A sequence of seven alanine residues-too short to form an ␣-helix and whose side chains do not interact with each other-is a particularly simple model for testing the common description of denatured proteins as structureless random coils. The 3 JHN␣ coupling constants of individual alanine residues have been measured from 2 to 56°C by using isotopically labeled samples. The results display a thermal transition between different backbone conformations, which is confirmed by CD spectra. The NMR results suggest that polyproline II is the dominant conformation at 2°C and the content of ␤ strand is increased by approximately 10% at 55°C relative to that at 2°C. The polyproline II conformation is consistent with recent studies of short alanine peptides, including structure prediction by ab initio quantum mechanics and solution structures for both a blocked alanine dipeptide and an alanine tripeptide. CD and other optical spectroscopies have found structure in longer ''random coil'' peptides and have implicated polyproline II, which is a major backbone conformation in residues within loop regions of protein structures. Our result suggests that the backbone conformational entropy in alanine peptides is considerably smaller than estimated by the random coil model. New thermodynamic data confirm this suggestion: the entropy loss on alanine helix formation is only 2.2 entropy units per residue. T anford's pioneering experiments on denatured proteins in 6 M guanidinium chloride (GdmCl) (1-5) were interpreted by using the random coil model, and they anchored a widespread belief that denatured proteins are structureless chains. Tanford emphasized that 6 M GdmCl is required to eliminate all residual structure, which was detected by optical rotatory dispersion in heat-denatured proteins (6). The random coil model has been applied to modern NMR studies of backbone conformation in denatured proteins (7,8) by assuming that the backbone conformations found in protein structures, including or excluding regions of regular secondary structure, are represented with the same frequencies in denatured proteins. One might suppose, however, that the energy differences between major backbone conformations are sufficiently large to favor one conformation over others, at least in a homopeptide.We address this question by using NMR to investigate the backbone conformation as a function of temperature for a sequence of seven alanine residues in a peptide solubilized in water by two basic residues at either end of the alanine sequence. This peptide presents an appealing model system for a structureless denatured protein. It is too short to form any detectable ␣-helix in water via peptide hydrogen bonds; moreover, the OCH 3 side chain is too short to form nonpolar clusters and too inert to form other side chain interactions. To characterize the backbone conformations of this peptide, we measure system properties that are related directly to either the or the backbone angles. It is possible today to resolve and assign most backbone resonances of de...

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There is growing appreciation of the functional relevance of unfolded proteins in biology. However, unfolded states of proteins have proven inaccessible to the usual techniques for high-resolution structural and energetic characterization. Unfolded states are still generally conceived of as statistical coils, based on the pioneering work of Flory [(1969 T he process by which a protein acquires its native structure is among the most complex reactions known, and challenges remain in defining the nature of the transition state(s), the structure and role of intermediates, and the properties of the starting ensemble of states (1-4). According to Flory (5) and Tanford (6), unfolded proteins can be represented as statistical random coils, in which a given residue has no strong preference for any specific conformation. Confirming earlier conclusions by Tiffany and Krimm (7-9), recent evidence from a variety of spectroscopic probes (10-22), theoretical studies (23-34), and coil library surveys (35-43) consistently point to a major role for the polyproline II (PPII, ⌽ ϭ Ϫ75°, ⌿ ϭ ϩ145°) conformation in oligo-Ala (for review, see ref. 3 and related articles in the same volume), oligo-Lys, and oligo-Glu peptides (44). We have reported that in a seven-Ala peptide model PPII converts to a ␤-like structure with increasing temperature (13). These findings raise several important questions regarding the structure of unfolded proteins: Although alanine is arguably a reasonable model for the unperturbed peptide backbone, is PPII also present in unfolded peptide chains composed of nonalanine nonproline residues? Is there an intrinsic PPII propensity for each individual side chain? If PPII is in equilibrium with ␤-structure, is there a correlation between scales of PPII propensity and analogous ␤-sheet scales? To what extent is PPII sequence and context dependent?Here, we address these questions by analyzing a series of end-blocked host pentapeptides AcGGXGGNH 2 , where X denotes 19 natural amino acids except glycine. Members of the series are found to differ in their extent of PPII conformation as determined by NMR and CD spectroscopy. Our results lead to the following conclusions: PPII is present as a dominant conformation in the majority of AcGGXGGNH 2 peptides. Different side chains show distinct propensities to adopt PPII in these unfolded molecules. Importantly, we find an inverse correlation between the determined PPII scale and the ␤-sheet-forming propensities derived from a zinc-finger model system (45) when 18 aa (except Gly and Pro) are divided into two groups: one, the nonpolar ␤-branched and bulky aromatic residues (VIWFY) and the other all of the remaining side chains. Finally, we find a correlation between our PPII scale in AcGGXGGNH 2 and a PPII scale derived from alternative model peptides such as AcPPPXPPPGYNH 2 (46). Still there are indications that the PPII scale is likely to be sequence and context dependent (47). Materials and MethodsPeptides Synthesis and Purification. Peptides were assembled on Rink Amide res...

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Cation-pi interactions are increasingly recognized as important in chemistry and biology. Here we investigate the cation-pi interaction by determining its effect on the helicity of model peptides using a combination of CD and NMR spectroscopy. The data show that a single Trp/Arg interaction on the surface of a peptide can make a significant net favorable free energy contribution to helix stability if the two residues are positioned with appropriate spacing and orientation. The solvent-exposed Trp-->Arg (i, i + 4) interaction in helices can contribute -0.4 kcal/mol to the helix stability, while no free energy gain is detected if the two residues have the reversed orientation, Arg-->Trp (i, i + 4). The derived free energy is consistent with other experimental results studied in proteins or model peptides on cation-pi interactions. However in the same system the postulated Phe/Arg (i, i + 4) cation-pi interaction provides no net free energy to helix stability. Thus the Trp-->Arg interaction is stronger than Phe-->Arg. The cation-pi interactions are not sensitive to the screening effect by adding neutral salt as indicated by salt titration. Our results are in qualitative agreement with theoretical calculations emphasizing that cation-pi interactions can contribute significantly to protein stability with the order Trp > Phe. However, our and other experimental values are significantly smaller than estimates from theoretical calculations.

Most of what we know about proteins reflects their native folded structure. Much less is understood about the structure of unfolded proteins, which tends to be referred to as "random coil", lacking extended alpha-helix or beta-strand structure. Recent work suggests that unfolded proteins might adopt significant population of PII structure, an extended left-handed helix found in collagen and proline-rich peptides. A series of short peptides AcGGXGGNH2 has been adopted as a model for studying unfolded protein structure because of the minimal steric effect imposed by flanking glycines. Peptide AcGGAGGNH2 makes possible a host-guest conformation analysis of the middle residue alanine. NMR experiments reveal that the Phi and Psi dihedral angles of the central alanine are -73 degrees and 125 degrees , respectively, placing the alanine in the PII region of the Ramachandran plot. Circular dichroism shows a typical PII spectrum with a strong negative absorbance at 190 nm. Temperature experiments show the alanine structure shifts to increasing beta-strand at high temperature. Because the alanine side chain most closely represents unsubstituted peptide backbone, these results have significant implications for the conformational entropy of unfolded polypeptide chains.

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Alanine residues in two model peptides, the pentapeptide AcGGAGGNH(2) and the 11mer AcO(2)A(7)O(2)NH(2), have been reported to have substantial PII conformation in water. The PII structure in both peptides is sensitive to solvent. In the presence of the organic solvent TFE, the conformation of the pentamer changes from PII to internally H-bonded gamma or beta turns, while the chain with seven alanines forms alpha helix. The PII structure in the 11mer is more stable than that in the shorter peptide as the TFE concentration increases. For the pentamer, a comparison of short-chain aliphatic alcohols to water shows that the PII content decreases in the order water > methanol > ethanol > 2-propanol, linearly according to empirical scales of solvent polarity. Thus, depending on the extent of local solvation as folding progresses, the peptide backbone as modeled by alanine oligomers shifts from PII to internally H-bonded (gamma or beta turn) conformations and to alpha helix in longer segments. On the other hand, the PII content of AcO(2)A(7)O(2)NH(2) increases significantly in the presence of guanidine, as does that of oligoproline peptides, while detergent sodium dodecyl sulfate (SDS) favors alpha helix in this peptide. The shorter peptide does not show a parallel increase in PII with guanidine.