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.     

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.     

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.     

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.     

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.     

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.     

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.     

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)     

Conformational transition between four and five-stranded phenylalanine zippers determined by a local packing interaction

Alpha-helical coiled coils play a crucial role in mediating specific protein-protein interactions. However, the rules and mechanisms that govern helix-helix association in coiled coils remain incompletely understood. Here we have engineered a seven heptad "Phe-zipper" protein (Phe-14) with phenylalanine residues at all 14 hydrophobic a and d positions, and generated a further variant (Phe-14(M)) in which a single core Phe residue is substituted with Met. Phe-14 forms a discrete alpha-helical pentamer in aqueous solution, while Phe-14(M) folds into a tetrameric helical structure. X-ray crystal structures reveal that in both the tetramer and the pentamer the a and d side-chains interlock in a classical knobs-into-holes packing to produce parallel coiled-coil structures enclosing large tubular cavities. However, the presence of the Met residue in the apolar interface of the tetramer markedly alters its local coiled-coil conformation and superhelical geometry. Thus, short-range interactions involving the Met side-chain serve to preferentially select for tetramer formation, either by inhibiting a nucleation step essential for pentamer folding or by abrogating an intermediate required to form the pentamer. Although specific trigger sequences have not been clearly identified in dimeric coiled coils, higher-order coiled coils, as well as other oligomeric multi-protein complexes, may require such sequences to nucleate and direct their assembly.     

Core side-chain packing and backbone conformation in Lpp-56 coiled-coil mutants

Native proteins exhibit precise geometric packing of atoms in their hydrophobic interiors. Nonetheless, controversy remains about the role of core side-chain packing in specifying and stabilizing the folded structures of proteins. Here we investigate the role of core packing in determining the conformation and stability of the Lpp-56 trimerization domain. The X-ray crystal structures of Lpp-56 mutants with alanine substitutions at two and four interior core positions reveal trimeric coiled coils in which the twist of individual helices and the helix-helix spacing vary significantly to achieve the most favored superhelical packing arrangement. Introduction of each alanine "layer" into the hydrophobic core destabilizes the superhelix by 1.4 kcal mol(-1). Although the methyl groups of the alanine residues pack at their optimum van der Waals contacts in the coiled-coil trimer, they provide a smaller component of hydrophobic interactions than bulky hydrophobic side-chains to the thermodynamic stability. Thus, specific side-chain packing in the hydrophobic core of coiled coils are important determinants of protein main-chain conformation and stability.     

The structure of the carboxyl terminus of striated alpha-tropomyosin in solution reveals an unusual parallel arrangement of interacting alpha-helices

Coiled coils are well-known as oligomerization domains, but they are also important sites of protein-protein interactions. We determined the NMR solution structure and backbone (15)N relaxation rates of a disulfide cross-linked, two-chain, 37-residue polypeptide containing the 34 C-terminal residues of striated muscle alpha-tropomyosin, TM9a(251-284). The peptide binds to the N-terminal region of TM and to the tropomyosin-binding domain of the regulatory protein, troponin T. Comparison of the NMR solution structure of TM9a(251-284) with the X-ray structure of a related peptide [Li, Y., Mui, S., Brown, J. H., Strand, J., Reshetnikova, L., Tobacman, L. S., and Cohen, C. (2002) Proc. Natl. Acad. Sci. U.S.A. 99, 7378-7383] reveals significant differences. In solution, residues 253-269 (like most of the tropomyosin molecule) form a canonical coiled coil. Residues 270-279, however, are parallel, linear helices, novel for tropomyosin. The packing between the parallel helices results from unusual interface residues that are atypical for coiled coils. Y267 has poor packing at the coiled-coil interface and a lower R(2) relaxation rate than neighboring residues, suggesting there is conformational flexibility around this residue. The last five residues are nonhelical and flexible. The exposed surface presented by the parallel helices, and the flexibility around Y267 and the ends, may facilitate binding to troponin T and formation of complexes with the N-terminus of tropomyosin and actin. We propose that unusual packing and flexibility are general features of coiled-coil domains in proteins that are involved in intermolecular interactions.     

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.     

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.     

Hetero-alpha-helical, two-chain, coiled coils: alpha beta hybrid tropomyosin

The nature of the interhelix interaction in two-chain, α-helical, coiled coils is studied by experiments on the formation of hydrid molecules in which one helical chain is an α-tropomyosin and the other a β-tropomoysin. By means of a recently developed assay, the population of heterohelical (i.e., αβ hybrid) molecules relative to their homohelical (αα and ββ) parent species is determined under a variety of conditions, both equilibrium and nonequilibrium. It is found that mixed intact αα and ββ molecules do not form hybrid species in detectible amounts even after incubation at room temperature (or below) for periods of over one week. That the lack of αβ species in this “native-exchange” system is a result of a kinetic barrier is evident from experiments involving a thermal denaturation–renaturation cycle in which the largely dissociated, unfolded chains at higher temperature are annealed to benign temperatures over a period of 6 h, thus assuring an equilibrium population of two-chain species. In the resulting equilibrium state, the αβ population is one-half the total, indicating that recombination is random. Furthermore, this same (equilibrium) state is reached if the separated, mostly unfolded chains are renatured by a rapid (～ 40 s) quench to benign temperatures. Some implications of these results for the thermodynamics of interhelix interation, for kinetics of chain dissociation and recombination, and for in vivo genesis of two-chain coiled coils are discussed.     

A parallel coiled-coil tetramer with offset helices

Specific helix-helix interactions are fundamental in assembling the native state of proteins and in protein-protein interfaces. Coiled coils afford a unique model system for elucidating principles of molecular recognition between alpha helices. The coiled-coil fold is specified by a characteristic seven amino acid repeat containing hydrophobic residues at the first (a) and fourth (d) positions. Nonpolar side chains spaced three and four residues apart are referred to as the 3-4 hydrophobic repeat. The presence of apolar amino acids at the e or g positions (corresponding to a 3-3-1 hydrophobic repeat) can provide new possibilities for close-packing of alpha-helices that includes examples such as the lac repressor tetramerization domain. Here we demonstrate that an unprecedented coiled-coil interface results from replacement of three charged residues at the e positions in the dimeric GCN4 leucine zipper by nonpolar valine side chains. Equilibrium circular dichroism and analytical ultracentrifugation studies indicate that the valine-containing mutant forms a discrete alpha-helical tetramer with a significantly higher stability than the parent leucine-zipper molecule. The 1.35 A resolution crystal structure of the tetramer reveals a parallel four-stranded coiled coil with a three-residue interhelical offset. The local packing geometry of the three hydrophobic positions in the tetramer conformation is completely different from that seen in classical tetrameric structures yet bears resemblance to that in three-stranded coiled coils. These studies demonstrate that distinct van der Waals interactions beyond the a and d side chains can generate a diverse set of helix-helix interfaces and three-dimensional supercoil structures.     

Mg2+ ions bind at the C‐terminal region of skeletal muscle α‐tropomyosin

Tropomyosin (Tm) is a dimeric coiled‐coil protein that polymerizes through head‐to‐tail interactions. These polymers bind along actin filaments and play an important role in the regulation of muscle contraction. Analysis of its primary structure shows that Tm is rich in acidic residues, which are clustered along the molecule and may form sites for divalent cation binding. In a previous study, we showed that the Mg²⁺‐induced increase in stability of the C‐terminal half of Tm is sensitive to mutations near the C‐terminus. In the present report, we study the interaction between Mg²⁺ and full‐length Tm and smaller fragments corresponding to the last 65 and 26 Tm residues. Although the smaller Tm peptide (Tm_{259‐284(W269)}) is flexible and to large extent unstructured, the larger Tm_{220‐284(W269)} fragment forms a coiled coil in solution whose stability increases significantly in the presence of Mg²⁺. NMR analysis shows that Mg²⁺ induces chemical shift perturbations in both Tm_{220‐284(W269)} and Tm_{259‐284(W269)} in the vicinity of His276, in which are located several negatively charged residues. © 2009 Wiley Periodicals, Inc. Biopolymers 91: 583–590, 2009. This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com     

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.     

Alpha-helix-to-random-coil transitions of two-chain, coiled coils: a theoretical model for the "pretransition" in cysteine-190-cross-linked tropomyosin

The thermal unfolding curve for alpha alpha tropomyosin in which the two chains are cross-linked at cysteine-190 shows two striking features that distinguish it from that of its counterpart for non-cross-linked molecules: a "pretransition" at 25-50 degrees C and a shift in the principal transition to higher temperature, but with the same steepness. Previously, the pretransition was explained by postulating that the cross-link produces local strains, yielding a pinched "bubble" of chain-separated random coil about C-190, whereas the rest of the coiled coil remains intact. Results from both enzymatic digestion kinetics and equilibrium calorimetric studies have been interpreted as consistent with the existence of such a bubble. To test this idea further, a theoretical model is devised whereby various physical features can be imposed and the resulting helix content and other properties calculated from the statistical mechanical theory of the helix-coil transition. Short-range interactions employed are the geometric mean values of those in alpha-tropomyosin. The helix-helix interaction free energy is also like that in alpha-tropomyosin, including its nonuniformity; i.e., it is made larger in the amino half of the molecule. Local strain is introduced by setting the helix-helix interaction to zero in a region about the cross-link. The results show that, alone, neither local strain nor nonuniformity serves to mimic the experiments. In concert, however, they reproduce all the main experimental features, if the strain is extensive (approximately 29 residues) and somewhat dissymmetric. Theoretical helix probability profiles, however, show that no bubble of unfolded chains forms about the cross-link. Instead, in the pretransition, residues unfold from the weakly interacting end (residue 284) in to, but not through, the cross-link at C-190. The theory also indicates that the augmented stability for the principal transition occurs largely as a result of loop entropy. The same strain and nonuniformity are then employed to explore the effects of other possible cross-link positions. The thermal curves are shown to depend markedly on cross-link location. The curves are discussed in terms of loop entropy, which has drastic, long-range effects. Under appropriate circumstances it can produce, in the coiled-coil model, a thermal transition that is essentially all or none.