X-ray scattering by single-headed heavy meromyosin. Cleavage of the myosin head from the rod does not change its shape

Low angle X-ray scattering from heavy meromyosin (HMM) and from single-headed heavy meromyosin (sHMM) have been examined to determine if the heads of myosin change shape when cleaved from the rod to form subfragment 1 (S1). The scattering intensities of intact HMM and sHMM were compared with those of their chymotryptic digestion products, S1 and subfragment 2 (S2). As the data with HMM were complicated by scattering between the two heads, the more extensive analysis was done with sHMM. Pseudo-Guinier plots of intact and digested sHMM, over the angular range used previously for S1, were linear and showed a difference in apparent radius of gyration (Rg) of only 0.07 +/- 0.04 nm. The absolute apparent Rg value of sHMM was 3.2 +/- 0.2 nm, which is comparable to the radius of gyration reported previously for S1 alone. A plot of the fractional differences in scattering intensities of intact and digested sHMM was flat to a reciprocal spacing of at least 1/3.5 nm-1. These results indicate that the head portions of sHMM and S1 have very similar structures at low resolution. Scattering curves for various models of sHMM and mixtures of S1 and S2 were calculated and the fractional difference plots of scattering intensities were made to determine how sensitive this type of analysis is to changes in the shape of the head. Changes in Rg of 0.1 nm or greater gave detectably non-flat difference plots. Thus, the X-ray scattering of sHMM (and HMM) demonstrated that differences in structure between the head of myosin and isolated S1 are likely to be small. Current controversies over myosin head structure are discussed in light of this result.     

Refined model of the 10S conformation of smooth muscle myosin by cryo-electron microscopy 3D image reconstruction

The actin-activated ATPase activity of smooth muscle myosin and heavy meromyosin (smHMM) is regulated by phosphorylation of the regulatory light chain (RLC). Complete regulation requires two intact myosin heads because single-headed myosin subfragments are always active. 2D crystalline arrays of the 10S form of intact myosin, which has a dephosphorylated RLC, were produced on a positively charged lipid monolayer and imaged in 3D at 2.0 nm resolution by cryo-electron microscopy of frozen, hydrated specimens. An atomic model of smooth muscle myosin was constructed from the X-ray structures of the smooth muscle myosin motor domain and essential light chain and a homology model of the RLC was produced based on the skeletal muscle S1 structure. The initial model of the 10S myosin, based on the previous reconstruction of smHMM, was subjected to real space refinement to obtain a quantitative fit to the density. The smHMM was likewise refined and both refined models reveal the same asymmetric interaction between the upper 50 kDa domain of the "blocked" head and parts of the catalytic, converter domains and the essential light chain of the "free" head observed previously. This observation suggests that this interaction is not simply due to crystallographic packing but is enforced by elements of the myosin heads. The 10S reconstruction shows additional alpha-helical coiled-coil not seen in the earlier smHMM reconstruction, but the location of one segment of S2 is the same in both.     

Proteolysis of smooth muscle myosin by Staphylococcus aureus protease: preparation of heavy meromyosin and subfragment 1 with intact 20 000-dalton light chains

The proteolysis of gizzard myosin by Staphylococcus aureus protease produces both heavy meromyosin and subfragment 1 in which the 20 000-dalton light chains are intact, and conditions are suggested for the preparation of each. Cleavage of the myosin heavy chain to produce subfragment 1 is dependent on the myosin conformation. Proteolysis of myosin in the 10S conformation yields predominantly heavy meromyosin, and myosin in the 6S conformation yields mostly subfragment 1 and some heavy meromyosin. Two sites are influenced by myosin conformation, and these are located at approximately 68 000 and 94 000 daltons from the N-terminus of the myosin heavy chain. The latter site is thought to be located at the subfragment 1-subfragment 2 junction, and cleavage at this site results in the production of subfragment 1. The time courses of phosphorylation of both heavy meromyosin and subfragment 1 can be fit by a single exponential. The actin-activated Mg2+-ATPase activity of heavy meromyosin is markedly activated by phosphorylation of the 20 000-dalton light chains. From the actin dependence of Mg2+-ATPase activity the following values are obtained: for phosphorylated heavy meromyosin, Vmax approximately 5.6 s-1 and Ka (the apparent dissociation constant for actin) approximately 2 mg/mL; for dephosphorylated heavy meromyosin, Vmax approximately 0.2 s-1 and Ka approximately 7 mg/mL. The actin-activated ATPase activity of subfragment 1 is not influenced by phosphorylation, and Vmax and Ka for both the phosphorylated and dephosphorylated forms are 0.4 s-1 and 5 mg/mL, respectively.(ABSTRACT TRUNCATED AT 250 WORDS)     

A new model for the surface arrangement of myosin molecules in tarantula thick filaments

Three-dimensional reconstructions of the negatively stained thick filaments of tarantula muscle with a resolution of 50 A have previously suggested that the helical tracks of myosin heads are zigzagged, short diagonal ridges being connected by nearly axial links. However, surface views of lower contour levels reveal an additional J-shaped feature approximately the size and shape of a myosin head.We have modelled the surface array of myosin heads on the filaments using as a building block a model of a two-headed regulated myosin molecule in which the regulatory light chains of the two heads together form a compact head-tail junction. Four parameters defining the radius, orientation and rotation of each myosin molecule were varied. In addition, the heads were allowed independently to bend in a plane perpendicular to the coiled-coil tail at three sites, and to tilt with respect to the tail and to twist at one of these sites. After low-pass filtering, models were aligned with the reconstruction, scored by cross-correlation and refined by simulated annealing.Comparison of the geometry of the reconstruction and the distance between domains in the myosin molecule narrowed the choice of models to two main classes. A good match to the reconstruction was obtained with a model in which each ridge is formed from the motor domain of a head pointing to the bare zone together with the head-tail junction of a neighbouring molecule. The heads pointing to the Z-disc intermittently occupy the J-position. Each motor domain interacts with the essential and regulatory light chains of the neighbouring heads. A near-radial spoke in the reconstruction connecting the backbone to one end of the ridge can be identified as the start of the coiled-coil tail.     

Molecular modeling of averaged rigor crossbridges from tomograms of insect flight muscle

Electron tomography, correspondence analysis, molecular model building, and real-space refinement provide detailed 3-D structures for in situ myosin crossbridges in the nucleotide-free state (rigor), thought to represent the end of the power stroke. Unaveraged tomograms from a 25-nm longitudinal section of insect flight muscle preserved native structural variation. Recurring crossbridge motifs that repeat every 38.7 nm along the actin filament were extracted from the tomogram and classified by correspondence analysis into 25 class averages, which improved the signal to noise ratio. Models based on the atomic structures of actin and of myosin subfragment 1 were rebuilt to fit 11 class averages. A real-space refinement procedure was applied to quantitatively fit the reconstructions and to minimize steric clashes between domains introduced during the fitting. These combined procedures show that no single myosin head structure can fit all the in situ crossbridges. The validity of the approach is supported by agreement of these atomic models with fluorescent probe data from vertebrate muscle as well as with data from regulatory light chain crosslinking between heads of smooth muscle heavy meromyosin when bound to actin.     

Fluorescence anisotropy of labeled F-actin: influence of divalent cations on the interaction between F-actin and myosin heads

The interaction between F-actin and soluble proteolytic fragments of myosin, heavy meromyosin and myosin subfragment 1 without ATP, has been studied by measuring the static anisotropy and the transient anisotropy decay of the fluorescent chromophore N-(iodoacetyl)-N'-(5-sulfo-1-naphthyl) ethylenediamine bound to F-actin. In the presence of Ca2+ ions, the mobility of the chromophore was strongly decreased by adding heavy meromyosin or myosin subfragment 1, and this conformation change of F-actin showed a strong cooperativity; that is, a very small amount of myosin heads induced the maximum anisotropy change. On the other hand, in the presence of Mg2+ ions, the addition of a small amount of myosin subfragment 1 or of heavy meromyosin increased the mobility of labeled F-actin that reached a maximum at a molar ratio of about 1/25 or 1/50, respectively. With further addition of myosin heads, the mobility of the labeled actin decreased. From these studies, one concludes that F-actin undergoes a conformation change by interacting with myosin heads, which depends on the nature of the divalent cations present in the solution.     

Structure of the myosin head in solution and the effect of light chain 2 removal.

Structural properties of rabbit skeletal myosin head (S1) and the influence of the DTNB light chain (LC2) on the size and shape of myosin heads in solution were investigated by small angle x-ray scattering. The LC2 deficient myosin head, S1 (-LC2), and the S1 containing LC2 light chain, S1 (+LC2) were studied in parallel. The respective values of the radius of gyration were found to be (40.2 +/- 0.5) A and (46.7 +/- 1) A, while the maximum dimension was (190 +/- 15) A for both species. The large difference between the two Rg values suggest that LC2 is located close to one extremity of the myosin head, in agreement with most electron microscopy observations. All models derived from the x-ray scattering pattern of the native myosin head share a common overall morphology, showing two main regions, an asymmetric globular portion which tapers smoothly into a thinner domain of roughly equivalent length making an angle of approximately 60 degrees, with a contour length of approximately 210 A.     

Shape and flexibility of the myosin molecule

Molecules of rabbit skeletal myosin have been examined in the electron microscope after drying at low temperature from solutions containing ethylene glycol or glycerol and rotary-shadowing with platinum. Analysis of the structure has been assisted by stereo-photography. While the general appearance, two heads attached to a long tail, is similar to that described by Slayter & Lowey (1967), more detail about the shape and size of the heads can be discerned and new information has been obtained about the flexibility of the tail and the head-tail junction.The heads are 190 Å long and wider at their ends than near the junction with the tail; the shape resembles that of a pear. The length is appreciably greater than the generally accepted value for subfragment 1, the proteolytic fragment of myosin. The heads are flexibly attached to the tail and can assume a wide range of tilt angles.Because the point where the two heads join the tail can be identified, the length of the tail, 1560 (±50) Å, can be measured more accurately than formerly. While all parts of the tail are somewhat flexible, sharp bends often occur at a well-defined site 430 Å from the head-tail junction. The demonstration of hinges at the head-tail junction and in the tail provides strong support for H. E. Huxley's (1969) hypothesis for the mechanism of muscle contraction.     

Phosphorylation-dependent structural changes in the regulatory light chain domain of smooth muscle heavy meromyosin.

Smooth muscle heavy meromyosin, a double-headed proteolytic fragment of myosin lacking the COOH-terminal two-thirds of the tail, has been shown previously to be regulated by phosphorylation. To examine phosphorylation-dependent structural changes near the head-tail junction, we prepared five well regulated heavy meromyosins containing single-cysteine mutants of the human smooth muscle regulatory light chain labeled with the photocross-linking reagent, benzophenone-iodoacetamide. For those mutants that generated cross-links, only one type of cross-linked species was observed, a regulatory light chain dimer. Irradiated mutants fell into two classes. First, for Q15C, A23C, and wild type (Cys-108), a regulatory light chain dimer was formed for dephosphorylated but not thiophosphorylated heavy meromyosin. These data provide direct chemical evidence that in the dephosphorylated state, Gln-15, Ala-23, and Cys-108 on one head are positioned near (within 8.9 A) the regulatory light chain of the partner head and that thiophosphorylation abolishes proximity. This behavior was also observed for the Q15C mutant on a truncated heavy meromyosin lacking both catalytic domains. For the actin-heavy meromyosin complex, cross-links were formed in both de- and thiophosphorylated states. S59C and T134C mutants were in a second mutant class, where regulatory light chain dimers were not detected in dephosphorylated or thiophosphorylated heavy meromyosin, suggesting positions outside the region of interaction of the regulatory light chains.     

Functional role of the C-terminal domain of smooth muscle myosin light chain kinase on the phosphorylation of smooth muscle myosin

Smooth muscle myosin light chain kinase (MLCK) is known to bind to thin filaments and myosin filaments. Telokin, an independently expressed protein with an identical amino acid sequence to that of the C-terminal domain of MLCK, has been shown to bind to unphosphorylated smooth muscle myosin. Thus, the functional significance of the C-terminal domain and the molecular morphology of MLCK were examined in detail. The C-terminal domain was removed from MLCK by alpha-chymotryptic digestion, and the activity of the digested MLCK was measured using myosin or the isolated 20-kDa light chain (LC20) as a substrate. The results showed that the digestion increased K(m) for myosin 3-fold whereas it did not change the value for LC20. In addition, telokin inhibited the phosphorylation of myosin by MLCK by increasing K(m) but only slightly increased K(m) for LC20. Electron microscopy indicated that MLCK was an elongated molecule but was flexible so as to form folded conformations. MLCK was crosslinked to unphosphorylated heavy meromyosin with 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide in the absence of Ca(2+)/calmodulin (CaM), and electron microscopic observation of the products revealed that the MLCK molecule bound to the head-tail junction of heavy meromyosin. These results suggest that MLCK binds to the head-tail junction of unphosphorylated myosin through its C-terminal domain, where LC20 can be promptly phosphorylated through its catalytic domain following the Ca(2+)/CaM-dependent activation.     

New method to prepare single-headed heavy meromyosin with high purity and a high yield

We have developed a new method to prepare single-headed heavy meromyosin with high purity and a high yield. To examine whether the two heads on the same myosin molecule work cooperatively or not, it is important to prepare pure single-headed heavy meromyosin. Myosin was extracted from myofibrils treated with a solution containing CyDTA, a strong divalent cation chelator. CyDTA treatment was essential to the production of sHMM. Then such myosin was digested with chymotrypsin in the presence of divalent cations at high ionic strength. Crude sHMM was separated from double-headed HMM by affinity chromatography using an ADP-column. Contaminating S1 was removed by gel filtration. Heavy chain of sHMM obtained by the present method had no nick. Purified sHMM showed normal EDTA-ATPase and Ca-ATPase. It interacted with thin filament and its ATPase was activated by actin normally.     

Shape of the myosin head in the rigor complex. Three-dimensional image reconstruction of the actin-tropomyosin-heavy meromyosin complex

The structure of the actin-tropomyosin-heavy meromyosin rigor complex was studied by image analysis of electron micrographs. The arrowhead of the rigor complex has a whisker-like structure with a dense turning point at the "barb" of the arrowhead. The neck region of the myosin head in the reconstructed three-dimensional image is present in the area corresponding to the dense point. It is concluded that at least one extra-thin area contributes to the neck region, and that the two heads in the heavy meromyosin molecule join a double helical rope beyond the end of the large head (G in this study). (This is different from previous interpretations). It is also concluded that the heavy meromyosin has a short bent part near the head/rod junction in the rigor complex.     

Skip residues correlate with bends in the myosin tail

Sharp bends have previously been observed in the tail of the skeletal myosin molecule at well-defined positions 44, 75 and 135 nm from the head-tail junction, and in vertebrate smooth myosin at two positions about 45 and 96 nm from this junction. The amino acid sequence of the heavy chain does not straightforwardly account for such bending on the original model of the tail in which an invariant proline residue is present at the head-tail junction and the repeating seven amino acid pattern of hydrophobic residues lies entirely in the tail. Recently, a revised model has been proposed by Rimm et al. in which the first seven to eight heptads lie in the heads. It is shown here that with this model the observed bends in the tail of skeletal myosin coincide with three of the four additional (skip) residues that interrupt the heptad repeat. It is concluded that the skip residues, by causing localized instability of the coiled-coil, are responsible for the bends. Smooth myosin lacks the second of these skip residues explaining the absence of a bend at 75 nm.     

Two-headed binding of the unphosphorylated nonmuscle heavy meromyosin.ADP complex to actin

The enzymatic and motor function of smooth muscle and nonmuscle myosin II is activated by phosphorylation of the regulatory light chains located in the head portion of myosin. Dimerization of the heads, which is brought about by the coiled-coil tail region, is essential for regulation since single-headed fragments are active regardless of the state of phosphorylation. Utilizing the fluorescence signal on binding of myosin to pyrene-labeled actin filaments, we investigated the interplay of actin and nucleotide binding to thiophosphorylated and unphosphorylated recombinant nonmuscle IIA heavy meromyosin constructs. We show that both heads of either thiophosphorylated or unphosphorylated heavy meromyosin bind very strongly to actin (K(d) < 10 nM) in the presence or absence of ADP. The heads have high and indistinguishable affinities for ADP (K(d) around 1 microM) when bound to actin. These findings are in line with the previously observed unusually loose coupling between nucleotide and actin binding to nonmuscle myosin IIA subfragment-1 (Kovács et al. (2003) J. Biol. Chem. 278, 38132.). Furthermore, they imply that the structure of the two heads in the ternary actomyosin-ADP complex is symmetrical and that the asymmetrical structure observed in the presence of ATP and the absence of actin in previous investigations (Wendt et al. (2001) Proc. Natl. Acad. Sci. U.S.A. 98, 4361) is likely to represent an ATPase intermediate that precedes the actomyosin-ADP state.     

Coiled-coil unwinding at the smooth muscle myosin head-rod junction is required for optimal mechanical performance

Myosin II has two heads that are joined together by an alpha-helical coiled-coil rod, which can separate in the region adjacent to the head-rod junction (Trybus, K. M. 1994. J. Biol. Chem. 269:20819-20822). To test whether this flexibility at the head-rod junction is important for the mechanical performance of myosin, we used the optical trap to measure the unitary displacements of heavy meromyosin constructs in which a stable coiled-coil sequence derived from the leucine zipper was introduced into the myosin rod. The zipper was positioned either immediately after the heads (0-hep zip) or following 15 heptads of native sequence (15-hep zip). The unitary displacement (d) decreased from d = 9.7 +/- 0.6 nm for wild-type heavy meromyosin (WT HMM) to d = 0.1 +/- 0.3 nm for the 0-hep zip construct (mean +/- SE). Native values were restored in the 15-hep zip construct (d = 7.5 +/- 0.7 nm). We conclude that flexibility at the myosin head-rod junction, which is provided by an unstable coiled-coil region, is essential for optimal mechanical performance.     

A spin-label study of phosphatidylcholine exchange protein. Regulation of the activity by phosphatidylserine and calcium ion.

The effects of the divalent cations Mg2+, Mn2+ and Ca2+ on the Brownian rotational motion of fluorescently labeled myosin, heavy meromyosin and myosin subfragment-1 were measured by the method of time-resolved fluorescence depolarization. When Mg2+ was added to solutions of myosin or heavy meromyosin and EDTA, their rotational mobility increased. Ca2+ had no effect. Mn2+ increased the mobility of heavy meromyosin but decreased that of myosin. None of these divalent cations effected the mobility of subfragment-1. The binding of heavy meromyosin to actin was affected very little by Mg2+ or EDTA over a wide range of conditions. Divalent cations appear to change the swivel about which the heads of myosin rotate, presumably by binding to light chain 2 (also called DTNB light chain). However, the heads are still able to bind actin in nearly the same way whether Mg2+ is present or not. The concentration of free Mg2+ for the mid-point of the change in heavy meromyosin mobility is in good agreement with that for EDTA activation of ATPase activity. This suggests that EDTA activation is due to removal of Mg2+ bound to myosin itself.     

Low-resolution structures of proteins in solution retrieved from X-ray scattering with a genetic algorithm.

Small-angle x-ray solution scattering (SAXS) is analyzed with a new method to retrieve convergent model structures that fit the scattering profiles. An arbitrary hexagonal packing of several hundred beads containing the problem object is defined. Instead of attempting to compute the Debye formula for all of the possible mass distributions, a genetic algorithm is employed that efficiently searches the configurational space and evolves best-fit bead models. Models from different runs of the algorithm have similar or identical structures. The modeling resolution is increased by reducing the bead radius together with the search space in successive cycles of refinement. The method has been tested with protein SAXS (0.001 < S < 0.06 A(-1)) calculated from x-ray crystal structures, adding noise to the profiles. The models obtained closely approach the volumes and radii of gyration of the known structures, and faithfully reproduce the dimensions and shape of each of them. This includes finding the active site cavity of lysozyme, the bilobed structure of gamma-crystallin, two domains connected by a stalk in betab2-crystallin, and the horseshoe shape of pancreatic ribonuclease inhibitor. The low-resolution solution structure of lysozyme has been directly modeled from its experimental SAXS profile (0.003 < S < 0.03 A(-1)). The model describes lysozyme size and shape to the resolution of the measurement. The method may be applied to other proteins, to the analysis of domain movements, to the comparison of solution and crystal structures, as well as to large macromolecular assemblies.     

The radius of gyration of native and reductively methylated myosin subfragment-1 from neutron scattering.

Reductive methylation of nearly all lysine groups of myosin subfragment-1 (S1) was required for crystallization and solution of its structure at atomic resolution. Possible effects of such methylation on the radius of gyration of chicken skeletal muscle myosin S1 have been investigated by using small-angle neutron scattering. In addition, we have investigated the effect of MgADP.Vi, which is thought to produce an analog of the S1.ADP.Pi state, on the S1 radius of gyration. We find that although methylation of S1, with or without SO42- ion addition, does not significantly alter the structure, addition of ADP plus vanadate does decrease the radius of gyration significantly. The S1 crystal structure predicts a radius of gyration close to that measured here by neutron scattering. These results suggest that the overall shape by crystallography resembles nucleotide-free S1 in solution. In order to estimate the effect of residues missing from the crystal structure, the structure of missing loops was estimated by secondary-structure prediction methods. Calculations using the complete crystal structure show that a simple closure of the nucleotide cleft by a rigid-body torsional rotation of residues (172-180 to 670) around an axis running along the base of the cleft alone does not produce changes as large as seen here and in x-ray scattering results. On the other hand, a rigid body rotation of either the light-chain binding domain (767 to 843 plus light chains) or of a portion of 20-kDa peptide plus this domain (706 to 843 plus light chains) is more readily capable of producing such changes.     

The binding of myosin heads on heavy meromyosin and assembled myosin to actin in the presence of nucleotides. Measurements by the proteolytic rates method

The initial rates of tryptic digestion at the 50/20-kDa junction in myosin and myosin subfragment 1 were determined for the free proteins and their complexes with actin in the presence and absence of MgATP. The proteolytic reactions were carried out at 24 degrees C and under ionic strength conditions (mu) adjusted to 35, 60, and 130 mM. The percentages of myosin heads and myosin subfragment 1 bound to actin in the presence of MgATP were calculated from the rates of proteolysis for each set of digestion experiments. In all cases, the myosin heads in the synthetic filaments showed greater binding to actin than myosin subfragment 1. This binding difference was most prominent (3-fold) at mu = 130 mM. The binding of heavy meromyosin (HMM) to actin in the presence of MgADP was measured at 4 degrees C by ultracentrifugation and the proteolytic rates methods. Ultracentrifugation experiments determined the fraction of HMM molecules bound to actin in the presence of MgADP, whereas the proteolytic measurements yielded the information on the fraction of HMM heads bound to actin. Taken together, these measurements show that a significant fraction of HMM is bound to actin with only one head in the presence of MgADP under ionic conditions of 180 and 280 mM.     

Identical behavior of the two active sites of myosin with respect to trinitrophenylation.

Myosin and its active subfragments were trinitrophenylated under conditions in which mainly the active site(s) was modified. Proteins modified at the active site(s) could be separated by affinity chromatography on agarose-ATP columns. By two independent methods, ATPase activity measurements and analysis of elution patterns on agarose-ATP columns, it was shown that the introduction of two trinitrophenyl groups per myosin or one per heavy meromyosin subfragment 1 molecule is responsible for the remarkable change in the ATPase activities. Heavy meromyosin subfragment 1 prepared from trinitrophenylated myosin retained the original degree of trinitrophenylation per "active head." The kinetic constant of trinitrophenylation of the epsilon-amino group of lysine at the active site was found to be 2000 S-1-M-1, whereas a much smaller constant of 2.2 S-1-M-1 was obtained for the trinitrophenylation of the unessential lysyl residues of myosin. By using affinity chromatography, we could follow the formation of mono- and ditrinitrophenyl myosin. The amounts of these myosin derivatives at various extents of the reaction corresponded approximately to the calculated amounts, assuming a random and independent trinitrophenylation of the two myosin "heads." It is concluded that in each of the two heads of myosin there is one ATPase active site and these two sites behave in an identical manner with respect to trinitrophenylation.