A reliable intrinsic propensity scale of amino acid residues is indispensable for an assessment of how local conformational distributions in the unfolded state can affect the folding of peptides and proteins. Short host-guest peptides, such as GxG tripeptides, are suitable tools for probing such propensities. To explore the conformational distributions sampled by the central amino acid residue in these motifs, we combined vibrational (IR, Raman, and VCD) with NMR spectroscopy. The data were analyzed in terms of a superposition of two-dimensional Gaussian distribution functions in the Ramachandran space pertaining to subensembles of polyproline II, beta-strand, right- and left-handed helical, and gamma-turn-like conformations. The intrinsic propensities of eight amino acid residues (x = A, V, F, L, S, E, K, and M) in GxG peptides were determined as mole fractions of these subensembles. Our results show that alanine adopts primarily (approximately 80%) a PPII-like conformation, while valine and phenylalanine were found to sample PPII and beta-strand-like conformations equally. The centers of the respective beta-strand distributions generally do not coincide with canonical values of dihedral angles of residues in parallel or antiparallel beta-strands. In fact, the distributions for most residues found in the beta-region significantly overlap the PPII-region. A comparison with earlier reported results for trivaline reveals that the terminal valines increase the beta-strand propensity of the central valine residue even further. Of the remaining investigated amino acids, methionine preferred PPII the most (0.64), and E, S, L, and K exhibit moderate (0.56-0.45) PPII propensities. Residues V, F, S, E, and L sample, to a significant extent, a region between the canonical PPII and (antiparallel) beta-strand conformations. This region coincides with the sampling reported for L and V using theoretical predictions (Tran et al. Biochemistry 2005, 44, 11369). The distributions of all investigated residues differ from coil library and computationally predicted distributions in that they do not exhibit a substantial sampling of helical conformations. We conclude that this sampling of helical conformations arises from the context dependence, for example, neighboring residues, in proteins and longer peptides, some of which is long-range.

Local structure in unfolded proteins, especially turn segments, has been suggested to initiate the hierarchical protein-folding process. To determine the intrinsic propensity to form such turn structures, amide I' band profiles of the Raman, IR, and vibrational circular dichroism (VCD) spectra, and several structure-sensitive NMR J-coupling constants, have been measured for a series of GxG (x=D, N, T, C) peptides, in which the central x residues are abundant in various turn motifs in folded proteins. In addition, we revisited earlier measured GSG experimental data. To check whether this relatively high propensity for these residues to sample turns reflects an intrinsic propensity, the experimental data were analyzed in terms of conformational distributions that can be described as a superposition of two-dimensional Gaussian distributions associated with different so-called mesostates. The analysis reveals that the investigated residues sample dihedral angles similar to those found in the corner residues of various turns, namely, type I/I', II/II', and IV β-turns. Aspartic acid (D) was found to predominantly sample regions attributed to turns, including distributions at the upper border of the upper-right quadrant of the Ramachandran plot, which bear some resemblance to asx-turns observed in proteins. This conformation enables hydrogen bonding between the side-chain carboxylate and the C-terminal amide group. Altogether, the study shows that the high propensity for T, S, C, N, and D to be located in turn motifs reflects, to a substantial degree, an intrinsic property and supports the role of these residues as initiation sites for hierarchical folding processes that can lead to compact structures in the unfolded state of peptides and proteins.

We performed a conformational analysis of the central residues of three tripeptides glycyl-L-isoleucyl-glycine (GIG), glycyl-L-tyrosyl-glycine (GYG) and glycyl-L-arginyl-glycine (GRG) in aqueous solution, based on a global analysis of amide I' band profiles and NMR J-coupling constants. The results are compared with recently reported distributions of GVG, GFG and GEG. For GIG and GYG, we found that even though the polyproline II (pPII) fraction is below 0.5, it is still the most populated conformation, whereas GVG and GFG show both a larger β-strand fraction. For GRG, we observed a clear dominance of pPII over β-strand, reminiscent of observations for GEG and GKG. This finding indicates that terminal charges on otherwise hydrophobic residue side chains stabilize pPII over β-strand conformations. For all peptides investigated we found that a variety of compact and turn-like conformations constitute nearly 20 percent of their conformational distributions. Attempts to analyze our data with a simple two-state pPII-->/<--β model therefore do not yield any satisfactory reproduction of experimental results. A comparison of the obtained GxG ensembles with conformational distributions of GxG segments in truncated coil libraries (helices and sheets omitted) revealed a much larger fraction of type II β(i+2) and type III β like conformations for the latter. Thus, a comparison of conformational distributions of unfolded peptide segments in solution and in coil libraries reveal interesting information on how the interplay between intrinsic propensities of amino acid residues and non-local interactions in polypeptide chains determine the conformations of loop segments in proteins.

We have measured the electronic circular dichroism (ECD) of the ferri- and ferro-states of several natural cytochrome c derivatives (horse heart, chicken, bovine, and yeast) and the Y67F mutant of yeast in the region between 300 and 750 nm. Thus, we recorded the ECD of the B- and Q-band region as well as the charge-transfer band at approximately 695 nm. The B-band region of the ferri-state displays a nearly symmetric couplet at the B0-position that overlaps with a couplet 790 cm-1 higher in energy, which we assigned to a vibronic side-band transition. For the ferro-state, the couplet is greatly reduced, but still detectable. The B-band region is dominated by a positive Cotton effect at energies lower than B0 that is attributed to a magnetically allowed iron-->heme charge-transfer transition as earlier observed for nitrosyl myoglobin and hemoglobin. The Q-band region of the ferri-state is poorly resolved, but displays a pronounced positive signal at higher wavenumbers. This must result from a magnetically allowed transition, possibly from the methionine ligand to the dxy-hole of Fe3+. For the ferro-state, the spectra resolve the vibronic structure of the Qv-band. A more detailed spectral analysis reveals that the positively biased spectrum can be understood as a superposition of asymmetric couplets of split Q0 and Qv-states. Substantial qualitative and quantitative differences between the respective B-state and Q-state ECD spectra of yeast and horse heart cytochrome c can clearly be attributed to the reduced band splitting in the former, which results from a less heterogeneous internal electric field. Finally, we investigated the charge-transfer band at 695 nm in the ferri-state spectrum and found that it is composed of at least three bands, which are assignable to different taxonomic substates. The respective subbands differ somewhat with respect to their Kuhn anisotropy ratio and their intensity ratios are different for horse and yeast cytochrome c. Our data therefore suggests different substate populations for these proteins, which is most likely assignable to a structural heterogeneity of the distal Fe-M80 coordination of the heme chromophore.

We measured the temperature-dependent electronic circular dichroism (ECD) spectra of AX, XA, and XG dipeptides in D2O. The spectra of all XA and AX peptides indicate a substantial population of the polyproline II (PPII) conformation, while the ECD spectra of LG, KG, PG, and AG were found to be quantitatively different from the alanine-based dipeptides. Additional UV absorption data indicate that the ECD spectra of the XG peptides stem from electronic coupling between the peptide and the C-terminal group, and that spectral differences reflect different orientations of the latter. We also measured the 1H NMR spectra of the investigated dipeptides to determine the 3JHalphaNH coupling constants for the C-terminal residue. The observed temperature dependence of the ECD spectra and the respective room-temperature 3JHalphaNH coupling constants were analyzed by a two-state model encompassing PPII and a beta-like conformation. The PPII propensity of alanine in the XA series is only slightly modulated by the N-terminal side chain, and is larger than 50%. As compared to AA, XA peptides containing L, P, S, K V, E, T, and I all cause a relative stabilization of the extended beta-strand conformation. The PPII fractions of XA peptides varied between 0.64 for AA and 0.58 for DA, whereas the PPII fractions of AX peptides were much lower. From the investigated AX peptides, only AL and AQ showed the expected PPII propensity. We found that AT, AI, and AV clearly prefer an extended beta-strand conformation. A quantitative comparison of AA, AAA, and AAAA revealed a hierarchy AAAA > AAA approximately AA for the PPII population, in agreement with predictions from MD calculations and results from Raman optical activity studies (McColl et al. J. Am. Chem. Soc. 2004, 126, 5076).

We have measured and analyzed the low-temperature (T=10 K) absorption spectrum of reduced horse heart and yeast cytochrome c. Both spectra show split and asymmetric Q(0) and Q(upsilon) bands. The spectra were first decomposed into the individual split vibronic sidebands assignable to B(1g) (nu15) and A(2g) (nu19, nu21, and nu22) Herzberg-Teller active modes due to their strong intensity in resonance Raman spectra acquired with Q(0) and Q(upsilon) excitations. The measured band splittings and asymmetries cannot be rationalized solely in terms of electronic perturbations of the heme macrocycle. On the contrary, they clearly point to the importance of considering not only electronic perturbations but vibronic perturbations as well. The former are most likely due to the heterogeneity of the electric field produced by charged side chains in the protein environment, whereas the latter reflect a perturbation potential due to multiple heme-protein interactions, which deform the heme structure in the ground and excited states. Additional information about vibronic perturbations and the associated ground-state deformations are inferred from the depolarization ratios of resonance Raman bands. The results of our analysis indicate that the heme group in yeast cytochrome c is more nonplanar and more distorted along a B(2g) coordinate than in horse heart cytochrome c. This conclusion is supported by normal structural decomposition calculations performed on the heme extracted from molecular-dynamic simulations of the two investigated proteins. Interestingly, the latter are somewhat different from the respective deformations obtained from the x-ray structures.

The oxidized state of cytochrome c is a subject of continuous interest, owing to the multitude of conformations which the protein can adopt in solution and on surfaces of artificial and cell membranes. The structural diversity corresponds to a variety of functions in electron transfer, peroxidase and apoptosis processes. In spite of numerous studies, a comprehensive analysis and comparison of native and non-native states of ferricytochrome c has thus far not been achieved. This results in part from the fact that the influence of solvent conditions (i.e., ionic strength, anion concentration, temperature dependence of pH values) on structure, function and equilibrium thermodynamics has not yet been thoroughly assessed. The current study is a first step in this direction, in that it provides the necessary experimental data to compare different non-native states adopted at high temperature and alkaline pH. To this end, we employed visible electronic circular dichroism (ECD) and absorption spectroscopy to probe structural changes of the heme environment in bovine and horse heart ferricytochrome c as a function of temperature between 278 and 363 K at different neutral and alkaline pH values. A careful selection of buffers enabled us to monitor the partial unfolding of the native state at room temperature while avoiding a change to an alkaline state at high temperatures. We found compelling evidence for the existence of a thermodynamic intermediate of the thermal unfolding/folding process, termed III h, which is structurally different from the alkaline states, IV 1 and IV 2, contrary to current belief. At neutral or slightly acidic pH, III h is populated in a temperature region between 320 and 345 K. The unfolded state of the protein becomes populated at higher temperatures. The ECD spectra of the B-bands of bovine and horse heart cytochrome c (pH 7.0) exhibit a pronounced couplet that is maintained below 343 K, before protein unfolding replaces it by a rather strong positive Cotton band. A preliminary vibronic analysis of the B-band profile reveals that the couplet reflects a B-band splitting of 350 cm (-1), which is mostly of electronic origin, due to the internal electric field in the heme cavity. Our results suggest that the conformational transition from the native state, III, into a thermally activated intermediate state, III h, does not substantially affect the internal electric field and causes only moderate rearrangements of the heme pocket, which involves changes, rather than a rupture, of the Fe (3+)-M80 linkage. In the unfolded state, as well as in the alkaline states IV and V, the band splitting is practically eliminated, but the positive Cotton effect observed for the B-band suggests that the proximal environment, encompassing H18 and the two cysteine residues 14 and 17, is most likely still intact and covalently bound to the heme chromophore. Both alkaline states IV and V were found to melt via intermediate states. Unfolded states probed at neutral and alkaline pH can be discriminated, owing to the differ...

A series of AX and XA dipeptides in D2O have been investigated by FTIR, isotropic, and anisotropic Raman spectroscopy at acidic, neutral, and alkaline pD, to probe the influence of amino acid side chains on the amide I' band. We obtained a set of spectral parameters for each peptide, including intensities, wavenumbers, half-widths, and dipole moments, and found that these amide I' parameters are indeed dependent on the side chain. Side chains with similar characteristic properties were found to have similar effects on the amide I'. For example, dipeptides with aliphatic side chains were found to exhibit a downshift of the amide I' wavenumber, while those containing polar side chains experienced an increase in wavenumber. The N-terminal charge causes a substantial upshift of amide I', whereas the C-terminal charge causes a moderate decrease of the transition dipole moment. Density functional theory (DFT) calculations on the investigated dipeptides in vacuo yielded different correlations between theoretically and experimentally obtained wavenumbers for aliphatic/aromatic and polar/charged side chains, respectively. This might be indicative of a role of the hydration shell in transferring side chain-backbone interactions. For Raman bands, we found a correlation between amide I' depolarization ratio and wavenumber which reflects that some side chains (valine, histidine) have a significant influence on the Raman tensor. Altogether, the obtained data are of utmost importance for utilizing amide I as a tool for secondary structure analysis of polypeptides and proteins and providing an experimental basis for theoretical modeling of this important backbone mode. This is demonstrated by a rather accurate modeling for the amide I' band profiles of the IR, isotropic Raman, and anisotropic Raman spectra of the beta-amyloid fragment Abeta(1-82).