Triaspartate: a model system for conformationally flexible DDD motifs in proteins.

Understanding the interactions that govern turn formation in the unfolded state of proteins is necessary for a complete picture of the role that these turns play in both normal protein folding and functionally relevant yet disordered linear motifs. It is still unclear, however, whether short peptides can adopt stable turn structures in aqueous environments in the absence of any nonlocal interactions. To explore the effect that nearest-neighbor interactions and the local peptide environment have on the turn-forming capability of individual amino acid residues in short peptides, we combined vibrational (IR, Raman, and VCD), UV-CD, and (1)H NMR spectroscopies in order to probe the conformational ensemble of the central aspartic acid residue of the triaspartate peptide (DDD). The study was motivated by the recently discovered turn propensities of aspartic acid in GDG (Hagarman; et al. Chem.-Eur. J. 2011, 17, 6789). We investigated the DDD peptide under both acidic and neutral conditions in order to elucidate the effect that side-chain protonation has on the conformational propensity of the central aspartic acid residue. Amide I' profiles were analyzed in terms of two-dimensional Gaussian distributions representing conformational subdistributions in Ramachandran space. Interestingly, our results show that while the protonated form of the DDD peptide samples various turn-like conformations similar to GDG, deprotonation of the peptide eliminates this propensity for turns, causing the fully ionized peptide to exclusively sample pPII and ß-strand-like structures. To further explore the factors stabilizing these more extended conformations in fully ionized DDD, we analyzed the temperature dependence of both the UV-CD spectrum and the (3)J(H(N),H(α)) coupling constants of the two amide protons (N- and C-terminal) in terms of a simple two-state (pPII-ß) thermodynamic model. Thus, we were able to obtain the enthalpic and entropic differences between the pPII and ß-strand conformations of the central and C-terminal residue. For the central residue, we obtained ΔH(3) = -12.0 kJ/mol and ΔS(3) = -73.8 J/mol·K, resulting in a much larger room-temperature Gibbs free energy of 10.0 kJ/mol, which effectively locks the C-terminal in a ß-like conformation. A comparison of the temperature dependence of the chemical shifts reveals that there is indeed some type of protection of the amide protons from solvent in ionized DDD. This finding and several other lines of evidence suggest that both conformations of ionized DDD are stabilized by hydrogen bonding between the carboxylate groups of the central and C-terminal residue and the respective amide protons. These hydrogen bonds can be expected to be eliminated by side-chain protonation and substituted by hydrogen bonds between the N-terminal amide proton and the C-terminal carbonyl group as well as between the central aspartate side chain and the N-terminal amide proton. Hence, our results are indicative of a pH-induced switch in hydrogen-bonding patterns of aspartic acid motifs.

Kinetics of the self-aggregation and film formation of poly-L-proline at high temperatures explored by circular dichroism spectroscopy.

Poly-L-proline has been used as a model system for various purposes over a period of more than 60 years. Its relevance among the protein/peptide community stems from its use as a reference system for determining the conformational distributions of unfolded peptides and proteins, its use as a molecular ruler, and from the pivotal role of proline residues in conformational transitions and protein-protein interactions. While several studies indicate that polyproline can aggregate and precipitate in aqueous solution, a systematic study of the aggregation process is still outstanding. We found, by means of UV-circular dichroism and IR measurements, that polyproline is predominantly monomeric at room temperature at millimolar concentrations. Upon heating, the polypeptide stays in its monomeric state until the temperature reaches a threshold of ca. 60 degrees C. At higher temperatures, the peptide aggregates as a film on the inside surface of the employed cuvette. The process proceeds on a time scale of 10(3) s and can best be described by a bi-exponential relaxation function. The respective CD and IR spectra are qualitatively different from the canonical spectra of polyproline in aqueous solution, and are indicative of a highly packed state.

The conformational manifold of ferricytochrome c explored by visible and far-UV electronic circular dichroism spectroscopy.

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 different intensities of the Cotton bands of the respective B-band transitions. Differences between the ECD intensities of the B-bands of the different unfolded states and alkaline states most likely reflect different degrees of openness of the corresponding heme crevice.