and Aggregation Properties of Helical Peptides

The amide I' band of a polypeptide is sensitive not only to its secondary structure content but also to its environment. In this study we show how degrees of hydration affect the underlying spectral features of the amide I' band of two alanine-based helical peptides. This is achieved by solubilizing these peptides in the water pool of sodium bis(2-ethylhexyl)sulfosuccinate reverse micelles with different water contents or w0 values. In agreement with several earlier studies, our results show that the amide I' band arising from a group of dehydrated helical amides is centered at approximately 1650 cm-1, whereas hydration shifts this frequency toward lower wavenumbers. More importantly, temperature-dependent infrared studies further show that these helical peptides undergo a thermally induced conformational transition in reverse micelles of low w0 values (e.g., w0=6), resulting in soluble peptide aggregates rich in antiparallel beta-sheets. Interestingly, however, increasing w0 or water content leads to an increase in the onset temperature at which such beta-aggregates begin to form. Therefore, these results provide strong evidence suggesting that dehydration facilitates aggregate formation and that removal of water imposes a free energy barrier to peptide association and aggregation, a feature that has been suggested in recent simulation studies focusing on the mechanism of beta-amyloid formation.

Further Evidence for the Absence of Polyproline II Stretch in the XAO Peptide

It has been suggested that the alanine-based peptide with sequence Ac-XX-[A] 7-OO-NH 2, termed XAO where X denotes diaminobutyric acid and O denotes ornithine, exists in a predominantly polyproline-helix (P II) conformation in aqueous solution. In our recent work, we demonstrated that this “polyproline conformation” should be regarded as a set of local conformational states rather than as the overall conformation of the molecule. In this work, we present further evidence to support this statement. Differential scanning calorimetry measurements showed only a very small peak in the heat capacity of an aqueous solution of XAO at 57°C, whereas the suggested transition to the P II structure should occur at ∼30°C. We also demonstrate that the temperature dependence of the 3 J HNH α coupling constants of the alanine residues can be explained qualitatively in terms of Boltzmann averaging over all local conformational states; therefore, this temperature dependence proves that a conformational transition does not occur. Canonical MD simulations with the solvent represented by the generalized Born model, and with time-averaged NMR-derived restraints, demonstrate the presence of an ensemble of structures with a substantial amount of local P II conformational states but not with an overall P II conformation.

Peptide Bond Vibrational Coupling

Neutral trialanine (Ala3), which is geometrically constrained to have its peptide bond at Phi and Psi angles of alpha-helix and PPII-like conformers, are studied at the B3LYP/6-31+G(d,p) level of theory to examine vibrational interactions between adjacent peptide units. Delocalization of the amide I, amide II, and amide III3 vibrations are analyzed by calculating their potential energy distributions (PED). The vibrational coupling strengths are estimated from the frequency shifts between the amide vibrations of Ala3 and the local amide bond vibrations of isotopically substituted Ala3 derivatives. Our calculations show the absence of vibrational coupling of the amide I and amide II bands in the PPII conformations. In contrast, the alpha-helical conformation shows strong coupling between the amide I vibrations due to the favorable orientation of the C=O bonds and the strong transitional dipole coupling. The amide III3 vibration shows weak coupling in both the alpha-helix and PPII conformations; this band can be treated as a local independent vibration. Our calculated results in general agree with our previous experimental UV Raman studies of a 21-residue mainly alanine-based peptide (AP).

Folding and unfolding of a photoswitchable peptide from picoseconds to microseconds.

Using time-resolved IR spectroscopy, we monitored the kinetics of folding and unfolding processes of a photoswitchable 16-residue alanine-based alpha-helical peptide on a timescale from few picoseconds to almost 40 micros and over a large temperature range (279-318 K). The folding and unfolding processes were triggered by an ultrafast laser pulse that isomerized the cross linker within a few picoseconds. The main folding and unfolding times (700 ns and 150 ns, respectively, at room temperature) are in line with previous T-jump experiments obtained from similar peptides. However, both processes show complex, strongly temperature-dependent spectral kinetics that deviate clearly from a single-exponential behavior. Whereas in the unfolding experiment the ensemble starts from a well defined folded state, the starting ensemble in the folding experiment is more heterogeneous, which leads to distinctly different kinetics of the experiments, because they are sensitive to different regions of the energy surface. A qualitative agreement with the experimental data-set can be obtained by a model where the unfolded states act as a hub connected to several separated "misfolded" states with a distribution of rates. We conclude that a rather large spread of rates (k(1) : k(n) approximately 9) is needed to explain the experimentally observed stretched exponential response with stretching factor beta = 0.8 at 279 K.

Examination of the Folding of a Short Alanine-Based Helical Peptide with Salt Bridges Using Molecular Dynamics Simulation

A molecular dynamics simulation of the folding of a short alanine-based helical peptide of 17 residues with three Glu...Lys (i, i + 4) salt bridge pairs, referred to as the AEK17 peptide, was carried out. The simulation gave an estimated simulation folding time of 2.5 ns, shorter than 12 ns for an alanine-based peptide of 16 residues with three Lys residues only, referred to as the AK16 peptide, simulated previously. After folded, the AEK17 peptide had a helical content of 77%, in excellent agreement with the experimentally determined value of 80%. An examination of the folding pathways of AEK17 indicated that the peptide proceeded via three-turn helix conformations more than the helix-turn-helix conformation in the folding pathways. An analysis of interactions indicated that the formation of hydrogen bonds between Lys residue side chains and backbone carbonyls is a major factor in the abundant conformation of the three-turn helix intermediate. The substitution of three Ala with Glu residues reduces the extent of hydrophobic interaction in alanine-based AK peptides with the result that the breaking of the interactions of Lys epsilon-NH3+(side chain)...C=O(backbone) is a major activation action for the AEK17 to achieve a complete fold, in contrast to the AK16 peptide, in which breaking non-native hydrophobic interaction is the rate-determining step.

Possible mechanisms for protecting N [sbnd]C α bonds in helical peptides from electron-capture (or transfer) dissociation

Ab initio electronic structure simulations are carried out on small alanine-based peptide fragments with an excess electron added to a Coulomb-stabilized amide OCN π* orbital that forms a C O − radical anion center. A focus of the study is to determine to what extent and by what means helix-involved N C α bonds are “protected” against cleavage compared to similar bonds in non-helical peptides. The primary findings, many of which support earlier suggestions, include: (1) There is little or no increase in the energy barriers for N C α bond cleavage caused by an amino acid being in a helix where its carbonyl oxygen is involved in a hydrogen bond to an H N bond of an amino acid displaced by one helix turn. (2) When an electron attaches to a helix-involved Coulomb-stabilized OCN π* orbital and the N C α bond cleaves, three hydrogen bonds act to bind together the c and z fragment ions. One of these hydrogen bonds is especially strong (ca. 16 kcal mol −1) because it involves a negatively charged oxygen center. This suggests that the “protection” against N C α cleavage of helix-involved amino acids may, as others suggested earlier, result from the strong hydrogen bonding that binds the c and z fragment ions. (3) When an electron attaches to a helix-involved OCN π* orbital, an electron can migrate to the π* orbital of another amino acid one turn down the helix, but only by overcoming a barrier. After migrating to a new amino acid, N C α cleavage can occur at the latter site, also in line with what earlier workers have suggested. Suggestions of experiments that might test the hypotheses treated here are also put forth.

Conformations of Alanine-Based Peptides in Water Probed by FTIR, Raman, Vibrational Circular Dichroism, Electronic Circular Dichroism, and NMR Spectroscopy

We have used a combination of FTIR, VCD, ECD, Raman, and NMR spectroscopies to probe the solution conformations sampled by H-(AAKA)-OH by utilizing an excitonic coupling model and constraints imposed by the 3JCalphaHNH coupling constants of the central residues to simulate the amide I' profile of the IR, isotropic Raman, anisotropic Raman, and VCD spectra in terms of a mixture of three conformations, i.e., polyproline II, beta-strand and right-handed helical. The representative coordinates of the three conformations were obtained from published coil libraries. Alanine was found to exhibit PPII fractions of 0.60 or greater, mixed with smaller fractions of helices and beta-strand conformations. Lysine showed no clear conformational propensity in that it samples polyproline II, beta-strand, and helical conformations with comparable probability. This is at variance with results obtained earlier for ionized polylysine, which suggest a high polyproline II propensity. We reanalyzed previously investigated tetra- and trialanine by combining published vibrational spectroscopy data with 3JCalphaHNH coupling constants and obtained again blends dominated by PPII with smaller admixtures of beta-strand and right-handed helical conformations. The polyproline II propensity of alanine was found to be higher in tetraalanine than in trialanine. For all peptides investigated, our results rule out a substantial population of turn-like conformations. Our results are in excellent agreement with MD simulations on short alanine peptides by Gnanakaran and Garcia [(2003) J. Phys. Chem. B 107, 12555-12557] but at variance with multiple MD simulations particularly for the alanine dipeptide.

Helix Propensity of Highly Fluorinated Amino Acids

Highly fluorinated amino acids have been used to stabilize helical proteins for potential application in various protein-based biotechnologies. To gain further insight into the effect of these highly fluorinated amino acids on helix formation exclusively, we measured the helix propensity of three highly fluorinated amino acids: (S)-5,5,5,5',5',5'-hexafluoroleucine (Hfl), (S)-2-amino-4,4,4-trifluorobutyric acid (Atb), and (S)-pentafluorophenylalanine (Pff). We have developed a short chemoenzymatic synthesis of Hfl with extremely high enantioselectivity (>99%). To measure the helix propensity (w) of the amino acids, alanine-based peptides were synthesized, purified, and investigated by circular dichroism spectroscopy (CD). On the basis of the CD data, the helix propensity of hydrocarbon amino acids can decrease up to 24-fold (1.72 kcal.mol-1.residue-1) upon fluorination. This difference in helix propensity has previously been overlooked in estimating the magnitude of the fluoro-stabilization effect (which has been estimated to be 0.32-0.83 kcal.mol-1.residue-1 for Hfl), resulting in a gross underestimation. Therefore, the full potential of the fluoro-stabilization effect should provide even more stable proteins than the fluoro-stabilized proteins to date.

Electron capture dissociation mass spectrometry of peptide cations containing a lysine homologue: a mobile proton model for explaining the observation of b‐type product ions

Eleven doubly protonated peptides with a residue homologous to lysine were investigated by electron capture dissociation mass spectrometry (ECD-MS). Lysine homologues provide the unique opportunity to examine the ECD fragmentation behavior by allowing us to vary the length of the lysine side chain, with minimal structural change. The lysine homologue has a primary amine side chain with a length that successively decreases by one methylene (CH(2)) unit from the --CH(2)CH(2)CH(2)CH(2)NH(2) of lysine and the accompanying decrease of its proton affinities: lysine (K), 1006.5(+/-7.2) kJ/mol; ornithine (K(*)), 1001.1(+/-6.6) kJ/mol; 2,4-diaminobutanoic acid (K(**)), 975.8(+/-7.4) kJ/mol; 2,3-diaminopropanoic acid (K(***)), 950.2(+/-7.2) kJ/mol. In general, the lysine-homologous peptides exhibited overall ECD fragmentation patterns similar to that of the lysine-containing peptides in terms of the locations, abundances, and ion types of products, such as yielding c(+) and z(+.) ions as the dominant product ions. However, a close inspection of product ion mass spectra showed that ECD-MS for the alanine-rich peptides with an ornithinyl or 2,4-diaminobutanoyl residue gave rise to b ions, while the lysinyl-residue-containing peptides did not, in most cases, produce any b ions. The peptide selectivity in the generation of b(+) ions could be understood from within the framework of the mobile proton model in ECD-MS, previously proposed by Cooper (Ref. 29). The exact mass analysis of the resultant b ions reveals that these b ions are not radical species but rather the cationic species with R-CO(+) structure (or protonated oxozalone ion), that is, b(+) ions. The absence of [M+2H](+.) species in the ECD mass spectra and the selective b(+)-ion formation are evidence that the peptides underwent H-atom loss upon electron capture, and then the resulting reduced species dissociated following typical MS/MS fragmentation pathways. This explanation was further supported by extensive b(+) ions generated in the ECD of alanine-based peptides with extended conformations.

Modeling of Folding and Unfolding Mechanisms in Alanine-Based α-Helical Polypeptides

alpha-Helix formation is known to be opposed by the entropy loss due to the folding and favored by the energy of molecular interactions. However, the underlying mechanism of these factors is still being discussed. Here we have used the experimental and calculation data for short alanine-based peptides embedded in water to model the mechanism of helix folding and unfolding and to calculate microscopically the free energy factors of alanine in the frame of helix coil conformational integrals. Classical helix-coil transition theories take into account the interactions in a peptide chain only if the i, i + 3 peptide bond participates in hydrogen bonding. But quantum mechanical calculations showed that interactions of the i, i + 2 peptide bond play an important role in helix folding too. We also included the short-range repulsive interactions due to molecular steric clashes and the end effects due to polar/hydrogen-bonding interactions at the N and C termini. The helix and coil regions of peptide conformational space were defined using an experimental steric criterion for hydrogen bonding. Arginine helix propensity was discussed and estimated. Monte Carlo numerical simulations of thermodynamics and kinetics for the 21 amino acid alpha-helical polypeptide Ac-A5(AAARA)3A-NMe were carried out and found to be in an agreement with the experimental results.

Unfolding of Alanine-Based Peptides Using Electron Spin Resonance Distance Measurements

We describe a scheme for tagging an alanine-based peptide with a Cu(II) and a nitroxide to measure unfolding transitions. The enhancement in longitudinal relaxation rate of the nitroxide due to the presence of Cu(II) was measured at physiological temperatures by pulsed electron spin resonance (ESR). The change in relaxation rate provided the average interspin distance between the Cu(II) and the nitroxide. Control experiments on a proline-based peptide verify the robustness of the method. The change in interspin distances with temperature for the alanine-based peptide is in accord with the change in helicity measured by circular dichroism. The data provide an opportunity to examine the unfolding process in polyalanine peptides. The distance in the folded state is in concordance with molecular dynamics. However, the ESR experiment measures an average distance of 17 A in the unfolded state, whereas molecular dynamics indicates a distance of 42 A if the unfolded geometry was a polyproline type II helix. Therefore, ESR demonstrates that the unfolded state of this alanine-based peptide is not an ideal extended polyproline type II helix.

Structural Characterization of α-Helices of Implicitly Solvated Poly-Alanine

The structural characteristics of alpha-helices in poly-alanine-based peptides have been investigated via molecular dynamics simulation with the goal of understanding the basic features of peptide simulations within the context of a model system, classical molecular dynamics with generalized Born (GB) solvation, and to shed insight into the formation and stabilization of alpha-helices in short peptides. The effects of peptide length, terminal charges, proline substitution, and temperature on the alpha-helical secondary structure have been studied. The simulations have shown that distinct secondary structure begins to develop in peptides with lengths approaching 10 residues while ambiguous structures occur in shorter peptides. The helical content of peptides with lengths > or =10 amino acids is observed to be nearly constant up to (Ala)(40). Interestingly, terminal charges and proline in the second position from the N-terminus alter the secondary structure locally with little effect on the overall alpha-helical content of the peptide. The free energy profile of helix formation was also investigated. A large increase in free energy accompanying the formation of helices with more than two consecutive hydrogen bonds in the (i, i + 4) pattern was observed while the free energy increases linearly with additional hydrogen bonds. Values for the change in enthalpy and entropy of helix nucleation and propagation are reported. Additionally the results obtained from the GB model are compared to explicit solvent simulations of two synthetic alanine-based peptides.

Polyproline II conformation is one of many local conformational states and is not an overall conformation of unfolded peptides and proteins.

The alanine-based peptide Ac-XX(A)7OO-NH2, referred to as XAO (where X, A, and O denote diaminobutyric acid, alanine, and ornithine, respectively), has recently been proposed to possess a well defined polyproline II (P(II)) conformation at low temperatures. Based on the results of extensive NMR and CD investigations combined with theoretical calculations, reported here, we present evidence that, on the contrary, this peptide does not have any significant amount of organized P(II) structure but exists in an ensemble of conformations with a distorted bend in the N- and C-terminal regions. The conformational ensemble was obtained by molecular dynamics/simulated annealing calculations using the amber suite of programs with time-averaged distance and dihedral-angle restraints obtained from rotating-frame nuclear Overhauser effect (ROE) volumes and vicinal coupling constants 3J(HN Eta alpha), respectively. The computed ensemble-averaged radius of gyration Rg (7.4 +/- 1.0) A is in excellent agreement with that measured by small-angle x-ray scattering (SAXS) whereas, if the XAO peptide were in the P(II) conformation, Rg would be 11.6 A. Depending on the pH, peptide concentration, and temperature, the CD spectra of XAO do or do not possess the maximum with positive ellipticity in the 217-nm region, which is characteristic of the P(II) structure, reflecting a shifting conformational equilibrium rather than an all-or-none transition. The "P(II) conformation" should, therefore, be considered as one of the accessible conformational states of individual amino acid residues in peptides and proteins rather than as a structure of most of the chain in the early stage of folding.