A model for length-regulation in thick filaments of vertebrate skeletal myosin.

A mechanism for length regulation in the parallel-packed section of the thick filament is proposed. It is based on experiments done on synthetic, mini- and native filaments, and its primary purpose is to explain the physical basis of the kinetic mechanism for the assembly of synthetic thick filaments from myosin alone. Kinetically, length is regulated by a dissociation rate constant that increases exponentially as the filament grows bi-directionally from its center. Growth ceases at the point of equilibrium between invariant on and length-dependent off rates. The three subfilaments structure of the parallel-packed region of the thick filament is fundamental to the proposed scheme. The intra-subfilament bonding is strong and predominantly ionic in character, whereas the inter-subfilament bonding is relatively weak. These strong and weak interactions participate directly in the strictly sequential mechanism of assembly of dimer subunit observed in the kinetics. A third domain, independent of the sequential mechanism, consists of opposing negative charges on the subfilament surface, juxtaposed at or close to the thick filament axis. The weak and repulsive domains are additively coupled to each other through the rigidity in the subfilaments. Length regulation occurs through the repulsive component rising in intensity more rapidly with length than the initially stronger positive interactions. Growth ceases at the point where the repulsive interactions weaken the attractive interactions to the extent that equilibrium is established between head-to-tail dimer subunit and its binding sites at the tips of the arms of thick filament.(ABSTRACT TRUNCATED AT 250 WORDS)     

Tryptophan pyrrolase in haem regulation. The mechanism of the opposite effects of tryptophan on rat liver 5-aminolaevulinate synthase activity and the haem saturation of tryptophan pyrrolase.

The self-assembly of myosin monomer into thick filament occurs via a two-step mechanism. At first a pair of myosin monomers reacts to form a parallel dimer; the dimer in turn adds to the filament ends at a rate that is independent of filament length. The rate of the dissociation reaction on the other hand is length-dependent. The 'off' rate constant has been shown to increase exponentially by a factor of 500 as the filament grows from the bare-zone out to its full length. The length of the filament is thus kinetically controlled; myosin is added to the filament at a fixed rate, whereas the dissociation rate increases to a point where equilibrium is established and the filament ceases to grow. The structural implications implicit in the mechanism are discussed.     

Periodically arranged interactions within the myosin filament backbone revealed by mechanical unzipping

Numerous types of biological motion are driven by myosin thick filaments. Although the exact structure of the filament backbone is not known, it has long been hypothesized that periodically arranged charged regions along the myosin tail are the main contributors to filament stability. Here we provide a direct experimental test of this model by mechanically pulling apart synthetic myosin thick filaments. We find that unzipping is accompanied by broad force peaks periodically spaced at 4-, 14- and 43-nm intervals. This spacing correlates with the repeat distance of highly charged regions along the myosin tail. Lowering ionic strength does not change force-peak periodicity but increases the forces necessary for unzipping. The force peaks are partially reversible, indicating that the interactions are rapidly re-established upon mechanical relaxation. Thus, the zipping together of myosin tails via consecutive formation of periodically spaced bonds may be the underlying mechanism of spontaneous thick filament formation.     

Kinetics of the structural transition of muscle thin filaments observed by fluorescence resonance energy transfer

Fluorescence resonance energy transfer showed that troponin-I changes the position on an actin filament corresponding to three states (relaxed, closed, and open) of the thin filament (Hai et al. (2002) J. Biochem. 131, 407-418). In combination with the stopped-flow method, fluorescence resonance energy transfer between probes attached to position 1, 133, or 181 of troponin-I and Cys-374 of actin on reconstituted thin filaments was measured to follow the transition between three states of the thin filament. When the free Ca(2+) concentration was increased, the transition from relaxed to closed states occurred with a rate constant of approximately 500 s(-1). For the reverse transition, the rate constant was approximately 60 s(-1). When myosin subfragment-1 was dissociated from thin filaments in the presence of Ca(2+) by rapid mixing with ATP, the transition from open to closed states occurred with a single rate constant of approximately 300 s(-1). Light-scattering measurements showed that the ATP-induced myosin subfragment-1 dissociation occurred with a rate constant of approximately 900 s(-1). In the absence of Ca(2+), the transition from open to relaxed states occurred with two rate constants of approximately 400 and approximately 80 s(-1). These transition rates are fast enough to allow the spatial rearrangement of thin filaments to be involved in the regulation mechanism of muscle contraction.     

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.     

The structure of thick filaments on longitudinal sections of rabbit psoas muscle

By means of electron microscopy the longitudinal sections of chemically skinned fibres of rigorised rabbit psoas muscle have been examined at pH of rigorising solutions equal to 6, 7, 8 (I = 0.125) and ionic strengths equal to 0.04, 0.125, 0.34 (pH 7.0). It has been revealed that at pH 6.0 the bands of minor proteins localization in A-disks were seen very distinctly, while at pH 7.0 and I = 0.125 these bands can be revealed only by means of antibody labelling technique. At the ionic strength of 0.34 (pH 7.0) the periodicity of 14.3 nm in thick filaments was clearly observed, which was determined by packing of the myosin rods into the filament shaft and of the myosin heads (cross-bridges) on the filament surface. The number of cross-bridge rows in the filament equals 102. A new scheme of myosin cross-bridge distribution in thick filaments of rabbit psoas muscle has been suggested according to which two rows of cross-bridges at each end of a thick filament are absent. The filament length equals 1.64 +/- 0.01 micron. It has been shown that the length of thick filament as well as the structural organization of their end regions in rabbit psoas muscle and frog sartorius one are different.     

Assembly of thick filaments and myofibrils occurs in the absence of the myosin head

We investigated the importance of the myosin head in thick filament formation and myofibrillogenesis by generating transgenic Drosophila lines expressing either an embryonic or an adult isoform of the myosin rod in their indirect flight muscles. The headless myosin molecules retain the regulatory light-chain binding site, the alpha-helical rod and the C-terminal tailpiece. Both isoforms of headless myosin co-assemble with endogenous full-length myosin in wild-type muscle cells. However, rod polypeptides interfere with muscle function and cause a flightless phenotype. Electron microscopy demonstrates that this results from an antimorphic effect upon myofibril assembly. Thick filaments assemble when the myosin rod is expressed in mutant indirect flight muscles where no full-length myosin heavy chain is produced. These filaments show the characteristic hollow cross-section observed in wild type. The headless thick filaments can assemble with thin filaments into hexagonally packed arrays resembling normal myofibrils. However, thick filament length as well as sarcomere length and myofibril shape are abnormal. Therefore, thick filament assembly and many aspects of myofibrillogenesis are independent of the myosin head and these processes are regulated by the myosin rod and tailpiece. However, interaction of the myosin head with other myofibrillar components is necessary for defining filament length and myofibril dimensions.     

Effect of H-protein on the formation of myosin filaments and light meromyosin paracrystals

H-protein is a component of the thick filaments of skeletal myofibrils. Its effects on the assembly of myosin into filaments and on the formation of light meromyosin (LMM) paracrystals at low ionic strength have been investigated. H-protein reduced the turbidities of myosin filament and LMM paracrystal suspensions. Electron microscopic observation showed that the appearances of the filaments prepared in the presence and absence of H-protein were different. The filament length was not substantially changed by H-protein, but the diameter of the myosin filament was markedly reduced. H-protein bound to LMM and co-sedimented with it at low ionic strength upon centrifugation. Two types of paracrystals, spindle-shaped and sheet-like, were observed in LMM suspensions. H-protein altered the structure of the LMM paracrystals, especially the spindle-shaped ones. The thickness of the spindle-shaped paracrystals was reduced when H-protein was present during LMM paracrystal formation. On the other hand, periodic features along the long axis of the sheet-like paracrystals were retained even at high ratios of H-protein to LMM. However, there were fewer sheet-like paracrystals in the LMM suspensions containing H-protein than in the control. These results suggest that H-protein interferes with self-association of myosin molecule into filaments due to its binding to the tail portion of the myosin. However, H-protein does not have a length-determining effect on the formation of myosin filaments.     

Hydrostatic pressure studies of native and synthetic thick filaments: II. Native thick filaments from rabbit skeletal muscle

Native thick filaments isolated from freshly prepared rabbit psoas muscle were found to be resistant to pressure-induced dissociation. With increasing pressure application and release, a bimodal distribution of filament lengths was observed. The shorter filament length is associated with filament breakage at the center of the bare zone, while the longer length is associated with relatively intact filaments. Intact filaments and filament halves decrease in length by no more than 20% after exposure to and release of 14,000 psi. Bimodal distributions were not observed in equivalent experiments performed on filaments isolated from muscle glycerinated and stored at -20 degrees C for 6 months. Instead, filament dissociation proceeds linearly as a function of increasing pressure. Filaments prepared from muscle glycerinated and stored for 2 and 4 months exhibited pressure-induced behavior intermediate between the filaments prepared from fresh muscle and filaments prepared from muscle stored for 6 months. Since there appears to be no difference in the protein profiles of the various muscle samples, it is possible that stabilization of the native thick filament against hydrostatic pressure arises from trapped ions that are leached out over time.     

Cardiac Myosin Filaments are Maintained by Stochastic Protein Replacement

Myosin and myosin-binding protein C are exquisitely organized into giant filamentous macromolecular complexes within cardiac muscle sarcomeres, yet these proteins must be continually replaced to maintain contractile fidelity. The overall hypothesis that myosin filament structure is dynamic and allows for the stochastic replacement of individual components was tested in vivo, using a combination of mass spectrometry– and fluorescence-based proteomic techniques. Adult mice were fed a diet that marked all newly synthesized proteins with a stable isotope-labeled amino acid. The abundance of unlabeled and labeled proteins was quantified by high-resolution mass spectrometry over an 8-week period. The rates of change in the abundance of these proteins were well described by analytical models in which protein synthesis defined stoichiometry and protein degradation was governed by the stochastic selection of individual molecules. To test whether the whole myosin filaments or the individual components were selected for replacement, cardiac muscle was chemically skinned to remove the cellular membrane and myosin filaments were solubilized with ionic solutions. The composition of the filamentous and soluble fractions was quantified by mass spectrometry, and filament depolymerization was visualized by real-time fluorescence microscopy. Myosin molecules were preferentially extracted from ends of the filaments in the presence of the ionic solutions, and there was only a slight bias in the abundance of unlabeled molecules toward the innermost region on the myosin filaments. These data demonstrate for the first time that the newly synthesized myosin and myosin-binding protein C molecules are randomly mixed into preexisting thick filaments in vivo and the rate of mixing may not be equivalent along the length of the thick filament. These data collectively support a new model of cardiac myosin filament structure, with the filaments being dynamic macromolecular assemblies that allow for replacement of their components, rather than rigid bodies.     

Hydrostatic pressure studies of native and synthetic thick filaments: in vitro myosin aggregates at pH 7.0 with and without C-protein

Column-purified myosin at pH 7.0 will reproducibly aggregate into filaments of known average length and structure when dialyzed against a low ionic strength medium under controlled conditions. When exposed to increased hydrostatic pressure, followed by quick return to atmospheric pressure, the original filaments shorten linearly with increasing pressure; in addition, a second population of filaments is seen, presumably the result of reaggregation of myosin after release of pressure. This second population is about 0.5 microns long, bipolar, and about half the diameter of the original filaments. The number of these filaments, but not their physical characteristics, is a function of the shortening of the original filament population. Both the remnants of the original population and the new aggregates, once formed, are stable over time and at room temperature. The addition of C-protein to myosin solutions before filament preparation results in a filament population of slightly shorter length. When these filaments are exposed to increased hydrostatic pressure, they are more resistant to disaggregation than myosin filaments without C-protein. However, like the filaments prepared in the absence of C-protein, a second population of shorter, thinner filaments is visible after exposure to pressure.     

The binding of skeletal muscle C-protein to F-actin, and its relation to the interaction of actin with myosin subfragment-1.

C-protein is a component of thick filaments of skeletal muscle myofibrils. It is bound to the assembly of myosin tails that forms the filament backbone. We report here that C-protein can also bind to F-actin, with a limiting stoichiometry of approximately one C-protein molecule per 3 to 5 actin subunits and a dissociation constant in the micromolar range at ionic strength 0·07. The binding is not significantly affected by ATP, calcium ions or temperature, or by the presence of tropomyosin on the actin, but it is weakened by increasing ionic strength. Myosin subfragment-1 (S-1) competes with C-protein for binding to actin. In the absence of ATP, S-1 displaces nearly all bound C-protein from actin, while in the presence of ATP, C-protein inhibits the actin activation of S-1 ATPase. Although there is no direct evidence that interaction of C-protein with actin is physiologically significant, the lenght of the C-protein molecule is sufficient so that it could make contact with the thin filaments in muscle while remaining attached to the thick filaments.     

Structure-function correlation in airway smooth muscle adapted to different lengths

Airway smooth muscle is able to adapt and maintain a nearly constant maximal force generation over a large length range. This implies that a fixed filament lattice such as that found in striated muscle may not exist in this tissue and that plastic remodeling of its contractile and cytoskeletal filaments may be involved in the process of length adaptation that optimizes contractile filament overlap. Here, we show that isometric force produced by airway smooth muscle is independent of muscle length over a twofold length change; cell cross-sectional area was inversely proportional to cell length, implying that the cell volume was conserved at different lengths; shortening velocity and myosin filament density varied similarly to length change: increased by 69.4% ± 5.7 (SE) and 76.0% ± 9.8, respectively, for a 100% increase in cell length. Muscle power output, ATPase rate, and myosin filament density also have the same dependence on muscle cell length: increased by 35.4% ± 6.7, 34.6% ± 3.4, and 35.6% ± 10.6, respectively, for a 50% increase in cell length. The data can be explained by a model in which additional contractile units containing myosin filaments are formed and placed in series with existing contractile units when the muscle is adapted at a longer length. muscle contraction; myosin filaments; ATPase activity; electron microscopy     

Effects of phosphorylation by myosin light chain kinase on the structure of Limulus thick filaments

The results discussed in the preceding paper (Levine, R. J. C., J. L. Woodhead, and H. A. King. 1991. J. Cell Biol. 113:563-572.) indicate that A-band shortening in Limulus muscle is a thick filament response to activation that occurs largely by fragmentation of filament ends. To assess the effect of biochemical changes directly associated with activation on the length and structure of thick filaments from Limulus telson muscle, a dually regulated tissue (Lehman, W., J. Kendrick-Jones, and A. G. Szent Gyorgyi. 1973. Cold Spring Harbor Symp. Quant. Biol. 37:319-330.) we have examined the thick filament response to phosphorylation of myosin regulatory light chains. In agreement with the previous work of J. Sellers (1981. J. Biol. Chem. 256:9274-9278), Limulus myosin, incubated with partially purified chicken gizzard myosin light chain kinase (MLCK) and [gamma 32P]-ATP, binds 2 mol phosphate/mole protein. On autoradiographs of SDS-PAGE, the label is restricted to the two regulatory light chains, LC1 and LC2. Incubation of long (greater than or equal to 4.0 microns) thick filaments, separated from Limulus telson muscle under relaxing conditions, with either intact MLCK in the presence of Ca2+ and calmodulin, or Ca2(+)-independent MLCK obtained by brief chymotryptic digestion (Walsh, M. P., R. Dabrowska, S. Hinkins, and D. J. Hartshorne. 1982. Biochemistry. 21:1919-1925), causes significant changes in their structure. These include: disordering of the helical surface arrangement of myosin heads as they move away from the filament backbone; the presence of distal bends and breaks, with loss of some surface myosin molecules, in each polar filament half; and the production of shorter filaments and end-fragments. The latter structures are similar to those produced by Ca2(+)-activation of skinned fibers (Levine, R. J. C., J. L. Woodhead, and H. A. King. J. Cell Biol. 113:563-572). Rinsing experimental filament preparations with relaxing solution before staining restores some degree of order of the helical surface array, but not filament length. We propose that outward movement of myosin heads and thick filament shortening in Limulus muscle are responses to activation that are dependent on phosphorylation of regulatory myosin light chains. Filament shortening may be due, in large part, to breakage at the filament ends.     

Control of filament length by the regulatory light chains in skeletal and cardiac myosins

The possible role of the regulatory light chains (LC2) in in vitro assembly of rabbit skeletal and dog cardiac myosins was examined by formation of minifilaments and synthetic thick filaments. After LC2 was removed, the resulting myosin preparations exhibited little aggregation in 0.5 M KCl and 0.05 M potassium phosphate (pH 6.5). Minifilaments migrated as a single, hypersharp peak during sedimentation velocity, but electron microscopic analysis revealed a more destabilized structure for LC2-deficient minifilaments. Thick filaments were formed in buffers containing 0.15 M KCl and the following: 20 mM imidazole; 20 mM imidazole, 5 mM ATP; or 20 mM imidazole, 5 mM ATP, and 5 mM MgCl2, all at pH 7.0. Skeletal and cardiac myosin filaments formed in imidazole buffer alone were bipolar, tapered at both ends, and about 1.6 micron long. Removal of LC2 resulted in the formation of shorter thick filaments (1.2 micron long). This effect could be reversed by reassociation with LC2. Inclusion of ATP in the buffer disrupted the filament structure, resulting in irregular, short filaments (less than 0.6 micron); addition of both ATP and MgCl2 largely reversed the effects of ATP alone. In cardiac myosin filaments, the bare zone diameter increased from 16 nm as measured in control and LC2-recombined samples to 20 nm in LC2-deficient myosin assemblies. These results implicate LC2 in an active role in controlling synthetic thick filament length in both skeletal and cardiac muscles.     

Structure of the cross-striated adductor muscle of the scallop

The structure of the cross-striated adductor muscle of the scallop has been studied by electron microscopy and X-ray diffraction using living relaxed, glycerol-extracted (rigor), fixed and dried muscles. The thick filaments are arranged in a hexagonal lattice whose size varies with sarcomere length so as to maintain a constant lattice volume. In the overlap region there are approximately 12 thin filaments about each thick filament and these are arranged in a partially disordered lattice similar to that found in other invertebrate muscles, giving a thin-to-thick filament ratio in this region of 6:1.The thin filaments, which contain actin and tropomyosin, are about 1 μm long and the actin subunits are arranged on a helix of pitch 2 × 38.5 nm. The thick filaments, which contain myosin and paramyosin, are about 1.76 μm long and have a backbone diameter of about 21 nm. We propose that these filaments have a core of paramyosin about 6 nm in diameter, around which the myosin molecules pack. In living relaxed muscle, the projecting myosin heads are symmetrically arranged. The data are consistent with a six-stranded helix, each strand having a pitch of 290 nm. The projections along the strands each correspond to the heads of one or two myosin molecules and occur at alternating intervals of 13 and 16 nm. In rigor muscle these projections move away from the backbone and attach to the thin filaments.In both living and dried muscle, alternate planes of thick filaments are staggered longitudinally relative to each other by about 7.2 nm. This gives rise to a body-centred orthorhombic lattice with a unit cell twice the volume of the basic filament lattice.     

Assembly of smooth muscle myosin minifilaments: effects of phosphorylation and nucleotide binding

Small bipolar filaments, or "minifilaments," are formed when smooth muscle myosin is dialyzed against low ionic strength pyrophosphate or citrate/Tris buffers. Unlike synthetic filaments formed at approximately physiological ionic conditions, minifilaments are homogeneous as indicated by their hypersharp boundary during sedimentation velocity. Electron microscopy and hydrodynamic techniques were used to show that 20-22S smooth muscle myosin minifilaments are 380 nm long and composed of 12-14 molecules. By varying solvents, a continuum of different size polymers in the range of 15-30S could be obtained. Skeletal muscle myosin, in contrast, preferentially forms a stable 32S minifilament (Reisler, E., P. Cheung, and N. Borochov. 1986. Biophys. J. 49:335-342), suggesting underlying differences in the assembly properties of the two myosins. Addition of salt to the smooth muscle myosin minifilaments caused unidirectional growth into a longer "side-polar" type of filament, whereas bipolar filaments were consistently formed by skeletal muscle myosin. As with synthetic filaments, addition of 1 mM MgATP caused dephosphorylated minifilaments to dissociate to a mixture of folded monomers and dimers. Phosphorylation of the regulatory light chain prevented disassembly by nucleotide, even though it had no detectable effect on the structure of the minifilament. These results suggest that differences in filament stability as a result of phosphorylation are due largely to conformational changes occurring in the myosin head, and are not due to differences in filament packing.     

Substructure and accessory proteins in scallop myosin filaments

Native myosin filaments from scallop striated muscle fray into subfilaments of approximately 100-A diameter when exposed to solutions of low ionic strength. The number of subfilaments appears to be five to seven (close to the sevenfold rotational symmetry of the native filament), and the subfilaments probably coil around one another. Synthetic filaments assembled from purified scallop myosin at roughly physiological ionic strength have diameters similar to those of native filaments, but are much longer. They too can be frayed into subfilaments at low ionic strength. Synthetic filaments share what may be an important regulatory property with native filaments: an order-disorder transition in the helical arrangement of myosin cross-bridges that is induced on activation by calcium, removal of nucleotide, or modification of a myosin head sulfhydryl. Some native filaments from scallop striated muscle carry short "end filaments" protruding from their tips, comparable to the structures associated with vertebrate striated muscle myosin filaments. Gell electrophoresis of scallop muscle homogenates reveals the presence of high molecular weight proteins that may include the invertebrate counterpart of titin, a component of the vertebrate end filament. Although the myosin molecule itself may contain much of the information required to direct its assembly, other factors acting in vivo, including interactions with accessory proteins, probably contribute to the assembly of a precisely defined thick filament during myofibrillogenesis.     

The myosin filament: V. Intermediate voltage electron microscopy and optical diffraction studies of the substructure

Using a 200 kV electron microscope (JEM 200 A), thick (up to 0.4 μm) crosssections of the myosin filaments of vertebrate striated muscle were studied. It was found that: (a) with increasing section thickness the cross-sectional profiles of the shaft of the filament were increasingly more triangular and in sections 0.4 μm thick each apex of the triangle was clearly blunted. This unique cross-sectional profile is predicted by the model proposed by Pepe (1966,1967) in which 12 parallel structural units are packed to form a triangular profile with a structural unit missing at each apex of the triangle. (b) With increasing section thickness the substructure of the myosin filament was enhanced, with the best substructure visible in sections 0.2 μm to 0.3 μm thick. This strongly supports parallel alignment of structural units in the shaft of the filament as proposed by Pepe (1966,1967). (c) The substructure spacing, determined by optical diffraction from electron micrographs of cross-sections of individual myosin filaments or groups of filaments is about 4 nm. (d) The different optical diffraction patterns observed from individual myosin filaments can be explained if the projection of each structural unit in the plane of the section has an elongated profile. With a substructure spacing of 4 nm an elongated cross-sectional profile could be produced by having two myosin molecules per structural unit. Models drawn with two myosin molecules per structural unit in the model proposed by Pepe (1966,1967) gave optical diffraction patterns similar to those observed from individual filaments. (e) The different optical diffraction patterns observed from individual myosin filaments can be explained if the elongated profiles in each structural unit are similarly oriented but with the orientation changing along the length of the filament. The change in orientation per unit length of the filament must be small enough to maintain an elongated profile for the projection of the structural unit in the plane of the sections 0.3 μm thick. All of these observations and conclusions strongly support the model for the myosin filament proposed by Pepe (1966,1967).     

Distribution of mass within native thick filaments of vertebrate skeletal muscle

The distribution of mass within the vertebrate skeletal thick filament has been determined by scanning transmission electron microscopy. Thick and thin filaments from fresh rabbit muscle were mixed with tobacco mosaic virus (TMV), fixed with formaldehyde, dried onto thin carbon films and viewed in a computer-linked microscope. Electron scattering data from both TMV and thick filaments were analysed with reference to the long axis of the particles so that the distribution of mass within the particles could be determined. While TMV appeared to be a uniform rod at the resolution employed (4.3 nm), the thick filament was clearly differentiated along its length. M-line remnants at the centre of the filament were flanked by regions of low mass per unit length, corresponding to the bare zone of the filament, and then by the more massive cross-bridge regions. The mass per unit length was approximately constant through most of the cross-bridge zone and declined at the filament tips, in a manner consistent with a constant number of myosin molecules per 14.3 nm interval (crown) throughout the cross-bridge zone. Fourier analysis of the data failed to detect the expected 43 nm periodicity of C-protein. The total mass of the thick filament was 184 Mdalton (s.e.m., 1.6 X 10(6); n = 70). The mass of adhering M-line proteins was highly variable but, on average, was about 4 Mdalton. The total mass of the filament and the mass distribution in the cross-bridge zone are consistent with three myosin molecules per crown.