Electron microscopy and image analysis of myosin filaments from scallop striated muscle

Thick filaments have been isolated from the striated adductor muscle of the scallop and examined by electron microscopy after negative staining. Many filaments appear intact, and reveal a centrally located bare-zone and a well-defined helical surface array of myosin crossbridges characterized by a 145 A axial period and prominent helical tracks of pitch 480 A. Heavy-metal shadowing shows that these helices are right-handed. A small perturbation of alternate crossbridge levels produces an axial period of 290 A, which is most prominent in a region on either side of the bare-zone. Image analysis reveals that the crossbridge array has 7-fold rotational symmetry, one of the possibilities suggested by earlier X-ray diffraction studies of native filaments in scallop muscle. A low-resolution three-dimensional reconstruction shows elongated surface projections ("crossbridges") that probably represent unresolved pairs of myosin heads. They run almost parallel to the filament surface, but are slewed slightly from the axis so that they lie along the right-handed helical tracks of pitch 480 A. The connection to the filament backbone probably occurs at the end of the crossbridges nearer the bare-zone; thus, their sense of tilt appears to be opposite to that of rigor attachment to actin. The 290 A period arises from a different distribution of crossbridge density at alternate levels; in addition, there are weak connections between the top of one crossbridge and the bottom of the next, 145 A away. The prominence of the 290 A period near the bare-zone suggests that anti-parallel molecular interactions are mainly responsible for this perturbation.     

Dynamic light-scattering study of synthetic myosin filaments

Synthetic myosin filaments of rabbit were prepared. Electron microscopy showed that the number-average length (L_n = 470 nm) and sharpness in length distribution (L_w/L_n = 1.03₆) were independent of ionic strengths of 134, 74, and 44 mM, whereas the number ratio of M-filaments (about 15 nm in diameter at the bare zone) to m-filaments (about 10 nm) strongly depended on ionic strength (IS); the major filaments were M-filaments at IS = 134 mM, m-filaments at IS = 74 mM, and almost exclusively m-filaments at IS = 44 mM. Dynamic light scattering showed that the change in diameter with the change in ionic strength by 2-h dialysis was reversible. Combination of dynamic light scattering and sedimentation studies suggested a dynamic equilibrium between M- and m-filaments. Dynamic light-scattering spectra at IS = 134 and 74 mM could be analyzed by a theory for rigid rods, whereas those at IS = 44 mM only by introducing semiflexibility of filaments; m-filaments are more flexible at IS = 44 than at 74 mM.     

Structural studies of synthetic filaments prepared from column-purified myosin.

Synthetic filaments prepared from column-purified rabbit skeletal myosin by slow dialysis exhibit characteristic bipolar organization and 14-nm axial subunit spacing. Backbone substructure can be discerned in high resolution micrographs in the form of striations of 3--4-nm width and slight angular tilt from the direction of the filament axis. Filament backbone diameters vary over the population, although remaining relatively constant for a single filament. Approximately 25% of the filaments appear poorly stained and frayed, which may be due to collapse on the electron microscope grid. Optical diffraction studies reveal a 43-nm axial repeat as well as the 14.3-nm subunit repeat, indicating a structural homology with natural filaments. A model for synthetic filament aggregation is presented that is consistent with observations of backbone diameter variation, absence of bare zones, and the presence of fraying filaments.     

Electron microscopy of cross-linked scallop myosin

The N-terminal regions of the regulatory light chains on the two heads of scallop myosin can be cross-linked to one another. Electron microscopy of cross-linked myosin molecules, and of dimers of myosin subfragment-1 produced by digesting them with papain, shows that the site of cross-linking is very close to the head-rod junction.     

Diffuse X-ray scatter from myosin heads in oriented synthetic filaments.

X-ray results are presented concerning the structural state of myosin heads of synthetic filaments in threads. These were made from purified rabbit skeletal muscle myosin and studied by x-ray diffraction and electron microscopy by Cooke et al. (Cooke, P. H., E. M. Bartels, G. F. Elliott, and R. A. Hughes, 1987, Biophys. J., 51:947-957). X-ray patterns show a meridional peak at a spacing of 14.4 nm. We concentrate here on the only other feature of the axial pattern: this is a central region of diffuse scatter, which we find to be similar to that obtained from myosin heads in solution (Mendelson, R. A., K. M. Kretzschmar, 1980, Biochemistry, 19:4103-4108). This means that the myosin heads have very large random displacements in all directions from their average positions, and that they are practically randomly oriented. The myosin heads do not contribute to the 14.4-nm peak, which must come entirely from the backbone. Comparison with x-ray data from the unstriated Taenia coli muscle of the guinea pig indicates that in this muscle at least 75% of the diffuse scatter comes from disordered myosin heads. The results confirm that the diffuse scatter in x-ray patterns from specimens that contain myosin filaments can yield information about the structural behavior of the myosin heads.     

Effect of pH on the cross-bridge arrangement in synthetic myosin filaments.

Synthetic thick filaments were cross-linked with dimethyl suberimidate at various pH values over the range pH 6.8---8.3. The rate of cross-linking myosin heads to the thick filament surface decreases significantly over a narrow pH range (7.4--8.0) despite the fact that the rate of the chemical reaction (amidination of lysine side chains) shows a positive pH dependence. The fall in rate cannot be ascribed to dissociation of the filament during the cross-linking reaction since the sedimentation boundary of the cross-linked filament (pH 8.3) remains unaltered in the presence of high salt (0.5 M). The decreased rate of cross-linking is also not caused by a shift in reactivity of a small number of highly reactive lysine groups, since the time course of cross-linking (pH 7.2) is unaffected by preincubation with a monofunctional imidate ester. Our results suggest that the heads of the myosin molecules move away from the thick filament surface at alkaline pH but are held close to the surface at neutral pH.     

Purification of uterine myosin and synthetic filament formation

Rabbit uterine myosin was purified by DEAE-Sephadex column chromatography. The purified myosin was shown to be free from contamination with actin or other impurities by sodium dodecyl sulfate gel electrophoresis. It was also shown to have two light chains with molecular weights of 22,000 and 17,000. The C protein normally found in crude, rabbit skeletal muscle myosin was not found in crude, rabbit uterine myosin.On reducing the ionic strength of a solution of rabbit uterine myosin, the myosin molecules first aggregated to form short, tapered bipolar filaments with bare zones. These were observed in the presence or absence of 10 mm-magnesium. These filaments ranged in length from 0.3 μm to 0.6 μm. On reaching 0.1 m-KCl, and only if 10 mm-magnesium was present, the filaments grew in length by linear overlap of the tapered bipolar filaments and obliteration of the bare zone regions. These filaments ranged in length from 0.7 μm to 1.2 μm.     

Frictional properties and molecular weight of native and synthetic myosin filaments from vertebrate skeletal muscle.

1. The molecular weights of a series of synthetic myosin filaments have been measured, using the transport-concentration dependence theory of Rowe, A.J. [Biopolymers, 1977, 16, 2595--2611]. It is shown that for preparations of narrow length distribution (0.60--0.77 micrometer), N, the number of myosin molecules/14.3 nm varies between 3 and 6. 2. The reduced specific viscosity of synthetic myosin filaments has been measured as a function of both concentration and shear rate. From the concentration dependence at zero rate of shear, a value for the "swelling" of the filaments Vs/-v = 2.3 has been calculated. 3. The frictional coefficient of synthetic myosin filaments has been shown to be anomalously but reproducibly high, as compared to that of prolate ellipsoids of the same length and mass. This additional frictional drag has been numerically characterised by a "frictional increment", fi = 1.76 +/- 0.11. 4. A procedure has been devised whereby for any elongated structure which can be assumed to show the same (or other known) fi value, the molecular weight can be estimated from s0 (extrapolated sedimentation coefficient) and 2b (length) alone. 5. An s0 value for natural A-filaments, isolated from rabbit psoas muscle, has been determined by the active enzyme centrifugation technique. From this value, s0 = 132 +/- 3 S, a molecular weight of 1.20 . 10(8) has been computed by the new procedure, for preparations of average length 1.27 micrometer. 6. Contingent upon the validity of the assumptions used (see 4 above) the N value is computed as 3.1 +/- 0.2, consistent with the native, fully intact A-filament having three-fold symmetry, containing 294 myosin molecules, and having a molecular weight based upon myosin and C-protein of 1.31 . 10(8).     

Truncation of vertebrate striated muscle myosin light chains disturbs calcium-induced structural transitions in synthetic myosin filaments

Electron microscopy and negative staining techniques have been used to show that the proteolytic removal of 13 amino acids from the N-terminus of essential light chain 1 and 19 amino acids from the N-terminus of the regulatory light chain of rabbit skeletal and cardiac muscle myosins destroys Ca(2+)-induced reversible movement of subfragment-2 (S2) with heads (S1) away from the backbone of synthetic myosin filaments observed for control assemblies of the myosin under near physiological conditions. This is the direct demonstration of the contribution of the S2 movement to the Ca(2+)-sensitive structural behavior of rabbit cardiac and skeletal myosin filaments and of the necessity of intact light chains for this movement. In muscle, such a mobility might play an important role in proper functioning of the myosin filaments. The impairment of the Ca(2+)-dependent structural behavior of S2 with S1 on the surface of the synthetic myosin filaments observed by us may be of direct relevance to some cardiomyopathies, which are accompanied by proteolytic breakdown or dissociation of myosin light chains.     

The actomyosin ATPase of synthetic myosin minifilaments, filaments, and heavy meromyosin

The actin-activated ATPase activities of myosin minifilaments and heavy meromyosin are similar at high actin concentrations. Under low ionic strength conditions, the minifilaments in Tris citrate buffer yield the same maximal turnover rate (Vmax) and apparent dissociation constant of actin from myosin (Kapp) as heavy meromyosin in standard low salt conditions. The time course of actin-activated ATP hydrolysis of minifilaments is similar to that observed for standard myosin preparations. Depending on the exact protein composition of the assay mixture, either the ATPase activity declines continuously with time, or is accelerated at the onset of superprecipitation. In analogy with myosin filaments, the ATPase of minifilaments shows a biphasic dependence on actin concentration. Super-precipitation of minifilaments follows a well resolved clearing phase during which their structural integrity appears to be fully preserved. These results indicate that minifilaments or similar small assemblies of myosin can fulfill contractile functions.     

Flexibility of Acanthamoeba myosin rod minifilaments.

Previous electric birefringence experiments have shown that the actin-activated Mg2+-ATPase activity of Acanthamoeba myosin II correlates with the ability of minifilaments to cycle between flexible and stiff conformations. The cooperative transition between conformations was shown to depend on Mg2+ concentration, on ATP binding, and on the state of phosphorylation of three serines in the C-terminal end of the heavy chains. Since the junction between the heavy meromyosin (HMM) and light meromyosin (LMM) regions is expected to disrupt the alpha-helical coiled-coil structure of the rod, this region was anticipated to be the flexible site. We have now cloned and expressed the wild-type rod (residues 849-1509 of the full-length heavy chain) and rods mutated within the junction in order to test this. The sedimentation and electric birefringence properties of minifilaments formed by rods and by native myosin II are strikingly similar. In particular, the Mg2+-dependent flexible-to-stiff transitions of native myosin II and wild-type rod minifilaments are virtually superimposable. Mutations within the junction between the HMM and LMM regions of the rod modulate the ability of Mg2+ to stabilize the stiff conformation. Less Mg2+ is required to induce minifilament stiffening if proline-1244 is replaced with alanine. Deleting the entire junction region (25 amino acids) results in a even greater decrease in the Mg2+ concentration necessary for the transition. The HMM-LMM junction does indeed seem to act as a Mg2+-dependent flexible hinge.