The repeat distance of myosin in the thick filaments of various muscles

The meridional spacing of the X-ray diffraction peak from the repeat of myosin along the thick filament of four muscles has been remeasured on the same apparatus. The frog sartorius gave a shorter repeat distance (143.7 A) than the three invertebrate muscles, which ranged from 144.9 to 145.4 A. These results confirm earlier measurements. Provided that the myosin molecules are staggered relative to one another by a constant 98 residues, it may be inferred that in vertebrate thick filaments part or all of the tail lies at a considerable angle to the filament axis, whereas in the invertebrates the angle is smaller.     

Lepidosaur ß-keratin chains with four 34-residue repeats: Modelling reveals a potential filament-crosslinking role

ß-keratin chains contain a characteristic and homologous 34-residue sequence, which is believed to adopt a twisted ß-sheet conformation that assembles in an antiparallel manner with a similar sheet in a second chain to form a ß-sandwich. These sandwiches are, in turn, related to one another by a left-handed four-fold screw axis to generate a helical structure that forms the core of the 3.4 nm diameter filaments observed by electron microscopy and deduced from X-ray fibre diffraction. Recently, it has been shown that one ß-keratin chain, with a molecular weight approximately twice that of the majority of ß-keratin chains, is conserved across the lepidosaurs (lizards, snakes and tuatara). Uniquely, it contains four 34-residue repeats. Although this chain is a minor component the observation that the entire chain shows a high degree of sequence conservation between species suggests an important structural/functional role in vivo. Modelling shows that only six families of structures are physically possible. In three of these the repeats exist within a single filament and might therefore act in a filament nucleation role. In the second three families the repeats exist in two, three or four filaments, implying that their function may be to act as an inter-filament crosslinker, thereby providing lateral reinforcement to the epidermal appendage. The favoured model is one in which the first two repeats form a β-sandwich in one filament and the second two repeats form a β-sandwich in a neighbouring filament. Links between alternating up- and down-pointing β-sheets would provide optimum connectivity.     

Structure of actin filament bundles from microvilli of sea urchin eggs

The detailed substructure of actin filament bundles in microvilli of fertilized sea urchin eggs has been studied by analysing electron microscope images of negatively stained specimens. Transverse stripes which repeat about every 130 Å along the axis of a bundle, as previously observed by Burgess & Schroeder (1977), reflect the positions of cross-bridges that connect the filaments into a bundle. Analysis of optical transforms of the micrographs reveals that there are approximately 14 actin monomers between cross-overs of the two long-pitch helical strands of the actin filaments, with three cross-bridges in this interval. The structure is basically similar to that of the hexagonally packed bundles prepared in vitro from high speed supernatants of sea urchin eggs by Kane (1975) and analyzed by DeRosier et al. (1977). One clear difference, however, is that the in vivo microvillar filament bundles are supercoiled, giving rise to long axial repeats of 1500 to 2000 Å.Computationally filtered images of regions that were only slightly supercoiled reveal the relative alignment of filaments within the bundles and show that crossbridges appear to interact with four actin monomers, apparently linking two actin monomers on one strand of one filament to the nearest two monomers on a neighbouring filament. However, the cross-bridges are not spaced at equal intervals corresponding to four actin subunits, presumably because of the lack of hexagonal symmetry in the individual filaments, which have about 14 actin monomers between cross-overs. Instead, the cross-bridges are arranged quasiequivalently along the longitudinal axis of the bundles, in steps of four or five actin subunit spacings (28 Å each).     

The chemical mechanism of microbioal denitrification

It is suggested that, in the conditions which exist in vivo, one head of a myosin molecule interacts with another head of the opposite molecule, inside the backbone of the thick filament. The other head lies outside and can interact with actin. This model is based on the fact that a dimer of the myosin heads exists and that there is a close correlation between the properties of the dimer and those of the thick filament diameter. In natural filaments, there are myosin molecules in excess and it is suggested that these molecules have their two heads outside the backbone.     

Stepping between Membrane Microdomains

In isolated thick filaments from many types of muscle, the two head domains of each myosin molecule are folded back against the filament backbone in a conformation called the interacting heads motif (IHM) in which actin interaction is inhibited. This conformation is present in resting skeletal muscle, but it is not known how exit from the IHM state is achieved during muscle activation. Here, we investigated this by measuring the in situ conformation of the light chain domain of the myosin heads in relaxed demembranated fibers from rabbit psoas muscle using fluorescence polarization from bifunctional rhodamine probes at four sites on the C-terminal lobe of the myosin regulatory light chain (RLC). The order parameter 〈P₂〉 describing probe orientation with respect to the filament axis had a roughly sigmoidal dependence on temperature in relaxing conditions, with a half-maximal change at ∼19°C. Either lattice compression by 5% dextran T500 or addition of 25 μM blebbistatin decreased the transition temperature to ∼14°C. Maximum entropy analysis revealed three preferred orientations of the myosin RLC region at 25°C and above, two with its long axis roughly parallel to the filament axis and one roughly perpendicular. The parallel orientations are similar to those of the so-called blocked and free heads in the IHM and are stabilized by either lattice compression or blebbistatin. In relaxed skeletal muscle at near-physiological temperature and myofilament lattice spacing, the majority of the myosin heads have their light chain domains in IHM-like conformations, with a minority in a distinct conformation with their RLC regions roughly perpendicular to the filament axis. None of these three orientation populations were present during active contraction. These results are consistent with a regulatory transition of the thick filament in skeletal muscle associated with a conformational equilibrium of the myosin heads.     

THE ULTRASTRUCTURE OF FLAGELLAR FIBRILS

The tips of rat sperm tails were slightly frayed by mechanical agitation, thus exposing the fibrils, which were then studied by electron microscopy after negative staining. Only the fibrils survived this treatment. Each fibril proved to be a cylinder with a hollow core. The walls of the cylinders were made up of 10 longitudinally oriented filaments. The filaments had a markedly beaded appearance, with a repeating period of 88 A. The filament thickness (bead width) was approximately 35 to 40 A. Beads of neighboring filaments were in register with each other so that cross-linking bound the filaments together to complete the wall structure of each fibril. The center-to-center spacing from one filament to the next was 55 to 60 A. The periodicity and the diameters of the filaments make it unlikely that the filaments are related to either actin or myosin. From the way the fibrils kinked, it can be inferred that they possessed considerable mechanical strength. It is consistent with present knowledge that fibrils of the mitotic apparatus may have the same basic structure as the flagellar fibrils. Under some circumstances, pairs of fibrils separated from one another along their length, except at their extreme tips. It was apparent that there was special bridging material to be found there. In other preparations, however, the paired fibrils remained together, indicating a powerful coupling mechanism.     

THE FILAMENT LATTICE OF COCKROACH THORACIC MUSCLE

The fine structure of the tergo-coxal muscle of the cockroach, Leucophaea maderae, has been studied with the electron microscope. This muscle differs from some other types of insect flight muscles inasmuch as the ratio of thin to thick filaments is 4 instead of the characteristic 3. The cockroach flight muscle also differs from the cockroach femoral muscle in thin to thick filament ratios and diameters and in lengths of thick filaments. A comparison of these latter three parameters in a number of vertebrate and invertebrate muscles suggests in general that the diameters and lengths of the thick filaments and thin to thick filament ratios are related.     

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.     

The fine structure of myocytes in the sponges microciona prolifera (Ellis and Solander) and tedania ignis (Duchassaing and Michelotti)

Myocytes are long, fusiform cells found in the osculum and other contractile areas of many sponges. Myocytes in the oscular sphincter of Tedania ignis and the osculum and dermal membrane of Microciona prolifera were studied with light- and electron-microscopes to compare their structure to that of muscles. Salient points of similarity between myocytes and smooth muscles were their long, fusiform shape, their red color after staining with Mallory's triple stain, and the presence of filaments running longitudinally in the cytoplasm. Microciona myocytes have thick filaments of 150–250 Å diameter and thin filament of 50–70 Å diameter, and in transverse sections the thin filaments occasionally appear as a ring of dots around a thick filament. Longitudinal sections of Tedania myocytes show only one type of filament, which varies from 100 Å to 200–300 Å diameter in thick regions of the filament. Although transverse sections show light material around the dense filaments, a distinct pattern of thick and thin filaments is not seen in Tedania. Due to infrequent contacts between cells, the large extra-cellular space observed with the electron microscope (49% in Tedania, 57% in Microciona), and the absence of nerves, each myocyte probably acts as an independent contractile unit.     

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.     

THE MYOFILAMENT ARRANGEMENT IN THE FEMORAL MUSCLE OF THE COCKROACH, LEUCOPHAEA MADERAE FABRICIUS

The structure of the femoral muscle of the cockroach, Leucophaea maderae, was investigated by light and electron microscopy. The several hundred fibers of either the extensor or flexor muscle are 20 to 40 µ in diameter in transverse sections and are subdivided into closely packed myofibrils. In glutaraldehyde-fixed and epoxy resin-embedded material of stretched fibers, the A band is about 4.5 µ long, the thin filaments are about 2.3 µ in length, the H zone and I band vary with the amount of stretch, and the M band is absent. The transverse sections of the filaments reveal in the area of a single overlap of thick and thin filaments an array of 10 to 12 thin filaments encircling each thick filament; whereas, in the area of double overlap in which the thin filaments interdigitate from opposite ends of the A band, the thin filaments show a twofold increase in number. The thick filament is approximately 205 to 185 A in diameter along most of its length, but at about 0.2 µ from the end it tapers to a point. Furthermore, some well oriented, very thin transverse sections show these filaments to have electron-transparent cores. The diameter of the thin filament is about 70 A. Transverse sections exhibit the sarcolemma invaginating clearly at regular intervals into the lateral regions of the A band. Three distinct types of mitochondria are associated with the muscle: an oval, an elongate, and a type with three processes. It is evident, in this muscle, that the sliding filament hypothesis is valid, and that perhaps the function of the extra thin filaments is to increase the tensile strength of the fiber and to create additional reactive sites between the thick and thin filaments. These sites are probably required for the functioning of the long sarcomeres.     

Myosin molecule packing within the vertebrate skeletal muscle thick filaments. A complete bipolar model

Computer modelling related to the real dimensions of both the whole filament and the myosin molecule subfragments has revealed two alternative modes for myosin molecule packing which lead to the head disposition similar to that observed by EM on the surface of the cross-bridge zone of the relaxed vertebrate skeletal muscle thick filaments. One of the modes has been known for three decades and is usually incorporated into the so-called three-stranded model. The new mode differs from the former one in two aspects: (1) myosin heads are grouped into asymmetrical cross-bridge crowns instead of symmetrical ones; (2) not the whole myosin tail, but only a 43-nm C-terminus of each of them is straightened and near-parallel to the filament axis, the rest of the tail is twisted. Concurrent exploration of these alternative modes has revealed their influence on the filament features. The parameter values for the filament models as well as for the building units depicting the myosin molecule subfragments are verified by experimental data found in the literature. On the basis of the new mode for myosin molecule packing a complete bipolar structure of the thick filament is created.     

ULTRASTRUCTURAL ORGANIZATION OF OBLIQUELY STRIATED MUSCLE FIBERS IN ASCARIS LUMBRICOIDES

The somatic musculature of the nematode, Ascaris, is currently thought to consist of smooth muscle fibers, which contain intracellular supporting fibrils arranged in a regular pattern. Electron microscopic examination shows that the muscle fibers are, in fact, comparable to the striated muscles of vertebrates in that they contain interdigitating arrays of thick and thin myofilaments which form H, A, and I bands. In the A bands each thick filament is surrounded by about 10 to 12 thin filaments. The earlier confusion about the classification of this muscle probably arose from the fact that in one longitudinal plane the myofilaments are markedly staggered and, as a result, the striations in that plane of section are not transverse but oblique, forming an angle of only about 6° with the filament axis. The apparent direction of the striations changes with the plane of the section and may vary all the way from radial to longitudinal. A three-dimensional model is proposed which accounts for the appearance of this muscle in various planes. Z lines as such are absent but are replaced by smaller, less orderly, counterpart "Z bundles" to which thin filaments attach. These bundles are closely associated with fibrillar dense bodies and with deep infoldings of the plasma membrane. The invaginations of the plasma membrane together with intracellular, flattened, membranous cisternae form dyads and triads. It is suggested that these complexes, which also occur at the cell surface, may constitute strategically located, low-impedance patches through which local currents are channeled selectively.     

THE STRUCTURE OF THE SMOOTH MUSCLE FIBRES IN THE BODY WALL OF THE EARTHWORM

1. The structure of the smooth muscle fibres in the longitudinal muscle coat of the body wall of Lumbricus terrestris has been investigated by phase contrast light microscopy and electron microscopy. 2. The muscle fibre is ribbon-shaped, and attached to each of its two surfaces is a set of myofibrils. These are also ribbon-shaped, and they lie with their surfaces perpendicular to the surfaces of the fibre, and their inner edges nearly meeting in the middle of the fibre. These fibrils are oriented at an angle to the fibre axis, and diminish greatly in width as they approach the edge of the fibre. The orientation of the set of fibrils belonging to one surface of the fibre is the mirror image of that of the set belonging to the other surface; thus, when both sets are in view in a fibre lying flat on one face, the fibre exhibits double oblique striation. A comparison of extended and contracted fibres indicates that as the fibre contracts, the angle made between fibre and fibril axes increases (e.g. from 5 to 30°) and so does the angle made between the two sets of fibrils (e.g. from 10 to 60°). 3. The myofibril, throughout its length, contains irregularly packed filaments, commonly 250 A in diameter, which are parallel to its long axis and remain straight in contracted muscles. Between them is material which probably consists of much finer filaments. Thus A and I bands are absent. 4. Bound to one face of each fibril, but not penetrating inside it, is a regularly spaced series of transverse stripes. They are of two kinds, alternating along the length of the fibril, and it is suggested that they are comparable to the Z and M lines of a cross-striated fibril. The spacing of these stripes is about 0.5 µ ("Z" to "Z") in extended muscles, and 0.25 µ in contracted muscles. A bridge extends from each stripe across to the stripeless surface of the next fibril.     

Three-dimensional structure of the vertebrate muscle A-band: II. The myosin filament superlattice

The three-dimensional arrangement of the myosin filaments in the A-band of frog sartorius muscle was studied using electron micrographs of very thin and accurately cut transverse sections through the bare region (on each side of the M-band) where the thick filament shafts are roughly triangular in shape. It was found that the orientations of these triangular profiles are arranged to give a superlattice of the same size and shape as that proposed by Huxley & Brown (1967) on the basis of X-ray diffraction evidence, but the contents of the superlattice may not be as they suggested. The results from detailed image analysis strongly suggest that myosin filaments (which have been shown to have 3-fold rotational symmetry, Luther, 1978; Luther, Munro and Squire, unpublished results) are arranged with one of two orientations which are 60 ° (or 180 °) apart. This arrangement of filaments with 3-fold symmetry is not that predicted for a superlattice with the symmetry suggested by Huxley & Brown.Two rules define the way in which the orientations of neighbouring filaments are defined. Rule (1): no three mutually adjacent filaments in the hexagonal array of filaments in the A-band can all have identical orientations; and rule (2): no three successive filaments along a 10$\text{1}\text{?}$ row in the filament array can have identical orientations. These two no-three-alike rules are sufficient to describe the observed arrangement of filament profiles in the frog bare region (except for some minor violations discussed in the text), and they lead automatically to the generation of the required superlattice. The A-band structure in fish muscle is different; there is no superlattice and the triangular bare region profiles have only one orientation. The frog superlattice and fish simple lattice are explained directly in terms of different interactions between the M-bridges in the M-bands of these muscles. The observed structures require that the myosin filament symmetry at the centre of the M-band is that of the dihedral point group 32. The two possible forms of interaction between filaments with this symmetry (apart from a completely random structure) give rise to the observed A-band lattices in frog and fish muscles. The 3-fold rotational symmetry of the myosin filaments required to explain the observed micrographs also requires that the myosin crossbridge arrangements around the actin filaments in frog and fish muscles will be different. It is suggested that the structure in the frog A-band (and in the A-bands of other higher vertebrates) has evolved from that in fish to improve the distribution of crossbridges around the aotin filaments. The X-ray diffraction evidence of Huxley & Brown (1967) will be accounted for in terms of the proposed A-band structure in a further paper in this series.     

Sudden increase in speed of an actin filament moving on myosin cross-bridges of "mismatched" polarity observed when its leading end begins to interact with cross-bridges of "matched" polarity.

Under in vitro movement assay conditions, actin filaments move about 10 times faster toward, than away from, the center of large bipolar thick filaments of molluscan smooth muscle. Using thick filaments isolated from the anterior byssus retractor muscle of Mytilus edulis, the two speed modes of movement were studied in detail. Some thick filaments crossed over each other on the surface of the assay chamber, allowing actin filaments that moved into the crossover region to transfer to other thick filaments. When an actin filament that had been moving in the low speed mode crossed over to another thick filament and the speed changed to fast, the entire actin filament started to move in the high speed mode at the moment of transfer of its leading end, leaving the trailing part still in contact with the original thick filament. This indicates that myosin cross-bridges interacting in the slow mode do not impose a significant load on the cross-bridges interacting in the fast mode. Assuming the theoretical model of Tawada and Sekimoto [Biophys. J. 59, 343-356 (1991)], we suggest that the magnitude of force developed, as well as the speed of unloaded movement, differs greatly, depending on the orientation of the myosin cross-bridges.     

THE FINE STRUCTURE OF THE VENTRAL INTERSEGMENTAL ABDOMINAL MUSCLES OF THE INSECT RHODNIUS PROLIXUS DURING THE MOLTING CYCLE : I. Muscle Structure at Molting

Rhodnius prolixus, a South American insect, molts five times in its development to an adult after emerging from the egg. Each molting cycle is triggered with a blood-meal. The ventral intersegmental abdominal muscles of Rhodnius develop during each molting cycle and are functional at molting. The fine structure of these fully developed muscles from fourth stage larval insects is studied. They have the characteristic structure of slow muscles. They have multiple motor nerve endings, and the myofibrils are poorly defined in cross-section. Longitudinal sections show long sarcomeres (8–10 µ), irregular Z-lines, and no apparent H zones. No M line is seen. Transverse sections through the A-band region show that each hexagonally arranged thick filament is surrounded by 12 thin filaments. Two thin filaments are shared by two neighboring thick filaments. The ratio of thin to thick filaments is 6:1. This structure is related to that found in vertebrate skeletal muscle and insect flight muscle.     

The myosin filament: VII. Changes in internal structure along the length of the filament

Improved fixation procedures have enabled substructure to be observed by electron microscopy in transverse sections of vertebrate skeletal muscle thick filaments as thin as 140 nm. Optical diffraction combined with digital autocorrelation analysis, focal series and tilting experiments have confirmed the presence of a regular substructure having a repeat near 4 nm and shown that it is highly unlikely to be an artifact associated with the electron microscope imaging system. The results obtained strongly suggest that the thick filament is constructed from a bundle of rod-like subfilaments arranged parallel to the thick filament axis to within less than a degree. This cannot easily be reconciled with the general theory of thick filament structure proposed by Squire (1973), but it is consistent with the model proposed by Pepe, 1966, Pepe, 1967. Optical diffraction of 140 nm thick serial transverse sections has also suggested a structural change along the length of the filament that is manifest by a variation in the proportion of filaments showing strong diffraction maxima in one, two or three directions.     

The titin A-band rod domain is dispensable for initial thick filament assembly in zebrafish

The sarcomeres of skeletal and cardiac muscle are highly structured protein arrays, consisting of thick and thin filaments aligned precisely to one another and to their surrounding matrix. The contractile mechanisms of sarcomeres are generally well understood, but how the patterning of sarcomeres is initiated during early skeletal muscle and cardiac development remains uncertain. Two of the most widely accepted hypotheses for this process include the “molecular ruler” model, in which the massive protein titin defines the length of the sarcomere and provides a scaffold along which the myosin thick filament is assembled, and the “premyofibril” model, which proposes that thick filament formation does not require titin, but that a “premyofibril” consisting of non-muscle myosin, α-actinin and cytoskeletal actin is used as a template. Each model posits a different order of necessity of the various components, but these have been difficult to test in vivo. Zebrafish motility mutants with developmental defects in sarcomere patterning are useful for the elucidation of such mechanisms, and here we report the analysis of the herzschlag mutant, which shows deficits in both cardiac and skeletal muscle. The herzschlag mutant produces a truncated titin protein, lacking the C-terminal rod domain that is proposed to act as a thick filament scaffold, yet muscle patterning is still initiated, with grossly normal thick and thin filament assembly. Only after embryonic muscle contraction begins is breakdown of sarcomeric myosin patterning observed, consistent with the previously noted role of titin in maintaining the contractile integrity of mature sarcomeres. This conflicts with the “molecular ruler” model of early sarcomere patterning and supports a titin-independent model of thick filament organization during sarcomerogenesis. These findings are also consistent with the symptoms of human titin myopathies that exhibit a late onset, such as tibial muscular dystrophy.     

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)