Skeletal Subfragment Research Articles

Similarities and Differences between Frozen-Hydrated, Rigor Acto–S1 Complexes of Insect Flight and Chicken Skeletal Muscles

The structure and function of myosin crossbridges in asynchronous insect flight muscle (IFM) have been elucidated in situ using multiple approaches. These include generating “atomic” models of myosin in multiple contractile states by rebuilding the crystal structure of chicken subfragment 1 (S1) to fit IFM crossbridges in lower-resolution electron microscopy tomograms and by “mapping” the functional effects of genetically substituted, isoform-specific domains, including the converter domain, in chimeric IFM myosin to sequences in the crystal structure of chicken S1. We prepared helical reconstructions (∼ 25 Å resolution) to compare the structural characteristics of nucleotide-free myosin0 S1 bound to actin (acto–S1) isolated from chicken skeletal muscle ( CSk) and the flight muscles of Lethocerus ( Leth) wild-type Drosophila ( wt Dros) and a Drosophila chimera ( IFI-EC) wherein the converter domain of the indirect flight muscle myosin isoform has been replaced by the embryonic skeletal myosin converter domain. Superimposition of the maps of the frozen-hydrated acto–S1 complexes shows that differences between CSk and IFM S1 are limited to the azimuthal curvature of the lever arm: the regulatory light-chain (RLC) region of chicken skeletal S1 bends clockwise (as seen from the pointed end of actin) while those of IFM S1 project in a straight radial direction. All the IFM S1s are essentially identical other than some variation in the azimuthal spread of density in the RLC region. This spread is most pronounced in the IFI-EC S1, consistent with proposals that the embryonic converter domain increases the compliance of the IFM lever arm affecting the function of the myosin motor. These are the first unconstrained models of IFM S1 bound to actin and the first direct comparison of the vertebrate and invertebrate skeletal myosin II classes, the latter for which, data on the structure of discrete acto-S1 complexes, are not readily available.

The Mechanism of the Reverse Recovery Step, Phosphate Release, and Actin Activation of Dictyostelium Myosin II

The rate-limiting step of the myosin basal ATPase (i.e. in absence of actin) is assumed to be a post-hydrolysis swinging of the lever arm (reverse recovery step), that limits the subsequent rapid product release steps. However, direct experimental evidence for this assignment is lacking. To investigate the binding and the release of ADP and phosphate independently from the lever arm motion, two single tryptophan-containing motor domains of Dictyostelium myosin II were used. The single tryptophans of the W129+ and W501+ constructs are located at the entrance of the nucleotide binding pocket and near the lever arm, respectively. Kinetic experiments show that the rate-limiting step in the basal ATPase cycle is indeed the reverse recovery step, which is a slow equilibrium step (k(forward) = 0.05 s(-1), k(reverse) = 0.15 s(-1)) that precedes the phosphate release step. Actin directly activates the reverse recovery step, which becomes practically irreversible in the actin-bound form, triggering the power stroke. Even at low actin concentrations the power stroke occurs in the actin-attached states despite the low actin affinity of myosin in the pre-power stroke conformation.

Evidence for an Interaction between the SH3 Domain and the N-terminal Extension of the Essential Light Chain in Class II Myosins

The function of the src-homology 3 (SH3) domain in class II myosins, a distinct β-barrel structure, remains unknown. Here, we provide evidence, using electron cryomicroscopy, in conjunction with light-scattering, fluorescence and kinetic analyses, that the SH3 domain facilitates the binding of the N-terminal extension of the essential light chain isoform (ELC-1) to actin. The 41 residue extension contains four conserved lysine residues followed by a repeating sequence of seven Pro/Ala residues. It is widely believed that the highly charged region interacts with actin, while the Pro/Ala-rich sequence forms a rigid tether that bridges the ∼9 nm distance between the myosin lever arm and the thin filament. In order to localize the N terminus of ELC in the actomyosin complex, an engineered Cys was reacted with undecagold-maleimide, and the labeled ELC was exchanged into myosin subfragment-1 (S1). Electron cryomicroscopy of S1-bound actin filaments, together with computer-based docking of the skeletal S1 crystal structure into 3D reconstructions, showed a well-defined peak for the gold cluster near the SH3 domain. Given that SH3 domains are known to bind proline-rich ligands, we suggest that the N-terminal extension of ELC interacts with actin and modulates myosin kinetics by binding to the SH3 domain during the ATPase cycle.

Behavior of caldesmon upon interaction of thin filaments with myosin subfragment 1 in ghost fibers

Caldesmon is a component of smooth muscle thin filaments which inhibits their interaction with myosin. We have used polarized fluorescence technique to study the behavior of caldesmon during the interaction of myosin subfragment 1 (S1) with thin filaments reconstituted in rabbit skeletal muscle ghost fibers by incorporation of smooth muscle tropomyosin and caldesmon labeled with acrylodan at cysteine residue located in the C-terminal region. Significant changes in acrylodan fluorescence intensity upon addition of skeletal muscle S1 reflected substantial displacement of caldesmon from thin filaments, while alterations in the calculated fluorescence parameters indicated the simultaneous rearrangement of the remaining caldesmon fraction. The orientation of caldesmon in the S1-thin filament complex relative to the fiber axis changes by approximately 7° and the mobility of the fluorescent probe by about 9%. The alterations in caldesmon orientation were proportional to the strength of S1 binding and diminished respectively upon addition of ADP and ADP-Vi. The changes in orientation of acrylodan-caldesmon evoked by the interaction of S1 with thin filaments were more pronounced than that in AEDANS-F-actin which suggests that the spatial arrangement of caldesmon in the complex is governed not only by F-actin but also by S1. The results may indicate that the changes in spatial arrangement of caldesmon are adjusted to the conformation of F-actin and S1 characteristic for particular steps of the ATP hydrolysis cycle.

Behavior of caldesmon upon interaction of thin filaments with myosin subfragment 1 in ghost fibers

Caldesmon is a component of smooth muscle thin filaments which inhibits their interaction with myosin. We have used polarized fluorescence technique to study the behavior of caldesmon during the interaction of myosin subfragment 1 (S1) with thin filaments reconstituted in rabbit skeletal muscle ghost fibers by incorporation of smooth muscle tropomyosin and caldesmon labeled with acrylodan at cysteine residue located in the C-terminal region. Significant changes in acrylodan fluorescence intensity upon addition of skeletal muscle S1 reflected substantial displacement of caldesmon from thin filaments, while alterations in the calculated fluorescence parameters indicated the simultaneous rearrangement of the remaining caldesmon fraction. The orientation of caldesmon in the S1-thin filament complex relative to the fiber axis changes by approximately 7° and the mobility of the fluorescent probe by about 9%. The alterations in caldesmon orientation were proportional to the strength of S1 binding and diminished respectively upon addition of ADP and ADP-V i. The changes in orientation of acrylodan-caldesmon evoked by the interaction of S1 with thin filaments were more pronounced than that in AEDANS-F-actin which suggests that the spatial arrangement of caldesmon in the complex is governed not only by F-actin but also by S1. The results may indicate that the changes in spatial arrangement of caldesmon are adjusted to the conformation of F-actin and S1 characteristic for particular steps of the ATP hydrolysis cycle.

Myosin isoforms show unique conformations in the actin-bound state.

Crystallographic data for several myosin isoforms have provided evidence for at least two conformations in the absence of actin: a prehydrolysis state that is similar to the original nucleotide-free chicken skeletal subfragment-1 (S1) structure, and a transition-state structure that favors hydrolysis. These weak-binding states differ in the extent of closure of the cleft that divides the actin-binding region of the myosin and the position of the light chain binding domain or lever arm that is believed to be associated with force generation. Previously, we provided insights into the interaction of smooth-muscle S1 with actin by computer-based fitting of crystal structures into three-dimensional reconstructions obtained by electron cryomicroscopy. Here, we analyze the conformations of actin-bound chicken skeletal muscle S1. We conclude that both myosin isoforms in the nucleotide-free, actin-bound state can achieve a more tightly closed cleft, a more downward position of the lever arm, and more stable surface loops than those seen in the available crystal structures, indicating the existence of unique actin-bound conformations.

Isolation and kinetic characterisation of myosin and myosin S1 from the Drosophila indirect flight muscles.

The potential to explore myosin function through the alternative exons and mutations of the single muscle myosin heavy chain gene, Mhc of Drosophila requires detailed kinetic analysis of the myosins. We have obtained microgram quantities of enzymatically active Drosophila myosin and subfragment 1 (S1) from dissected indirect flight muscles. Using recent developments in stopped-flow and flash-photolysis methods combined with fluorescent/light scattering technologies we have determined some of the key kinetic parameters of actin-myosin and myosin-nucleotide interactions. The rate of ATP-induced dissociation of actin from Drosophila myosin (0.23 microM(-1) s(-1)) and subfragment 1 (S1, 0.82 microM(-1) s(-1)) are both fast and similar to values measured for mammalian skeletal muscle myosins and S1 fragments respectively. The ATP-induced cross bridge dissociation of Drosophila acto.S1 is expected to be fast since, for a rapidly contracting muscle like the Drosophila flight muscle, the post power stroke cross bridge must detach rapidly from actin or become a drag on the contracting filament. ATP-induced detachment is preceded by ADP release and this is proposed as the rate-limiting step that defines muscle shortening velocity. We show that the affinity of ADP for acto.S1 at 400 microM is 2-3 fold weaker than fast vertebrate myosins. This leads to an estimate of the ADP release rate constant of 4000 s(-1). We show that this predicts a maximum shortening velocity very similar to that obtained from in vivo estimates of indirect flight muscle shortening. The data is therefore compatible with ADP dissociation limiting the in vivo shortening velocity.

The power stroke causes changes in the orientation and mobility of the termini of essential light chain 1 of myosin.

Binding of ATP to the catalytic domain of myosin induces a local conformational change which is believed to cause a major rotation of an 8.5 nm alpha-helix that is stabilized by the regulatory and essential light chains. Here we attempt to follow this rotation by measuring the mobility and orientation of a fluorescent probe attached near the C- or N-terminus of essential light chain 1 (LC1). Cysteine 178 of wild-type LC1, or Cys engineered near the N-terminus of mutant LC1, was labeled with tetramethylrhodamine and exchanged into skeletal subfragment-1 (S1) or into striated muscle fibers. In the absence of ATP, the fluorescence anisotropy (r) and the rotational correlation time (rho) of S1 reconstituted with LC1 labeled near the C-terminus were 0.195 and 66.6 ns, respectively. In the presence of ATP, r and rho increased to 0.233 and 233 ns, indicating considerable immobilization of the probe. A related parameter indicating the degree of order of cross-bridges in muscle fibers, Deltar, was small in rigor fibers (-0.009) and increased in relaxed fibers (0.030). For S1 reconstituted with LC1 labeled near the N-terminus, the steady-state anisotropy was 0.168 in rigor, and increased to 0.223 in relaxed state. In fibers, the difference in rigor was large (Deltar = 0.080), because of binding to the thin filaments, and decreased to 0.037 in relaxed fibers. These results suggest that before the power stroke, in the presence of ATP or its products of hydrolysis, the termini of LC1 are immobilized and ordered, and after the stroke, they become more mobile and partially disordered. The results are consistent with crystallographic structures that show that the level of putative stabilizing interactions of LC1 with the heavy chain of S1 in the transition state is reduced as the regulatory domain rotates to its post-power stroke position.

X-ray diffraction evidence for the lack of stereospecific protein interactions in highly activated actomyosin complex

The structure of actomyosin complex while hydrolyzing ATP was investigated by recording X-ray diffraction patterns from rabbit skeletal muscle fibers, in which exogenously introduced rabbit skeletal subfragment-1 (S1) was covalently cross-linked to the endogenous actin filaments in rigor by 1-ethyl-3-(3-dimethylaminopropyl) carbodiimide (EDC). Approximately two-thirds of the introduced S1 was cross-linked. The cross-linking procedure did not affect the profile of the S1-induced enhancement of the actin-based layer line reflections in rigor, indicating that the acto-S1 interactions remained highly stereospecific. In the presence of ATP, the MgATPase of the S1 was highly activated regardless of calcium levels, presumably because the availability of the stereospecific binding sites for both proteins was maximized by the cross-linking. However, the diffraction pattern in the presence of ATP was striking in that the intensity profile of the strong 1/5.9 nm −1layer lines was indistinguishable from that from bare actin filaments, despite the fact that the majority of the S1 was still associated with actin. The change of the intensity profiles upon addition of ATP was completely reversible. Model calculations showed that this result can be explained if the S1 is not only swinging around its pivoting point, but the pivoting point itself is also moving on the actin surface in a range of a few nanometers. The results suggest that the stereospecific binding sites, which have been considered important for actomyosin cycling, are paradoxically left unoccupied for most of the time in this highly activated actomyosin complex.

Solution properties of full length and truncated forms of myosin subfragment 1 from Dictyostelium discoideum.

The atomic structures for several myosin head isoforms in different nucleotide states have been determined in recent years. The comparison of these structures is complicated by the use of myosin subfragment 1 (S1) constructs of different length in different studies. Several atomic structures of the S1 nucleotide complex were obtained using Dictyostelium discoideum S1dC, a genetically truncated form of S1 lacking the light chain binding domain (LCBD) and both light chains. The goal of the present study has been to assess the effects of such a truncation on the solution properties of S1 and in particular, on its active site, actin binding site and the converter region. The nucleotide and actin binding properties, CD spectra and the reactivities of Lys-84 (corresponds to the 'reactive lysine', Lys-83 in rabbit skeletal S1) and Cys-678 (corresponds to the 'SH2-group', Cys-697 in rabbit S1) were compared for the full length (flS1) and the truncated (S1dC) forms of Dictyostelium S1. The two forms showed similar nucleotide binding properties. However, SldC had a lower structural stability and a significantly higher Km value for actin-activated ATPase as compared to flS1. Differences were found also in the near-UV CD spectrum between flS1 and S1dC. SH2 reactivity in SldC appeared to be greatly inhibited compared with that in flS1. The modification of Lys-84 caused a greater increase in the MgATPase activity in S1dC than in flS1. ADP inhibited this activation for both SldC and flS1. Taken together our results identify both truncation-caused differences between S1dC and flS1, as well as isoform-related differences between skeletal and Dictyostelium S1.

Isolating and Localizing ATP-Sensitive Tryptophan Emission in Skeletal Myosin Subfragment 1

The fluorescence intensity difference between rabbit skeletal myosin subfragment 1 (S1) and nucleotide-bound or trapped S1 isolates ATP-sensitive tryptophans (ASTs) emission from the total tryptophan signal. Neutral (acrylamide) quenching of the ASTs is sensitive to the binding or trapping of nucleotide to the active site of S1. Anion (I(-)) quenching of the ASTs, sensitive to charge separation in the tryptophan micro environment, is negligible. These findings suggest the ASTs sense conformational change during ATPase from negatively charged surroundings. Specific chemical modifications of S1 identified the location of the ASTs. Trp131 was quenched by chemical modification, and its emission was isolated by taking the intensity difference between unmodified and modified S1. Trp131 fluorescence intensity and quenching constant do not distinguish among the bound or trapped nucleotides, suggesting that the vicinity of Trp131 does not change conformation during the ATPase cycle and eliminating Trp131 as an AST. Trp510 fluorescence was quenched by 5'-iodoacetamidofluorescein (5'IAF) modification of the reactive thiol (SH1) of S1. The tryptophan emission enhancement increment due to active site trapping decreases linearly with SH1 modification and extrapolates to 0 for 100% modification. These data identify Trp510 as the primary AST in skeletal S1 in agreement with observations from Dictyostelium (Batra and Manstein (1999) Biol. Chem. 380, 1017-1023) and smooth muscle S1 (Yengo et al. (2000) Biophys. J. 78, 242A). With Trp510 identified as the sole AST, fluorescence difference spectroscopy provides a novel means to monitor the concentration of myosin transient intermediates in ATP hydrolysis.

The Identification of Tryptophan Residues Responsible for ATP-Induced Increase in Intrinsic Fluorescence of Myosin Subfragment 1

ATP binding to myosin subfragment 1 (S1) induces an increase in tryptophan fluorescence. Chymotryptic rabbit skeletal S1 has 5 tryptophan residues (Trp113, 131, 440, 510 and 595), and therefore the identification of tryptophan residues perturbed by ATP is quite complex. To solve this problem we resolved the complex fluorescence spectra into log-normal and decay-associated components, and carried out the structural analysis of the microenvironment of each tryptophan in S1. The decomposition of fluorescence spectra of S1 and S1-ATP complex revealed 3 components with maxima at ca. 318, 331 and 339–342 nm. The comparison of structural parameters of microenvironment of 5 tryptophan residues with the same parameters of single- tryptophan-containing proteins with well identified fluorescence properties applying statistical method of cluster analysis, enabled us to assign Trp595 to 318 nm, Trp440 to 331 nm, and Trp113, 131 and 510 to 342 nm spectral components. ATP induced an almost equal increase in the intensities of the intermediate (331 nm) and long-wavelength (342 nm) components, and a small decrease in the short component (318 nm). The increase in the intermediate component fluorescence most likely results from an immobilization of some quenching groups (Met437, Met441 and/or Arg444) in the environment of Trp440. The increase in the intensity and a blue shift of the long component might be associated with conformational changes in the vicinity of Trp510. However, these conclusions can not be extended directly to the other types of myosins due to the diversity in the tryptophan content and their microenvironments.

Size and Charge Requirements for Kinetic Modulation and Actin Binding by Alkali 1-type Myosin Essential Light Chains

The alkali 1-type isoforms of myosin essential light chains from vertebrate striated muscles have an additional 40 or so amino acids at their N terminus compared with the alkali 2-type. Consequently two light chain isoenzymes of myosin subfragment-1 can be isolated. Using synthesized peptide mimics of the N-terminal region of alkali 1-type essential light chains, we have found by 1H NMR that the major actin binding region occurred in the N-terminal four residues, APKK. These results were confirmed by mutating this region of the human atrial essential light chain, resulting in altered actin-activated MgATPase kinetics when the recombinant light chains were hybridized into rabbit skeletal subfragment 1. Substitution of either Lys3 or Lys4 with Ala resulted in increased Km and kcat and decreased actin binding (as judged by chemical cross-linking). Replacement of Lys4 with Asp reduced actin binding and increased Km and kcat still further. Alteration of Ala1 to Val did not alter the kinetic parameters of the hybrid subfragment 1 or the essential light chain's ability to bind actin. Furthermore, we found a significant correlation between the apparent Km for actin and the kcat for MgATP turnover for each mutant hybrid, strengthening our belief that the binding of actin by alkali 1-type essential light chains results directly in modulation of the myosin motor.

Thin-filament linked regulation of smooth muscle myosin.

Phosphorylation of the regulatory light chain subunit of smooth muscle myosin is sufficient, but not necessary for muscle contraction. It has been suggested that thin-filament regulation may also contribute to the regulation of contraction. A hallmark feature of regulated thin filaments, previously described for vertebrate skeletal muscle, is the capacity of strong-binding or rigor-like cross bridges to "turn-on" the actin filament. Turned-on thin filaments stimulate cross-bridge attachment even in the absence of calcium. The present study utilized an in vitro sliding-filament motility assay to test for thin-filament regulation of both unphosphorylated and phosphorylated smooth muscle myosins. Regulated thin-filaments were reconstituted from skeletal muscle actin and chicken gizzard smooth muscle tropomyosin (TmCG), and then turned-on either (1) by rigor cross bridges at low concentrations of MgATP, or (2) by adding N-ethyl-maleimide-modified skeletal subfragment S1(NEM-S1), which forms rigor-like bonds in the presence of MgATP. For control actin.TmCG filaments, force production by unphosphorylated myosin was 0.5% of that produced by thiophosphorylated myosin. The force exerted on actin.Tm filaments by both unphosphorylated and phosphorylated myosins was increased by reducing the [MgATP] to 10-100 microM MgATP (rigor-dependent activation). Force was also increased by actin.TmCG filaments that had been turned-on by NEM-S1 binding, with force production by unphosphorylated myosin increased 80-fold vs. 2.3-fold for thiophosphorylated myosin. TmCG was required for increased force production with both low MgATP and NEM-S1. Unloaded filament velocity for NEM-S1-activated thin filaments was 0.72 micron/sec with unphosphorylated myosin compared to 1.24 microns/sec with thiophosphorylated myosin. Taken together, these results suggest that thin-filament regulation may play a role in the activation of both unphosphorylated and phosphorylated smooth muscle myosins and suggest a possible mechanism for activation of slowly cycling unphosphorylated cross bridges (i.e. latch-state) during tonic contractions of smooth muscle.

Conformational changes between the active-site and regulatory light chain of myosin as determined by luminescence resonance energy transfer: the effect of nucleotides and actin.

Myosin is thought to generate movement of actin filaments via a conformational change between its light-chain domain and its catalytic domain that is driven by the binding of nucleotides and actin. To monitor this change, we have measured distances between a gizzard regulatory light chain (Cys 108) and the active site (near or at Trp 130) of skeletal myosin subfragment 1 (S1) by using luminescence resonance energy transfer and a photoaffinity ATP-lanthanide analog. The technique allows relatively long distances to be measured, and the label enables site-specific attachment at the active-site with only modest affect on myosin's enzymology. The distance between these sites is 66.8 +/- 2.3 A when the nucleotide is ADP and is unchanged on binding to actin. The distance decreases slightly with ADP-BeF3, (-1.6 +/- 0.3 A) and more significantly with ADP-AlF4 (-4.6 +/- 0.2 A). During steady-state hydrolysis of ATP, the distance is temperature-dependent, becoming shorter as temperature increases and the complex with ADP.Pi is favored over that with ATP. We conclude that the distance between the active site and the light chain varies as Acto-S1-ADP approximately S1-ADP > S1-ADP-BeF3 > S1-ADP-AlF4 approximately S1-ADP-Pi and that S1-ATP > S1-ADP-Pi. The changes in distance are consistent with a substantial rotation of the light-chain binding domain of skeletal S1 between the prepowerstroke state, simulated by S1-ADP-AlF4, and the post-powerstroke state, simulated by acto-S1-ADP.

Effect of ADP on binding of skeletal S1 to F-actin.

The proximity of skeletal myosin subfragment-1 (S1) to actin, and its orientation with respect to thin filaments of single muscle fibers, were compared in the presence and in the absence of ADP. The proximity was assessed by the efficiency of carbodiimide-induced cross-linking and the orientation by polarization of fluorescence of probes attached to the essential light chains. ADP made no difference in proximity or orientation when the molar ratio of S1 to actin was low or high. However, at the intermediate ratios, ADP made a significant difference. Strong dissociating agents, AMP-PNP and PPi, made significant differences at all ratios. To explain this behavior, it is unnecessary to invoke the ADP-induced "swinging" of the tail of S1. Rather, it is simply explained by the "two-state" model which we proposed earlier, in which S1 binds to one or to two actin protomers, depending on the saturation of the filaments with S1s. The dissociation induced by the ADP shifts the equilibrium between the two bound states. At high and low degrees of saturation, ADP is unable to significantly decrease the amount of S1 bound to F-actin. However, at intermediate saturation levels, ADP causes significantly more S1s to bind to two actins. These results suggest that the ADP-induced changes seen at the intermediate molar ratios are due to the dissociation-induced reorientation of S1.

Crystal Structure of a Vertebrate Smooth Muscle Myosin Motor Domain and Its Complex with the Essential Light Chain: Visualization of the Pre–Power Stroke State

The crystal structures of an expressed vertebrate smooth muscle myosin motor domain (MD) and a motor domain–essential light chain (ELC) complex (MDE), both with a transition state analog (MgADP·AlF 4 −) in the active site, have been determined to 2.9 Å and 3.5 Å resolution, respectively. The MDE structure with an ATP analog (MgADP·BeF x) was also determined to 3.6 Å resolution. In all three structures, a domain of the C-terminal region, the “converter,” is rotated ∼70° from that in nucleotide-free skeletal subfragment 1 (S1). We have found that the MDE–BeF x and MDE–AlF 4 − structures are almost identical, consistent with the fact that they both bind weakly to actin. A comparison of the lever arm positions in MDE–AlF 4 − and in nucleotide-free skeletal S1 shows that a potential displacement of ∼10 nm can be achieved during the power stroke.

The N-terminus of A1-type myosin essential light chains binds actin and modulates myosin motor function.

There are two isoforms (A1 and A2) of the myosin essential light chain (ELC) and consequently two isoenzymes of myosin subfragment 1 (S1), S1(A1) and S1(A2). The two isoenzymes differ in their kinetic properties with S1(A1) having a lower apparent Km for actin and a slower turnover of MgATP (k(cat)) than S1(A2). The two forms of the ELC differ only at their N-termini where A1 has an additional 40-odd amino acids that are not present in A2. The human atrial ELC (an A1-type ELC) was overexpressed in Escherichia coli and purified by ammonium sulphate fractionation and ion-exchange chromatography. The recombinant ELC had actin-activated MgATPase kinetics similar to those for rabbit skeletal S1(A1) under the same conditions. Deletion of the first 45 amino acid residues resulted in an ELC similar to the rabbit skeletal A2 isoform and, when hybridised into S1, in S1(A2)-like kinetic properties. Results obtained with an ELC mutant that lacks the first 11 residues were intermediate between these two extremes but tending towards the S1(A2)-like phenotype. The wild-type ELC (both hybridised into S1 or free in solution) could be cross-linked to F-actin, whereas the deletion mutant lacking the first 45 amino acids could not. The deletion mutant lacking the first 11 amino acids cross-linked only poorly under the same conditions, consistent with the MgATPase data. We therefore conclude that these N-terminal eleven amino acids predominantly encode an actin-binding site which modulates the kinetics of the myosin motor. Furthermore, while free A1-type ELC cross-linked to both polymeric F-actin and the monomeric G-actin:DNase-I complex, the same ELC in S1(A1) could only cross-link to F-actin. This suggests that the light chain binds to a different actin monomer than the heavy chain.

Effect of ATP analogues on the actin-myosin interface.

The interaction between skeletal myosin subfragment 1 (S1) and filamentous actin was examined at various intermediate states of the actomyosin ATPase cycle by chemical cross-linking experiments. Reaction of the actin-S1 complex with 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide and N-hydroxysuccinimide generated products with molecular masses of 165 and 175 kDa, in which S1 loops of residues 626-647 and 567-578 were cross-linked independently to the N-terminal segment of residues 1-12 of one actin monomer, and of 265 kDa, in which the two loops were bound to the N termini of two adjacent monomers. In strong-binding complexes, i.e., without nucleotide or with ADP, S1 was sequentially cross-linked to one and then to two actin monomers. In the weak-binding complexes, two types of cross-linking pattern were observed. First, during steady-state hydrolysis of ATP or ATPgammaS at 20 degreesC, the cross-linking reaction gave rise to a small amount of unknown 200 kDa product. Second, in the presence of AMPPNP, ADP.BeFx, ADP.AlF4-, or ADP.VO43- or with S1 internally cross-linked by N,N'-p-phenylenedimaleimide, only the 265 kDa product was obtained. The presence of 200 mM salt inhibited cross-linking reactions in both weak- and strong-binding states, while it dissociated only weak-binding complexes. These results indicate that, in the weak-binding state populated with the ADP.Pi analogues, skeletal S1 interacts predominantly and with an apparent equal affinity with the N termini of two adjacent actin monomers, while these ionic contacts are much less significant in stabilizing the rigor actin-S1 complexes. They also suggest that the electrostatic actin-S1 interface is not influenced by the type of ADP.Pi analogue bound to the active site.

X-ray crystal structure and solution fluorescence characterization of Mg·2′(3′)- O-( N-methylanthraniloyl) nucleotides bound to the Dictyostelium discoideum myosin motor domain

Mant (2′(3′)- O-( N-methylanthraniloyl)) labeled nucleotides have proven to be useful tools in the study of the kinetic mechanism of the myosin ATPase by fluorescence spectroscopy. The sensitivity of the mant fluorophore to its local environment also makes it suitable to investigate the exposure of bound nucleotides to solvent from collisional quenching measurements. Here we present the crystal structure of mant-ADP and beryllium fluoride complexed with Dictyostelium discoideum myosin motor domain (S1dC) at 1.9 Å resolution. We complement the structural approach with an investigation of the accessibility of the mant moiety to solvent using acrylamide quenching of fluorescence emission. In contrast to rabbit skeletal myosin subfragment 1, where the mant group is protected from acrylamide ( K sv=0.2 M −1), the fluorophore is relatively exposed when bound to Dictyostelium myosin motor domain ( K sv=1.4 M −1). Differences between the Dictyostelium structure and that of vertebrate skeletal subfragment 1, in the region of the nucleotide binding pocket, are proposed as an explanation for the differences observed in the solvent accessibility of complexed mant-nucleotides. We conclude that protection of the mant group from acrylamide quenching does not report on overall closure of the nucleotide binding pocket but reflects more local structural changes.