Alpha-helix to random-coil transitions of two-chain coiled coils: the use of physical models in treating thermal denaturation equilibria of isolated subsequences of alpha alpha-tropomyosin

Two extant models of thermal folding/unfolding equilibria in two-chain, alpha-helical coiled coils are tested by comparison with experimental results on excised, isolated subsequences of rabbit alpha alpha-tropomyosin (Tm). These substances are designated iTmj where i and j are, respectively, the residue numbers (in the 284-residue parent chain) of the N- and C-terminal residues of the subsequence. One model postulates that a coiled coil consists of segments, each denaturing in an all-or-none manner, like small globular proteins. Thus this model yields a small number of populated molecular species. In an extant calorimetry study of 11Tm127 and of 190Tm284, each required only two all-or-none-segments, and their enthalpies and transition temperatures were assigned. These assignments are shown here to yield the concentration of all molecular species, and therefore the helix content, as a function of temperature. Such calculations for 190Tm284 are in tolerable agreement with CD experiments, but those for 11Tm127 are in gross disagreement. Thus, either the model itself or the calorimetric assignment is faculty. In the second model, all conformational states are counted and weighted, as in the Zimm-Bragg theory for single-chain polypeptides. This theory has been extended (by Skolnick) to two-chain coiled coils and is here used to fit CD data for 11Tm127, 142Tm281, and 190Tm284. The fit is tolerable for 11Tm127, good for 142Tm281, and quantitative for 190Tm284. Thus this comparison does not falsify this second model. The helix-helix interaction free energy, obtainable from the fit, shows nonadditivity when isolated subsequences are compared with the parent. This suggests that removal of a region from a long coiled coil allows energetically substantial adjustments in side-chain packing in the helix-helix interface. Thus, the helix-helix interaction in long coiled coils is characteristic of a global free energy minimum and not just of the regional constellation of side chains.     

Alpha-helix to random coil transitions of two-chain coiled coils: experiments on the thermal denaturation of isolated segments of alpha alpha-tropomyosin

Circular dichroism (CD) experiments in the backbone (200-240 nm) region are reported for four isolated, excised two-chain, coiled-coil segments whose chains comprise, respectively, residues 11-127, 142-281, 1-189, and 190-284 of the rabbit alpha alpha-tropomyosin (Tm) sequence. The uv and CD spectra for the noncross-linked segments are very similar to those for parent Tm. At 3 degrees C, all have a helix content of 90% or more; moreover, all thermal denaturation curves depend on concentration, as required by mass action, and are completely reversible. At comparable concentrations, solutions show values of T1/2 (the temperature at which the helix content is 50%) following the order of 11Tm127 approximately 1Tm189 greater than 142Tm281 greater than 190Tm284. The thermal unfolding data for 11Tm127, 190Tm284, and 142Tm281 fall on apparently monophasic curves (single inflection point). However, curves for 1Tm189 show a heretofore unknown low temperature transition in which the helix content drops from approximately 90% at 2 degrees C to approximately 73% at 20 degrees C, indicating that this segment has one or more weak sections totaling approximately 50 residues per chain. Since thermal denaturation curves for noncross-linked 11Tm127, 142Tm281, and Tm have no such low temperature transition, i.e., the helix content is not additive, the weak region probably comprises the bulk of the residues between 127 and 189 in 1Tm189, but is somehow stabilized in 142Tm281 and in parent Tm.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Calponin and tropomyosin interactions.

The interaction between chicken gizzard calponin and tropomyosin was examined using viscosity, light scattering, electron microscopy and affinity chromatography. At neutral pH, 10 mM NaCl and in the absence of Mg2+, calponin induced tropomyosin filaments to form paracrystals thus decreasing the viscosity while increasing dramatically the light scattering of the tropomyosin solution. Electron micrographs of the uranyl acetate stained calponin-tropomyosin complex showed the presence of spindle shaped paracrystals with regular striation patterns and repeating units of about 400 A. Under similar conditions, smooth muscle caldesmon also induced tropomyosin to form paracrystals. To localize the calponin-binding site on tropomyosin, binding of fragments of tropomyosin, generated by chemical and mutational means, to a calponin-affinity column was studied. The COOH-terminal tropomyosin fragment Cn1B(142-281) and the NH2-terminal fragment CSM-beta(1/8/12-227) bound to a calponin-affinity column with an affinity similar to that of intact tropomyosin; while the NH2-terminal fragment, Cn1A(11-127), did not bind, indicating that the calponin-binding site(s) resides within residues 142-227 of tropomyosin. To determine the involvement in calponin binding of the area around Cys-190 of tropomyosin, fragments with cleavage sites near or at Cys-190 were used. Thus, while fragments Cy2(190-284) and CSM-beta(1/8/12-200) bound weakly to the calponin-affinity column, fragment Cy1(1-189) did not. These results demonstrate that calponin binds to tropomyosin between residues 142 and 227, and that the integrity of the region around Cys-190 of tropomyosin is important for strong interaction between the two proteins.     

Kinetics of folding and unfolding of alpha alpha-tropomyosin and of nonpolymerizable alpha alpha-tropomyosin.

Stopped flow CD (SFCD) kinetic studies of self-assembly of coiled coils of rabbit alpha alpha-tropomyosin and of nonpolymerizable alpha alpha-tropomyosin (NPTm) are reported. The protein was denatured in 6 M urea buffer, then renatured by 10-fold dilution into benign saline buffer. Folding was monitored by SFCD in the backbone region (222 nm). Protein chains are shown to be totally unfolded (and separated in the reduced species) in the initial denaturing medium and fully folded as two-chain coiled coils in the final benign medium. In all cases of folding in benign buffer of totally unfolded chains, two phases were found in the folding process: a fast phase (less than 0.04 s, the SFCD dead time), in which an intermediate state with about 70% of the equilibrium ellipticity forms; followed by a slower, observable phase that completes the folding. The slow phase is first order (k-1 = 1.6 s at 20 degrees C), signifying that chain association for reduced samples occurs in the fast phase. In contrast, folding in benign buffer from an initial state with 70% of the equilibrium ellipticity is all fast, suggesting that the folding intermediate is not an equilibrium species. Cross-linking at Cys-190 increases the helix content of the fast-formed intermediate state to about 85% of the equilibrium value, but leaves the rate constant of the slow phase unchanged. In NPTm, which does not form high aggregates at low ionic strength, the rate of the observable phase is almost independent of ionic strength in the range of approximately 0.15-0.6 M, but is reduced one to two orders of magnitude by further reduction to 0.026 M. In folding from totally unfolded chains, the rate is reduced less than one order of magnitude by changing the final state to about 50% folded. In contrast to folding, unfolding of alpha alpha-tropomyosin from the native state is all fast.     

The CD of two-chain coiled coils: experiments on tropomyosin and tropomyosin segments in the tyrosine/disulfide spectral region

CD experiments are reported for several coiled-coil species in the tyrosine/disulfide (approximately 250-350-nm) region. Intact noncross-linked tropomyosin (approximately 3 degrees C) shows a negative nonsymmetric band maximal at 280 nm. This spectrum is the sum over six tyrosines/chain, and has conformational significance, since it disappears on denaturation. Experiments on an excised coiled-coil segment, each of whose chains comprise residues 11-127 of the tropomyosin sequence and only one tyrosine (Y60), reveal that not all tyrosines are alike. The spectrum at 3 degrees C shows a small negative maximum at approximately 285 nm and a substantial, hitherto unknown, positive band at approximately 270 nm, the latter masked in the parent protein by the negative contribution from the other tyrosines. A noncross-linked coiled-coil segment comprising residues 142-281, in which Y60 is absent, shows no such positive band. This peculiarity of Y60 is confirmed by absorbance spectra, with the extinction coefficient of Y60 larger in benign media than the average of the other tyrosines. Intact (3 degrees C) C190 cross-linked tropomyosin is known to yield, besides tyrosine contributions, a positive maximum at approximately 300 nm. Subtracting the corresponding data for noncross-linked tropomyosin shows that the disulfide spectrum itself actually has two equal, partly resolved bands at, respectively, 250 and 280 nm. The existence of a chiral disulfide argues for a relatively rigid, perhaps strained, local coiled coil. A C190 cross-linked segment comprising residues 142-281 shows a chiral disulfide spectrum like tropomyosin's, but another segment, comprising residues 168-284, shows none; thus removal of residues 142-167 causes loss of chirality at C190, over 20 residues away. These spectra thus contain important information on the subtle local differences in coiled-coil structures.     

Specific sequences determine the stability and cooperativity of folding of the C-terminal half of tropomyosin

Tropomyosin is a flexible 410 A coiled-coil protein in which the relative stabilities of specific regions may be important for its proper function in the control of muscle contraction. In addition, tropomyosin can be used as a simple model of natural occurrence to understand the inter- and intramolecular interactions that govern the stability of coiled-coils. We have produced eight recombinant tropomyosin fragments (Tm(143-284(5OHW),) Tm(189-284(5OHW)), Tm(189-284), Tm(220-284(5OHW)), Tm(220-284), Tm(143-235), Tm(167-260), and Tm(143-260)) and one synthetic peptide (Ac-Tm(215-235)) to investigate the relative conformational stability of different regions derived from the C-terminal region of the protein, which is known to interact with the troponin complex. Analytical ultracentrifugation experiments show that the fragments that include the last 24 residues of the molecule (Tm(143-284(5OHW)), Tm(189-284(5OHW)), Tm(220-284(5OHW)), Tm(220-284)) are completely dimerized at 10 microm dimer (50 mm phosphate, 100 mm NaCl, 1.0 mm dithiothreitol, and 0.5 mm EDTA, 10 degrees C), whereas fragments that lack the native C terminus (Tm(143-235),Tm(167-260), and Tm(143-260)) are in a monomer-dimer equilibrium under these conditions. The presence of trifluoroethanol resulted in a reduction in the [theta](222)/[theta](208) circular dichroism ratio in all of the fragments and induced stable trimer formation only in those containing residues 261-284. Urea denaturation monitored by circular dichroism and fluorescence revealed that residues 261-284 of tropomyosin are very important for the stability of the C-terminal half of the molecule as a whole. Furthermore, the absence of this region greatly increases the cooperativity of urea-induced unfolding. Temperature and urea denaturation experiments show that Tm(143-235) is less stable than other fragments of the same size. We have identified a number of factors that may contribute to this particular instability, including an interhelix repulsion between g and e' positions of the heptad repeat, a charged residue at the hydrophobic coiled-coil interface, and a greater fraction of beta-branched residues located at d positions.     

Different effects of trifluoroethanol and glycerol on the stability of tropomyosin helices and the head-to-tail complex

Tropomyosin (Tm) is a dimeric coiled-coil protein, composed of 284 amino acids (410 A), that forms linear homopolymers through head-to-tail interactions at low ionic strength. The head-to-tail complex involves the overlap of approximately nine N-terminal residues of one molecule with nine C-terminal residues of another Tm molecule. In this study, we investigate the influence of 2,2,2-trifluoroethanol (TFE) and glycerol on the stability of recombinant Tm fragments (ASTm1-142, Tm143-284(5OHW269)) and of the dimeric head-to-tail complex formed by the association of these two fragments. The C-terminal fragment (Tm143-284(5OHW269)) contains a 5-hydroxytryptophan (5OHW) probe at position 269 whose fluorescence is sensitive to the head-to-tail interaction and allows us to accompany titrations of Tm143-284(5OHW269) with ASTm1-142 to calculate the dissociation constant (Kd) and the interaction energy at TFE and glycerol concentrations between 0% and 15%. We observe that TFE, but not glycerol, reduces the stability of the head-to-tail complex. Thermal denaturation experiments also showed that the head-to-tail complex increases the overall conformational stability of the Tm fragments. Urea and thermal denaturation assays demonstrated that both TFE and glycerol increase the stability of the isolated N- and C-terminal fragments; however, only TFE caused a significant reduction in the cooperativity of unfolding these fragments. Our results show that these two cosolvents stabilize the structures of individual Tm fragments in different manners and that these differences may be related to their opposing effects on head-to-tail complex formation.     

Further characterization of the kinetic folding intermediate of αα-tropomyosin and of its 142–281 subsequence

The backbone CD spectrum from 250 to 212 nm for the kinetic folding intermediate of αα-tropomyosin (αα-Tm) and nonpolymerizable αα-Tm was obtained. The spectrum shows that the intermediate is indeed α-helical with about 70% of the equilibrium α-helix content. Subsequence ₁₄₂Tm₂₈₁ of the α-tropomyosin chain has five tyrosine residues (at positions 162, 214, 221, 261, 267). Stopped flow CD at the negative peak in the tyrosine spectral region (280 nm) shows that any tyrosine residues that contribute to the spectrum in the region have already reached their final state in the fast phase of folding ( < 0.04 s). © 1993 John Wiley & Sons, Inc.     

Structural stability of short subsequences of the tropomyosin chain

The native tropomyosin molecule is a parallel, registered, α-helical coiled coil made from two 284-residiic chains. Long excised subsequences (≥ 95 residues) form the same structure with comparable thermal stability. Here, we investigate local stability using shorter subsequences (20-50 residues) that are chemically synthesized or excised from various regions along the protein chain. Thermal unfolding studies of such shorter peptides by CD in the same solvent medium used in extant studies of the parent protein indicate very low helix content, almost no coiled-coil formation, and high thermal lability of such secondary structure as does form. This behavior is in stark contrast to extant data on leucine-zipper peptides and short “designed” synthetic peptides, many of which have high α-helix content and form highly stable coiled coils. The existence of short coiled coils calls into question the older idea that short subsequences of a protein have little structure. The present study supports the older view, at least in its application to tropomyosin. The intrinsic local α-helical propensity and helix–helix interaction in this prototypical α-helical protein is sufficiently weak as to require not only dimerization, but macro-molecular amplification in order to attain its native conformation in common benign media near neutral pH. © 1995 John Wiley & Sons, Inc.     

A specific C-terminal deletion in tropomyosin results in a stronger head-to-tail interaction and increased polymerization.

Tropomyosin is a 284 residue dimeric coiled-coil protein that interacts in a head-to-tail manner to form linear filaments at low ionic strengths. Polymerization is related to tropomyosin's ability to bind actin, and both properties depend on intact N- and C-termini as well as alpha-amino acetylation of the N-terminus of the muscle protein. Nalpha-acetylation can be mimicked by an N-terminal Ala-Ser fusion in recombinant tropomyosin (ASTm) produced in Escherichia coli. Here we show that a recombinant tropomyosin fragment, corresponding to the protein's first 260 residues plus an Ala-Ser fusion [ASTm(1-260)], polymerizes to a much greater extent than the corresponding full-length recombinant protein, despite the absence of the C-terminal 24 amino acids. This polymerization is sensitive to ionic strength and is greatly reduced by the removal of the N-terminal Ala-Ser fusion [nfTm(1-260)]. CD studies show that nonpolymerizable tropomyosin fragments, which terminate at position 260 [Tm(167-260) and Tm(143-260)], as well as Tm(220-284), are able to interact with ASTm(1-142), a nonpolymerizable N-terminal fragment, and that the head-to-tail interactions observed for these fragment pairs are accompanied by a significant degree of folding of the C-terminal tropomyosin fragment. These results suggest that the new C-terminus, created by the deletion, polymerizes in a manner similar to the full-length protein. Head-to-tail binding for fragments terminating at position 260 may be explained by the presence of a greater concentration of negatively charged residues, while, at the same time, maintaining a conserved pattern of charged and hydrophobic residues found in polymerizable tropomyosins from a variety of sources.     

Caldesmon-binding sites on tropomyosin

The interaction of chicken gizzard caldesmon with fragments of tropomyosin, generated by chemical, enzymatic, and mutational means, was studied to determine the caldesmon-binding site(s) on tropomyosin. Binding was examined by fluorescence spectroscopy and affinity chromatography. Removal of residues 1-141 and 228-284, respectively, from the NH2 and COOH ends of tropomyosin did not affect its binding to caldesmon significantly, indicating that the major, caldesmon-binding region lies between residues 142-227. The Escherichia coli produced chicken gizzard beta-tropomyosin mutant, CSM-beta (1/8/12-227), bound caldesmon about 2-fold stronger than a similar mutant of residues 8-200. This further focused the primary caldesmon-binding site to residues 201-227. Cleavage of tropomyosin at CYS-190 weakened markedly the binding of the two resulting fragments, residues 1-189 and 190-284, to caldesmon suggesting the requirement for the integrity of the caldesmon-binding region between residues 142227 of tropomyosin for strong interaction with caldesmon. Based on data from this study and others, we have proposed models for the interaction of tropomyosin with caldesmon in vitro, as well as the possible arrangement of the smooth muscle thin filament proteins in vivo.     

Probing the folding and unfolding dynamics of secondary and tertiary structures in a three-helix bundle protein

Fast relaxation kinetics studies of the B-domain of staphylococcal protein A were performed to characterize the folding and unfolding of this small three-helix bundle protein. The relaxation kinetics were initiated using a laser-induced temperature jump and probed using time-resolved infrared spectroscopy. The kinetics monitored within the amide I' absorbance of the polypeptide backbone exhibit two distinct kinetics phases with nanosecond and microsecond relaxation times. The fast kinetics relaxation time is close to the diffusion limits placed on protein folding reactions. The fast kinetics phase is dominated by the relaxation of the solvated helix (nu = 1632 cm(-1)), which reports on the fast relaxation of the individual helices. The slow kinetics phase follows the cooperative relaxation of the native helical bundle core that is monitored by both solvated (nu = 1632 cm(-1)) and buried helical IR bands (nu = 1652 cm(-1)). The folding rates of the slow kinetics phase calculated over an extended temperature range indicate that the core formation of this protein follows a pathway that is energetically downhill. The unfolding rates are much more strongly temperature-dependent indicating an activated process with a large energy barrier. These results provide significant insight into the primary process of protein folding and suggest that fast formation of helices can drive the folding of helical proteins.     

Investigating the tolerance of coiled-coil peptides to nonheptad sequence inserts

Coiled-coil motifs foster a wide variety of protein-protein interactions. Canonical coiled coils are based on 7-residue repeats, which guide the folding and assembly of amphipathic alpha-helices. In many cases such repeats remain unbroken for tens to hundreds of residues. However, the sequences of an increasing number of putative and characterised coiled coils digress from this pattern. We probed the consequences of nonheptad inserts using a designed leucine-zipper system. The parent peptide, SKIP0, which had four contiguous heptads, was confirmed as a parallel homodimer by circular dichroism spectroscopy and analytical ultracentrifugation. Seven daughter peptides were constructed in which 1 to 7 alanine residues were inserted between the central heptads of SKIP0. Like SKIP0, SKIP7 formed a stable helical dimer, but the other peptides were highly destabilised, with the order of dimer stability SKIP4 > SKIP5 > SKIP6 > SKIP3 > SKIP2 > SKIP1. These results are consistent with an extended theory of coiled-coil assembly in which coiled-coil-compatible motifs are based on 3- and 4-residue spacings and most notably heptad (7-residue) and hendecad (11-residue) repeats. Thus, they help explain why in natural sequences, inserts after canonical heptad repeats most commonly comprise 4 residues. Possible biological roles for nonheptad inserts are discussed.     

Unique fluorophores in the dimeric archaeal histones hMfB and hPyA1 reveal the impact of nonnative structure in a monomeric kinetic intermediate

Homodimeric archaeal histones and heterodimeric eukaryotic histones share a conserved structure but fold through different kinetic mechanisms, with a correlation between faster folding/association rates and the population of kinetic intermediates. Wild-type hMfB (from Methanothermus fervidus) has no intrinsic fluorophores; Met35, which is Tyr in hyperthermophilic archaeal histones such as hPyA1 (from Pyrococcus strain GB-3A), was mutated to Tyr and Trp. Two Tyr-to-Trp mutants of hPyA1 were also characterized. All fluorophores were introduced into the long, central alpha-helix of the histone fold. Far-UV circular dichroism (CD) indicated that the fluorophores did not significantly alter the helical content of the histones. The equilibrium unfolding transitions of the histone variants were two-state, reversible processes, with DeltaG degrees (H2O) values within 1 kcal/mol of the wild-type dimers. The hPyA1 Trp variants fold by two-state kinetic mechanisms like wild-type hPyA1, but with increased folding and unfolding rates, suggesting that the mutated residues (Tyr-32 and Tyr-36) contribute to transition state structure. Like wild-type hMfB, M35Y and M35W hMfB fold by a three-state mechanism, with a stopped-flow CD burst-phase monomeric intermediate. The M35 mutants populate monomeric intermediates with increased secondary structure and stability but exhibit decreased folding rates; this suggests that nonnative interactions occur from burial of the hydrophobic Tyr and Trp residues in this kinetic intermediate. These results implicate the long central helix as a key component of the structure in the kinetic monomeric intermediates of hMfB as well as the dimerization transition state in the folding of hPyA1.     

The thermal denaturation of nonpolymerizable alpha alpha-tropomyosin and its segments as a function of ionic strength

Nonpolymerizable tropomyosin (NPTm) is found to unfold thermally at high ionic strength almost exactly as the parent protein, but it does not aggregate at low ionic strength. Thus, NPTm can be used as a tropomyosin surrogate whose coiled-coil structural stability can be probed by varying the ionic strength. Studies of NPTm by CD show that increasing ionic strength stabilizes the coiled-coil structure. CD spectra over a wide range of helix content, obtained by varying either temperature or ionic strength, show an isodichroic point at 203 nm, suggesting a local, residue-level, two-state model. At given temperature, such a local helix in equilibrium random equilibrium suggests ln [phi h/(1-phi h)] = A1 + A2In, wherein phi h is the fraction helix, and A1, A2, and n are constants. In the low ionic strength region, theoretical limiting laws for ionic strength mediated charge-charge, dipole-dipole, and apolar-apolar (salting out) interactions give, respectively, n = 0.5, 1.0, and 1.0. Our experimental values for 40 degrees C, where the data span a wide range of helix content, show n = 1.0, suggesting that ionic strength stabilizes either by reducing dipole-dipole repulsions or by enhancing hydrophobic interactions, both probably interhelix in nature. Two segments of tropomyosin, 11Tm127 and 142Tm281, neither of which aggregate at low ionic strength, give results similar to those for NPTm, i.e., n = 0.96 and 0.84, respectively.     

Folding of the multidomain ribosomal protein L9: the two domains fold independently with remarkably different rates

The folding and unfolding behavior of the multidomain ribosomal protein L9 from Bacillus stearothermophilus was studied by a novel combination of stopped-flow fluorescence and nuclear magnetic resonance (NMR) spectroscopy. One-dimensional 1H spectra acquired at various temperatures show that the C-terminal domain unfolds at a lower temperature than the N-terminal domain (Tm = 67 degrees C for the C-terminal domain, 80 degrees C for the N-terminal domain). NMR line-shape analysis was used to determine the folding and unfolding rates for the N-terminal domain. At 72 degrees C, the folding rate constant equals 2980 s-1 and the unfolding rate constant equals 640 s-1. For the C-terminal domain, saturation transfer experiments performed at 69 degrees C were used to determine the folding rate constant, 3.3 s-1, and the unfolding rate constant, 9.0 s-1. Stopped-flow fluorescence experiments detected two resolved phases: a fast phase for the N-terminal domain and a slow phase for the C-terminal domain. The folding and unfolding rate constants determined by stopped-flow fluorescence are 760 s-1 and 0.36 s-1, respectively, for the N-terminal domain at 25 degrees C and 3.0 s-1 and 0.0025 s-1 for the C-terminal domain. The Chevron plots for both domains show a V-shaped curve that is indicative of two-state folding. The measured folding rate constants for the N-terminal domain in the intact protein are very similar to the values determined for the isolated N-terminal domain, demonstrating that the folding kinetics of this domain is not affected by the rest of the protein. The remarkably different rate constants between the N- and C-terminal domains suggest that the two domains can fold and unfold independently. The folding behavior of L9 argues that extremely rapid folding is not necessarily functionally important.     

Exploring deltorphin II binding to the third extracellular loop of the delta-opioid receptor

The third extracellular loop of the human delta-opioid receptor (hDOR) is known to play an important role in the binding of delta-selective ligands. In particular, mutation of three amino acids (Trp(284), Val(296), and Val(297)) to alanine significantly diminished delta-opioid receptor affinity for delta-selective ligands. To assess the changes in conformation accompanying binding of the endogenous opioid peptide deltorphin II to the delta-opioid receptor at both the receptor and ligand levels as well as to determine points of contact between the two, an in-depth spectroscopic study that addressed these points was initiated. Fragments of the delta-opioid receptor of variable length and containing residues in the third extracellular loop were synthesized and studied by NMR and CD spectroscopy in a membrane-mimetic milieu. The receptor peptides examined included hDOR-(279-299), hDOR-(283-299), hDOR-(281-297), and hDOR-(283-297). A helical conformation was observed for the longest receptor fragment between Val(283) and Arg(291), whereas a nascent helix occurred in a similar region for hDOR-(281-297). Further removal of N-terminal residues Val(281) and Ile(282) abolished helical conformation completely. Binding of the delta-selective ligand deltorphin II to hDOR-(279-299) destabilized the helix at the receptor peptide N terminus. Dramatic changes in the alpha-proton chemical shifts for Trp(284) and Leu(286) in hDOR-(279-299) also accompanied this loss of helical conformation. Large upfield displacement of alpha-proton chemical shifts was observed for Leu(295), Val(296), and Val(297) in hDOR-(279-299) following its interaction with deltorphin II, thus identifying a gain in beta-conformation at the receptor peptide C terminus. Similar changes did not occur for the shorter peptide hDOR(281-297). A hypothesis describing the conformational events accompanying selective deltorphin II binding to the delta-opioid receptor is presented.     

Kinetics of folding and unfolding of beta beta-tropomyosin.

The kinetics of folding from random coils to two-chain coiled coils of beta beta-tropomyosin was studied by stopped-flow CD (SFCD) in the backbone region (222 nm). Two species were studied: the reduced form and the doubly disulfide cross-linked form. The proteins were totally unfolded in 6M urea-saline buffer, then refolded by tenfold dilution into benign buffer. In the refolding medium, they spontaneously recover the two-chain coiled-coil structure. Reduced beta beta refolds in at least two stages: one or more fast phases (< 0.04 s), in which an intermediate with 71% of the equilibrium ellipticity forms, followed by a slower time-resolvable phase that completes the folding. The slow phase is first order, signifying that dimerization occurs in the fast phase. The time constant of the slow phase is 2 s at 20 degrees C and requires activation parameters of delta S not equal to = -7 +/- 0.3 cal/mol.K, delta H not equal to = 15 +/- 1 kcal/mol. These results are very similar to those previously found for the reduced genetic variant alpha alpha-tropomyosin. In contrast, refolding of doubly disulfide cross-linked beta beta is complete within the dead time (< 0.04 s), whereas the singly cross-linked alpha alpha species also displays a slow phase. The opposite process, unfolding reduced beta beta from the coiled-coil state, is complete within the dead time, as in the alpha alpha variant.     

Consequences of stabilizing the natively disordered f helix for the folding pathway of apomyoglobin

The F helix region of sperm whale apomyoglobin is disordered, undergoing conformational fluctuations between a folded helical conformation and one or more locally unfolded states. To examine the effects of F helix stabilization on the folding pathway of apomyoglobin, we have introduced mutations to augment intrinsic helical structure in the F helix of the kinetic folding intermediate and to increase its propensity to fold early in the pathway, using predictions based on plots of the average area buried upon folding (AABUF) derived from the primary sequence. Two mutant proteins were prepared: a double mutant, P88K/S92K (F2), and a quadruple mutant, P88K/A90L/S92K/A94L (F4). Whereas the AABUF for F2 predicts that the F helix will not fold early in the pathway, the F helix in F4 shows a significantly increased AABUF and is therefore predicted to fold early. Protection of amide protons by formation of hydrogen-bonded helical structure during the early folding events has been analyzed by pH-pulse labeling. Consistent with the AABUF prediction, many of the F helix residues for F4 are significantly protected in the kinetic intermediate but are not protected in the F2 mutant. F4 folds via a kinetically trapped burst-phase intermediate that contains stabilized secondary structure in the A, B, F, G, and H helix regions. Rapid folding of the F helix stabilizes the central core of the misfolded intermediate and inhibits translocation of the H helix back to its native position, thereby decreasing the overall folding rate.