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.     

A new protein of the thick filaments of vertebrate skeletal myofibrils. Extractions, purification and characterization

A new protein component of skeletal myofibrils has been isolated and characterized. It is prepared from impure myosin preparations and corresponds to band C, the principal contaminant observed in sodium dodecyl sulphate polyacrylamide gel electrophoresis patterns of such preparations (Starr and Offer, 1971).The C-protein, as we term it, is deduced to be a component of the skeletal myofibril because (i) glycerinated or fresh myoflbrils contain a component with a mobility identical to C-protein on sodium dodecyl sulphate gels, (ii) this component is extracted from myofibrils by the same solvent which extracts C-protein and (iii) C-protein may be prepared from preparations of isolated myofibrils. It is presumed to be a component of the thick filaments because it binds strongly to myosin at low ionic strength; immunological evidence which confirms this view is presented elsewhere.The quantity of C-protein in the myofibril has been estimated to be 2.0% by densitometry of sodium dodecyl sulphate gels of glycerinated myofibrils using actin as an internal reference. About forty molecules of C-protein are present in a thick filament.The properties of C-protein distinguish it from the other well-characterized myoflbrillar proteins. The C-protein molecule contains a single polypeptide chain of molecular weight 140,000. The intrinsic viscosity of 13.6 ml/g suggests that the molecule is neither completely globular nor as elongated as molecules like paramyosin or tropomyosin. The α-helical content is very low and the proline content higher than the other myofibrillar proteins. The molecule associates at low ionic strength.C-protein has no ATPase activity, nor does it affect the ATPase of pure myosin. But it reduces the activity of the actin-activated myosin ATPase by about half, this inhibition being independent of the level of Ca²⁺. C-protein does not bind Ca²⁺ in the presence of Mg²⁺. Its possible location and function are discussed.     

Myosin content and filament structure in smooth and striated muscle

Fibres from four different muscles (rabbit psoas, guinea pig taenia coli, Lethocerus flight and leg) were glycerol-extracted, homogenized and dissolved in a sodium dodecyl sulphate solution. The relative mass of the myosin heavy chain and actin polypeptides present in these extracts was measured by polyacrylamide gel electrophoresis. The ratio was found to be consistent for each muscle and to differ widely between muscles. The results were used to calculate the number of myosin molecules per subunit repeat along the thick filaments of the striated muscles and ribbon-like filaments, and so to test a theory of filament structure.     

Titin organisation and the 3D architecture of the vertebrate-striated muscle I-band

The giant muscle protein titin (connectin) is known to serve as a cytoskeletal element in muscle sarcomeres. It elastically restrains lengthening sarcomeres, it aids the integrity and central positioning of the A-band in the sarcomere and it may act as a template upon which some sarcomeric components are laid down during myogenesis. A puzzle has been how titin molecules, arranged systematically within the hexagonal A-band lattice of myosin filaments, can redistribute through the I-band to their anchoring sites in the tetragonal Z-band lattice. Recent work by Liversage and colleagues has suggested that there are six titin molecules per half myosin filament. Since there are two actin filaments per half myosin filament in a half sarcomere, this means that there are three titin molecules interacting with each Z-band unit cell containing one actin filament in the same sarcomere and one of opposite polarity from the next sarcomere. Liversage et al. suggested that the three titins might be distributed with two on an actin filament of one polarity and one on the filament of opposite polarity. Here, we build on this suggestion and discuss the transition of titin from the A-band to the Z-band. We show that there are good structural and mechanical reasons why titin might be organised as Liversage et al., suggested and we discuss the possible relationships between A-band arrangements in successive sarcomeres along a myofibril.     

Effects of C-protein on synthetic myosin filament structure.

In the absence of C-protein, synthetic filaments prepared from column-purified myosin exhibit the following features: individual filament diameters are uniform over a long length, but a wide distribution of diameters is apparent over the population; approximately 25% of the filaments have a frayed appearance and take up stain poorly, whereas the remaining 75% are well-stained; optical diffraction of well-stained filaments reveals a 14.3-nm subunit period and a 43-nm axial period (Koretz, 1978; Koretz, 1979). Addition of C-protein to myosin before filament formation affects all of these features in a manner related to C-protein concentration. At the physiological ratio of C-protein to myosin in the banded region of the natural thick filament, synthetic aggregates are uniform in diameter over the population and show less than 10% frays. Whereas the subunit period remains unchanged, the axial period has increased to 114.4 nm, or eight times the subunit repeat. Above and below the physiological ratio, disorder of a specific nature is apparent. Addition of C-protein after filament formation appears to coat the aggregates so that elements of backbone ultrastructure are obscured, and some evidence of axial period change is visible in diffraction patterns. A model is presented for the binding of C-protein to myosin, and its observed effects on filament structure are explained in terms of this model.     

Movement of myosin fragments in vitro: domains involved in force production

We have used the Nitella-based movement assay to localize the site of force production in myosin. Methods were developed to use nonfilamentous myosin or proteolytic fragments of myosin in place of the thick filaments used in the original assay. In the experiments described here, the tail of myosin or its subfragments is anchored via antibodies to the surface of small particles. Nonfilamentous myosin or its subfragments move along Nitella actin cables at speeds similar to those obtained with filamentous myosin. We generated short HMM, a myosin fragment containing the heads and only 400 A of the tail. Although short HMM lacks the "hinge" region proposed by Harrington to be the site of force generation, and is incapable of forming thick filaments, it moves along actin at speeds above 1 micron/sec. Therefore, neither a thick filament nor the carboxy-terminal 1100 A of the tail is required for movement along actin. The results indicate that force production occurs in or near the myosin heads.     

Alterations in Ca2+ sensitive tension due to partial extraction of C- protein from rat skinned cardiac myocytes and rabbit skeletal muscle fibers

C-protein, a substantial component of muscle thick filaments, has been postulated to have various functions, based mainly on results from biochemical studies. In the present study, effects on Ca(2+)-activated tension due to partial removal of C-protein were investigated in skinned single myocytes from rat ventricle and rabbit psoas muscle. Isometric tension was measured at pCa values of 7.0 to 4.5: (a) in untreated myocytes, (b) in the same myocytes after partial extraction of C-protein, and (c) in some myocytes, after readdition of C-protein. The solution for extracting C-protein contained 10 mM EDTA, 31 mM Na2HPO2, 124 mM NaH2PO4, pH 5.9 (Offer et al., 1973; Hartzell and Glass, 1984). In addition, the extracting solution contained 0.2 mg/ml troponin and, for skeletal muscle, 0.2 mg/ml myosin light chain-2 in order to minimize loss of these proteins during the extraction procedure. Between 60 and 70% of endogenous C-protein was extracted from cardiac myocytes by a 1-h soak in extracting solution at 20-23 degrees C; a similar amount was extracted from psoas fibers during a 3-h soak at 25 degrees C. For both cardiac myocytes and skeletal muscle fibers, partial extraction of C-protein resulted in increased active tension at submaximal concentrations of Ca2+, but had little effect upon maximum tension. C-protein extraction also reduced the slope of the tension-pCa relationships, suggesting that the cooperativity of Ca2+ activation of tension was decreased. Readdition of C-protein to previously extracted myocytes resulted in recovery of both tension and slope to near their control values. The effects on tension did not appear to be due to disruption of cooperative activation of the thin filament, since C-protein extraction from cardiac myocytes that were 40-60% troponin-C (TnC) deficient produced effects similar to those observed in cells that were TnC replete. Measurements of the tension-pCa relationship in skeletal muscle fibers were also made at a sarcomere length of 3.5 microns which, because of the distribution of C-protein on the thick filament, should eliminate any interaction between C-protein and actin. The effects of C-protein extraction were similar at long and short sarcomere lengths. These data are consistent with a model in which C-protein modulates the range of movement of myosin, such that the probability of myosin binding to actin is increased after its extraction.     

Structural evidence for the interaction of C-protein (MyBP-C) with actin and sequence identification of a possible actin-binding domain

C-protein (MyBP-C) is a myosin-binding protein that is usually seen in two sets of seven to nine positions in the C-zones in each half of the vertebrate striated muscle A-band. Skeletal muscle C-protein is a modular structure containing ten sub-domains (C1 to C10) of which seven are immunoglobulin-type domains and three (C6, C7 and C9) are fibronectin-like domains. Cardiac muscle C-protein has an extra N-terminal domain (C0) and also some sequence insertions, one of which provides phosphorylation sites. It is conceivable that C-protein has both a structural and regulatory role within the sarcomere. The precise mode of binding of C-protein to the myosin filament has not been determined. However, detailed ultrastructural studies have suggested that C-protein, which binds to myosin, can give rise to a longer periodicity (about 435A) than the intrinsic myosin filament repeat of 429A. The reason for this has remained a puzzle for over 25 years. Here we show by modelling and computation that the presence of this longer periodicity could be explained if the myosin-binding part of C-protein binds to myosin with the expected 429A repeat, but if there are systematic interactions of the N-terminal end of C-protein with the neighbouring actin filaments in the hexagonal lattice of filaments in the A-band. We also show that if they occur these interactions would probably only arise in defined muscle states. Further analysis of the MyBP-C sequence identifies a possible actin-binding domain in the Pro-Ala-rich sequence found at the N terminus of skeletal MyBP-C and between domains C0 and C1 in the cardiac sequence.     

Modeling rigor cross-bridge patterns in muscle I. Initial studies of the rigor lattice of insect flight muscle.

We have undertaken some computer modeling studies of the cross-bridge observed by Reedy in insect flight muscle so that we investigate the geometric parameters that influence the attachment patterns of cross-bridges to actin filaments. We find that the appearance of double chevrons along an actin filament indicates that the cross-bridges are able to reach 10--14 nm axially, and about 90 degrees around the actin filament. Between three and five actin monomers are therefore available along each turn of one strand of actin helix for labeling by cross-bridges from an adjacent myosin filament. Reedy's flared X of four bridges, which appears rotated 60 degrees at successive levels on the thick filament, depends on the orientation of the actin filaments in the whole lattice as well as on the range of movement in each cross-bridge. Fairly accurate chevrons and flared X groupings can be modeled with a six-stranded myosin surface lattice. The 116-nm long repeat appears in our models as "beating" of the 14.5-nm myosin repeat and the 38.5-nm actin period. Fourier transforms of the labeled actin filaments indicate that the cross-bridges attach to each actin filament on average of 14.5 nm apart. The transform is sensitive to changes in the ease with which the cross-bridge can be distorted in different directions.     

Movement of smooth muscle tropomyosin by myosin heads.

It has been proposed that during the activation of muscle contraction the initial binding of myosin heads to the actin thin filament contributes to switching on the thin filament and that this might involve the movement of actin-bound tropomyosin. The movement of smooth muscle tropomyosin on actin was investigated in this work by measuring the change in distance between specific residues on tropomyosin and actin by fluorescence resonance energy transfer (FRET) as a function of myosin head binding to actin. An energy transfer acceptor was attached to Cys374 of actin and a donor to the tropomyosin heterodimer at either Cys36 of the beta-chain or Cys190 of the alpha-chain. FRET changed for the donor at both positions of tropomyosin upon addition of skeletal or smooth muscle myosin heads, indicating a movement of the whole tropomyosin molecule. The changes in FRET were hyperbolic and saturated at about one head per seven actin subunits, indicating that each head cooperatively affects several tropomyosin molecules, presumably via tropomyosin's end-to-end interaction. ATP, which dissociates myosin from actin, completely reversed the changes in FRET induced by heads, whereas in the presence of ADP the effect of heads was the same as in its absence. The results indicate that myosin with and without ADP, intermediates in the myosin ATPase hydrolytic pathway, are effective regulators of tropomyosin position, which might play a role in the regulation of smooth muscle contraction.     

Differential labeling of myosin V heads with quantum dots allows direct visualization of hand-over-hand processivity

The double-headed myosin V molecular motor carries intracellular cargo processively along actin tracks in a hand-over-hand manner. To test this hypothesis at the molecular level, we observed single myosin V molecules that were differentially labeled with quantum dots having different emission spectra so that the position of each head could be identified with approximately 6-nm resolution in a total internal reflectance microscope. With this approach, the individual heads of a single myosin V molecule were observed taking 72-nm steps as they alternated positions on the actin filament during processive movement. In addition, the heads were separated by 36 nm during pauses in motion, suggesting attachment to actin along its helical repeat. The 36-nm interhead spacing, the 72-nm step size, and the observation that heads alternate between leading and trailing positions on actin are obvious predictions of the hand-over-hand model, thus confirming myosin V's mode of walking along an actin filament.     

Effects of phosphorylated and unphosphorylated C-protein on cardiac actomyosin ATPase

C-protein, a component of the thick filaments of striated muscles, is reversibly phosphorylated and dephosphorylated in heart. It has been hypothesized that C-protein may be involved in regulating contraction, because the extent of C-protein phosphorylation correlates with the rate of cardiac relaxation. To test this hypothesis, the effects of phosphorylated and unphosphorylated C-protein on the actin-activated ATPase activity of myosin filaments prepared from DEAE-Sephadex-purified myosin were examined. Unphosphorylated C-protein (0.1 microM to 1.5 microM) stimulated actin-activated myosin ATPase activity in a dose-dependent manner. With a myosin: C-protein molar ratio of approximately 1, actin-activated myosin ATPase activity was elevated up to 3.2 times that of the control. Phosphorylated C-protein (2.5 mol PO4/mol C-protein) stimulated the activity somewhat less (2.5 times that of control). The stimulation of ATPase activity by C-protein was due to an increase in the Vmax value (from 0.25/second to 0.62/second) and a decrease in the Km value (from 11.9 microM to 6.7 microM). The addition of C-protein to actomyosin solutions produced an increase in the light-scattering of the actomyosin solution and a distinct precipitation of the actomyosin with time. Phosphorylated C-protein had a smaller effect on light-scattering than dephosphorylated C-protein. C-protein had a negligible effect on Ca-ATPase, EDTA-K-ATPase, or Mg-ATPase activities in the absence of actin. C-protein had only small effects on the actin-activated ATPase of heavy meromyosin. These results suggest that C-protein stimulates actin-activated myosin ATPase activity by enhancing the formation of stable aggregates between actin and myosin filaments.     

General model of myosin filament structure. 3. Molecular packing arrangements in myosin filaments

Following the original proposals about myosin filament structure put forward as part of a general myosin filament model (Squire, 1971, 1972) it is here shown what the most likely molecular packing arrangements within the backbones of certain myosin filaments would be assuming that the model is correct. That this is so is already indicated by recently published experimental results which have confirmed several predictions of the model (Bullard and Reedy, 1972; Reedy et al., 1972; Tregear and Squire, 1973).The starting point in the analysis of the myosin packing arrangements is the model for the myosin ribbons in vertebrate smooth muscle proposed by Small &; Squire (1972). It is shown that there is only one reasonable type of packing arrangement for the rod portions of the myosin molecules which will account for the known structure of the ribbons and which is consistent with the known properties of myosin molecules. The dominant interactions in this packing scheme are between parallel myosin molecules which are related by axial shifts of 430 Å and 720 Å. In this analysis the myosin rods are treated as uniform rods of electron density and only the general features of two-strand coiled-coil molecules are considered.Since the general myosin filament model is based on the assumption that the structures of different types of myosin filament must be closely related, the packing scheme derived for the myosin ribbons is used to deduce the structures of the main parts (excluding the bare zones) of the myosin filaments in a variety of muscles. It is shown in each case that there is only one packing scheme consistent with all the available data on these filaments and that in each filament type exactly the same interactions between myosin rods are involved. In other words the myosin-myosin interactions involved in filament formation are specific, they involve molecular shifts of either 430 Å or 720 Å, and are virtually identical in all the different myosin filaments which have been considered. Apart from the myosin ribbons, these are the filaments in vertebrate skeletal muscle, insect flight muscle and certain molluscan muscles.In the case of the thick filaments in vertebrate skeletal muscle the form of the myosin packing arrangement in the bare zone is considered and a packing scheme proposed which involves antiparallel overlaps between myosin rods of 1300 Å and 430 Å. It is shown that this scheme readily explains the triangular profiles of the myosin filaments in the bare zone (Pepe, 1967, 1971) and many other observations on the form of these myosin filaments.Finally it is shown that the cores of several different myosin filaments, assuming they contain protein, may consist of different arrangements of one or other of two types of core subfilament.     

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.     

Orientation dependence of displacements by a single one-headed myosin relative to the actin filament.

Displacements of single one-headed myosin molecules in a sparse myosin-rod cofilament were measured from bead displacements at various angles relative to an actin filament by dual optical trapping nanometry. The sparse myosin-rod cofilaments, 5-8 micron long, were synthesized by slowly mixing one-headed myosin prepared by papain digestion with myosin rods at molar ratios of 1:400 to 1:1500, so that one to four one-headed myosin molecules were on average scattered along the cofilament. The bead displacement was approximately 10 nm at low loads ( approximately 0.5 pN) and at angles of 5-10 degrees between the actin and myosin filaments (near physiologically correct orientation). The bead displacement decreased with an increase in the angle. The bead displacement at nearly 90 degrees was approximately 0 nm. When the angle was increased to approximately 150 degrees-170 degrees, the bead displacements increased to 5 nm. A native two-headed myosin showed similar size and orientation dependence of bead displacements as a one-headed myosin.     

Packing of myosin molecules in muscle thick filaments

The backbone of the myosin filament is an aggregate of alpha-helical coiled coil myosin rods. Its surface forms a three-stranded helix composed of myosin heads. Currently there is no adequate model to describe the organization of the myosin filament. It is proposed here that, in cross-section the light meromyosin (LMM) of 18 myosin molecules form an outer tube, with nine S2 forming the interior core. At the surface of the thick filament, myosin heads are arranged in three rows, giving the filament a periodicity of 14.3 nm per three myosin molecules. Two of these molecules are organized at an angle of 120 degrees to each other on the same level, while the third is shifted 7.2 nm along the filament axis. This packing gives a striation pattern of 7.2 nm by electron microscopy. An alternative model is also possible, in which the heads of the myosin molecules are uniformly spaced at an interval of 14.3 nm along the filament axis. The packing of individual molecules within the myosin filament is based on a regular pattern of charge on the 28 amino-acid repeat in the rod domain.     

Direct observation of molecular motility by light microscopy

We used video-fluorescence microscopy to directly observe the sliding movement of single fluorescently labeled actin filaments along myosin fixed on a glass surface. Single actin filaments labeled with phalloidin-tetramethyl-rhodamine, which stabilizes the filament structure of actin, could be seen very clearly and continuously for at least 60 min in 02-free solution, and the sensitivity was high enough to see very short actin filaments less than 40 nm long that contained less than eight dye molecules. The actin filaments were observed to move along double-headed and, similarly, single-headed myosin filaments on which the density of the heads varied widely in the presence of ATP, showing that the cooperative interaction between the two heads of the myosin molecule is not essential to produce the sliding movement. The velocity of actin filament independent of filament length (greater than 1 micron) was almost unchanged until the density of myosin heads along the thick filament was decreased from six heads/14.3 nm to 1 head/34 nm. This result suggests that five to ten heads are sufficient to support the maximum sliding velocity of actin filaments (5 micron/s) under unloaded conditions. In order for five to ten myosin heads to achieve the observed maximum velocity, the sliding distance of actin filaments during one ATP cycle must be more than 60 nm.     

The aggregation characteristics of column-purified rabbit skeletal myosin in the presence and absence of C-protein at pH 7.0.

The aggregation properties of column-purified rabbit skeletal myosin at pH 7.0 were investigated as functions of ionic strength, protein concentration, and time. Filaments prepared by dialysis exhibited the same average length and population distribution at 0.10 and 0.15 M KCl at protein concentrations greater than 0.10 mg/ml; similar results were obtained at .0.20 M KCl, although average filament length was approximately 0.5 micrometer shorter. Once formed, these length distributions remained virtually unchanged over an 8-d period. At and below 0.10 mg/ml, average filament length decreased as a function of protein concentration; filaments prepared from an initial concentration of 0.02 mg/ml were half the length of those prepared at 0.2 mg/ml. Filaments prepared by dilution exhibited a sharp increase in average length as the time-course increased up to 40 s, then altered only slightly over a further period of 4 min. Addition of C-protein in a molar ratio of 1-3.3 myosin molecules affected most of these results. Average filament length was affected neither by ionic strength nor by initial protein concentration down to 0.04 mg/ml or over an 8-d period. Filaments formed by dilution in the presence of C-protein exhibited a constant average length and hypersharp length distribution over variable time courses up to 7 min. It is possible that C-protein acts to stabilize the antiparallel intermediate during filamentogenesis, and may also affect subunit addition to this nucleus.     

Oblique section 3-D reconstruction of relaxed insect flight muscle reveals the cross-bridge lattice in helical registration.

In this work we examined the arrangement of cross-bridges on the surface of myosin filaments in the A-band of Lethocerus flight muscle. Muscle fibers were fixed using the tannic-acid-uranyl-acetate, ("TAURAC") procedure. This new procedure provides remarkably good preservation of native features in relaxed insect flight muscle. We computed 3-D reconstructions from single images of oblique transverse sections. The reconstructions reveal a square profile of the averaged myosin filaments in cross section view, resulting from the symmetrical arrangement of four pairs of myosin heads in each 14.5-nm repeat along the filament. The square profiles form a very regular right-handed helical arrangement along the surface of the myosin filament. Furthermore, TAURAC fixation traps a near complete 38.7 nm labeling of the thin filaments in relaxed muscle marking the left-handed helix of actin targets surrounding the thick filaments. These features observed in an averaged reconstruction encompassing nearly an entire myofibril indicate that the myosin heads, even in relaxed muscle, are in excellent helical register in the A-band.     

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.