Bidirectional movement of actin filaments along tracks of myosin heads

It is well established that muscle contraction results from the relative sliding of actin and myosin filaments. Both filaments have definite polarities and well-ordered structures. Thick filaments, however, are not vital for supporting movement in vitro. Previously we have demonstrated that actin filaments can move continuously on myosin fragments (subfragment-1 or heavy meromyosin (HMM] that are bound to a nitrocellulose surface. Here we report that actin filaments can move in opposite directions on tracks of myosin heads formed when actin filaments decorated with HMM are placed on a nitrocellulose surface. The actin filaments always move forward, frequently changing the direction of the movement, but never move backward reversing the polarity of the movement. The direction of movement is therefore determined by the polarity of the actin filament. These results indicate that myosin heads have considerable flexibility.     

Sliding distance between actin and myosin filaments per ATP molecule hydrolysed in skinned muscle fibres

Muscle contraction is generally thought to be driven by tilting of the 19-nm-long myosin head, part of the thick filament, while attached to actin, part of the thin filament. This motion would produce about 12 nm of filament sliding. Recent estimates of the sliding distance per ATP molecule hydrolysed by actomyosin in vitro vary widely from 8 nm to greater than or equal to 200 nm. The latter value is incompatible with a power stroke incorporating a single tilting motion of the head. We have measured the isotonic sliding distance per ATP molecule hydrolysed during the interaction between myosin and actin in skinned muscle fibres. We directly estimated the proportion of simultaneously attached actomyosin complexes and their ATP use. We report here that at low loads the interaction distance is at least 40 nm. This distance corresponds to the length of the power stroke plus the filament sliding while actomyosin crossbridges bear negative drag forces. If the power stroke is 12 nm, then our results indicate the drag distance to be at least 28 nm. Our results could also be explained by multiple power strokes per ATP molecule hydrolysed.     

Can a myosin molecule bind to two actin filaments?

It is suggested that in striated muscles the two heads of one myosin molecule are able to interact with different actin filaments. This would provide a simple explanation for the appearance and arrangement of cross-bridges in insect flight muscle in rigor.     

Direct observation of motion of single F-actin filaments in the presence of myosin

Actin is found in almost all kinds of non-muscle cells where it is thought to have an important role in cell motility. A proper understanding of that role will only be possible when reliable in vitro systems are available for investigating the interaction of cellular actin and myosin. A start has been made on several systems, most recently by Sheetz and Spudich who demonstrated unidirectional movement of HMM-coated beads along F-actin cables on arrays of chloroplasts exposed by dissection of a Nitella cell. As an alternative approach, we report here the direct observation by fluorescence microscopy of the movements of single F-actin filaments interacting with soluble myosin fragments energized by Mg2+-ATP.     

Sliding distance of actin filament induced by a myosin crossbridge during one ATP hydrolysis cycle

Muscle contraction results from a sliding movement of actin filaments induced by myosin crossbridges on hydrolysis of ATP, and many non-muscle cells are thought to move using a similar mechanism. The molecular mechanism of muscle contraction, however, is not completely understood. One of the major problems is the mechanochemical coupling at high velocity under near-zero load. Here, we report measurements of the sliding distance of an actin filament induced by a myosin crossbridge during one ATP hydrolysis cycle in an unloaded condition. We used single sarcomeres from which the Z-lines, structures which anchor the thin filaments in the sarcomere, had been completely removed by calcium-activated neutral protease (CANP) and trypsin, and measured both the sliding velocity of single actin filaments along myosin filaments and the ATPase activity during sliding. Our results show that the average sliding distance of the actin filament is less than or equal to 600 A during one ATP cycle, much longer than the length of power stroke of myosin crossbridges deduced from mechanical studies of muscle, which is of the order of 80 A (for example, ref. 15).     

Structure of the backbone in myosin filaments of muscle

New X-ray data suggest how myosin rods, themselves alpha-helical coiled coils, form the thick filament backbone of crustacean muscles by additional supercoiling. Natural transformations of this structure may describe the myosin backbone in many other animals also.     

Movement of myosin-coated beads on oriented filaments reconstituted from purified actin

Although the biochemical properties of the actin/myosin interaction have been studied extensively using actin activation of myosin ATPase as an assay, until recently no well-defined assay has been available to measure the mechanical properties of ATP-dependent movement of myosin along actin filaments. The first direct measurements of the rate of myosin movement in vitro used a naturally occurring, biochemically ill-defined array of actin filaments from the alga Nitella. We report here the construction of an oriented array of filaments reconstituted from purified muscle actin and the use of this array in a biochemically defined quantitative assay for the directed movement of myosin-coated polystyrene beads. We demonstrate for the first time that actin alone, linked to a substratum by a protein anchor, is sufficient to support movement of myosin at rates consistent with the speeds of muscle contraction and other forms of cell motility.     

Light-chain movement and regulation in scallop myosin

Photo-cross-linking techniques show that when scallop myosin or myofibrils are subjected to experimental conditions that cause relaxed muscles to go into rigor, the N-terminal portion of the regulatory light chain of myosin moves towards the essential light chain while the C-terminal portion stays in place. These changes occur on the myosin before combination with actin. Cross-linking of the N-terminal region to the essential light chain in rigor locks the myosin into a conformation such that calcium sensitivity of the actin-activated Mg-ATPase is lost.     

Propulsion of organelles isolated from Acanthamoeba along actin filaments by myosin-I

Eukaryotic cells are dependent on their ability to translocate membraneous elements about the cytoplasm. In many cells long translocations of organelles are associated with microtubules. In other cases, such as the rapid cytoplasmic streaming in some algae, organelles appear to be propelled along actin filaments. It has been assumed, but not proven, that myosin produces these movements. We have tested vesicles from another eukaryotic cell for their ability to move on the exposed actin bundles of Nitella as an indiction that actin-based organelle movements may be a general property of cells. We found that organelles from Acanthamoeba castellanii can move along Nitella actin filaments. Here, we report two different experiments indicating that the single-headed non-polymerizable myosin isozyme myosin-I is responsible for this organelle motility. First, monoclonal antibodies to myosin-I inhibit movement, but antibodies that inhibit double-headed myosin-II do not. Second, approximately 20% of the myosin-I in homogenates co-migrates with motile vesicles during Percoll density-gradient ultracentrifugation. This is the first indication of a role for myosin-I within the cell and supports the suggestion of Albanesi et al. that myosin-I moves vesicles in this way.     

Peptide mimetics of an actin-binding site on myosin span two functional domains on actin

The sites on the myosin heavy chain that interact with actin and are responsible for force generation are ill-defined: crosslinking and experiments with isolated domains of the myosin head implicate regions in both the 50K and 20K (molecular weights in thousands) domains of the myosin head (subfragment 1, S1) in this process. We have synthesized peptides from the sequence around the fast-reacting SH1 thiol residue in the 20K domain of S1 in order to delineate precisely an actin-binding site. We used a combination of 1H-NMR and enzyme inhibition assay and also assessed the effects of peptides on skinned rabbit psoas muscle fibres to show that the region of amino acids 690-725 contains an actin-binding site. Peptides from this region bind to actin, act as mixed inhibitors of the actin-stimulated S1 Mg2(+)-ATPase, and influence the contractile force developed in skinned fibres, whereas peptides flanking this sequence are without effect in our test systems. Remarkably, peptides from the N-terminal half of this segment 690-725 increase force development in skinned fibres at submaximal activating concentrations of Ca2+, that is, they behave as calcium-sensitizers; C-terminal peptides, however, inhibit force development without effecting sensitivity to calcium. These different responses indicate that this region is probably binding at two functionally distinct sites on actin.     

Myosin subfragment-1 is sufficient to move actin filaments in vitro

The rotating crossbridge model for muscle contraction proposes that force is produced by a change in angle of the crossbridge between the overlapping thick and thin filaments. Myosin, the major component of the thick filament, is comprised of two heavy chains and two pairs of light chains. Together they form two globular heads, which give rise to the crossbridge in muscle, and a coiled-coil rod, which forms the shaft of the thick filament. The isolated head fragment, subfragment-1 (S1), contains the ATPase and actin-binding activities of myosin (Fig. 1). Although S1 seems to have the requisite enzymatic activity, direct evidence that S1 is sufficient to drive actin movement has been lacking. It has long been recognized that in vitro movement assays are an important approach for identifying the elements in muscle responsible for force generation. Hynes et al. showed that beads coated with heavy meromyosin (HMM), a soluble proteolytic fragment of myosin consisting of a part of the rod and the two heads, can move on Nitella actin filaments. Using the myosin-coated surface assay of Kron and Spudich, Harada et al. showed that single-headed myosin filaments bound to glass support movement of actin at nearly the same speed as intact myosin filaments. These studies show that the terminal portion of the rod and the two-headed nature of myosin are not required for movement. To restrict the region responsible for movement further, we have modified the myosin-coated surface assay by replacing the glass surface with a nitrocellulose film. Here we report that myosin filaments, soluble myosin, HMM or S1, when bound to a nitrocellulose film, support actin sliding movement (Fig. 2). That S1 is sufficient to cause sliding movement of actin filaments in vitro gives strong support to models of contraction that place the site of active movement in muscle within the myosin head.     

Reversible cyclic AMP-dependent change in distribution of myosin thick filaments in Dictyostelium

Myosin is thought to act as a major mechanochemical transducer in non-muscle cell motility, but the in situ organization of the molecules has not yet been determined. Here we report the localization of myosin 'rods', analogous to the thick filaments of muscle, by ameliorated immunofluorescence and demonstrate the dynamic translocation of these rods in response to exogenously added cyclic AMP, which is a chemoattractant for Dictyostelium amoebae. On addition of cyclic AMP, we observed instantaneous shedding of the endoplasmic myosin followed by an increase in cortical rods, the original distribution being recovered in a few minutes. We conclude that myosin filaments mediate Dictyostelium cell movement, probably by an assembly/disassembly cycle of the molecules in response to a chemotactic stimulus.     

Calcium regulation of molluscan myosin ATPase in the absence of actin

In the myosin-linked regulatory mechanism typified by the molluscan scallop adductor muscle, contraction is controlled by Ca2+ binding to sites on the thick filament protein, myosin. The regulatory light chains of myosin heads are involved directly in this mechanism and early studies suggested that, in the absence of Ca2+, these subunits prevent the interaction of a myosin-adenosine nucleotide complex with the actin-containing thin filament. Subsequently, Ashiba et al. reported that the steady-state ATPase of molluscan myosin exhibits a limited degree of Ca2+ activation in the absence of actin. Recently, however, we have shown that steady-state ATPase activity in relaxing conditions is dominated by the unregulated molecules in the myosin preparation. Single-turnover kinetic methods are required to monitor the highly suppressed ATPase activity of the regulated population. Using the latter approach, we report here that scallop myosin ATPase is reduced about 100-fold on removal of Ca2+. The regulatory light chains maintain the relaxed state via conformational changes which suppress the product release steps, irrespective of the presence of actin.     

Direct observation of individual RecA filaments assembling on single DNA molecules

Escherichia coli RecA is essential for the repair of DNA double-strand breaks by homologous recombination. Repair requires the formation of a RecA nucleoprotein filament. Previous studies have indicated a mechanism of filament assembly whereby slow nucleation of RecA protein on DNA is followed by rapid growth. However, many aspects of this process remain unclear, including the rates of nucleation and growth and the involvement of ATP hydrolysis, largely because visualization at the single-filament level is lacking. Here we report the direct observation of filament assembly on individual double-stranded DNA molecules using fluorescently modified RecA. The nucleoprotein filaments saturate the DNA and extend it approximately 1.6-fold. At early time points, discrete RecA clusters are seen, permitting analysis of single-filament growth from individual nuclei. Formation of nascent RecA filaments is independent of ATP hydrolysis but is dependent on the type of nucleotide cofactor and the RecA concentration, suggesting that nucleation involves binding of approximately 4-5 ATP-RecA monomers to DNA. Individual RecA filaments grow at rates of 3-10 nm s(-1). Growth is bidirectional and, in contrast to nucleation, independent of nucleotide cofactor, suggesting addition of approximately 2-7 monomers s(-1). These results are in accord with extensive genetic and biochemical studies, and indicate that assembly in vivo is controlled at the nucleation step. We anticipate that our approach and conclusions can be extended to the related eukaryotic counterpart, Rad51 (see ref.), and to regulation by assembly mediators.