IR spectroscopy of isotope-labeled helical peptides: probing the effect of N-acetylation on helix stability

The effect of N-acetylation on the conformation of alanine-rich helical peptides is examined using isotope-edited Fourier transform infrared (FTIR) spectroscopy. A series of peptides with sequence AA(AAKAA)(3)AAY has been prepared; each peptide incorporates four (13)C-labeled alanines. These peptides have two amide I' bands in their FTIR spectra: one corresponding to the (12)C amino acids, and one assigned to the (13)C amino acids. The intensity and frequency of the (13)C amide I' band varies systematically with the position of the labels in the sequence and the presence or absence of an N-acetyl capping group. The intensity of the (13)C amide I' band correlates with helix stability at the labeled residues as predicted by thermodynamic models of the helix-coil transition. These results suggest that FTIR spectroscopy combined with specific isotope labeling can be used to dissect the conformation of helical peptides at the residue level.     

Proline affects oligomerization of a coiled coil by inducing a kink in a long helix

The structural effect of a proline in a helix in trifluoroethanol (TFE)/water medium was examined on a 29-mer peptide and its proline analog derived from the leucine zipper (LZ)-like motif of gp41 (the transmembrane glycoprotein of HIV-1) by NMR and circular dichroism (CD) spectroscopies. Lower helical content was found for the proline mutant from the CD study. NMR data show that distortion of the helix by proline is local and occurs mainly on the N-terminal side of the substitution site. Molecular dynamics computation exhibits a bending of the helical axis of 30 degrees +/- 10 degrees, in agreement with X-ray diffraction results. Light-scattering experiments indicated that the average aggregation number of the proline-substituted mutant is substantially lower than that of the wild-type peptide. From the ratio of dissociation constants of the wild-type and the proline mutant peptides, the difference in free energy of trimeric formation is calculated to be 2.1 kcal/mol. Thermal stability, helicity, and the average aggregation number for the helix oligomers were found to be correlated. The structural alteration and the reduced coiled coil stability may account for the deficiency in the biological functions of the proline mutants of gp41 and in the inhibitory action of proline-substituted peptides. These effects may also be important in unraveling the roles played by proline in transmembrane proteins.     

vpu transmembrane peptide structure obtained by site-specific fourier transform infrared dichroism and global molecular dynamics searching.

The recently developed method of site-directed Fourier transform infrared dichroism for obtaining orientational constraints of oriented polymers is applied here to the transmembrane domain of the vpu protein from the human immunodeficiency virus type 1 (HIV-1). The infrared spectra of the 31-residue-long vpu peptide reconstituted in lipid vesicles reveal a predominantly alpha-helical structure. The infrared dichroism data of the (13)C-labeled peptide yielded a helix tilt beta = (6.5 +/- 1.7) degrees from the membrane normal. The rotational pitch angle omega, defined as zero for a residue located in the direction of the helix tilt, is omega = (283 +/- 11) degrees for the (13)C labels Val(13)/Val(20) and omega = (23 +/- 11) degrees for the (13)C labels Ala(14)/Val(21). A global molecular dynamics search protocol restraining the helix tilt to the experimental value was performed for oligomers of four, five, and six subunits. From 288 structures for each oligomer, a left-handed pentameric coiled coil was obtained, which best fits the experimental data. The structure reveals a pore occluded by Trp residues at the intracellular end of the transmembrane domain.     

Medium-dependence of the secondary structure of exendin-4 and glucagon-like-peptide-1.

Exendin-4 is a natural, 39-residue peptide first isolated from the salivary secretions of a Gila Monster (Heloderma suspectum) that has some pharmacological properties similar to glucagon-like-peptide-1 (GLP-1). This paper reports differences in the structural preferences of these two peptides. For GLP-1 in aqueous buffer (pH 3.5 or 5.9), the concentration dependence of circular dichroism spectra suggests that substantial helicity results only as a consequence of helix bundle formation. In contrast, exendin-4 is significantly helical in aqueous buffer even at the lowest concentration examined (2.3 microM). The pH dependence of the helical signal for exendin-4 indicates that helicity is enhanced by a more favorable sequence alignment of oppositely charged sidechains. Both peptides become more helical upon addition of either lipid micelles or fluoroalcohols. The stabilities of the helices were assessed from the thermal gradient of ellipticity (partial differential theta(221)/partial differential T values); on this basis, the exendin helix does not melt appreciably until temperatures significantly above ambient. The extent of helix formation for exendin-4 in aqueous buffer (and the thermal stability of the resulting helix) suggests the presence of a stable helix-capping interaction which was localized to the C-terminal segment by NMR studies of NH exchange protection. Solvent effects on the thermal stability of the helix indicate that the C-terminal capping interaction is hydrophobic in nature. The absence of this C-capping interaction and the presence of a flexible, helix-destabilizing glycine at residue 16 in GLP-1 are the likely causes of the greater fragility of the monomeric helical state of GLP-1. The intramolecular hydrophobic clustering in exendin-4 also appears to decrease the extent of helical aggregate formation.     

Probing the effect of side chains on the conformation and stability of helical peptides via isotope-edited infrared spectroscopy

The mechanism of helix stabilization or destabilization by different amino acids has been the subject of several experimental and theoretical studies; these studies suggest that large or bulky side chains may modulate helix stability by altering the hydration of the helix backbone. In this paper, we report a spectroscopic study to determine the effect of alanine to leucine substitutions on the conformation and solvation of specific segments of a model helical peptide. A 25-residue, alanine-rich, helical peptide [Ac-(AAAAK)(4)-AAAAY-NH(2) (AKA)] and its two leucine variants [Ac-LLLLK-(AAAAK)(3)-AAAAY-NH(2) (LKA) and Ac-(AAAAK)(4)-LLLLY-NH(2) (AKL)] were characterized by infrared (IR) and electronic circular dichroism (ECD) spectroscopies. Introduction of (13)C isotopes into specific, consecutive, backbone carbonyls for certain blocks of each of the peptides mentioned above allows the IR spectra to be interpreted in terms of the conformation and solvation of specific residues within the helix. These isotope-edited IR spectra of the leucine peptides do not show evidence of a decrease in the degree of backbone solvation compared to the alanines, but suggest that the peptide may adopt a distorted conformation to accommodate the larger leucine side chains at the N-terminus. These experiments demonstrate the power of isotope-edited IR in dissecting subtle changes in helix conformation at the residue level.     

Structure and conformation of the disulfide bond in dimeric lung surfactant peptides SP-B1-25 and SP-B8-25

Raman spectroscopy was used to determine the conformation of the disulfide linkage between cysteine residues in the homodimeric construct of the N-terminal alpha helical domain of surfactant protein B (dSP-B(1-25)). The conformation of the disulfide bond between cysteine residues in position 8 of the homodimer of dSP-B(1-25) was compared with that of a truncated homodimer (dSP-B(8-25)) of the peptide having a disulfide linkage at the same position in the alpha helix. Temperature-dependent Raman spectra of the S-S stretching region centered at approximately 500 cm(-1) indicated a stable, although highly strained disulfide conformation with a chi(CS-SC) dihedral angle of +/-10 degrees for the dSP-B(1-25) dimer. In contrast, the truncated dimer dSP-B(8-25) exhibited a series of disulfide conformations with the chi(CS-SC) dihedral angle taking on values of either +/-30 degrees or 85+/-20 degrees . For conformations with chi(CS-SC) close to the +/-90 degrees value, the Raman spectra of the 8-25 truncated dimers exhibited chi(SS-CC) dihedral angles of 90/180 degrees and 20-30 degrees . In the presence of a lipid mixture, both constructs showed a nu(S-S) band at approximately 488 cm(-1), corresponding to a chi(CS-SC) dihedral angle of +/-10 degrees . Polarized infrared spectroscopy was also used to determine the orientation of the helix and beta-sheet portion of both synthetic peptides. These calculations indicated that the helix was oriented primarily in the plane of the surface, at an angle of approximately 60-70 degrees to the surface normal, while the beta structure had approximately 40 degrees tilt. This orientation direction did not change in the presence of a lipid mixture or with temperature. These observations suggest that: (i) the conformational flexibility of the disulfide linkage is dependent on the amino acid residues that flank the cysteine disulfide bond, and (ii) in both constructs, the presence of a lipid matrix locks the disulfide bond into a preferred conformation.     

NMR and CD studies of triple-helical peptides.

Triple-helix formation of the peptide (Pro-Hyp-Gly)10 was monitored by nmr and CD spectroscopy. The two-dimensional nmr spectra indicated that the Gly C alpha H and Pro C delta H proton resonances shift upfield in going from the nonhelical to helical form, while hydroxy-proline resonances are unchanged. The integrated areas of the helical and nonhelical resonances could be monitored in the one-dimensional nmr spectrum, and indicate that in the (Pro-Hyp-Gly)10 about 90% of the residues are in a defined triple-helical conformation. The introduction of a glycine to alanine substitution or the deletion of a single hydroxyproline residue in the stable triple-helical peptide (Pro-Hyp-Gly)10 still allows trimers to be formed, but the trimers show a substantial loss of triple helix and decreased thermal stability compared with (Pro-Hyp-Gly)10. Two computer models were generated for the Gly----Ala peptide, one with the Ala side chains packed inside the helix and the other with the region containing the alanines forming a beta-bend that loops out from the helix. The nmr data is more consistent with the latter model.     

Positional independence and additivity of amino acid replacements on helix stability in monomeric peptides

The 17-residue peptide acetylAEAAAKEAAAKEAAAKAamide, described as an autonomous folding unit (Marqusee & Baldwin, 1987), has been used to examine the effect of amino acid replacements on helix stability. Alanine residues(s) at positions 4, 9, and 14 in the peptide sequence were replaced either singly or multiply by either serine or methionine residues with solid-phase peptide synthesis. The thermal dependence of the helix/coil transition of each peptide was observed by far-ultraviolet circular dichroism. Within experimental variation, all three single replacements exhibit a common thermal transition, and all three double replacements exhibit a different common thermal transition. These results suggest that replacement of the central alanine residue in the repeat EAAAK located in the N-terminus, in the middle, or in the C-terminus of the peptide helix has the same effect on helix stability. The melting temperature of each thermal transition was estimated by assuming a linear van't Hoff plot and a change in molar ellipticity of 33,500 deg cm2 dmol-1. Such analysis indicates that each replacement of an alanine residue by a serine residue diminishes the melting temperature by 11 +/- 1 degrees C and that each replacement of an alanine residue by a methionine residue diminishes the melting temperature by 6 +/- 1 degrees C. These results suggest that the effect of these replacements on helix stability is additive.     

Studies of synthetic helical peptides using circular dichroism and nuclear magnetic resonance

We have designed a set of 17-residue synthetic peptides to be monomeric helices in aqueous solution. Circular dichrosim experiments indicate the presence of helical structure in aqueous solution at low temperature and low pH. The two-dimensional nuclear magnetic resonance results for one of the peptides show a segment of ten residues which clearly meets all of the criteria for the existence of helical structure at both 5 degrees C and 15 degrees C. The first four residues of the peptide are in a largely extended conformation. Calculations suggest that residues 5 through 14 are significantly helical at 5 degrees C. When the temperature is increased, circular dichroism spectra indicate that the helical content decreases. At 15 degrees C, the 3JN alpha coupling constants increase in the helical region, indicating an increase in motion or conformational averaging in the helical segment. None of the peptides has pH titration behavior consistent with salt bridge stabilization of helical conformation. Our data lend themselves to interpretation with the helix dipole model and specific side-chain interactions. When the N and C termini charges are removed the helical content of the peptides increases. The amount of helicity increases as the pH is lowered, due to the ionization of His16. Much of the helical stabilization appears to be due to a specific side-chain interaction between His16 and Tyr12.     

Effect of the N3 residue on the stability of the alpha-helix

N3 is the third position from the N terminus in the alpha-helix with helical backbone dihedral angles. All 20 amino acids have been placed in the N3 position of a synthetic helical peptide (CH(3)CO-[AAX AAAAKAAAAKAGY]-NH(2)) and the helix content measured by circular dichroism spectroscopy at 273 K. The dependence of peptide helicity on N3 residue identity has been used to determine a free energy scale by analysis with a modified Lifson-Roig helix coil theory that includes a parameter for the N3 energy (n3). The most stabilizing residues at N3 in rank order are Ala, Glu, Met/Ile, Leu, Lys, Ser, Gln, Thr, Tyr, Phe, Asp, His, and Trp. Free energies for the most destabilizing residues (Cys, Gly, Asn, Arg, and Pro) could not be fitted. The results correlate with N1, N2, and helix interior energies and not at all with N-cap preferences. This completes our work on studying the structural and energetic preferences of the amino acids for the N-terminal positions of the alpha-helix. These results can be used to rationally modify protein stability, help design helices, and improve prediction of helix location and stability.     

Stabilization of helical structure in two 17-residue amphipathic analogues of the C-terminal peptide of cytochrome C

The conformations of two 17-residue peptide analogues derived from the C-terminal sequence of pigeon cytochrome c (native sequence = KAERADLIAYLKQATAK) were examined in aqueous and lipid environments by CD spectroscopy. The two analogues, KKLLKKLIAYLKQATAK (K peptide) and EELLEELIAYLKQATAK (E peptide), were made amphipathic with respect to helical segregation by substituting a 6-residue sequence at the N-terminus of the native peptide. Their structures were compared to the native peptide under aqueous conditions of varying pH and temperature, and in the presence of liposomes composed of phosphatidylcholine and phosphatidylserine in the ratio of 9:1. The results indicated that the native peptide remains unstructured under all the conditions examined even though this region of the native molecule is surface exposed and helical. The E peptide, however, was helical under aqueous conditions at 25 degrees C from pH 2-10 with a maximum helicity at pH 4 (54% helix from analysis of CD data). The ellipticity of the E peptide at pH 4 and 8 was concentration dependent, indicating an aggregation phenomenon. In studies in which the CD spectrum was measured at different temperatures, the E peptide became more helical at lower temperatures at pH 4 but not at pH 8. Upon interaction with a lipid membrane in the form of liposomes, there appeared to be a slight destabilization in the structure of the E peptide. The K peptide in an aqueous environment behaved like the native peptide in that it was structureless at all pHs and temperatures examined. In the presence of liposomes, however, this peptide had a high helical content (75% helix from analysis of CD data). These findings suggest that while stabilization of the helix dipole with negative charges at the N-terminus are important in inducing helical conformation in the E peptide, hydrophobic interactions created during aggregation appear to provide the principal stabilizing force. The results with the K peptide demonstrate that the positive N-terminal sequence of this peptide is able to interact with the negatively charged head groups in the phospholipid membrane in such a fashion as to stabilize a helical structure that is not apparent in an aqueous environment alone.     

Length‐dependent stability of α‐helical peptide upon adsorption to single‐walled carbon nanotube

Earlier studies have shown that the helical content of α‐helical peptide decreases upon its interaction with carbon nanotube (CNT). Further, the length of the α‐helix varies from few residues in the small globular protein to several number of residues in structural and membrane proteins. In structural and membrane proteins, helices are widely present as the supercoil i.e., helical bundles. Thus, in this study, the length‐dependent interaction pattern of α‐helical peptides with CNT and the stability of isolated α‐helical fragment versus supercoiled helical bundle upon interaction with CNT have been investigated using classical molecular dynamics (MD) simulation. Results reveal that the disruption in the helical motif on interaction with CNT is directly proportional to the length of the helix. Also it is found that the shorter helix does not undergo noticeable changes in the helicity upon adsorption with CNT. On the other hand, helicity of longer peptides is considerably affected by its interaction with CNT. In contrast to the known fact that the stability of the helix increases with its length, the disruption in the helical peptide increases with its length upon its interaction with CNT. Comparison of results shows that structural changes in the isolated helical fragment are higher than that in supercoiled helix. In fact, helical chain in supercoiled bundle does not undergo significant changes in the helicity upon interaction with CNT. Both the length of the helical peptide and the inherent stability of the helical unit in the supercoiled helix influence the interaction pattern with the CNT. © 2012 Wiley Periodicals, Inc. Biopolymers 99: 357–369, 2013.     

Conformations of isolated fragments of pancreatic polypeptide

In spite of its short polypeptide chain, the pancreatic polypeptide molecule consists of a polyproline II type helix and alpha-helix. To understand the stability and formation of the alpha-helical region, we prepared some peptide fragments including the helical segment of chicken pancreatic polypeptide and studied their conformations by circular dichroism (CD). PP7-36 (a peptide fragment corresponding to residues 7-36 of chicken pancreatic polypeptide) showed a CD spectrum characteristic of the helix at pH 4.6 and at peptide concentrations as low as 1 microM. PP11-36 was able to form a helical conformation only at high peptide concentrations and not at concentrations lower than 10 microM. However, acetyl PP11-36 (in which the alpha-amino group is acetylated so that no positive charge exists at the N terminus) was able to form the helical conformation at pH 4.6 and at the peptide concentrations where PP11-36 could not. Succinyl PP12-36 (in which the alpha-amino group is succinylated to introduce a negative charge) was also able to form the helical conformation. The CD spectra of PP12-36 and PP13-36 were not characteristic of the helical conformation at all the pH values and peptide concentrations studied. Acetyl PP13-36, which has no charge at the N terminus, did not form the helix. On the other hand, succinyl PP13-36, which has a negative charge at the N-terminal end, did form the helix at pH 4.6. These findings indicate that the presence of the negative charge of carboxylate at the N-terminal region of a peptide fragment is important for helix formation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformationally driven protease-catalyzed splicing of peptide segments: V8 protease-mediated synthesis of fragments derived from thermolysin and ribonuclease A.

We have studied the conformation as well as V8 protease-mediated synthesis of peptide fragments, namely amino acid residues 295-316 (TC-peptide) of thermolysin and residues 1-20 (S-peptide) of ribonuclease A, to examine whether "conformational trapping" of the product can facilitate reverse proteolysis. The circular dichroism study showed cosolvent-mediated cooperative helix formation in TC-peptide with attainment of about 30-35% helicity in the presence of 40% 1-propanol and 2-propanol solutions at pH 6 and 4 degrees C. The thermal melting profiles of TC-peptide in the above cosolvents were very similar. V8 protease catalyzed the synthesis of TC-peptide from a 1:1 mixture of the non-interacting complementary fragments (TC295-302 and TC303-316) in the presence of the above cosolvents at pH 6 and 4 degrees C. In contrast, V8 protease did not catalyze the ligation of S1-9 and S10-20, although S-peptide could assume helical conformation in the presence of the cosolvent used for the semisynthetic reaction. V8 protease was able to synthesize an analog of S-peptide (SA-peptide) in which residues 10-14 were substituted (RQHMD-->VAAAK). While S-peptide exhibited helical conformation in the presence of aqueous propanol solutions, SA-peptide displayed predominantly beta-sheet conformation. SA-peptide showed enhanced resistance to proteolysis as compared with S-peptide. Thus, failure of semisynthesis of S-peptide may be a consequence of high flexibility around the 9-10 peptide bond due to its proximity to the helix stop signal. The results suggest that protease-mediated ligations may be achieved by design and manipulation of the conformational aspects of the product.     

Conformational analysis of a set of peptides corresponding to the entire primary sequence of the N-terminal domain of the ribosomal protein L9: evidence for stable native-like secondary structure in the unfolded state

There is considerable interest in the structure of the denatured state and in the role local interactions play in protein stability and protein folding. Studies of peptide fragments provide one method to assess local conformational preferences which may be present in the denatured state under native-like conditions. A set of peptides corresponding to the individual elements of secondary structure derived from the N-terminal domain of the ribosomal protein L9 have been synthesized. This small 56 residue protein adopts a mixed alpha-beta topology and has been shown to fold rapidly in an apparent two-state fashion. The conformational preferences of each peptide have been analyzed by proton nuclear magnetic resonance spectroscopy and circular dichroism spectroscopy. Peptides corresponding to each of the three beta-stands and to the first alpha-helix are unstructured as judged by CD and NMR. In contrast, a peptide corresponding to the C-terminal helix is remarkably structured. This 17 residue peptide is 53 % helical at pH 5.4, 4 degrees C. Two-dimensional NMR studies demonstrate that the helical structure is distributed approximately uniformly throughout the peptide, although there is some evidence for fraying at the C terminus. Detailed analysis of the NMR spectra indicate that the helix is stabilized, in part, by a native N-capping interaction involving Thr40. A mutant peptide which lacks Thr40 is only 32 % helical. pH and ionic strength-dependent studies suggested that charge charge interactions make only a modest net contribution to the stability of the peptide. The protein contains a trans proline peptide bond located at the first position of the C-terminal helix. NMR analysis of the helical peptide and of a smaller peptide containing the proline residue indicates that only a small amount of cis proline isomer (8 %) is likely to be populated in the unfolded state.     

Conformational study of peptides containing dehydrophenylalanine: helical structures without hydrogen bond

The conformational behaviour of deltaZPhe has been investigated in the model dipeptide Ac-deltaZPhe-NHMe and in the model tripeptides Ac-X-deltaZPhe-NHMe with X=Gly,Ala,Val,Leu,Abu,Aib and Phe and is found to be quite different. In the model tripeptides with X=Ala,Val,Leu,Abu,Phe the most stable structure corresponds to phi1=-30 degrees, psi1=120 degrees and phi2=psi2=30 degrees. This structure is stabilized by the hydrogen bond formation between C=O of acetyl group and the NH of the amide group, resulting in the formation of a 10-membered ring but not a 3(10) helical structure. In the peptides Ac-Aib-deltaZPhe-NHMe and Ac-(Aib-deltaZPhe)3-NHMe, the helical conformers with phi = +/-30 degrees, psi = +/-60 degrees for Aib residue and phi=psi= +/-30 degrees for deltaZPhe are predicted to be most stable. The computational studies for the positional preferences of deltaZPhe residue in the peptide containing one deltaZPhe and nine Ala residues reveal the formation of a 3(10) helical structure in all the cases with terminal preferences for deltaZPhe. The conformational behaviour of Ac-(deltaZPhe)n-NHMe with n< or =4 is predicted to be very labile. With n > 4, degenerate conformational states with phi,psi values of 0 degrees +/- 90 degrees adopt helical structures which are stabilized by carbonyl-carbonyl interactions and the N-H-pi interactions between the amino group of every deltaZPhe residue with one C-C edge of its own phenyl ring. The results are in agreement with the experimental finding that screw sense of helix for peptides containing deltaZPhe residues is ambiguous in solution. The helical structures stabilized by hydrogen bond formation are found to be at least 3kCalmol(-1) less stable. Conformational studies have also been carried out for the peptide Ac-(deltaEPhe)6-NHMe and the peptide Ac-deltaAla-(deltaZPhe)6-NHMe containing deltaAla residue at the N-terminal. The N-H-pi interactions are absent in peptide Ac-(deltaEPhe)6-NHMe.     

Sterically hindered disulfide bridges in cystine diketopiperazine, cysteinyl-cysteine disulfide and derivatives.

L-Cystine diketopiperazine (1), L-cysteinyl-cysteine disulfide -HCl (2), L-cysteinyl-cysteine disulfide methyl ester -HCl (3), and t-butyloxycarbonyl-L-cysteinyl-cysteine disulfide methyl ester (4) are investigated by CD, ultraviolet, 13C NMR, infrared and laser Raman spectroscopy. The temperature dependence of the 13C NMR signals of 1 reveals an exceptionally high energy barrier of deltaGNo. = 15.8 +/- 0.2 kcal/mol for the reversible change in helicity of the inherently dissymmetric disulfide bridge of 1. The P-helical diastereomer predominates in dimethyl-sulfoxide at 25 degrees C, with 80-85% of the molecules having this configuration. The Cotton effects of 1 are larger and show smaller temperature coefficients than the conformationally more mobile cystine compounds 2 and 3. After dissolving crystals of 1 in 95% ethanol there is a time-dependent decrease of the ellipticity of the negative Cotton effect at 225 nm, indicating a conformational change in going from crystal to solution. Besides 1, 2 and 3 are at present the only known examples of cystine derivatives with C-S-S-C torsional angles around 90 degrees, which do not exhibit optical activity in the long wavelength disulfide absorption, as is predicted for 1 from the Linderberg-Michl model. At 305 nm a new weak Cotton effect was discovered for 1. The solvent dependence of the CD spectra is discussed and the infrared and Raman spectra are assigned.     

CD and (13)C(alpha)-NMR studies of folding equilibria in a two-stranded coiled coil formed by residues 190-254 of alpha-tropomyosin

Synthesis and CD and (13)C(alpha)-NMR studies in a near-neutral saline buffer are reported for a 65-residue peptide ((190)Tm(254)) comprising residues 190-254 of the alpha-tropomyosin chain. CD on a version disulfide cross-linked via the N-terminal cysteine side chains indicates that this dimer is highly helical and melts near 48 degrees C. The CD is independent of peptide concentration, showing that association of (190)Tm(254) stops at the two-strand level. Similar studies on the reduced version show much lower helix content at low temperature, melting points below room temperature, and the expected concentration dependence. The observed melting temperature of the reduced peptide is far below (by 27 degrees C) that expected from an extant analysis of calorimetry data on parent tropomyosin that designates (190)Tm(254) as an independently melting "cooperative block." This disagreement and the pronounced nonadditivity seen when data for (190)Tm(254) are combined with extant data for other subsequences argue decisively against the concept of specific independently melting blocks within the tropomyosin chain. The data for (190)Tm(254) also serve to test recent ideas on the sequence determinants of structure and stability in coiled coils. Analysis shows that some ideas, such as the stabilizing effect of leucine in the d heptad position, find support, but others--such as the destabilizing effect of alanine in d, the dimer-disfavoring effect of beta-branching in d and its dimer-favoring effect in a, and the dimer-directing effect of asparagine in a--are more questionable in tropomyosin than in the leucine zipper coiled coils. (13)C(alpha)-NMR data at two labeled sites, L228(d) and V246(a), of (190)Tm(254) display well-separated resonances for folded and unfolded forms at each site, indicating that the transition is slow on the NMR time scale and thus demonstrating the possibility of obtaining thermodynamic and kinetic information on the transition at the residue level.     

Molecular dynamics simulations of helix denaturation.

An understanding of the structural transitions that an alpha-helix undergoes will help to elucidate such motions in proteins and their role in protein folding. We present the results of molecular dynamics simulations to investigate these transitions in a short polyalanine peptide (13 residues) both in vacuo and in the presence of solvent. The denaturation of this peptide was monitored as a function of temperature (ranging from 5 to 200 degrees C). In vacuo, the helical state predominated at all temperatures, whereas in solution the helix melted with increasing temperature. The peptide was predominantly helical at low temperature in solution, while at intermediate temperatures the peptide spent the bulk of the time fluctuating between different conformations with intermediate amounts of helix, e.g. not completely helical nor entirely non-helical. Many of these conformations consisted of short helical segments with intervening non-helical residues. At high temperature the peptide unfolded and adopted various collapsed unstructured states. The intrahelical hydrogen bonds that break at high temperature were not fully compensated by hydrogen bonds with water molecules in the partially unfolded forms of the peptide. Increases in temperature disrupted both the helical structure and the peptide-water interactions. Water played a major but indirect role in facilitating unfolding, as opposed to specifically competing for the intrapeptide hydrogen bonds. The implications of our results to protein folding are discussed.