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 kinetics of chain exchange in two-chain coiled coils: alpha alpha- and beta beta-tropomyosin.

Measurements are presented on the time course of chain exchange among two-chain alpha-helical coiled coils of rabbit tropomyosin. All experiments are in a regime (temperature, protein concentration) in which coiled-coil dimers are the predominant species. Self-exchange in alpha alpha-tropomyosin was investigated by mixing alpha alpha species with alpha* alpha*, the asterisk designating an alpha-chain whose lone sulfhydryl (C190) has been blocked by carboxyamidomethylation. The overall process alpha alpha + alpha* alpha* in equilibrium with 2 alpha alpha* is followed by measurement of the fraction (h) of alpha alpha* species as a function of time. Similarly, self-exchange in beta beta-tropomyosin is examined by measurements of the overall process: beta beta + beta* beta* in equilibrium with 2 beta beta*, in which beta* signifies a beta-chain blocked at both sulfhydryls (C36 and C190). The observed time course for both chains is well fit by the first-order equation: h (t) = h (infinity) (1-e-k1t), with h (infinity) congruent to 0.5. This long-time limit is as expected for self-exchange, and agrees with experiments that attain equilibrium after slow cooling of thermally dissociated and unfolded chains. The simplest consonant mechanism is chain exchange by rate-limiting dissociation of dimers followed by random reassociation. Kinetic analysis shows k1 to be the rate constant for the chain dissociation step, a quantity not previously measured for any coiled coil. This rate constant for beta beta species is about an order of magnitude greater than for alpha alpha. In both, the activation enthalpy and entropy are very large, suggesting that activation to an extensively (greater than 50%) unfolded species necessarily precedes dissociation. Experiments are also reported for overall processes: alpha alpha + beta* beta* in equilibrium with 2 alpha beta* and alpha* alpha* + beta beta in equilibrium with 2 alpha* beta. Results are independent of which chain is blocked. Again h (infinity) congruent to 0.5, in agreement with equilibrium experiments, and the time course is first order. The rate constants and activation parameters are intermediate between those for self-exchange.     

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.     

Application of the augmented theory of alpha-helix-to-random-coil transitions of two-chain, coiled coils to extant data on synthetic, tropomyosin-analog peptides

The statistical mechanical theory for the helix-to-random-coil transition in two-chain coiled coils is applied to extant data for two synthetic coiled-coil polypeptides. These peptides have the primary structure K(LEALEGK)_n, in which n = 4, 5. This repeating heptet sequence mimics the pattern of hydrophobic, acidic, and basic residues characteristic of the 284-residue tropomyosin molecule, the prototypical coiled-coil protein. Theoretical calculations for single chains show that such model peptides cannot be directly compared to proteins like tropomyosin because of differences in chain length (29 and 36 residues vs 284) and in intrachain interactions, the latter caused by the differences in amino acid composition and seqeunce between protein and model. Application of the theory to extant data on the two synthetic peptides provides a semiquantitative fit and results in an assessment of the interhelix interaction in the model peptides. The value obtained, ～ 2000 cal · (mol of turn pairs)^–1, is four to five times larger than has been obtained for tropomyosin. This probably is a result of greater regularity in the structure of the synthetics and of the exclusive presence of leucine in the hydrophobic interface. The theory employed here insists that this powerful interhelix interaction in the synthetic is the principal reason that such short chains can be so highly helical at moderate and low temperatures. Theory predicts, indeed, that a tropomyosin-length chain with a sequence homologous to these synthetics would be completely thermally stable in the entire temperature range accessible in aqueous solutions. Theory also predicts a much more pronounced effect of concentration on the 29- and 36-residue synthetic polymers than is predicted or observed in the case of tropomyosin, and it also predicts a pronounced stabilizing effect of pH-reduction on the thermal curves. On the last two points, sufficient data are not yet available with which to test the theory.     

Coiled-coil trigger motifs in the 1B and 2B rod domain segments are required for the stability of keratin intermediate filaments

Many alpha-helical proteins that form two-chain coiled coils possess a 13-residue trigger motif that seems to be required for the stability of the coiled coil. However, as currently defined, the motif is absent from intermediate filament (IF) protein chains, which nevertheless form segmented two-chain coiled coils. In the present work, we have searched for and identified two regions in IF chains that are essential for the stability necessary for the formation of coiled-coil molecules and thus may function as trigger motifs. We made a series of point substitutions with the keratin 5/keratin 14 IF system. Combinations of the wild-type and mutant chains were assembled in vitro and in vivo, and the stabilities of two-chain (one-molecule) and two-molecule assemblies were examined with use of a urea disassembly assay. Our new data document that there is a region located between residues 100 and 113 of the 2B rod domain segment that is absolutely required for molecular stability and IF assembly. This potential trigger motif differs slightly from the consensus in having an Asp residue at position 4 (instead of a Glu) and a Thr residue at position 9 (instead of a charged residue), but there is an absolute requirement for a Glu residue at position 6. Because these 13 residues are highly conserved, it seems possible that this motif functions in all IF chains. Likewise, by testing keratin IF with substitutions in both chains, we identified a second potential trigger motif between residues 79 and 91 of the 1B rod domain segment, which may also be conserved in all IF chains. However, we were unable to find a trigger motif in the 1A rod domain segment. In addition, many other point substitutions had little detectable effect on IF assembly, except for the conserved Lys-23 residue of the 2B rod domain segment. Cross-linking and modeling studies revealed that Lys-23 may lie very close to Glu-106 when two molecules are aligned in the A(22) mode. Thus, the Glu-106 residue may have a dual role in IF structure: it may participate in trigger formation to afford special stability to the two-chain coiled-coil molecule, and it may participate in stabilization of the two-molecule hierarchical stage of IF structure.     

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.     

Role of topological constraints in the all-or-none transition of a globular protein model: theory of the helix-coil transition in doubly crosslinked, coiled coils

Employing a recently developed statistical mechanical theory, the alpha-helix-to-random-coil transition in two-chain, coiled coils is shown to possess many of the essential qualitative features of the equilibrium folding process in globular proteins. The role of short vs. long range interactions in stabilizing the native structure is examined. We demonstrate in doubly crosslinked coiled coils how, due to the role of loop entropy, an intrinsically continuous conformational transition evolves into one well approximated by an all-or-none transition. Thus the present work points out the crucial role played by loop entropy in the conformational transition in coiled coils in particular and perhaps in globular proteins in general.     

Hetero-α-helical,two-chain coiled-coils. Clam–worm hybrid paramyosins

The specificity of the interaction between the α-helices in two-chain coiled-coils is investigated by studying the formation of hybrid molecules in which one α-helix is a clam paramyosin chain and the other a worm paramyosin chain. Hybrids are formed by mixing, denaturation, and subsequent renaturation. Comparison is made with a blank solution in which renaturation precedes mixing, thus precluding hybridization. Hybrids are detected by a ruse based on the presence of free sulfhydryl functions on calm chains. This allows molecules comprising two clam chains to be covalently crosslinked by oxidation with 5,5′-dithiobis(2-nitrobenzoate). Worm paramyosin chains have no sulfhydryl, so molecules comprising two worm chains or hybrid molecules comprising one chain of each type cannot crosslink. When run on sodium dodecyl sulfate polyacrylamide gel electrophoresis, therefore, the protein separates into two well-resolved regions, one containing one-chain species and the other two-chain species. When the gels are scanned and quantitated, the hybrids show up as an increase in the fraction of material in the one-chain band compared with the fraction in the blank solution. When renaturation is direct, we find that the fraction of renaturated molecules that are hybrids varies from ～10% at 5°C to ～5% at 25°C. These are judged to be nonequilibrium (quenched) values. When renaturation is by slow annealing, the equilibrium fraction hybrids are ～4% and show a modest, but measurable, increase with increasing temperature. These data allow calculation of the equilibrium constant K_h and standard free energy for the hybridization reaction: (1/2)CC + (½)WW = CW, in which C(W) stands for an α-helical clam (worm) polypeptide chain. The temperature dependence gives the standard enthalpy and entropy of the reaction. We find ΔH ? 1800 cal mol^?1 and ΔH ? 1.4 cal mol^?1 K^?1, using molarity concentration units and the infinitely dilute solution in NaCl/phosphate buffer as reference state. The possible molecular significance of these values is discussed, and it is concluded that the observed standard entropy arises essentially entirely from the rotational dissymmetry of the hybrids.     

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.     

Alpha-helix to random-coil transition of two-chain, coiled coils: experiments on the thermal denaturation of doubly cross-linked beta beta tropomyosin

Equilibrium thermal denaturation curves (by circular dichroism) are reported for doubly cross-linked beta beta tropomyosin two-chain coiled coils. Cross-linking was performed by reaction of sulfhydryls with either ferricyanide or 5,5'-dithiobis(2-nitrobenzoate) (NbS2). The extent of reaction was determined by sodium dodecyl sulfate-polyacrylamide gel electrophoresis and either by titration of residual sulfhydryls with NbS2 (ferricyanide cross-linking) or by determination of mixed disulfide (protein-S-SbN) through reaction with dithiothreitol (NbS2 cross-linking). The results indicate approximately 90% conversion to molecules with interchain cross-links at both C-36 and C-190. Thermal unfolding curves are compared with those obtained previously for non-cross-linked species. The curves are indistinguishable up to approximately 40 degrees C. Above approximately 40 degrees C, the doubly cross-linked species is more stable, but the transition is less steep. This relationship is also compared with that found between alpha alpha tropomyosin (a similar coiled coil made of a genetic variant chain having a sulfhydryl only at C-190) and its singly cross-linked derivative. Thermal curves for alpha alpha and beta beta non-cross-linked species are very similar, alpha alpha being somewhat more stable. For cross-linked alpha alpha, however, the curve sags at temperatures somewhat below the region of principal cooperative loss of helix, the latter occurring at higher temperature but with the same steepness as in the non-cross-linked case. The sag has been ascribed to a "pretransition" in the region of C-190. Thus, doubly and singly cross-linked species differ in that the former show no pretransition and decreased steepness in the principal transition.(ABSTRACT TRUNCATED AT 250 WORDS)     

Folding of a three-stranded coiled coil

Coiled coils consist of two or more amphipathic a-helices wrapped around each other to form a superhelical structure stabilized at the interhelical interface by hydrophobic residues spaced in a repeating 3-4 sequence pattern. Dimeric coiled coils have been shown to often form in a single step reaction in which association and folding of peptide chains are tightly coupled. Here, we ask whether such a simple folding mechanism may also apply to the formation of a three-stranded coiled coil. The designed 29-residue peptide LZ16A was shown previously to be in a concentration-dependent equilibrium between unfolded monomer (M), folded dimer (D), and folded trimer (T). We show by time-resolved fluorescence change experiments that folding of LZ16A to D and T can be described by 2M (k1)<==>(k(-1)) D and M + D (k2)<==>(k(-2)) T. The following rate constants were determined (25 degrees C, pH 7): k1 = 7.8 x 10(4) M(-1) s(-1), k(-1) = 0.015 s(-1), k2 = 6.5 x 10(5) M(-1) s(-1), and k(-2) = 1.1 s(-1). In a separate experiment, equilibrium binding constants were determined from the change with concentration of the far-ultraviolet circular dichroism spectrum of LZ16A and were in good agreement with the kinetic rate constants according to K(D) = k1/2k(-1) and K(T) = k2/k(-2). Furthermore, pulsed hydrogen-exchange experiments indicated that only unfolded M and folded D and T were significantly populated during folding. The results are compatible with a two-step reaction in which a subpopulation of association competent (e.g., partly helical) monomers associate to dimeric and trimeric coiled coils.     

Some properties of acid-reassembled tropomyosin

The preference for parallelism of the two chains in tropomyosin coiled coils is thought to result from interchain salt bridges. To examine this idea, studies are presented of tropomyosin molecules reassembled from chaotropic solvents in acid solution, where cross-links cannot exist. The acid-reassembled molecules are appreciably less disulfide cross-linkable in acid than native molecules, a result explainable if some antiparallel dimers indeed form at low pH. Physical studies (backbone- and tyrosine-region CD and intrinsic viscosity) indicate that refolding in acid yields a molecular population demonstrably different in tyrosine-region CD from native, but having comparable (but not identical) helix content, thermal stability, and dimensions. Moreover, the refolding in acid after either thermal or chaotropic-solvent denaturation yields the same final state, arguing that it is an equilibrium state. All these results are consistent with, but do not prove, that the acid-reassembled population includes an appreciable fraction (2/3) of antiparallel coiled-coil dimers. © 1995 John Wiley & Sons, Inc.     

Monoclonal antibodies reveal the alteration of the rhodocetin structure upon α2β1 integrin binding

The α2β1 antagonist rhodocetin from Calloselasma rhodostoma is a heterotetrameric CLRP (C-type lectin-related protein) consisting of four distinct chains, α, β, γ and δ. Via their characteristic domain-swapping loops, the individual chains form two subunits, αβ and γδ. To distinguish the four chains which share similar molecular masses and high sequence homologies, we generated 11 mAbs (monoclonal antibodies) with different epitope specificities. Four groups of distinct mAbs were generated: the first targeted the rhodocetin β chain, the second group bound to the αβ subunit mostly in a conformation-dependent manner, the third group recognized the γδ subunit only when separated from the αβ subunit, whereas a fourth group interacted with the γδ subunit both in the heterotetrameric molecule and complexed with the integrin α2 A-domain. Using the specific mAbs, we have shown that the rhodocetin heterotetramer dissociates into the αβ and γδ subunit upon binding to the integrin α2 A-domain at both the molecular and cellular levels. After dissociation, the γδ subunit firmly interacts with the α2β1 integrin, thereby blocking it, whereas the rhodocetin αβ subunit is released from the complex. The small molecular interface between the αβ and γδ subunits within rhodocetin is mostly mediated by charged residues, which causes the two dissociated subunits to have hydrophilic surfaces.     

Designed coiled-coil proteins: synthesis and spectroscopy of two 78-residue alpha-helical dimers.

Receptor-adhesive modular proteins are nongenetic proteins designed to contain ligand, spacer, coil, and linker modules and to interact strongly with integrins or other types of cell-surface receptors. We have designed, chemically synthesized, and characterized a 39-residue peptide chain having a 6-residue ligand module (Gly-Arg-Gly-Asp-Ser-Pro-) for adherence to Arg-Gly-Asp-binding integrin receptors, a 3-residue spacer module (-Gly-Tyr-Gly-) for flexibility, and a 30-residue coil module [-(Arg-Ile-Glu-Ala-Ile-Glu-Ala) 4-Arg-Cys-NH2] containing four 7-residue repeats for dimerization. This chain was designed to form a 78-residue noncovalent dimer (P39) by folding the coils of two chains into an alpha-helical coiled coil through hydrophobic interaction of eight pairs of Ile residues. Air oxidation of P39 gave P78, a 78-residue covalent dimer having a disulfide bridge linking its C termini. Raman spectroscopy indicated that both synthetic proteins have high alpha-helical content. Ultraviolet circular dichroic spectroscopy indicated that both dimers contain stable alpha-helical coiled coils. Its C-terminal disulfide bridge renders P78 significantly more stable than P39 to thermal denaturation or denaturation by urea. The coiled coil of P39 was 30% unfolded near 55 degrees C and half-unfolded in 8 M urea, while that of P78 was 30% unfolded only near 85 degrees C. These studies have demonstrated the feasibility of using these ligand, spacer, and coil modules to construct the designed coiled-coil proteins P39 and P78, a stage in the nanometric engineering of receptor-adhesive modular proteins.     

Separation, purification, partial characterization and comparison of the heavy and light chains of botulinum neurotoxin types A, B, and E

Clostridium botulinum produces botulinum neurotoxin (NT) in antigenically distinct forms. When isolated from bacterial cultures type E is a single chain, type B is a mixture of single and two-chain molecules, and type A is essentially a two-chain molecule (Mr approximately 150,000). Protease(s) in the cultures or trypsin nick single-chain NT to the two-chain form. The heavy (Mr approximately 100,000) and light (Mr approximately 50,000) chains of the two-chain molecule remain held together by -S-S-bond(s). The two chains are presumed to have different functions. NT binds to nerve cells via the heavy chain and then light chain enters the cell and blocks release of acetylcholine (Simpson, L. L. (1981) Pharmacol. Rev. 33, 155-188). We nicked single-chain NT to form the two-chain form with trypsin, minimizing secondary cleavages, then separated and purified the heavy and light chains using ion-exchange chromatography. The technique, with minor modifications, is a generalized method for types A, B, and E. These subunit chains (each a single band in sodium dodecyl sulfatepolyacrylamide gel electrophoresis) were analyzed for their complete amino acid compositions. The amino acid contents of the heavy and light chains agreed well with the parent two-chain molecule. This affirms that NT is composed of two chains. The two subunit chains are now usable for amino acid sequence and other studies. Comparison of the amino acid contents indicates more similarity among the light chains than the heavy chains of the three NT types, a similarity that agrees with our published partial amino acid sequences (first 13-18 residues) of these chains. Several (up to 9) different amino acid residues of the heavy chain (which is twice the size of the light chain) are present in double the number of corresponding residues in the light chain.     

Thermal unfolding in a GCN4-like leucine zipper: 13C alpha NMR chemical shifts and local unfolding curves.

13C alpha chemical shifts and site-specific unfolding curves are reported for 12 sites on a 33-residue, GCN4-like leucine zipper peptide (GCN4-lzK), ranging over most of the chain and sampling most heptad positions. Data were derived from NMR spectra of nine synthetic, isosequential peptides bearing 99% 13C alpha at sites selected to avoid spectral overlap in each peptide. At each site, separate resonances appear for unfolded and folded forms, and most sites show resonances for two folded forms near room temperature. The observed chemical shifts suggest that 1) urea-unfolded GCN4-lzK chains are randomly coiled; 2) thermally unfolded chains include significant transient structure, except at the ends; 3) the coiled-coli structure in the folded chains is atypical near the C-terminus; 4) only those interior sites surrounded by canonical interchain salt bridges fail to show two folded forms. Local unfolding curves, obtained from integrated resonance intensities, show that 1) sites differ in structure content and in melting temperature, so the equilibrium population must comprise more than two molecular conformations; 2) there is significant end-fraying, even at the lowest temperatures, but thermal unfolding is not a progressive unwinding from the ends; 3) residues 9-16 are in the lowest melting region; 4) heptad position does not dictate stability; 5) significant unfolding occurs below room temperature, so the shallow, linear decline in backbone CD seen there has conformational significance. It seems that only a relatively complex array of conformational states could underlie these findings.     

ATP synthase b subunit dimerization domain: a right-handed coiled coil with offset helices

The dimerization domain of Escherichia coli ATP synthase b subunit forms an atypical parallel two-stranded coiled coil. Sequence analysis reveals an 11-residue abcdefghijk repeat characteristic of right-handed coiled coils, but no other naturally occurring parallel dimeric structure of this class has been identified. The arrangement of the helices was studied by their propensity to form interhelix disulfide linkages and analysis of the stability and shape of disulfide-linked dimers. Disulfides formed preferentially between cysteine residues in an a position of one helix and either of the adjacent h positions of the partner. Such heterodimers were far more stable to thermal denaturation than homodimers and, on the basis of gel-filtration chromatography studies, were similar in shape to both non-covalent dimers and dimers linked through flexible Gly(1-3)Cys C-terminal extensions. The results indicate a right-handed coiled-coil structure with intrinsic asymmetry, the two helices being offset rather than in register. A function for the right-handed coiled coil in rotational catalysis is proposed.     

Kinetics of folding of alpha alpha-tropomyosin subsequences.

The kinetics of folding random coils of alpha alpha-tropomyson (Tm) subsequences to two-chain coiled coils was studied by stopped-flow CD. Subsequences studied were those comprising residues 11-127 (11Tm127), 142-281 (142Tm281), 1-189 (1Tm189), and 190-284 (190Tm284) of the parent 284-residue alpha-tropomyosin chain. Unlike the parent, subsequences 1Tm189 and 11Tm127 fold within the dead time of the instrument (less than 0.04 s). Like the parent, subsequences 142Tm281 and 190Tm284 fold in two phases. In the fast phase, 45% and 32%, respectively, of the equilibrium helical content form. In the time-resolvable, first-order slow phase (k-1 = 2.7 s at 20 degrees C for 142Tm281 and k-1 = 2.0 s at 15 degrees C for 190Tm284), the remaining structure forms. Neither reduced 142Tm281 nor 190Tm284 show any dependence of the rate on concentration, so chain association occurs in the fast phase. Like the parent 142Tm281 forms more helical content in the fast phase when cross-linked at C-190, and the remaining structure forms slowly with rate parameters similar to those of the reduced species. Comparison of the folding behavior of C- and N-terminal subsequences with that of the parent protein suggests that the slow phase in the parent is caused by a folding bottleneck somewhere nearer the C-terminus. However, rapid association and partial folding near the N-terminus is not necessary for prompt folding, since even 190Tm284 chains associate and partially fold very rapidly (less than 0.04 s), and then complete the folding in seconds.     

A procedure for refining a coiled coil protein structure using x-ray fiber diffraction and modeling

We describe a combined use of experimental and simulation techniques to configure side chains in a coiled coil structure. As already demonstrated in a previous work, x-ray diffraction patterns from hard alpha-keratin fibers in the 5.15 A meridian zone reflect the global configuration of the chi(1) dihedral angle of the coiled coil side chains. Molecular simulations, such as energy minimization and molecular dynamics, and rotameric representation in the PDB, are used here on a heterodimeric coiled coil to investigate the dihedral angle distribution along the sequence. Different procedures have been used to build the structure, the quality assessment was based on the agreement between the simulated diffraction patterns and the experimental ones in the fingerprint region of coiled coils (5.15 A). The best one for building a realistic coiled coil structure consists of placing the side chains using molecular dynamics (MD) simulations, followed by side chain positioning using SMD or SCWRL procedures. The side chains and the backbone are equilibrated during the MD until they reach an equilibrium state for the t/g(+) ratio. Positioning the side chains on the resulting backbone, using the above procedures, gives rise to a well-defined 5.15 A meridian reflection.