A scanning calorimetric study of unfolding equilibria in homodimeric chicken gizzard tropomyosins.

Using both circular dichroism (CD) and differential scanning calorimetry (DSC), several laboratories find that the thermal unfolding transitions of alpha alpha and beta beta homodimeric coiled coils of rabbit tropomyosin are multistate and display an overall unfolding enthalpy of near 300 kcal (mol dimer)(-1). In contrast, an extant CD study of beta beta and gamma gamma species of chicken gizzard tropomyosin concludes that their unfolding transitions are simple two-state transitions, with much smaller overall enthalpies (98 kcal mol(-1) for beta beta and 162 kcal mol(-1) for gamma gamma). However, these smaller enthalpies have been questioned, because they imply a concentration dependence of the melting temperatures that is far larger than observed by CD. We report here DSC studies of the unfolding of both beta beta and gamma gamma chicken gizzard homodimers. The results show that these transitions are very similar to those in rabbit tropomyosins in that 1) the overall unfolding enthalpy is near 300 kcal mol(-1); 2) the overall delta C(rho) values are significantly positive; 3) the various transitions are multistate, requiring at least two and as many as four domains to fit the DSC data. DSC studies are also reported on these homodimeric species of chicken gizzard tropomyosin with a single interchain disulfide cross-link. These results are also generally similar to those for the correspondingly cross-linked rabbit tropomyosins.     

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)     

α-Helix-to-random-coil transitions of two-chain coiled coils: Experiments on the thermal denaturation of ββ tropomyosin cross-linked selectively at C-190

A method is described for preparation of a species of β tropomyosin that is sulfhydryl-blocked at C36 and disulfide-cross-linked at C190. Five steps are involved: (1) Rabbit skeletal muscle tropomyosin, comprising αα and αβ species, is oxidized with ferricyanide, disulfide-cross-linking both species at C190. (2) The product is treated with iodoacetamide, blocking the only remaining free sulfhydryl, i.e., C36 of the β-chains. (3) The C36-blocked, C190-cross-linked product is reduced with dithiothreitol (DTT), unfolded in urea, and α and β chains separated by ion-exchange chromatography. (4) The C36-blocked β chains are refolded by dialysis. (5) The refolded, C36-blocked ββ species are cross-linked at C190 by ferricyanide oxidation. The resulting C36-blocked, C190-cross-linked ββ product is separated from contaminating species—mostly completely blocked β-chains and multichain cross-linked molecules—by size-exclusion chromatography in denaturing (guanidinium chloride) solvent. The five-step process and the final product were monitored by titration of free sulfhydryls and by NaDodSO₄/polyacrylamide gel electrophoresis (PAGE). Thermal unfolding curves from CD are reported for the resulting pure, C36-blocked, C190-cross-linked ββ species and for its DTT-reduction product, the noncross-linked C36-blocked species. The latter shows almost the same thermal unfolding transition as intact, noncross-linked ββ species. The former shows a pretransition similar to, but larger in extent than, the one well known to occur in the analogous case of C190-cross-linked αα tropomyosin. These unfolding transitions are compared with one another and with that previously reported for doubly cross-linked (at C36 and C190) ββ species. These comparisons are made in the light of current physical models for coiled-coil unfolding equilibria. It is concluded that although no extent model is demonstrably satisfactory, any successful model must include strain at the cross-link, loop entropy, and regional nonuniformities as essential parts of the physics.     

Alpha-helix to random coil transitions of two-chain coiled coils: experiments on the thermal denaturation of beta beta tropomyosin cross-linked selectively at C36

Current ideas on unfolding equilibria in two-chain, coiled-coil proteins are examined by studies of a species of beta beta tropomyosin that is sulfhydryl blocked at C190 and disulfide cross-linked at C36 (.beta-beta.). The desired species is produced by a seven-step process: (1) Rabbit skeletal muscle, comprising predominantly alpha alpha and alpha beta species, is oxidized with ferricyanide, cross-linking both species at C190. (2) The product is carbamylated at C36 of beta chains, using cyanate in denaturing medium at pH 6. (3) All C190 cross-links are reduced with dithiothreitol (DTT). (4) All C190 sulfhydryls are permanently blocked by carboxyamidomethylation. (5) Chromatography on carboxymethylcellulose in denaturing medium is used to separate C190-blocked alpha chains from C190-blocked, C36-carbamylated beta chains. (6) The latter are decarbamylated in denaturing medium by raising the pH to 8.0. (7) The C190-blocked beta chains are renatured and cross-linked at C36 by ferricyanide. The procedure and the quality of the final product are judged by NaDodSO4/polyacrylamide gel electrophoresis, titration of free sulfhydryls, and electrophoretic analysis of trypsin digestion products. Thermal unfolding curves are reported for the resulting pure .beta-beta. species and for its DTT-reduction product. The latter (.beta beta.) show equilibrium thermal unfolding curves that are very similar to those of the parent beta beta noncross-linked species. The .beta-beta. cross-linked species unfolds in a single-phase, cooperative transition with a melting temperature intermediate between the pretransition and posttransition shown by its cross-linked counterpart, the C190 cross-linked, C36-blocked species (.beta-beta.), which was studied earlier. These transitions are compared with one another and with that of the doubly cross-linked species, beta-(-)beta, in the light of two extant physical models for such transitions. The all-or-none segments model successfully rationalizes the data qualitatively for the .beta-beta. and .beta-beta. species if the usual postulates of greater inherent stability of the amino vs the carboxyl end of the molecule and of strain at each cross-link are accepted. However, the same model then requires that the beta-(-)beta species be the least stable of the three, whereas experiment shows the opposite, thus falsifying the all-or-none segments model. The continuum-of-states model is also qualitatively in accord with data on the .beta-beta. and .beta-beta. species.(ABSTRACT TRUNCATED AT 400 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.     

Complexes of smooth muscle tropomyosin with F-actin studied by differential scanning calorimetry.

Differential scanning calorimetry (DSC) and light scattering were used to analyze the interaction of duck gizzard tropomyosin (tropomyosin) with rabbit skeletal-muscle F-actin. In the absence of F-actin, tropomyosin, represented mainly by heterodimers, unfolds at 41 degrees C with a sharp thermal transition. Interaction of tropomyosin heterodimers with F-actin causes a 2-6 degrees C shift in the tropomyosin thermal transition to higher temperature, depending on the tropomyosin/actin molar ratio and protein concentration. A pronounced shift of the tropomyosin thermal transition was observed only for tropomyosin heterodimers, and not for homodimers. The most pronounced effect was observed after complete saturation of F-actin with tropomyosin molecules, at tropomyosin/actin molar ratios > 1 : 7. Under these conditions, two well-separated peaks of tropomyosin were observed on the thermogram besides the peak of F-actin, the peak characteristic of free tropomyosin heterodimer, and the peak with a maximum at 45-47 degrees C corresponding to tropomyosin bound to F-actin. By measuring the temperature-dependence of light scattering, we found that thermal unfolding of tropomyosin is accompanied by its dissociation from F-actin. Thermal unfolding of tropomyosin is almost completely reversible, whereas F-actin denatures irreversibly. The addition of tropomyosin has no effect on thermal unfolding of F-actin, which denatures with a maximum at 64 degrees C in the absence and at 78 degrees C in the presence of a twofold molar excess of phalloidin. After the F-actin-tropomyosin complex had been heated to 90 degrees C and then cooled (i.e. after complete irreversible denaturation of F-actin), only the peak characteristic of free tropomyosin was observed on the thermogram during reheating, whereas the thermal transitions of F-actin and actin-bound tropomyosin completely disappeared. Therefore, the DSC method allows changes in thermal unfolding of tropomyosin resulting from its interaction with F-actin to be probed very precisely.     

A scanning calorimetric study of the thermally induced unfolding of various forms of tropomyosin

The reversible thermally induced unfolding of various forms of tropomyosin, a two-chain alpha-helical coiled coil, has been studied by high-sensitivity differential scanning calorimetry (DSC). Included in the study are the reduced and oxidized (disulfide cross-linked) forms of alpha alpha- and beta beta-tropomyosin, and the forms of alpha alpha-tropomyosin in which all sulfhydryl groups have been blocked by carboxymethylation or carboxyamidomethylation. Oxidation or blocking of the sulfhydryl groups of tropomyosin strongly affect the thermotropic behavior of the protein in unpredictable ways. The empirical results presented here are in qualitative agreement with those from an earlier DSC study of the oxidized and carboxymethylated forms of alpha alpha-tropomyosin [S.A. Potekhin and P.L. Privalov (1982) Journal of Molecular Biology, Vol. 159, pp. 519-535], but we find that a different decomposition into subtransitions is possible. Comparison of the alpha alpha and beta beta species indicates, in agreement with extant CD studies, that the noncross-linked beta beta species is somewhat less stable than its alpha alpha counterpart, but that cross-linking enhances the stability of the beta beta doubly cross-linked species by a greater amount and does not lead to the small low-temperature transition ("pretransition") seen in the singly cross-linked alpha alpha species.     

Folding/Unfolding Kinetics of Apomyoglobin

The equilibrium and kinetic folding/unfolding of apomyoglobin (ApoMb) were studied at pH 6.2, 11 °C by recording tryptophan fluorescence. The equilibrium unfolding of ApoMb in the presence of urea was shown to involve accumulation of an intermediate state, which had a higher fluorescence intensity as compared with the native and unfolded states. The folding proceeded through two kinetic phases, a rapid transition from the unfolded to the intermediate state and a slow transition from the intermediate to the native state. The accumulation of the kinetic intermediate state was observed in a wide range of urea concentrations. The intermediate was detected even in the region corresponding to the unfolding limb of the chevron plot. Urea concentration dependence was obtained for the observed folding/unfolding rate. The shape of the dependence was compared with that of two-state proteins characterized by a direct transition from the unfolded to the native state.     

Influence of an extrinsic cross-link on the folding pathway of ribonuclease A. Kinetics of folding-unfolding

The kinetics of folding/unfolding of cross-linked Lys7-dinitrophenylene-Lys41-ribonuclease A were studied and compared to those of unmodified ribonuclease A (RNase A) at various concentrations of guanidine hydrochloride. The folding of the denatured cross-linked protein involved one fast-folding species (22 +/- 4%) and two slow-folding species, as observed in unmodified ribonuclease A. Also, a nativelike intermediate, analogous to that reported previously for unmodified ribonuclease A [Cook, K. H., Schmid, F. X., & Baldwin, R. L. (1979) Proc. Natl. Acad. Sci. U.S.A. 76, 6157], has been detected on the folding pathway of cross-linked ribonuclease A. The extrinsic cross-link between Lys7 and Lys41 did not affect the rate constants for the folding kinetics of these three species. The cross-link did, however, significantly affect the rate constant for unfolding of the native protein. The conformation of the protein in the transition state of the unfolding pathway was deduced from an analysis of the kinetic data. It appears that the 41 N-terminal residues are unfolded in the transition state of the unfolding pathway. Thus, the unfolding pathway of RNase A is sequential in that further unfolding (after the transition state) follows the unfolding of the 41 N-terminal residues. Also, the conformation of the 41 N-terminal residues does not play a role in the folding pathway. Presumably, if the cross-link were introduced instead between two other residues that are in the segment(s) involved in the rate-limiting step(s), it could increase the refolding rate constants and possibly the concentration of fast-folding species.     

Effects of an interchain disulfide bond on tropomyosin structure: intrinsic fluorescence and circular dichroism studies

An interchain disulfide crosslink was introduced into rabbit skeletal tropomyosin (TM) at Cys190 by two different methods under non-denaturing conditions. The effects of the crosslink on the structure of tropomyosin were investigated by fluorescence and circular dichroism methods as a function of temperature and guanidine · hydrochloride concentration. Four different preparations were studied: Nbs₂-TM, red-TM crosslinked with Ellman's reagent, 5,5′-dithiobis(2-nitrobenzoate); O₂-TM, TM whose SH groups were air-oxidized; red-TM, TM reduced with dithiothreitol; IA-TM, red-TM whose SH groups were blocked with iodoacetamide. Sodium dodecyl sulfate/polyacrylamide gel electrophoresis studies indicated that SS crosslinks were quantitatively introduced between the subunits of TM for Nbs₂-TM and O₂-TM. In the completely folded state (below 25 °C or in the absence of denaturant) and in the unfolded state (above 65 °C or greater than 4 m-guanidine · hydrochloride) all of the samples had the same Tyr fluorescence quantum yield, accessibility to acrylamide fluorescence quenching, fluorescence polarization and mean residue rotation at 222 nm. Thermal and denaturant-induced unfolding profiles at pH 7.5 were obtained for each sample with measurements of these parameters. The main transition at about 45 °C or 2 m-guanidine · hydrochloride was shifted about +7 deg. C and 0.8 m in guanidine · hydrochloride, respectively, for the crosslinked samples as compared to the uncrosslinked samples. In addition, a destabilizing pretransition was observed in the 30 to 45 °C region or the 0 to 2 m-guanidine · hydrochloride region only for the crosslinked samples when polarization or ellipticity was measured. Studies of the ability of Nbs₂ to crosslink red-TM as a function of guanidine · hydrochloride concentration indicated that the chains separate at Cys190 between 0 and 2 m-guanidine · hydrochloride before they dissociate. Thus, the effect of the SS crosslink at Cys190 on the conformation of TM at physiological temperatures appears to be related to the inherent instability of the molecule in this region of the sequence.     

Calorimetric study of the effect of intrachain cross-linking on lysozyme unfolding

Thermodynamics of unfolding of lysozyme cross-linked between Glu 35 and Trp 108 were studied in solutions of various concentrations of 1-propanol (1-PrOH) at pH 3.7 by means of scanning microcalorimetry. The transition temperature for the cross-linked lysozyme increases by 17-19 degrees C due to cross-linking at every concentration of 1-PrOH. This corresponds to the increase in the unfolding Gibbs free energy of about 28 kJ.mol-1, which is independent of the concentration of 1-PrOH. It was found that the unfolding enthalpy of cross-linked lysozyme is only slightly larger than that of intact one, and the unfolding entropy of the cross-linked one is nearly equal to that of the intact one, if both are compared at the same temperature. The stabilization mechanism for the cross-linked lysozyme is discussed on the basis of these calorimetric data.     

Effect of the state of oxidation of cysteine 190 of tropomyosin on the assembly of the actin-tropomyosin complex

Tropomyosin, cross-linked at cysteine 190, was found to bind more weakly to actin filaments than uncross-linked tropomyosin. Cross-linking of tropomyosin can cause actin filaments nearly completely covered with tropomyosin to be uncovered almost completely. The critical monomer concentration of actin is not significantly changed by binding of cross-linked or uncross-linked tropomyosin to actin filaments. The binding curves were analyzed quantitatively, thereby taking into account the polar end-to-end contact of tropomyosin molecules bound by actin and the overlap of the seven subunit binding sites along the actin filament. Under the conditions of the experiment (80 mM KCl, 1 mM MgCl2, pH 7.5, 38-42 degrees C), the equilibrium constant for isolated binding of tropomyosin to actin filaments is in the range 1 x 10(3)-3 x 10(3) M-1. The equilibrium constants for binding of tropomyosin to binding sites along the actin filament with one or two neighbouring tropomyosin molecules are in the range of 10(6) or 10(8) to 10(9) M-1, respectively. The equilibrium constants for binding of tropomyosin to binding sites along the actin filament with one or two neighbouring tropomyosin molecules are in the range of 10(6) or 10(8) to 10(9) M-1, respectively. The equilibrium constants for cross-linked and uncross-linked tropomyosin differ by a factor of only about two. Owing to the highly cooperative binding, these differences are sufficient so that actin filaments nearly completely covered with uncross-linked tropomyosin are uncovered almost completely by cross-linking tropomyosin at cysteine 190.     

Electric birefringence studies of rabbit skeletal tropomyosin

The electric birefringence of rabbit skeletal tropomyosin and its nonpolymerizable derivative was studied as a function of protein concentration, pulse length, and electric field strength. Analyses of the zero field birefringence decay curves show that nonpolymerizable tropomyosin, which has had on average six C-terminal residues removed, and tropomyosin are both well approximated by rigid cylinders in solution at low salt concentrations at 20°C. The measured relaxation times for the monomers of polymerizable and nonpolymerizable tropomyosin are 1.5 ± 0.4 μs and 1.30 ± 0.2 μs, respectively, in good agreement with the values calculated from the known dimensions. For tropomyosin the electrical pulse induces the formation of linear dimers. Orientation occurs primarily by a permanent dipole mechanism. Permanent and induced dipole moments were calculated from reversing field experiments and from the saturation of the birefringence. Removal of the six C-terminal residues decreases the measured permanent dipole moment by 9.5%, from 6300 to 5700 Debyes, which is in good agreement with the 7% decrease calculated for permanent dipole contributions arising from the peptide dipoles and from the asymmetric distribution of the formal charges. This change is due primarily to the removal of Asp 280.     

Unfolding domains of recombinant fusion alpha alpha-tropomyosin.

The thermal unfolding of the coiled-coil alpha-helix of recombinant alpha alpha-tropomyosin from rat striated muscle containing an additional 80-residue peptide of influenza virus NS1 protein at the N-terminus (fusion-tropomyosin) was studied with circular dichroism and fluorescence techniques. Fusion-tropomyosin unfolded in four cooperative transitions: (1) a pretransition starting at 35 degrees C involving the middle of the molecule; (2) a major transition at 46 degrees C involving no more than 36% of the helix from the C-terminus; (3) a major transition at 56 degrees C involving about 46% of the helix from the N-terminus; and (4) a transition from the nonhelical fusion domain at about 70 degrees C. Rabbit skeletal muscle tropomyosin, which lacks the fusion peptide but has the same tropomyosin sequence, does not exhibit the 56 degrees C or 70 degrees C transition. The very stable fusion unfolding domain of fusion-tropomyosin, which appears in electron micrographs as a globular structural domain at one end of the tropomyosin rod, acts as a cross-link to stabilize the adjacent N-terminal domain. The least stable middle of the molecule, when unfolded, acts as a boundary to allow the independent unfolding of the C-terminal domain at 46 degrees C from the stabilized N-terminal unfolding domain at 56 degrees C. Thus, strong localized interchain interactions in coiled-coil molecules can increase the stability of neighboring domains.     

Effect of mutation Arg91Gly on the thermal stability of β-tropomyosin

The mutation Arg91Gly (R91G) in β-tropomyosin (β-TM) is known to cause distal arthrogryposis, a severe congenital disorder of muscle tissues. The influence of this mutation in β-TM on its structure and thermal denaturation was demonstrated. It was shown by the differential scanning calorimetry and circular dichroism that this point mutation dramatically decreased the thermal stability of the significant part of the β-TM (about a half of the molecule). This part of the β-TM molecule carrying R91G mutation unfolds at ～28°C, i.e., at a much lower temperature than the other part of the molecule, which melts at ～40°C. The data of the differential scanning calorimetry were compared with the results of temperature dependence of pyrene eximer fluorescence, which decreased upon the dissociation of two β-TM chains in the region of pyrene-labeled Cys-36. This comparison allowed one to conclude that this thermal transition reflected the thermal unfolding of the whole N-terminal part of β-TM. Interestingly, the destabilizing effect of Arg91Gly mutation spread for a rather long distance along the tropomyosin coiled-coil indicating a high cooperativity of the thermal denaturation within this part of β-TM.     

13C-NMR off-resonance rotating frame spin-lattice relaxation studies of bovine lens γ-crystallin self association: effect of ‘macromolecular crowding’

The NMR technique of ¹³C off-resonance rotating frame spin-lattice relaxation, which provides an accurate assessment of the effective rotational correlation time (τ_0,eff) for macromolecular rotational diffusion, was applied to the study of γ-crystallin association as a function of protein concentration and temperature. Values of the effective rotational correlation time for γ-crystallin rotational diffusion were obtained at moderate to high protein concentrations (80–350 mg/ml) and at temperatures above, and below, the cold cataract phase transition temperature. With increasing concentration γ-crystallin was observed to increasingly associate as reflected by larger values of τ_0,eff Decreasing temperature in the range of 35 to 22°C was found to result in no change in the temperature corrected value of τ_0,eff at a γ-crystallin concentration of 80 mg/ml, whereas at temperatures of 18°C or below, this parameter was approx. twofold larger, suggesting the occurrence of a well defined phase transition, which correlated well with the cold cataract phase transition temperature. At higher protein concentrations, by contrast, τ_0,eff (temperature corrected) was found to increase by approx. 1.6- to 2-times in the temperature interval 35°C to 22°C, a result consistent with the dependence of the cold cataract phase transition temperature on γ-crystallin concentration. Analysis of intensity ratio dispersion curves, using an assumed model of isodesmic association, permitted the estimation of the association constant characterizing the aggregation under particular conditions of concentration and temperature. The significant increase in the value of the association constant with moderate increases in protein concentration was rationalized by invoking the effect of ‘macromolecular crowding’. The results obtained in this study suggest that in the intact lens, where high protein concentrations prevail, γ-crystallin is unlikely to be found in the monomeric state, but more likely, as a significantly aggregated species, representing a broad molecular weight distribution.     

The transition state in the folding-unfolding reaction of four species of three-disulfide variant of hen lysozyme: the role of each disulfide bridge

The effects of lacking a specific disulfide bridge on the transition state in folding were examined in order to explore the folding-unfolding mechanism of lysozyme. Four species of three-disulfide variant of hen lysozyme (3SS-lysozyme) were prepared by replacing two Cys residues with Ala or Ser: C6S/C127A, C30A/C115A, C64A/C80A and C76A/C94A. The recombinant hen lysozyme was studied as the standard reference containing four authentic disulfide bridges and the extra N-terminal Met: the recombinant hen lysozyme containing the extra N-terminal. Folding rates were measured by monitoring the change in fluorescence intensity associated with tri-N-acetyl-d-glucosamine binding to the active site of refolded lysozyme. It was confirmed that the folding rate of the recombinant hen lysozyme containing the extra N-terminal was the same as that of wild-type lysozyme, and that the folding rate was little affected by the presence of tri-N-acetyl-d-glucosamine (triNAG). The folding rate of C64A/C80A was found to be the fastest and almost the same as that of the recombinant hen lysozyme containing the extra N-terminal, and that of C30A/C115A the second, and that of C6S/C127A the third. The folding rate of C76A/C94A was particularly slow. On the other hand, the unfolding rates which were measured in the presence of triNAG showed the dependence on the concentration of triNAG. The intrinsic unfolding rate in the absence of triNAG was determined by extrapolation. Also in the unfolding rate, C76A/C94A was markedly slower than the others. It was found from the analysis of binding constants of triNAG to C64A/C80A during the unfolding process that the active site of C64A/C80A partly unfolds already prior to the unfolding transition. On the basis of these kinetic data, we suggest that C64A/C80A folding transition can occur with leaving the loop region around SS3 (C64-C80) flexible, while cross-linking by SS4 (C76-C94) is important for the promotion of folding, because it is an indispensable constraint on the way towards the folding transition state.     

Differential binding of tropomyosin isoforms to actin modified with m-maleimidobenzoyl-N-hydroxysuccinimide ester and fluorescein-5-isothiocyanate

Differential interactions of tropomyosin (TM) isoforms with actin can be important for determination of the thin filament functions. A mechanism of tropomyosin binding to actin was studied by comparing interactions of five αTM isoforms with actin modified with m-maleimidobenzoyl-N-hydroxysuccinimide ester (MBS) and with fluorescein-5-isothiocyanate (FITC). MBS attachment sites were revealed with mass spectrometry methods. We found that the predominant actin fraction was cross-linked by MBS within subdomain 3. A smaller fraction of the modified actin was cross-linked within subdomain 2 and between subdomains 2 and 1. Moreover, investigated actins carried single labels in subdomains 1, 2, and 3. Such extensive modification caused a large decrease in actin affinity for skeletal and smooth muscle tropomyosins, nonmuscle TM2, and chimeric TM1b9a. In contrast, binding of nonmuscle isoform TM5a was less affected. Isoform’s affinity for actin modified in subdomain 2 by binding of FITC to Lys61 was intermediate between the affinity for native actin and MBS-modified actin except for TM5a, which bound to FITC–actin with similar affinity as to actin modified with MBS. The analysis of binding curves according to the McGhee–von Hippel model revealed that binding to an isolated site, as well as cooperativity of binding to a contiguous site, was affected by both actin modifications in a TM isoform-specific manner.     

A theoretical model simulating the anomalous concentration dependence of the equilibrium thermal unfolding curve of noncrosslinked tropomyosin

Thermal unfolding curves of tropomyosin have so far been fit only semi-quantitatively by the statistical-mechanical theory of the helix-coil transition. The calculated values of helix content are a bit too small for the most dilute solutions and a bit too large for the most concentrated ones. The theory, as hitherto used, assumes a uniform helix-helix interaction, whereas evidence from studies on molecular segments suggests otherwise. A theoretical model incorporating such non-uniformity in helix-helix interaction is used to produce simulated thermal unfolding curves. These simulated curves, when fit to the theory using the assumption of uniformity, reveal precisely the same discrepancies seen with the experimental data. We conclude that non-uniformity in helix-helix interaction along the tropomyosin molecule is responsible for the small discrepancy between experimental data and the uniform-model theory previously employed.     

Combined spectroscopic and calorimetric characterisation of rubredoxin reversible thermal transition

Rubredoxins are small iron proteins containing the simplest type of iron–sulphur centre, consisting of an iron atom coordinated by the thiol groups of four cysteines. Here we report studies on the conformational stability of a new type of rubredoxin from the hyperthermophile Methanocaldococcus jannaschii, having an atypical metal site geometry resulting from a modified iron-binding motif. Absorption and fluorescence spectroscopies were used in combination with differential scanning calorimetry to probe different aspects of the thermal unfolding transition: iron site degradation (absorption at 380 nm), tertiary structure unfolding (Trp emission), exposure of hydrophobic regions (1-anilinonaphalene-8-sulphonate fluorescence enhancement) and iron release. Thermal denaturation was found to be irreversible and caused by decomposition of the metal centre. The protein is hyperstable and between pH 4 and 10 it is only thermally denatured in the presence of a strong chemical denaturant. The study of the heating rate dependence of the melting temperature allowed us to determine the reaction equilibrium thermodynamic parameters. At pH 2 the protein is destabilised owing to the absence of salt bridges and it has a T _m of 65 °C. In these conditions, there is excellent agreement between the parameters determined by the different spectroscopic methods and calorimetry. The highest stability was found to be at pH 8, and a detailed study of the heating rate dependence in the presence of guanidine thiocyanate in this condition allowed the determination of a reversible T _m of 118 °C.