Parameters of helix-coil transition theory for alanine-based peptides of varying chain lengths in water

Membrane interaction of synthetic peptides related to the putative fusogenic region of PH-30 alpha, a protein in sperm-egg fusion

In order to investigate the relationship between structure and function of a putative fusogenic region of PH-30a, a protein active in sperm-egg fusion, two peptides, SFP22 and SFP23, whose sequences correspond to the residues 90-111 and 89-111 of PH-30 alpha, respectively, were chemically synthesized. An analog of SFP23, SFP23AA, which has an Ala-Ala sequence instead of the Pro-Pro sequence in SFP23, was also prepared. The CD study indicated that SFP22 and SFP23 mainly took a beta-structure in the presence of DPPC and DPPC/DPPG (3/1) vesicles, while SFP23AA showed an alpha-helical pattern though the alpha-helical content calculated was low (25-30%). alpha-Helical CD curve was observed for these peptides in trifluoroethanol. The membrane-perturbing activity of SFP22 and SFP23 was weaker than that of SFP23AA. On the other hand, the membrane-fusogenic activity of SFP22 and SFP23 to acidic phospholipid bilayers was much stronger than that of SFP23AA. All the peptides caused very weak cell lysis. These results are consistent with the reported speculation [Blobel, C. P. et al. (1992), Nature (London) 356, 248-252] that residues 90-111 of PH-30 alpha may be the fusogenic region and suggest that the Pro-Pro sequence is one of the important factors for holding the active secondary structure of the fusogenic region of PH-30 alpha in membranes.

The stability and dynamics of ribosomal protein L9: investigations of a molecular strut by amide proton exchange and circular dichroism

Nuclear magnetic resonance and circular dichroism experiments were used to investigate the stability and dynamic aspects of ribosomal protein L9 from Bacillus stearothermophilus in solution. This unusually shaped protein, with its two widely spaced RNA-binding domains linked by a connecting helix, has been hypothesized to serve as a "molecular strut", most likely playing a role in ribosome assembly and/or maintaining the catalytically active conformation of ribosomal RNA. Protection factors for amide proton exchange were quantitatively measured in an extensive series of NMR experiments, providing probes of the stability and dynamics of localized regions of the protein. Results show that each of the two RNA-binding domains contains a highly stable core. The exposed central helix that connects the two domains is helical in solution, albeit not rigid, a result that is supported by amide proton protection factors, circular dichroism measurements, and carbon-13 and proton chemical shift index values. A conserved glycine and lysine-rich loop in the N-terminal domain is ordered and quite stable, a surprising result, since this loop had been presumed to be disordered in the original crystallographic analysis. Interestingly, the most dynamic parts of the protein are the regions that contain the likely RNA-binding residues in each of the two domains. The present results add further support to the notion that the L9 protein plays an architectural role within the ribosome, with the central helix serving as a molecular strut, or perhaps a spring, linking the two widely spaced RNA-binding domains.

NMR and circular dichroism studies on the conformation of a 44-mer peptide from a CD4-binding domain of human immunodeficiency virus envelope glycoprotein

Two-dimensional NMR, circular dichroism (CD) experiments and molecular modeling were performed to study the secondary structure of a 44-mer peptide fragment derived from the C4 region of gp120 of human immunodeficiency virus in aqueous solution. It was found a nascent helical structure exists following a type I turn near the N-terminus of the peptide. The proline residue in the turn appears to serve as a helix initiator. The helical structure was in fast dynamic equilibrium with beta- or random coil form on the NMR scale. A reverse turn was identified at a section containing two consecutive proline residues. A nascent helical structure has been detected for the region near the C-terminus of the 44-mer peptide. Higher helical content for the peptide is also indicated by CD studies on TFE titration. Thus it is proposed that, in more apolar medium, the Pro-Pro turn and the segment amino-terminal to it, spanning about 20 amino acids, may be converted into helix structure. Moreover, the region near the C-terminus of the peptide may also be induced into helix, so that a helix-turn-helix structure may be formed in the C4 domain of gp120. A helical wheel representation of this stretch shows amphipathicity of the helix. The biological implication of the conformational adaptibility of the peptide was discussed.

Formation of a molten-globule-like state of myoglobin in aqueous hexafluoroisopropanol

The effects of aqueous hexafluoroisopropanol (HFIP) media on the structure of myoglobin are reported. Circular dichroism (CD) spectra of this alpha-helical protein in as little as 4% (v/v) HFIP indicate that native-like amounts of secondary structure remain while rigid tertiary structure is lost. However, thermal studies suggest some residual cooperativity of unfolding in this state. At much higher HFIP concentrations, the helicity exceeds the native value and the protein behaves as a series of independent helices which do not interact with each other. We did not observe cold denaturation of myoglobin, even though this phenomenon has been observed for molten globule states of myoglobin, as well as for monomeric amphipathic alpha-helices when moderate quantities of HFIP are present. The pH dependence of trifluoroethanol-induced disruption of tertiary structure revealed that the degree of disruption increases as the enthalpic advantage of the folded state is diminished at low pH.

Development of the multiple sequence approximation within the AGADIR model of alpha-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 (AGADIRls) within the framework of AGADIR's alpha-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 AGADIRls. The other energy contributions to alpha-helix stability are not affected by the original statistical approximation. We also discuss the particularities of the model for alpha-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 alpha-helix formation.

Conformation of a protein kinase C substrate NG(28-43), and its analog in aqueous and sodium dodecyl sulfate micelle solutions

A peptide corresponding to the neuronal protein neurogranin (NG) residues 28-43, NG(28-43), and its analog, [A35]NG(28-43), have been investigated by NMR, electron paramagnetic resonance (EPR), and circular dichroism (CD) spectroscopies. The peptides existed in aqueous solution predominantly in random form. However, a nascent helical structure was detected in the central region of the parent peptide from NMR data. Furthermore, a helical structure can be detected for both peptides with greater induced secondary structure for the parent peptide in the presence of sodium dodecyl sulfate (SDS) micelle. The formation of micelles for SDS was confirmed by results from EPR as well as 13C NMR. As shown by CD experiments, helical conformer was induced for NG(28-43) in vesicular solution containing phosphatidyl serine (PS), whereas no helix can be discerned for the peptide in phosphatidyl choline (PC)-containing vesicular solution. Together with the induction of the peptide into helix in SDS micellar solution as suggested by both NMR and CD data, these results underscored the electrostatic contribution to the interaction of the PKC substrate peptides and proteins with membrane. According to NMR and CD data, a dynamic equilibrium existed between free and micelle-bound states for the peptide. Moreover, proton-deuterium exchange results and SDS-induced linewidth broadening of proton resonances allowed delineation of the orientation of the amphipathic helix on the surface of SDS micelle. The result was supported by spin label experiments that indicated F35 of NG(28-43) interacted strongly with the hydrocarbon interior of micelle. Based on the experimental findings, a working model was proposed that attempted to partly explain the roles played by the nonpolar amino acid near the phosphorylation site, by the negatively charged phospholipids, and by the basic amino acids of the substrate.

Spectroscopic studies of the C-terminal secretion signal of the Serratia marcescens haem acquisition protein (HasA) in various membrane-mimetic environments

The structure of a peptide comprising the last 56 C-terminal residues of the Serratia marcescens haem acquisition protein (HasA) secreted by an ATP-binding cassette exporter was examined by 1H-NMR, circular dichroic and fluorescence spectroscopies. The peptide, which contains the secretion signal of HasA, is efficiently secreted by the HasA transporter. It is largely unstructured and flexible in aqueous buffer solution, but its helical content increases upon addition of trifluoroethanol, detergents and lipids. By circular dichroism, a stable helical conformation is observed between 20% and 70% (by vol.) trifluoroethanol. The 1H-NMR spectrum was analysed at these two trifluoroethanol concentrations; residues 7-15, 21-30 and 40-50 were shown to form relatively stable helices. In the presence of neutral detergent, alpha-helix is induced to a similar extent upon micelle formation; in this case, fluorescence data indicate that at least the N-terminus of the peptide interacts with the micelle. In the presence of negatively charged detergent, alpha-helix is induced before micelle formation and the N-terminus of the peptide seems not to be involved in this interaction. In the presence of negatively charged liposomes, the peptide interacts with the vesicle, again inducing a helical conformation. However, the helical content remains lower than upon addition of trifluoroethanol or neutral micelles. These results are compared to those previously obtained with the secretion signal of one of the Erwinia chrysanthemi metalloproteases which are transported efficiently by the HasA transporter. Both signals exhibit similar conformational features, despite their low sequence similarity.

The interactions with solvent, heat stability, and 13C-labelling of alamethicin, an ion-channel-forming peptide

The peptide alamethicin was labelled with 13C and 15N by growing the fungus Trichoderma viride in a medium containing [U-13C] glucose and K15NO3. Spin-echo difference spectroscopy showed that 13C was incorporated to a level of about 50% and 15N to about 98%. Incorporation of 13C into the peptide provided residue-specific probes of the interactions with solvent and heat stability of this ion-channel-forming peptide. All of the carbonyl carbons and the alpha-carbons of the alpha-aminoisobutyric acid [Ala(Me)] residues of alamethicin in methanol were assigned using two-dimensional and three-dimensional heteronuclear correlation experiments. Measurements of 1JC'N revealed hydrogen bonding with solvent at residues 1 and 19 at the ends of the peptide and at Gly11 in the middle. The data also support the thesis [see Juranic, N., Ilich, P. K. & Macara, S. (1995) J. Am. Chem. Soc. 117, 405-410 that intramolecular hydrogen bonds in proteins and peptides are weaker than hydrogen bonds to solvent. The sensitivity of alamethicin carbonyl and proton chemical shifts to perturbation by dimethyl sulfoxide correlates well with the calculated solvent accessibilities of the carbonyls in the crystal structures and reveals residues in the middle of the peptide and at the C-terminus which interact with solvent. Taken together with the 1JC'N measurements, the data support a model in which hydrogen bonding to solvent at the Gly11/Leu12 amide could provide a site of hydration in the interior of the alamethicin channel structure. The temperature dependencies of the carbonyl chemical shifts support the suggestion that the peptide is flexible in the regions where solvent interacts with the backbone of the peptide. The linear temperature dependence of the carbonyl chemical shifts and molar ellipticity indicate that, due to steric constraints at the Ala(Me) residues, the peptide folding/unfolding transition is non-cooperative and that the peptide is remarkably heat stable.

Local interactions in a Schellman motif dictate interhelical arrangement in a protein fragment

BACKGROUND

As an approach to understanding the role of local sequence in determining protein tertiary structure, we have examined the conformation of a 23-residue peptide fragment corresponding to the structurally conserved helix-Schellman motif-helix (H-Sm-H) domain (residue 10-32) of cellular retinoic acid binding protein, along with variants designed to probe the contributions of the helix-terminating Gly23 and the hydrophobic interactions between Leu 19 and Val24 in stabilizing the Schellman motif and hence helix termination.

RESULTS

In aqueous solution, NMR data for the H-Sm-H peptide show that it samples a largely helical conformation with a break in the helix at the point of the turn in the protein. The data also establish the presence of local hydrophobic interactions and intramolecular hydrogen bonds characteristic of a Schellman motif. Absence of helix termination in trifluoroethanol, a solvent known to disrupt hydrophobic interactions, along with an analysis of H alpha chemical shifts and NOEs in the variant peptides, suggest a major role for glycine in terminating the helix, with local hydrophobic interactions further stabilizing the Schellman motif.

CONCLUSIONS

The presence of a Schellman motif in this isolated fragment in water is governed by local interactions and specifies the interspatial arrangement of the helices. This observation underlines the structure predictive value of folding motifs. As proposed for a Schellman motif, helix termination in this fragment is dictated by the local distribution of polar/apolar residues, which is reminiscent of the binary code for protein folding.

Efforts toward deriving the CD spectrum of a 3(10) helix in aqueous medium

There have been two recent reports suggesting that 3(10) helices can be distinguished from alpha helices by circular dichroism. The differentiating feature is stated to be a [theta]222:[theta]208 ratio (R2) distinctly smaller than unity. This has been reported for a C(alpha)alpha'-disubstituted homooctamer [Toniolo et al. (1996), J. Am. Chem. Soc. 118, 2744-2745] and for alanine-rich systems of 16-21 residue length with modest fractional helicity [Millhauser (1995) Biochemistry 34, 3873-3877]. We report here the changes in the CD spectrum produced by inserting aminoisobutyric acid (Aib) residues into the helical domain of human pancreatic amylin. In order to examine this effect at comparable net fractional helicities, CD spectra were measured for each species during the course of a helicity titration by trifluoroethanol addition. The addition of five Aib residues gave results of particular interest. At low net fractional helicity, this Aib-rich system displays a diminished pi-->pi* (circa 208 nm) rotational strength versus the less Aib-rich species. However, NMR data and comparisons of CD difference spectra suggest that fluoroalcohol-induced extension of the short Aib-rich helix is in the form of an alpha helix. Given the diminished intensity of the minimum at 208 nm at low net helicity when 3(10) conformations should contribute, we urge extreme caution in using a [theta]222:[theta]208 ratio smaller than unity as a diagnostic for 3(10) helices.

Helix propagation and N-cap propensities of the amino acids measured in alanine-based peptides in 40 volume percent trifluoroethanol

The helix propagation and N-cap propensities of the amino acids have been measured in alanine-based peptides in 40 volume percent trifluoroethanol (40% TFE) to determine if this helix-stabilizing solvent uniformly affects all amino acids. The propensities in 40% TFE are compared with revised values of the helix parameters of alanine-based peptides in water. Revision of the propensities in water is the result of redefining the capping statistical weights and evaluating the helix nucleation constant with N-capping explicitly included in the helix-coil model. The propagation propensities of all amino acids increase in 40% TFE relative to water, but the increases are highly variable. In water, all beta-branched and beta-substituted amino acids are helix breakers. In 40% TFE, the propagation propensities of the nonpolar amino acids increase greatly, leaving charged and neutral polar, beta-substituted amino acids as helix breakers. Glycine and proline are strong helix breakers in both solvents. Free energy differences for helix propagation (delta delta G) between alanine and other nonpolar amino acids are twice as large in water as predicted from side-chain conformational entropies, but delta delta G values in 40% TFE are close to those predicted from side-chain entropies. This dependence of delta delta G on the solvent points to a specific role of water in determining the relative helix propensities of the nonpolar amino acids. The N-cap propensities converge toward a common value in 40% TFE, suggesting that differential solvation by water contributes to the diversity of N-cap values shown by the amino acids.

Structure of a methionine-rich segment of Escherichia coli Ffh protein

The methionine-rich segments of the Ffh protein of Escherichia coli and its eukaryotic counterpart SRP54 are thought to bind signal sequences of secretory proteins. The structure of a chemically synthesized 25-residue-long peptide corresponding to one of the proposed methionine-rich amphiphilic helices of Ffh was determined in water and in aqueous trifluroethanol (TFE) solution using CD and NMR. An appreciable alpha-helix conformation exists even in water and this peptide assumes a stable alpha-helix along most of its length in aqueous TFE solution. It is clear that this segment of Ffh protein has a very strong propensity to form alpha-helical structure.

Predicted and trifluoroethanol-induced alpha-helicity of polypeptides

The alpha-helix stabilizing solvent 2,2,2-trifluoroethanol (TFE) is frequently used as a medium for determining the average alpha-helicity of polypeptides by CD spectroscopy. CD spectra measured in solutions containing 10, 15, 20, 50, and 90% (vol/vol) TFE are presented for 5 peptides that were selected to demonstrate possible variations in the effect of TFE concentration on the secondary structure. The analysis is extended to 6 further peptides whose CD spectra as measured in TFE are documented in the literature. The observed alpha-helicity at a high TFE concentration is compared with the alpha-helicity determined by a structure prediction method that combines conformational filtering [S. Vajda, (1993) Journal of Molecular Biology, Vol. 229, pp. 125-145], and a Monte Carlo simulation [J. Figge et al. (1993) Protein Science, Vol. 2, pp. 155-164]. For the set of 11 peptides we find a correlation of 0.84 between the predicted [theta]222 values and the corresponding values observed by CD spectroscopy in a high concentration of TFE (p < 0.01). Although we generally find a good correlation at high TFE concentration between observed and predicted alpha-helicity, there are several peptides that do not follow the predicted behavior. An analysis of the TFE titration curves in one such case revealed that TFE can induce a sharp transition from a partial beta-sheet conformation to an alpha-helical conformation as the TFE concentration is increased above a critical value.

Target recognition by calmodulin: dissecting the kinetics and affinity of interaction using short peptide sequences

The interaction between calmodulin (CaM) and peptide M13, its target binding sequence from skeletal muscle myosin light chain kinase, involves predominantly two sets of interactions, between the N-terminal target residues and the C-domain of calmodulin, and between the C-terminal target residues and the N-domain of calmodulin (Ikura M et al., 1992, Science 256:632-638). Using short synthetic peptides based on the two halves of the target sequence, the interactions with calmodulin and its separate C-domain have been studied by fluorescence and CD spectroscopy, calcium binding, and kinetic techniques. Peptide WF10 (residues 1-10 of M13) binds to CaM with Kd approximately 1 microM; peptide FW10 (residues 9-18 of M13, with Phe-17-->Trp substitution) binds to CaM with Kd approximately 100 microM. The effect of peptide WF10 on calcium binding to calmodulin produces a biphasic saturation curve, with marked enhancement of affinity for the binding of two calcium ions to the C-domain, forming a stable half-saturated complex, Ca2-CaM-peptide, and confirming the functional importance of the interaction of this sequence with the C-domain. Stopped-flow studies show that the EGTA-induced dissociation of WF10 from Ca4-CaM proceeds by a reversible relaxation mechanism from a kinetic intermediate state, also involving half-saturation of CaM, and the same mechanism is evident for the full target peptide. Interaction of the N-terminal target residues with the C-domain is energetically the most important component, but interaction of calmodulin with the whole target sequence is necessary to induce the full cooperative interaction of the two contiguous elements of the target sequence with both N- and C-domains of calmodulin. Thus, the interaction of calmodulin with the M13 sequence can be dissected on both a structural and kinetic basis into partial reactions involving intermediates comprising distinct regions of the target sequence. We propose a general mechanism for the calcium regulation of calmodulin-dependent enzyme activation, involving an intermediate complex formed by interaction of the calmodulin C-domain and the corresponding part of the target sequence. This intermediate species can function to regulate the overall calcium sensitivity of activation and to determine the affinity of the calmodulin target interaction.

Synthesis of alpha-helix-forming peptides by gene engineering methods and their characterization by circular dichroism spectra measurements

Two kinds of peptides which were considered to form alpha-helices were designed and characterized. One was "alpha(3)-peptide' with 21 residues comprising three repeats of the seven-residue sequence Leu-Glu-Thr-Leu-Ala-Lys-Ala. This peptide appeared to be amphipathic due to a hydrophobic surface of Leu residues and a hydrophilic surface of Lys and Glu residues, thus forming a bundle structure. The other was "alpha(3)-GPRRG-alpha(3) peptide' with 47 residues in which two alpha(3)-peptides were connected by the five-residue sequence Gly-Pro-Arg-Arg-Gly. The genes encoding these peptides were fused to the adenylate kinase gene via a methionine codon. The resulting fused protein was expressed as an inclusion body, and the peptides were purified after cleavage with BrCN. The stability of the peptides in various buffers was then examined by measuring their circular dichroism spectra. The alpha(3)-peptide showed concentration-dependent stabilization of the alpha-helix. Sedimentation equilibrium ultracentrifugation indicated that it formed a bundle structure composed of four polypeptide chains, and a dimer intermediate during oligomerization was also detected by analytical gel-filtration. The stability of the alpha(3)-peptide was decreased by shifting the pH to 2 or 12, due to electrostatic repulsion of charged residues. Thus, the alpha(3)-peptide was stabilized by increasing the ionic strength, particularly in acidic or alkaline buffer, through the masking of the repulsion by high salt concentration. In buffer of neutral pH and a high salt concentration, the alpha(3)-peptide at high concentration formed visible aggregates, due possibly to the exposed hydrophobic surfaces of the alpha-helical bundles. On the other hand, alpha(3)-GPRRG-alpha(3) peptide did not show concentration-dependent reversible dissociation and association. It was shown to exist as a trimer even at low concentration, indicating very tight association of the alpha(3)-GPRRG-alpha(3) peptide. In contrast to the alpha(3)-peptide, the alpha(3)-GPRRG-alpha(3) peptide was very stable at various pH values and salt concentrations. This seemed to be due to increased hydrophobic interactions resulting from the increase in the number of seven-residue repeats from three to six, even though each group of three repeats was separated by a five-residue sequence.

Template-nucleated alanine-lysine helices are stabilized by position-dependent interactions between the lysine side chain and the helix barrel

The helicity in water has been determined for several series of alanine-rich peptides that contain single lysine residues and that are N-terminally linked to a helix-inducing and reporting template termed Ac-Hel1. The helix-propagating constant for alanine (sAla value) that best fits the properties of these peptides lies in the range of 1.01-1.02, close to the value reported by Scheraga and coworkers [Wojcik, J., Altmann, K.-H. & Scheraga, H.A. (1990) Biopolymers 30, 121-134], but significantly lower than the value assigned by Baldwin and coworkers [Chakrabartty, A., Kortemme, T. & Baldwin, R.L. (1994) Protein Sci. 3,843-852]. From a study of conjugates Ac-Hel1-Ala(n)-Lys-Ala(m)-NH2 and analogs in which the methylene portion of the lysine side chain is truncated, we find that the unusual helical stability of Ala(n)Lys peptides is controlled primarily by interactions of the lysine side chain with the helix barrel, and only passively by the alanine matrix. Using 1H NMR spectroscopy, we observe nuclear Overhauser effect crosspeaks consistent with proton-proton contacts expected for these interactions.

High helicity of peptide fragments corresponding to beta-strand regions of beta-lactoglobulin observed by 2D-NMR spectroscopy

BACKGROUND

Whereas protein fragments, when they are structured, adopt conformations similar to that found in the native state, the high helical propensity of beta-lactoglobulin, a predominantly beta-sheet protein, suggested that the fragments of beta-lactoglobulin can assume the non-native helical conformation. In order to assess this possibility, we synthesized four 17-18-residue peptides corresponding to three beta-strand regions and one helical region (as a control) of beta-lactoglobulin and examined their conformation.

RESULTS

We observed residual helicities of up to 17% in water, by far-UV CD, for all four peptide fragments. The helices could be significantly stabilized by the addition of TFE, and the NMR analyses in a mixture of 50% water/TFE indicated that helical structures are formed in the central region whereas both termini are frayed. Thus, the very same residues that form strands in the native beta-lactoglobulin showed high helical preferences.

CONCLUSIONS

These results stand out from the current general view that peptide fragments isolated from proteins either are unfolded or adopt native-like secondary structures. The implications of the results in the mechanism of protein folding and in designing proteins and peptides are significant.

Addition of side chain interactions to modified Lifson-Roig helix-coil theory: application to energetics of phenylalanine-methionine interactions

We introduce here i, i + 3 and i, i + 4 side chain interactions into the modified Lifson-Roig helix-coil theory of Doig et al. (1994, Biochemistry 33:3396-3403). The helix/coil equilibrium is a function of initiation, propagation, capping, and side chain interaction parameters. If each of these parameters is known, the helix content of any isolated peptide can be predicted. The model considers every possible conformation of a peptide, is not limited to peptides with only a single helical segment, and has physically meaningful parameters. We apply the theory to measure the i, i + 4 interaction energies between Phe and Met side chains. Peptides with these residues spaced i, i + 4 are significantly more helical than controls where they are spaced i, i + 5. Application of the model yields delta G for the Phe-Met orientation to be -0.75 kcal.mol-1, whereas that for the Met-Phe orientation is -0.54 kcal.mol-1. These orientational preferences can be explained, in part, by rotamer preferences for the interacting side chains. We place Phe-Met i, i + 4 at the N-terminus, the C-terminus, and in the center of the host peptide. The model quantitatively predicts the observed helix contents using a single parameter for the side chain-side chain interaction energy. This result indicates that the model works well even when the interaction is at different locations in the helix.

Characterization of leucine zipper complexes by electrospray ionization mass spectrometry

The development of "soft" ionization methods has enabled the mass spectrometric analysis of higher-order structural features of proteins. We have applied electrospray ionization mass spectrometry (ESI-MS) to the analysis of the number and composition of polypeptide chains in homomeric and heteromeric leucine zippers. In comparison with other methods that have been used to analyze leucine zippers, such as analytical ultracentrifugation, gel chromatography, or electrophoretic band shift assays, ESI-MS is very fast and highly sensitive and provides a straightforward way to distinguish between homomeric and heteromeric coiled-coil structures. ESI-MS analyses were carried out on the parallel dimeric leucine zipper domain GCN4-p1 of the yeast transcription factor GCN4 and on three synthetic peptides with the sequences Ac-EYEALEKKLAAX1EAKX2QALEKKLEALEHG-amide: peptide LZ (X1, X2 = Leu), peptide LZ(12A) (X1 = Ala, X2 = Leu), and peptide LZ(16N) (X1 = Leu, X2 = Asn). Equilibrium ultracentrifugation analysis showed that LZ forms a trimeric coiled coil and this could be confirmed unequivocally by ESI-MS as could the dimeric nature of GCN4-p1. The formation of heteromeric two- and three-stranded leucine zippers composed of chains from LZ and LZ(12A), or from GCN4-p1 and LZ, was demonstrated by ESI-MS and confirmed by fluorescence quenching experiments on fluorescein-labeled peptides. The results illustrate the adaptability and flexibility of the leucine zipper motif, properties that could be useful to the design of specific protein assemblies by way of coiled-coil domains.

N- and C-capping preferences for all 20 amino acids in alpha-helical peptides

We have determined the N- and C-capping preferences of all 20 amino acids by substituting residue X in the peptides NH2-XAKAAAAKAAAAKAAGY-CONH2 and in Ac-YGAAKAAAAKAAAAKAX-CO2H. Helix contents were measured by CD spectroscopy to obtain rank orders of capping preferences. The data were further analyzed by our modified Lifson-Roig helix-coil theory, which includes capping parameters (n and c), to find free energies of capping (-RT ln n and -RT ln c), relative to Ala. Results were obtained for charged and uncharged termini and for different charged states of titratable side chains. N-cap preferences varied from Asn (best) to Gln (worst). We find, as expected, that amino acids that can accept hydrogen bonds from otherwise free backbone NH groups, such as Asn, Asp, Ser, Thr, and Cys generally have the highest N-cap preference. Gly and acetyl group are favored, as are negative charges in side chains and at the N-terminus. Our N-cap preference scale agrees well with preferences in proteins. In contrast, we find little variation when changing the identity of the C-cap residue. We find no preference for Gly at the C-cap in contrast to the situation in proteins. Both N-cap and C-cap results for Tyr and Trp are inaccurate because their aromatic groups affect the CD spectrum. The data presented here are of value in rationalizing mutations at capping sites in proteins and in predicting the helix contents of peptides.

Alpha-helix formation by peptides of defined sequence

The factors controlling alpha-helix formation in water by peptides of defined sequence are beginning to be understood. The field is close to the point where the extent of helix formation can be predicted for peptides of any sequence. Our own approach to the problem, and the main results obtained by following this approach, are summarized below. The chief reason for studying alpha-helix formation by peptides is to understand precisely and in detail one part of the protein folding problem. Questions about peptide helix formation can be answered at a fundamental level, in terms of the physico-chemical mechanisms involved.

Models of cooperativity in protein folding

What is the basis for the two-state cooperativity of protein folding? Since the 1950s, three main models have been put forward. 1. In 'helix-coil' theory, cooperativity is due to local interactions among near neighbours in the sequence. Helix-coil cooperativity is probably not the principal basis for the folding of globular proteins because it is not two-state, the forces are weak, it does not account for sheet proteins, and there is no evidence that helix formation precedes the formation of a hydrophobic core in the following pathways. 2. In the 'sidechain packing' model, cooperativity is attributed to the jigsaw-puzzle-like complementary fits of sidechains. This too is probably not the basis of folding cooperativity because exact models and experiments on homopolymers with sidechains give no evidence that sidechain freezing is two-state, sidechain complementarities in proteins are only weak trends, and the molten globule model predicted by this model is far more native-like than experiments indicate. 3. In the 'hydrophobic core collapse' model, cooperativity is due to the assembly of non-polar residues into a good core. Exact model studies show that this model gives two-state behaviour for some sequences of hydrophobic and polar monomers. It is based on strong forces. There is considerable experimental evidence for the kinetics this model predicts: the development of hydrophobic clusters and cores is concurrent with secondary structure formation. It predicts compact denatured states with sizes and degrees of disorder that are in reasonable agreement with experiments.

Principles of protein folding--a perspective from simple exact models

General principles of protein structure, stability, and folding kinetics have recently been explored in computer simulations of simple exact lattice models. These models represent protein chains at a rudimentary level, but they involve few parameters, approximations, or implicit biases, and they allow complete explorations of conformational and sequence spaces. Such simulations have resulted in testable predictions that are sometimes unanticipated: The folding code is mainly binary and delocalized throughout the amino acid sequence. The secondary and tertiary structures of a protein are specified mainly by the sequence of polar and nonpolar monomers. More specific interactions may refine the structure, rather than dominate the folding code. Simple exact models can account for the properties that characterize protein folding: two-state cooperativity, secondary and tertiary structures, and multistage folding kinetics--fast hydrophobic collapse followed by slower annealing. These studies suggest the possibility of creating "foldable" chain molecules other than proteins. The encoding of a unique compact chain conformation may not require amino acids; it may require only the ability to synthesize specific monomer sequences in which at least one monomer type is solvent-averse.

Kinetics of folding of leucine zipper domains

Leucine zippers are short coiled coils frequently found in transcription factors where they serve as dimerization domains. The basic features contributing to the thermodynamic stability of leucine zippers are well understood, but very little is known about their folding kinetics. Leucine zippers have a simple and well defined structure and are, therefore, excellent models for the study of the concerted folding and assembly of polypeptide chains. Here we report on a fluorescence stopped flow investigation of the kinetics of association and dissociation of a series of model leucine zippers based on the common sequence Xzero-EYEALEKKLAAX1EAKX2QALEKKLEALEHG-amide (Xzero = N alpha-acetyl, N alpha-fluorescein-GGG, or N alpha-dimethylaminocoumarin-GGG; Xl = Leu or Ala; X2 = Leu, Ala, or Asn). When Xzero is fluorescein, self-quenching between adjacent fluorophores leads to a decrease in fluorescence emission intensity whereas unfolding of the coiled coil leads to an increase. In a heteromeric coiled coil containing both fluorophores, resonance energy transfer between the donor coumarin and the acceptor fluorescein is observed, and the mixing of labeled and nonlabeled peptides allows the measurement of the rates of strand exchange between leucine zippers. Exchange rates do not depend on peptide concentration, indicating that strand exchange is governed by the rate of dissociation of the coiled coil. Strand exchange between leucine zippers with X1 and X2 = Leu occurs with a half-time of approximately 30 min. A single Leu/Ala substitution at X1 or X2 decreases the half-time to approximately 1 s. Folding was also studied in a relaxation experiment in which a preexisting equilibrium between monomeric chains and coiled coils was rapidly disturbed by dilution with buffer, and the relaxation to the new equilibrium was followed by the increase in fluorescence. In peptides with X1, X2 = Ala or X1 = Ala, X2 = Asn the folding process can be described by a simple two-state monomer<-->dimer equilibrium with k(on) approximately 4 x 10(6) M-1 s-1 and k(off) approximately 10 s-1. Kd = k(off)/k(on) approximately 2.5 microM is in good agreement with the value of Kd obtained from equilibrium measurements. The peptides with a single Ala at X1 or X2 exhibit biphasic folding kinetics. One phase is concentration dependent and the other apparently concentration independent. This behavior can be interpreted as a monomer<-->dimer equilibrium coupled to an equilibrium between different conformational isomers. Leu to Ala and Leu to Asn substitutions in the hydrophobic core alter the folding kinetics in a position-dependent manner.(ABSTRACT TRUNCATED AT 400 WORDS)

The receptor binding affinity of monocyclic [Ala3,Xaa11]endothelin-1 analogs correlates with inducible helix length

Endothelin-1, a bicyclic 21-amino acid peptide with disulfide bridges between cysteines 1 and 15 as well as between cysteines 3 and 11, has been reported to be partially helical based on both CD and NMR data. However, this remains an area of controversy with some claims that CD data indicate no alpha-helical structure (Calas, B.; Harricane, M.-C.; Gulmard, L.; Heitz, F.; Mendre, C.; Chabrier, P.E.; Bennes, R. Peptide Res. 1992, 5, 97) and a recent X-ray crystal structure placing the helix at a different locus (Janes, R.W.; Peapus, D.H.; Wallace, B.A. Structural Biology 1994, 1, 311). The CD studies reported herein indicate that the helical structures reported in NMR studies (e.g. Andersen, N.H.; Chen, C.; Marschner, T.M.; Krystek, Jr. S.R.; Bassolino, D.A. Biochemistry 1992, 31, 1280) apply to pure aqueous media as well. The helix located from Lys9 to the Cys15/His16 juncture is ca 75% populated in pH 4 aqueous buffer. Titration difference CDs reveal that the helix extent increases by one to two residues and that the 'helical conformation' is more completely populated upon addition of TFE to 50+ volume-%. Comparison with a more helical analog suggests that the helix propagates towards (but not to the end of) the C-terminus upon fluoroalcohol addition. A variety of monocyclic derivatives of [Nle7] ET-1 lacking the 3,11-disulfide were evaluated for biological activity and examined by TFE titration difference CD. The series included an Aib11 and a Pro11 analog. The helix promoting Aib analog was the most active while the Pro analog exhibited significantly lower vasoconstrictor activity and binding affinity for the ETA receptor. All of the monocyclic analogs became significantly more helical upon addition of fluoroalcohols. The inclusion of a proline residue at position 11 does not preclude helix formation upon addition of fluoroalcohols. Rather, helix formation is relatively easily induced but limited to a 5 residue span. Apparently this is insufficient to orient required side chains optimally for interaction with the ETA receptor. For the 1,15-monocyclic analogs differing only at position 11, ETA binding affinity and vasoconstrictor potency correlate with the facility which a 7-8 residue long helix can be induced. This presumably includes the segment Glu10-->Cys15 in all cases and may represent the full sequence from Lys9-->His16. CD studies also reveal that the C-terminal fragment of endothelins is not a fully disordered 'random coil' either alone or attached to the endothelin core.

Urea unfolding of peptide helices as a model for interpreting protein unfolding

To provide a model system for understanding how the unfolding of protein alpha-helices by urea contributes to protein denaturation, urea unfolding was measured for a homologous series of helical peptides with the repeating sequence Ala-Glu-Ala-Ala-Lys-Ala and chain lengths varying from 14 to 50 residues. The dependence of the helix propagation parameter of the Zimm-Bragg model for helix-coil transition theory (s) on urea molarity ([urea]) was determined at 0 degree C with data for the entire set of peptides, and a linear dependence of In s on [urea] was found. The results were fitted by the binding-site model and by the solvent-exchange model for the interaction of urea with the peptides. Each of these thermodynamic models is able to describe the data quite well and we are not able to discern any difference between the ability of each model to fit the data. Thus a linear relation, ln s = ln s0 - (m/RT).[urea], fits the data for alpha-helix unfolding, just as others have found for protein unfolding. When the m value determined here for alpha-helix unfolding is multiplied by the number of helical residues in partly helical protein molecules, the resulting values agree within a factor of 2 with observed m values for these proteins. This result indicates that the interaction between urea and peptide groups accounts for a major part of the denaturing action of urea on proteins, as predicted earlier by some model studies with small molecules.

Helix formation in model peptides based on nucleolin TPAKK motifs

The structures formed by peptide models of the N-terminal domain of the nucleolar protein nucleolin were studied by CD and nmr. The sequences of the peptides are based on the putative nucleic acid binding sequence motif TPAKK. The peptides TP1 and TP2 have the sequence acetyl-G(ATPAKKAA)nG-amide, with n = 1 and 2, respectively. CD measurements indicate structural changes in both peptides when the lysine side chains are uncharged by increasing the pH or acetylation of the side-chain amines. When trifluoroethanol (TFE) is added, more extensive structural changes are observed, resembling helical structure based on nmr nuclear Overhauser effect (NOE) and C alpha proton chemical shift changes, and CD spectra. The structure formed in 0.5M NaClO4 as observed by nmr is similar to that when the lysine side chains are acetylated, due presumably to interactions of perchlorate ion with side-chain charges on lysines. The helical structure observed in TPAKK motifs may be stabilized via N-capping interactions involving threonine. The structures observed in TFE suggest that the Thr-Pro sequence initiates short helical segments in TPAKK motifs, and these helical structures might interact with nucleic acids, presumably via interactions between lysines and threonines of nucleolin.

Tests for helix-stabilizing interactions between various nonpolar side chains in alanine-based peptides

Straight-chain, non-natural, nonpolar amino acids norleucine, norvaline, and alpha-amino-n-butyric acid at various spacings do not interact with themselves to stabilize helix formation in alanine-based peptides, but do interact with a Tyr spaced i, i + 4 to stabilize alanine helices, similar to the helix-stabilizing i, i + 4 Tyr-Leu and Tyr-Val interactions reported earlier (Padmanabhan S, Baldwin RL, 1994, J Mol Biol 241:706-713). Leu spaced i, i + 4 from another Leu is measurably helix-stabilizing relative to the corresponding i, i + 3 pair, but less so than for i, i + 4 Val-Leu, Ile-Leu, or Phe-Leu pairs (relative to the corresponding i, i + 3 pairs) when Leu is C-terminal to the other nonpolar amino acid. Our results indicate that limited side-chain flexibility in an alpha-helix strongly favors the interaction between 2 nonpolar residues to stabilize an isolated alpha-helix.

Tandemly arranged repeats of a novel highly charged 16-amino-acid motif representing the major component of the sperm-tail-specific axoneme-associated protein family Dhmst101 form extended alpha-helical rods within the extremely elongated spermatozoa of Drosophila hydei

We have previously reported that the sperm-tail-specific proteins in Drosophila hydei, encoded by the small Dhmst101 gene family, contained several tandem repeats of a novel highly charged, well-conserved cysteine-containing motif of 16 amino acids, KKKCAEAAKKEKEAAE [Neesen, J., Bünemann, H. & Heinlein, U. A. O. (1994) Dev. Biol. 162, 414-425] and suggested that this motif might be important in the structural and functional integrity of the sperm tail. We tested this suggestion by examining structure formation by model synthetic peptides containing the 16-residue sequence and corresponding peptides with one and two repeats of the sequence with Cys being replaced by Ala. We find that all these peptides form monomeric alpha-helices and that the helix content is considerably enhanced as the number of tandem repeats increases. These results are consistent with tandemly arranged 16-amino-acid repeats in Dhmst101 proteins forming extended alpha-helical rods, with the highly conserved Cys present in each 16-amino-acid motif being involved in regular interhelical cross-linking, thus providing a rigid, stable framework within the extremely elongated spermatozoa of Drosophila hydei.

Stabilizing and destabilizing effects of placing beta-branched amino acids in protein alpha-helices

In order to gain greater insight into the effects of beta-branched amino acids on protein alpha-helices, hydrophobic amino acids with varying degrees of beta-branching, including the fully beta-substituted L-2-amino-3,3-dimethylbutanoic acid (ADBA), were incorporated into the protein T4 lysozyme. The unnatural and natural amino acids were substituted at two solvent-exposed alpha-helical sites, Ser 44 and Asn 68, in the protein using the technique of unnatural amino acid mutagenesis. The stabilities of the mutant proteins were determined by using a heat of inactivation assay and from their circular dichroism thermal denaturation curves. Surprisingly, while substitution of the amino acid with the greatest degree of beta-branching, ADBA, destabilizes the protein by 2.5 +/- 0.1 degrees C (0.69 +/- 0.03 kcal/mol) relative to Ala at site 44, the same substitution stabilizes the protein by 1.0 +/- 0.1 degree C (0.27 +/- 0.03 kcal/mol) at site 68. The difference observed at these two positions illustrates the extent to which the local context can mediate the impact of a particular mutation. Molecular dynamics simulations were carried out in parallel to model the structures of the mutant proteins and to examine the energetic consequences of incorporating ADBA. Together, these results suggest that the conformationally restricted beta-branched amino acids are destabilizing, in part, because the beta-branched methyl groups can cause distortions in the local helix backbone. In addition, it is proposed that in some contexts the conformational rigidity of beta-branched amino acids may be stabilizing because it lowers the entropic cost of forming favorable side-chain van der Waals interactions.

Structural studies on peptides corresponding to mutants of the major alpha-helix of barnase

The structures of a family of peptides that contain variants of the major alpha-helix of barnase (residues 6-18) have been analyzed in solution by circular dichroism (CD) and 1H NMR at various concentrations of the helix-inducing cosolvent trifluoroethanol (TFE). The very low equilibrium constant (approximately 10(-2) for the formation of helix in water KH2O was estimated from titration of the helical ellipticity signal at 222 nm with [TFE] using the equation, KTFE = KH2O exp((m/RT) [TFE]/[H2O]), where KTFE is the equilibrium constant for the formation of helix in TFE/H2O and m is characteristic for each peptide but appears to be proportional to the lengths of related helices. NMR studies show that the peptide is mainly random coil in water, but that the helix is induced cooperatively by TFE and extends from residues 6 to 18 for wild-type peptide in 35% TFE. The mutant peptide Tyr-17-->Ala, however, has a helical region extending only for residues 9-15. Truncation of the helix upon mutation is also detected in the TFE titration procedure, which finds correspondingly lowered m-values upon mutation. This is is also supported by measurements of the pH dependence of KH2O, which is caused by the ionization of the C-cap residue, His-18, whose pKa is raised by the interaction of the protonated form with the helix dipole. Whereas there is an apparent charge/dipole interaction energy of 1.1 kcal mol-1 in the wild-type peptide, similar to that measured in the native protein, this drops dramatically upon mutations that disrupt the C-terminus of the helix. Mutation of Tyr-17-->Ala lowers KH2O only slightly, as do the other helix-destabilizing mutations. The combined results show that the helix-weakening effects of mutations act here primarily by shortening the length of the helix, with smaller effects on the equilibrium constants between helix and coil (KH2O).(ABSTRACT TRUNCATED AT 250 WORDS)

A thermodynamic model for the helix-coil transition coupled to dimerization of short coiled-coil peptides

A simple thermodynamic formalism is presented to model the conformational transition between a random-coil monomeric peptide and a coiled-coil helical dimer. The coiled-coil helical dimer is the structure of a class of proteins also called leucine zipper, which has been studied intensively in recent years. Our model, which is appropriate particularly for short peptides, is an alternative to the theory developed by Skolnick and Holtzer. Using the present formalism, we discuss the multi-equilibriatory nature of this transition and provide an explanation for the apparent two-state behavior of coiled-coil formation when the helix-coil transition is coupled to dimerization. It is found that such coupling between multi-equilibria and a true two-state transition can simplify the data analysis, but care must be taken in using the overall association constant to determine helix propensities (w) of single residues. Successful use of the two-state model does not imply that the helix-coil transition is all-or-none. The all-or-none assumption can provide good numerical estimates when w is around unity (0.35 < or = w < or = 1.35), but when w is small (w < 0.01), similar estimations can lead to large errors. The theory of the helix-coil transition in denaturation experiments is also discussed.

Elucidating the folding problem of helical peptides using empirical parameters

Using an empirical analysis of experimental data we have estimated a set of energy contributions which accounts for the stability of isolated alpha-helices. With this database and an algorithm based on statistical mechanics, we describe the average helical behaviour in solution of 323 peptides and the helicity per residue of those peptides analyzed by nuclear magnetic resonance. Moreover the algorithm successfully detects the alpha-helical tendency, in solution, of a peptide corresponding to a beta-strand of ubiquitin.

Helix propensities of the amino acids measured in alanine-based peptides without helix-stabilizing side-chain interactions

Helix propensities of the amino acids have been measured in alanine-based peptides in the absence of helix-stabilizing side-chain interactions. Fifty-eight peptides have been studied. A modified form of the Lifson-Roig theory for the helix-coil transition, which includes helix capping (Doig AJ, Chakrabartty A, Klingler TM, Baldwin RL, 1994, Biochemistry 33:3396-3403), was used to analyze the results. Substitutions were made at various positions of homologous helical peptides. Helix-capping interactions were found to contribute to helix stability, even when the substitution site was not at the end of the peptide. Analysis of our data with the original Lifson-Roig theory, which neglects capping effects, does not produce as good a fit to the experimental data as does analysis with the modified Lifson-Roig theory. At 0 degrees C, Ala is a strong helix former, Leu and Arg are helix-indifferent, and all other amino acids are helix breakers of varying severity. Because Ala has a small side chain that cannot interact significantly with other side chains, helix formation by Ala is stabilized predominantly by the backbone ("peptide H-bonds"). The implication for protein folding is that formation of peptide H-bonds can largely offset the unfavorable entropy change caused by fixing the peptide backbone. The helix propensities of most amino acids oppose folding; consequently, the majority of isolated helices derived from proteins are unstable, unless specific side-chain interactions stabilize them.

Thermodynamic characterization of an artificially designed amphiphilic alpha-helical peptide containing periodic prolines: observations of high thermal stability and cold denaturation

To investigate the structural stability of proteins, we analyzed the thermodynamics of an artificially designed 30-residue peptide. The designed peptide, NH2-EELLPLAEALAPLLEALLPLAEALAPLLKK-COOH (PERI COIL-1), with prolines at i + 7 positions, forms a pentameric alpha-helical structure in aqueous solution. The thermal denaturation curves of the CD at 222 nm (pH 7.5) show an unusual cold denaturation occurring well above 0 degrees C and no thermal denaturation is observable under 90 degrees C. This conformational change is reversible and depends on peptide concentration. A 2-state model between the monomeric denatured state (5D) and the pentameric helical state (H5) was sufficient to analyze 5 thermal denaturation curves of PERI COIL-1 with concentrations between 23 and 286 microM. The analysis was carried out by a nonlinear least-squares method using 3 fitting parameters: the midpoint temperature, Tm, the enthalpy change, delta H(Tm), and the heat capacity change, delta Cp. The association number (n = 5) was determined by sedimentation equilibrium and was not used as a fitting parameter. The heat capacity change suggests that the hydrophobic residues are buried in the helical state and exposed in the denatured one, as it occurs normally for natural globular proteins. On the other hand, the enthalpy and the entropy changes have values close to those found for coiled-coils and are quite distinct from typical values reported for natural globular proteins. In particular, the enthalpy change extrapolated at 110 degrees C is about 3 kJ/mol per amino acid residue, i.e., half of the value found for globular proteins.(ABSTRACT TRUNCATED AT 250 WORDS)

De novo design and structural characterization of an alpha-helical hairpin peptide: a model system for the study of protein folding intermediates

The de novo design and structural characterization of an alpha-helical hairpin peptide (alpha-helix/turn/alpha-helix, alpha t alpha) are reported. The peptide is intended to provide a model system for the study of the interactions of secondary structural elements during protein folding. Both the diffusion-collision and framework models of protein folding envision that the earliest intermediates in protein folding are transient secondary structures or microdomains which interact and become mutually stabilizing. Design principles for the alpha t alpha peptide were drawn from the large body of work on the structure of peptides in solution. Computer modeling was not used in the design process. Study of alpha t alpha by circular dichroism and two-dimensional nuclear magnetic resonance indicates that the designed peptide is monomeric, helical, and stable in aqueous solution at room temperature. Analysis of two-dimensional nuclear magnetic resonance experiments indicates that the two helices and the turn form in the intended positions and that the helices associate in the designed orientation. Development of alpha t alpha represents an advance in protein design in that both the secondary structural elements and designed tertiary interactions have been realized and can be detected in solution by nuclear magnetic resonance. The resulting model system resembles a protein folding intermediate and will allow the study of interacting helices in a context that approximates an early stage in protein folding.

The effect of N-terminal acetylation on the structure of an N-terminal tropomyosin peptide and alpha alpha-tropomyosin

We have used a synthetic peptide consisting of the first 30 residues of striated muscle alpha-tropomyosin, with GlyCys added to the C-terminus, to investigate the effect of N-terminal acetylation on the conformation and stability of the N-terminal domain of the coiled-coil protein. In aqueous buffers at low ionic strength, the reduced, unacetylated 32mer had a very low alpha-helical content (approximately 20%) that was only slightly increased by disulfide crosslinking or N-terminal acetylation. Addition of salt (> 1 M) greatly increased the helical content of the peptide. The CD spectrum, the cooperativity of folding of the peptide, and sedimentation equilibrium ultracentrifugation studies showed that it formed a 2-chained coiled coil at high ionic strength. Disulfide crosslinking and N-terminal acetylation both greatly stabilized the coiled-coil alpha-helical conformation in high salt. Addition of ethanol or trifluoroethanol to solutions of the peptide also increased its alpha-helical content. However, the CD spectra and unfolding behavior of the peptide showed no evidence of coiled-coil formation. In the presence of the organic solvents, N-terminal acetylation had very little effect on the conformation or stability of the peptide. Our results indicate that N-terminal acetylation stabilizes coiled-coil formation in the peptide. The effect cannot be explained by interactions with the "helix-dipole" because the stabilization is observed at very high salt concentrations and is independent of pH. In contrast to the results with the peptide, N-terminal acetylation has only small effects on the overall stability of tropomyosin.

A simplified amino acid potential for use in structure predictions of proteins

A simplified description and a corresponding force field for polypeptides is introduced. Each amino acid residue is reduced to one interaction site, representing the backbone, and one or two side chain sites depending on its size and complexity. Site-site interactions are parameterized after a hydrophobicity criterium. The treatment of backbone sites is in addition designed to reproduce typical polypeptide hydrogen bonding patterns, as well as yielding conformations in accord with the allowed phi and psi angles through an effective angle potential. There are no explicit charges in the model. The derived energy functions, which are based on thermodynamic data and sterical consideration of allowed backbone conformations, correspond to the introduction of an effective potential. The model is tested on two small proteins, avian pancreatic polypeptide and a parathyroid hormone-related protein, by simulating folding from an initially extended state using Monte Carlo methods. The reduced amino acid description is able to satisfactorily reproduce the experimentally determined native structures.

Coupling of local folding to site-specific binding of proteins to DNA

Thermodynamic studies have demonstrated the central importance of a large negative heat capacity change (delta C degree assoc) in site-specific protein-DNA recognition. Dissection of the large negative delta C degree assoc and the entropy change of protein-ligand and protein-DNA complexation provide a thermodynamic signature identifying processes in which local folding is coupled to binding. Estimates of the number of residues that fold on binding obtained from this analysis agree with structural data. Structural comparisons indicate that these local folding transitions create key parts of the protein-DNA interface. The energetic implications of this "induced fit" model for DNA site recognition are considered.

Fluorescence study of conformational flexibility of RNase S-peptide: distance-distribution, end-to-end diffusion, and anisotropy decays

Frequency-domain fluorescence resonance energy transfer and anisotropy measurements were performed to characterize conformational dynamics of an analog of the RNase S-peptide (residues 1-20). Trp was used as a donor by replacing Phe 8, and a dansyl acceptor group was introduced at position 1 or 18. The distance-distribution parameters, half width of the distribution, end-to-end diffusion coefficient, and to some extent anisotropy decays were sensitive to changes in the S-peptide conformation. The observed mean distance of about 13-14 A between residues 1 and 8 in the presence of 50% TFE and when bound to RNase S-protein is in reasonable accord with the X-ray structure of RNase. The mean distance of 9.3 A between residues 8 and 18 in the presence of 50% TFE is, however, significantly smaller than 15.3 A found for the S-protein complex. The half-width of the distance distribution increased from about 9 to 18 A for residues 1-8 and from about 6 to 14 A for segment 8-18 with the loss of helical structure. The half-widths of 9 A in the case of 1-8 segment when peptide is helical suggests the presence of considerable conformational heterogeneity. Also, the 14 A half-width for segment 8-18 when it is random-coil is smaller than that expected for a random coil 11-residue segment. The donor-to-acceptor diffusion coefficients were less than 1 x 10(-7) cm2/s at 2 degrees C for both segments and increased to 1-2 x 10(-6) cm2/s at 35 degrees C.(ABSTRACT TRUNCATED AT 250 WORDS)

Single-residue substitution in homopolypeptides: perturbative helix-coil theory at a single site

Based on Lifson-Roig's helix-coil transition theory, substitution of a single heteroresidue into a homopolymer host is studied. This study models recent experiments that substitute a single amino acid into a small peptide in water [A. Chakrabartty, J. A. Schellman, and R. L. Baldwin (1991), Nature, Vol. 351, pp. 586-688]. Our formalism, which is based on a perturbation method, differs from the existing theory for sequenced polymers and is naturally analogous, hence likely to be useful, to substitution experiments in the laboratory. It is shown that the intrinsic helix propensity w is directly proportional to the equilibrium constant for the helix-coil equilibrium of a single residue in a host peptide. This intuitive new result will simplify experimental data interpretations for measurements of the helical conformation on the single amino acid level. It is also shown that substitution affects the total helicity of the host peptide according to two considerations: the helicity of the replaced residue prior to the substitution, and the sensitivity of the site, a measure of neighboring interactions. The relationship between substitution stability and thermal stability is explored.

Effect of a single aspartate on helix stability at different positions in a neutral alanine-based peptide

A single aspartate residue has been placed at various positions in individual peptides for which the alanine-based reference peptide is electrically neutral, and the helix contents of the peptides have been measured by circular dichroism. The dependence of peptide helix content on aspartate position has been used to determine the helix propensity (s-value). Both the charged (Asp-) and uncharged (Asp0) forms of the aspartate residue are strong helix breakers and have identical s-values of 0.29 at 0 degree C. The interaction of Asp- with the helix dipole affects helix stability at positions throughout the helix, not only near the N-terminus, where the interaction is helix stabilizing, and the C-terminus, where it is destabilizing. Comparison of the helix contents at acidic pH (Asp0) and at neutral pH (Asp-) shows that the charge-helix dipole interaction is screened slowly with increasing NaCl concentration, and screening is not complete even at 4.8 M NaCl. Lastly, a helix-stabilizing hydrogen-bond interaction between glutamine and aspartate (spacing i, i + 4) has been found. This side-chain interaction is specific for both the orientation and spacing of the glutamine and aspartate residues and is resistant to screening by NaCl.

A noncovalent peptide complex as a model for an early folding intermediate of cytochrome c

Horse heart cytochrome c is one of a small number of proteins for which the folding pathway has been elucidated in structural detail by pulsed hydrogen exchange and NMR. Those studies indicated that a partially folded intermediate with interacting N- and C-terminal helices is formed at an early stage of folding when most of the chain is still disordered. This report describes a peptide model for this early intermediate, consisting of a noncovalent complex between a heme-containing N-terminal fragment (residues 1-38) and a synthetic peptide corresponding to the C-terminal helix (residues 87-104). Far-UV circular dichroism and proton NMR indicate that the isolated peptides are largely disordered, but when combined, they form a flexible, yet tightly bound complex with enhanced helical structure. These results emphasize the importance of interactions between marginally stable elements of secondary structure in forming tertiary subdomains in protein folding.

The energetics of ion-pair and hydrogen-bonding interactions in a helical peptide

A single pair of Glu and Lys residues has been placed at four different spacings, and in both orientations, in an otherwise neutral alanine-glutamine peptide helix, and the contribution to helix stability of the different Glu-Lys interactions has been measured. The contribution from the interaction of each charged side chain with the helix macrodipole has also been determined. A side-chain interaction between Gln and Glu, when the spacing is (i,i+4), has been detected and quantified. The interactions have been divided into contributions from hydrogen bonds (independent of the concentration of NaCl) and from electrostatic interactions (present in 10 mM NaCl, absent in 2.5 M NaCl). The major results are as follows: (1) The (i,i+3) and (i,i+4) Glu-Lys interactions are helix-stabilizing and are similar in strength to each other, regardless of the orientation of the side chains. (2) Hydrogen bonds provide the major contribution to these side-chain interactions, as shown by the following facts. First, the major part of the interaction observed in 10 mM NaCl, pH 7, is still present in 2.5 M NaCl. Second, the interaction found at pH 2 is equally as strong as that found in 2.5 M NaCl at pH 7. (3) The (i,i+4) Gln-Glu side-chain hydrogen bond is as strong as the hydrogen-bond component of the Glu-Lys interaction at both pH 2 and pH 7. The Gln-Glu interaction differs from the Glu-Lys interaction in being specific both for the orientation and the spacing of the residues. (4) No significant hydrogen-bonding interaction was found for the (i,i+1) or (i, i+2) Glu-Lys spacings, either at pH 2 or at pH 7, in 2.5 M NaCl. At 10 mM NaCl and pH 7, these spacings show a helix-destabilizing electrostatic interaction which probably results from stabilization of the coil conformation.

Probing the influence of sequence-dependent interactions upon alpha-helix stability in alanine-based linear peptides

The observation that short, linear alanine-based polypeptides form stable alpha-helices in aqueous solution has allowed the development of well-defined experimental systems with which to study the influence of amino acid sequence upon the stability of secondary structure. We have performed detailed conformational searches upon six alanine-based peptides in order to rationalize the observed variation in the alpha-helical stability in terms of side-chain-backbone and side-chain-side-chain interactions. Although a simple, gas-phase, potential model was used to obtain the conformational energies for these peptides, good agreement was obtained with experiment regarding their relative alpha-helical stabilities. Our calculations clearly indicate that valine, isoleucine, and phenylalanine residues should destabilize the alpha-helical conformation when included within alanine-based peptides because of energetically unfavorable side-chain-backbone interactions, which tend to result in the formation of regions of 3(10)-helix. In the case of valine, the destabilization most probably arises from entropic effects as the isopropyl side chain can assume more orientations in the 3(10)-helical form of the peptide. A detailed examination of very short-range interactions in these peptides has also indicated that an interaction, involving fewer than five consecutive residues, whose stabilizing effect reinforces that of the (i, i + 4) hydrogen bond may be the basis of the requirement for increased nucleation (sigma) and propagation parameters (s) required by Zimm-Bragg theory to predict the alpha-helical content for compounds in this class of short peptides. Our calculations complement recent work using modified Zimm-Bragg and Lifson-Roig theories of the helix-coil transition, and are consistent with molecular dynamics simulations upon linear peptides in aqueous solution.

Residual helical structure in the C-terminal fragment of cytochrome c

Several reports have pointed out the existence of both kinetic and equilibrium intermediate states in protein folding. In cytochrome c, it has been shown that the N- and C-terminal helices form in the early stages of folding and remain stable in the molten globule state (a compact equilibrium intermediate). These two facts prompted me to synthesize and examine the helical content, in aqueous solution, of the peptides corresponding to the three major helices of cytochrome c. These peptides are 15 residues long. This paper reports that little if any helix is present in the N-terminal and 61-75 peptides, regardless of the pH and salt concentration. However, the C-terminal peptide showed a far-UV CD spectrum characteristic of an alpha-helix (27% helicity). The helical content of the C-terminal peptide increased to 43% as salt (2 M Na2SO4) was added. The dimerization of the C-terminal peptide with the N-terminal peptide by an SS bridge stabilized the helical structures (14% to 63% helicity). These results strongly suggest that the C-terminal helix is essential for both the folding and the stability of cytochrome c. Furthermore, although the N-terminal segment does not form helices by itself, its interaction with the C-terminal helix would enhance the stability of the subdomain containing the two helices.