Use of stable analogs of myosin ATPase intermediates for kinetic studies of the "weak" binding of myosin heads to F-actin.

It is known that ternary complexes of myosin subfragment 1 (S1) with ADP and the Pi analogs beryllium fluoride (BeFx) and aluminum fluoride (AlF4-) are stable analogs of the myosin ATPase intermediates M* x ATP and M** x ADP x Pi, respectively. Using kinetic approaches, we compared the rate of formation of the complexes S1 x ADP x BeFx and S1 x ADP x AlF4- in the absence and in the presence of F-actin, as well as of the interaction of these complexes with F-actin. We show that in the absence of F-actin the formation of S1 x ADP x BeFx occurs much faster (3-4 min) than that of S1 x ADP x AlF4- (hours). The formation of these complexes in the presence of F-actin led to dissociation of S1 from F-actin, this process being monitored by a decrease in light scattering. The light scattering decrease of the acto-S1 complex occurred much faster after addition of BeFx (during 1 min) than after addition of AlF4- (more than 20 min). In both cases the light scattering of the acto-S1 complex decreased by 40-50%, but it remained much higher than that of F-actin measured in the absence of S1. The interaction of the S1 x ADP x BeFx and S1 x ADP x AlF4- complexes with F-actin was studied by the stopped-flow technique with high time resolution (no more than 0.6 sec after mixing of S1 with F-actin). We found that the binding of S1 x ADP x BeFx or S1 x ADP x AlF4- to F-actin is accompanied by a fast increase in light scattering, but it does not affect the fluorescence of a pyrene label specifically attached to F-actin. We conclude from these data that within this time range a "weak" binding of the S1 x ADP x BeFx and S1 x ADP x AlF4- complexes to F-actin occurs without the subsequent transition of the "weak" binding state to the "strong" binding state. Comparison of the light scattering kinetic curves shows that S1 x ADP x AlF4- binds to F-actin faster than S1 x ADP x BeFx does: the second-order rate constants for the "weak" binding to F-actin are (62.8 +/- 1.8) x 10(6) M-1 x sec-1 in the case of S1 x ADP x AlF4- and (22.6 +/- 0.4) x 10(6) M-1 x sec-1 in the case of S1 x ADP x BeFx. We conclude that the stable ternary complexes S1 x ADP x BeFx and S1 x ADP x AlF4- can be successfully used for kinetic studies of the "weak" binding of the myosin heads to F-actin.     

Effects of nucleotide binding on thermal transitions and domain structure of myosin subfragment 1.

The thermal unfolding and domain structure of myosin subfragment 1 (S1) from rabbit skeletal muscles and their changes induced by nucleotide binding were studied by differential scanning calorimetry. The binding of ADP to S1 practically does not influence the position of the thermal transition (maximum at 47.2 degrees C), while the binding of the non-hydrolysable analogue of ATP, adenosine 5'-[beta, gamma-imido]triphosphate (AdoPP[NH]P) to S1, or trapping of ADP in S1 by orthovanadate (Vi), shift the maximum of the heat adsorption curve for S1 up to 53.2 and 56.1 degrees C, respectively. Such an increase of S1 thermostability in the complexes S1-AdoPP[NH]P and S1-ADP-Vi is confirmed by results of turbidity and tryptophan fluorescence measurements. The total heat adsorption curves for S1 and its complexes with nucleotides were decomposed into elementary peaks corresponding to the melting of structural domains in the S1 molecule. Quantitative analysis of the data shows that the domain structure of S1 in the complexes S1-AdoPP[NH]P and S1-ADP-Vi is similar and differs radically from that of nucleotide-free S1 and S1 in the S1-ADP complex. These data are the first direct evidence that the S1 molecule can be in two main conformations which may correspond to different states during the ATP hydrolysis: one of them corresponds to nucleotide-free S1 and to the complex S1-ADP, and the other corresponds to the intermediate complexes S1-ATP and S1-ADP-Pi. Surprisingly it turned out that the domain structure of S1 with ADP trapped by p-phenylene-N, N'-dimaleimide (pPDM) thiol cross-linking almost does not differ from that of the nucleotide-free S1. This means that pPDM-cross-linked S1 in contrast to S1-AdoPP[NH]P and S1-ADP-Vi can not be considered a structural analogue of the intermediate complexes S1-ATP and S1-ADP-Pi.     

Charge changes in loop 2 affect the thermal unfolding of the myosin motor domain bound to F-actin

The thermal unfolding of Dictyostelium discoideum myosin head fragments with alterations in the actin-binding surface loop 2 was studied by differential scanning calorimetry. Lengthening of loop 2 without concomitant charge changes led to decreases in the transition temperature of not more than 1.8 degrees C. Insertions with multiple positive or negative charges had a stronger destabilizing effect and led to reductions in the thermal transition temperature of up to 3.7 degrees C. In the presence of nucleotide, most mutants displayed similar or higher transition temperatures than M765. Only constructs M765(11/+6) and M765(20/+12) with long positively charged inserts showed transition temperatures that were more than 2 degrees C below the values measured for M765 in the presence of ADP, ADP-V(i), and ADP-BeF(3). Interaction with F-actin in the presence of ADP shifted the thermal transition of M765 by 6 degrees C, from 49.1 to 55.1 degrees C. The actin-induced increase in thermal stability varied between 1.2 and 9.1 degrees C and showed a strong correlation with the mutant constructs' affinity for actin. Our results show that length and charge changes in loop 2 do not significantly affect nucleotide-induced structural changes in the myosin motor domain, but they affect structural changes that occur when the motor domain is strongly bound to actin and affect the coupling between the actin- and nucleotide-binding sites.     

Effect of actin on the tryptic digestion of myosin subfragment 1 in the weakly attached state.

The structure of myosin subfragment 1 (S1) in the weakly attached complex with actin was studied at three specific sites, at the 50-kDa/20-kDa and 27-kDa/50-kDa junctions, and at the N-terminal region, using tryptic digestion as a structure-exploring tool. The structure of S1 at the vicinity of the 50-kDa/20-kDa junction is pH dependent in the weakly attached state because the tryptic cleavage at this site was fully protected by actin at pH 6.2, but the protection was only partial at pH 8.0. Since the actin protection is complete in rigor at both pH values, the results indicate that the structure of S1 at the 50-kDa/20-kDa junction differs in the two states at pH 8.0, but not at pH 6.2. Actin restores the ADP-suppressed tryptic cleavage after Lys213 at the 27-kDa/50-kDa junction in the strongly attached state, but not in the weakly attached state, which indicates structural difference between the two states at this site. ATP and ADP open a new site for tryptic cleavage in the N-terminal region of the S1 heavy chain between Arg23 and Ile24. Actin was found to suppress this cleavage in both weakly and strongly attached states, which shows that, in the vicinity of this site, the structure of S1 is similar in both states. The results indicate that the binding of S1 to actin induces localized changes in the S1 structure, and the extent of these changes is different in the various actin-S1 complexes.     

Dissociative mechanism of F-actin thermal denaturation

We have applied differential scanning calorimetry to investigate thermal unfolding of F-actin. It has been shown that the thermal stability of F-actin strongly depends on ADP concentration. The transition temperature, T(m), increases with increasing ADP concentration up to 1 mM. The T(m) value also depends on the concentration of F-actin: it increases by almost 3 degrees C as the F-actin concentration is increased from 0.5 to 2.0 mg/ml. Similar dependence of the T(m) value on protein concentration was demonstrated for F-actin stabilized by phalloidin, whereas it was much less pronounced in the presence of AlF4(-). However, T(m) was independent of protein concentration in the case of monomeric G-actin. The results suggest that at least two reversible stages precede irreversible thermal denaturation of F-actin; one of them is dissociation of ADP from actin subunits, and another is dissociation of subunits from the ends of actin filaments. The model explains why unfolding of F-actin depends on both ADP and protein concentration.     

Differential scanning calorimetry of the unfolding of myosin subfragment 1, subfragment 2, and heavy meromyosin

The thermal unfolding of rabbit skeletal heavy meromyosin (HMM), myosin subfragment 1, and subfragment 2 has been studied by differential scanning calorimetry (DSC). Two distinct endotherms are observed in the DSC scan of heavy meromyosin. The first endotherm, with a Tm of 41 degrees C at pH 7.9 in 0.1 M KCl, is assigned to the unfolding of the subfragment 2 domain of HMM based on scans of isolated subfragment 2. The unfolding of the subfragment 2 domain is reversible both in the isolated form and in HMM. The unfolding of subfragment 2 in HMM can be fit as a single two-state transition with a delta Hvh and delta Hcal of 161 kcal/mol, indicating that subfragment 2 exists as a single domain in HMM. The unfolding of subfragment 2 is characterized by an extraordinarily large delta Cp of approximately 30,000 cal/(deg.mol). In the presence of nucleotides, the high-temperature HMM endotherm with a Tm of 48 degrees C shifts to higher temperature, indicating that this peak corresponds to the unfolding of the subfragment 1 domain. This assignment has been confirmed by comparison with isolated subfragment 1. The stabilizing effect of AMPPNP was significantly greater than that of ADP. The vanadate-trapped ADP species was slightly more stable than M.AMPPNP with a Tm at 58 degrees C. The unfolding of subfragment 1, both in the isolated form and in HMM, was irreversible. Only a single endotherm was noted in the DSC scans of the subfragment 1 domain of HMM and in freshly prepared subfragment 1 complexes.(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermal unfolding of G-actin monitored with the DNase I-inhibition assay stabilities of actin isoforms.

Actin is one of the proteins that rely on chaperonins for proper folding. This paper shows that the thermal unfolding of G-actin, as studied by CD and ultraviolet difference spectrometry, coincides with a loss in DNase I-inhibiting activity of the protein. Thus, the DNase I inhibition assay should be useful for systematic studies of actin unfolding and refolding. Using this assay, we have investigated how the thermal stability of actin is affected by either Ca2 + or Mg2 + at the high affinity divalent cation binding site, by the concentration of excess nucleotide, and by the nucleotide in different states of phosphorylation (ATP, ADP.Pi, ADP. Vi, ADP.AlF4, ADP.BeFx, and ADP). Actin isoforms from different species were also compared, and the effect of profilin on the thermal stability of actin was studied. We conclude that the thermal unfolding of G-actin is a three-state process, in which an equilibrium exists between native actin with bound nucleotide and an intermediate free of nucleotide. Actins in the Mg-form were less stable than the Ca-forms, and the stability of the different isoforms decreased in the following order: rabbit skeletal muscle alpha-actin = bovine cytoplasmic gamma-actin > yeast actin > cytoplasmic beta-actin. The activation energies for the thermal unfolding reactions were in the range 200-290 kJ.mol- 1, depending on the bound ligands. Generally, the stability of the actin depended on the degree with which the nucleotide contributed to the connectivity between the two domains of the protein.     

Conformational changes of the beta chain of the outer-arm dynein from sea urchin sperm flagella coupled with ATP hydrolysis

Conformational changes of the beta chain of the outer-arm dynein from sea urchin sperm flagella in relation to ATP hydrolysis was examined by tryptic digestion. Tryptic digestion of the beta chain in the presence of 2 mM ATP (ADP) and 100 microM vanadate (Vi) or in the presence of 4 mM ATP gamma S produced different polypeptides from in the case of no addition. The difference was similar to the result previously reported for 21S outer-arm dynein heavy chains [Inaba, K. & Mohri, H. (1989) J. Biol. Chem. 264, 8384-8388]. Unlike the tryptic digestion pattern of 21S dynein heavy chains, however, the 135-kDa polypeptide was consistently produced from the beta chain, even in the presence of ATP (ADP) and Vi. The tryptic digestion pattern of the 21S particle reconstituted from the separated a chain, the beta/IC1 complex and the IC2/IC3 complex [Tang, W.-J.Y., Bell, C.W., Sale, W.S., & Gibbons, I.R. (1982) J. Biol. Chem. 257, 508-515] was similar to that of intact 21S dynein; the 135-kDa polypeptide was only slightly produced in the presence of ATP and Vi. The digestion rate constant of the 135-kDa polypeptide from the beta chain in the presence of ATP and Vi was significantly decreased as compared with in the case of 21S dynein or that of the reconstituted 21S particle. These results suggest that the trypsin sensitivity of the 135-kDa region of the beta chain changes with the association of the beta/ICI complex with the alpha chain and the IC2/IC3 complex in the presence of ATP and Vi.     

Effects of two familial hypertrophic cardiomyopathy mutations in alpha-tropomyosin, Asp175Asn and Glu180Gly, on the thermal unfolding of actin-bound tropomyosin

Differential scanning calorimetry was used to investigate the thermal unfolding of native alpha-tropomyosin (Tm), wild-type alpha-Tm expressed in Escherichia coli and the wild-type alpha-Tm carrying either of two missense mutations associated with familial hypertrophic cardiomyopathy, D175N or E180G. Recombinant alpha-Tm was expressed with an N-terminal Ala-Ser extension to substitute for the essential N-terminal acetylation of the native Tm. Native and Ala-Ser-Tm were indistinguishable in our assays. In the absence of F-actin, the thermal unfolding of Tm was reversible and the heat sorption curve of Tm with Cys-190 reduced was decomposed into two separate calorimetric domains with maxima at approximately 42 and 51 degrees C. In the presence of phalloidin-stabilized F-actin, a new cooperative transition appears at 46-47 degrees C and completely disappears after the irreversible denaturation of F-actin. A good correlation was found to exist between the maximum of this peak and the temperature of half-maximal dissociation of the F-actin/Tm complex as determined by light scattering experiments. We conclude that Tm thermal denaturation only occurs upon its dissociation from F-actin. In the presence of F-actin, D175N alpha-Tm shows a melting profile and temperature dependence of dissociation from F-actin similar to those for wild-type alpha-Tm. The actin-induced stabilization of E180G alpha-Tm is significantly less than for wild-type alpha-Tm and D175N alpha-Tm, and this property could contribute to the more severe myopathy phenotype reported for this mutation.     

Changes in the thermal unfolding of p-phenylenedimaleimide-modified myosin subfragment 1 induced by its 'weak' binding to F-actin

Differential scanning calorimetry (DSC) was used to analyze the thermal unfolding of myosin subfragment 1 (S1) with the SH1 (Cys-707) and SH2 (Cys-697) groups cross-linked by N,N'-p-phenylenedimaleimide (pPDM-S1). It has been shown that F-actin affects the thermal unfolding of pPDM-S1 only at very low ionic strength, when some part of pPDM-S1 binds weakly to F-actin, but not at higher ionic strength (200 mM KCl). The weak binding of pPDM-S1 to F-actin shifted the thermal transition of pPDM-S1 by about 5 degrees C to a higher temperature. This actin-induced increase in thermal stability of pPDM-S1 was similar to that observed with 'strong' binding of unmodified S1 to F-actin. Our results show that actin-induced structural changes revealed by DSC in the myosin head occur not only upon strong binding but also on weak binding of the head to F-actin, thus suggesting that these changes may occur before the power-stroke and play an important role in the motor function of the head.     

Antagonistic effects of cofilin, beryllium fluoride complex, and phalloidin on subdomain 2 and nucleotide-binding cleft in F-actin

Cofilin/ADF, beryllium fluoride complex (BeFx), and phalloidin have opposing effects on actin filament structure and dynamics. Cofilin/ADF decreases the stability of F-actin by enhancing disorder in subdomain 2, and by severing and accelerating the depolymerization of the filament. BeFx and phalloidin stabilize the subdomain 2 structure and decrease the critical concentration of actin, slowing the dissociation of monomers. Yeast cofilin, unlike some other members of the cofilin/ADF family, binds to F-actin in the presence of BeFx; however, the rate of its binding is strongly inhibited by BeFx and decreases with increasing pH. The inhibition of the cofilin binding rate increases with the time of BeFx incubation with F-actin, indicating the existence of two BeFx-F-actin complexes. Cofilin dissociates BeFx from the filament, while BeFx does not bind to F-actin saturated with cofilin, presumably because of the cofilin-induced changes in the nucleotide-binding cleft of F-actin. These changes are apparent from the increase in the fluorescence intensity of F-actin bound epsilon-ADP upon cofilin binding and a decrease in its accessibility to collisional quenchers. BeFx also affects the nucleotide-binding cleft of F-actin, as indicated by an increase in the fluorescence intensity of epsilon-ADP-F-actin. Phalloidin and cofilin inhibit, but do not exclude each other binding to their complexes with F-actin. Phalloidin promotes the dissociation of cofilin from F-actin and slowly reverses the cofilin-induced disorder in the DNase I binding loop of subdomain 2.     

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.     

Evidence for the existence of two equilibrium conformations of the ternary complex of myosin subfragment-1, ADP, and orthovanadate

In order to investigate the flexibility of the ternary complex consisting of myosin subfragment-1 (S1), ADP, and orthovanadate (Vi), i.e., S1.ADP.Vi, the exchangeability of the bound ADP was examined. After isolation of the ternary complex of S1.ADP.Vi by gel filtration, 3'-O-(N-methylanthraniloyl)-ADP (Mant-ADP), a fluorescent analogue of ADP, was added at 0.5 degrees C. The added Mant-ADP was incorporated into the ternary complex very slowly by replacing the bound ADP. The nucleotide exchange occurred without regeneration of the ATPase activity of S1. Similarly, the ternary complex of S1.Mant-ADP.Vi prepared and isolated by gel filtration according to Hiratsuka (3, 4), was incubated with ADP (2.4 mM) at 4.5 degrees C. The nucleotide exchange of S1.Mant-ADP.Vi with ADP occurred in two phases with the apparent rates of 4.5 x 10(-4) s-1 (the fast phase) and 6.7 x 10(-6) s-1 (the slow phase). Biphasic exchange of the bound nucleotide was also observed with S1(A1) isozyme, indicating that the biphasic exchange did not correspond to two S1 isozymes. The apparent rates of the fast and the slow phases increased with the concentration of the added ADP, but they became saturated at an ADP concentration of the order of 2 mM, indicating that the nucleotide exchange reaction involves a step (or steps) which is insensitive to the concentration of free ADP in the solution. This step might be a reversible isomerization.     

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.     

Dynamic conformational changes of 21 S dynein ATPase coupled with ATP hydrolysis revealed by proteolytic digestion

Conformational changes of 21 S dynein ATPase from sea urchin sperm flagella were examined by tryptic digestion under physiological conditions. In the presence of 2 mM ATP or ADP plus 100 microM inorganic vanadate (Vi), dynein heavy chains were digested by trypsin into quite different polypeptides from those obtained in other cases (no addition, 2 mM ATP, 4 mM adenosine 5'-(beta,gamma-imido)triphosphate, 4 mM adenosine 5'-(beta,gamma-methylene)triphosphate, 2 mM ADP, 100 microM Vi). In the presence of 4 mM adenosine 5'-O-(3-thiotriphosphate), however, the digestion pattern was similar to that in the presence of ATP (ADP) and Vi, to a certain extent. In all conditions other than the presence of ATP (ADP) and Vi, 165- and 135-kDa polypeptides were the main products, whereas in the presence of ATP (ADP) and Vi, 200-, 150/148-, and 105/96-kDa peptides were produced and 320-kDa peptide became rather inaccessible to trypsin. The latter digestion pattern was not observed in the absence of divalent cations. These results suggest that, in the ATP hydrolysis cycle, dynein changes its conformation remarkably in the dynein-ADP-Pi state, which is presumably responsible for force generation.     

Dynamic reorganization of the motor domain of myosin subfragment 1 in different nucleotide states.

Atomic models of the myosin motor domain with different bound nucleotides have revealed the open and closed conformations of the switch 2 element [Geeves, M.A. & Holmes, K.C. (1999) Annu. Rev. Biochem.68, 687-728]. The two conformations are in dynamic equilibrium, which is controlled by the bound nucleotide. In the present work we attempted to characterize the flexibility of the motor domain in the open and closed conformations in rabbit skeletal myosin subfragment 1. Three residues (Ser181, Lys553 and Cys707) were labelled with fluorophores and the probes identified three fluorescence resonance energy transfer pairs. The effect of ADP, ADP.BeFx, ADP.AlF4- and ADP.Vi on the conformation of the motor domain was shown by applying temperature-dependent fluorescence resonance energy transfer methods. The 50 kDa lower domain was found to maintain substantial rigidity in both the open and closed conformations to provide the structural basis of the interaction of myosin with actin. The flexibility of the 50 kDa upper domain was high in the open conformation and further increased in the closed conformation. The converter region of subfragment 1 became more rigid during the open-to-closed transition, the conformational change of which can provide the mechanical basis of the energy transduction from the nucleotide-binding pocket to the light-chain-binding domain.     

Characterization of the ethenoadenosine diphosphate binding site of myosin subfragment 1. Energetics of the equilibrium between two states of nucleotide.S1 and vanadate-induced global conformation changes detected by energy transfer

The fluorescence decay of 1,N6-ethenoadenosine diphosphate (epsilon ADP) bound to myosin subfragment 1 (S1) was studied as a function of temperature. The decay was biexponential, and the two lifetimes were quenched relative to the single lifetime of free epsilon ADP. The temperature dependence of the fractional intensities of the decay components showed two states of the S1.epsilon ADP complex. At pH 7.5 in 30 mM TES, 60 mM KCl, and 3 mM MgCl2, the equilibrium constant for the conversion of the low-temperature state (S1L.epsilon ADP) to the high-temperature state (S1H.epsilon ADP) was 40 at physiological temperatures, and delta H degrees = 13 kcal.mol-1 and delta S degrees = 49 cal.deg-1.mol-1. At 10 degrees C the equilibrium constant of S1 for epsilon ADP was 5, indicating that S1H.epsilon ADP was the dominant state, and that for the vanadate complex epsilon ADP.Vi was 0.7, suggesting that in S1.epsilon ADP.Vi the dominant state of the S1-nucleotide complex was converted from S1H.epsilon ADP to S1L.epsilon ADP. The single rotational correlation time of bound epsilon ADP at 10 degrees C decreased from 107 ns in S1.epsilon ADP to 74 ns in S1+.epsilon ADP.Vi. Conversion of the binary complex to the ternary vanadate complex resulted in a 3-A decrease in the energy transfer distance between bound epsilon ADP and N-[4-(dimethylamino)-3,5-dinitrophenyl]maleimide attached to SH1 and a decrease of the average distance between bound epsilon ADP and bound Co2+ from 12.6 to 8.3 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Interaction of the heavy chain of gizzard myosin heads with skeletal F-actin

To probe the molecular properties of the actin recognition site on the smooth muscle myosin heavy chain, the rigor complexes between skeletal F-actin and chicken gizzard myosin subfragments 1 (S1) were investigated by limited proteolysis and by chemical cross-linking with 1-ethyl-3-[3-(dimethyl-amino)propyl]carbodiimide. Earlier, these approaches were used to analyze the actin site on the skeletal muscle myosin heads [Mornet, D., Bertrand, R., Pantel, P., Audemard, E., & Kassab, R. (1981) Biochemistry 20, 2110-2120; Labbé, J.P., Mornet, D., Roseau, G., & Kassab, R. (1982) Biochemistry 21, 6897-6902]. In contrast to the case of the skeletal S1, the cleavage with trypsin or papain of the sensitive COOH-terminal 50K-26K junction of the head heavy chain had no effect on the actin-stimulated Mg2+-ATPase activity of the smooth S1. Moreover, actin binding had no significant influence on the proteolysis at this site whereas it abolished the scission of the skeletal S1 heavy chain. The COOH-terminal 26K segment of the smooth papain S1 heavy chain was converted by trypsin into a 25K peptide derivative, but it remained intact in the actin-S1 complex. A single actin monomer was cross-linked with the carbodiimide reagent to the intact 97K heavy chain of the smooth papain S1. Experiments performed on the complexes between F-actin and the fragmented S1 indicated that the site of cross-linking resides within the COOH-terminal 25K fragment of the S1 heavy chain. Thus, for both the striated and smooth muscle myosins, this region appears to be in contact with F-actin.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fourier transform infrared spectroscopy suggests unfolding of loop structures precedes complete unfolding of pig citrate synthase

Pig citrate synthase (PCS) can be used as a model enzyme to gain some insight into the structural basis of protein thermostability. The thermal unfolding characteristics of the specific secondary structure elements within PCS were monitored in detail by following changes in its amide I band components. The result of our study indicates that PCS undergoes irreversible thermal denaturation. Detailed analysis reveals that the different secondary structures display a multistep transition with a major and a minor transition at different temperatures and a very small initial transition at the same temperature (30 degrees C). A plot of temperature-induced changes in (1)H-(2)H exchange, the decrease in the absorbance of the alpha-helical structures, and the increase in the absorbance of aggregated structures all have in common a multistep transition, the minor one centered at 45 degrees C and the major one around 59 degrees C. In contrast, a band that is tentatively assigned to loop structures displays these same minor and major transitions but at lower temperatures (39 and 52 degrees C, respectively). The transition, which occurs at 39-45 degrees C, is not associated with the appearance of aggregated structures. This transition may reflect a change in the tertiary structure of the protein. However, the final transition, which occurs at a higher temperature (52-59 degrees C), reflects unfolding and aggregation of the polypeptide chains. The Fourier transform infrared (FTIR) analysis suggests that PCS has a thermolabile region that unfolds first, some 7 degrees C below the main unfolding of the protein. We propose that this reflects the unfolding of the highly flexible loop segments, which in turn triggers the unfolding of the predominantly helical core structure of PCS.     

Mutation of Cys-67 alters the thermodynamic stability of the human leukocyte antigen HLA0-B*2705

The B pocket of the class I major histocompatibility complex-encoded protein HLA-B*2705 has recently been suggested to be responsible for the misfolding of this HLA haplotype and thus to induce susceptibility to autoimmune inflammatory diseases. Four mutants of the B*2705 heavy chain were refolded in the presence of three control peptides. The monitoring of the thermal unfolding of the B*2705-peptide complexes by circular dichroism spectroscopy showed that all heterotrimeric mutants were markedly less stable than the corresponding complexes with the wild-type heavy chain. Among the four heavy chain mutations, the C67S change was investigated for unfolding and peptide binding properties because this position may mediate disulfide pair bridging and alter T-cell recognition of HLA-B*2705. Wild-type heterotrimers completely unfold in a single transition at mild acidic pH whereas increase of the pH to mild basic conditions induce only a partial biphasic unfolding. Cys-67 seems to play a crucial role in controlling the thermodynamic stability of the B*2705-peptide complexes as the C67S mutant unfolds faster and with a single transition, independent of pH. Fluorescence polarization and size exclusion chromatography of unfolding intermediates suggest that the peculiar unfolding of the B*2705 wild-type heavy chain cannot be explained by modified peptide binding properties but more likely by the formation of high molecular weight species.