The binding of myosin heads on heavy meromyosin and assembled myosin to actin in the presence of nucleotides. Measurements by the proteolytic rates method

The initial rates of tryptic digestion at the 50/20-kDa junction in myosin and myosin subfragment 1 were determined for the free proteins and their complexes with actin in the presence and absence of MgATP. The proteolytic reactions were carried out at 24 degrees C and under ionic strength conditions (mu) adjusted to 35, 60, and 130 mM. The percentages of myosin heads and myosin subfragment 1 bound to actin in the presence of MgATP were calculated from the rates of proteolysis for each set of digestion experiments. In all cases, the myosin heads in the synthetic filaments showed greater binding to actin than myosin subfragment 1. This binding difference was most prominent (3-fold) at mu = 130 mM. The binding of heavy meromyosin (HMM) to actin in the presence of MgADP was measured at 4 degrees C by ultracentrifugation and the proteolytic rates methods. Ultracentrifugation experiments determined the fraction of HMM molecules bound to actin in the presence of MgADP, whereas the proteolytic measurements yielded the information on the fraction of HMM heads bound to actin. Taken together, these measurements show that a significant fraction of HMM is bound to actin with only one head in the presence of MgADP under ionic conditions of 180 and 280 mM.     

A new, smaller actin-activatable myosin subfragment 1 which lacks the 20-kDa, SH1 and SH2 peptide

The actin-dependent ATPase activity of myosin is retained in the separated heads (S1) which contain the NH2-terminal 95-kDa heavy chain fragment and one or two light chains. The S1 heavy chain can be degraded further by limited trypsin treatment into characteristic 25-, 50-, and 20-kDa peptides, in this order from the NH2-terminal end. The 20-kDa peptide contains an actin-binding site and SH1 and SH2, two thiols whose modification dramatically affects ATPase activity. By treating myosin filaments with trypsin at 4 degrees C in the presence of 2 mM MgCl2, we have now obtained preferential cleavage at the 50-20-kDa heavy chain site without any cleavage at the head-rod junction and hinge region in the rod. Incubation of these trypsinized filaments at 37 degrees C in the presence of MgATP released a new S1 fraction which lacked the COOH-terminal 20-kDa heavy chain peptide region. This fraction, termed S1'(75K), has more than 50% of the actin-activated Mg2+-ATPase activity of S1 and the characteristic Ca2+-ATPase and K+-EDTA ATPase activities of myosin. These results show that SH1 and SH2 are not essential for ATPase activity and that binding of actin to the 20-kDa region is not essential for the enhancement of the Mg2+-ATPase activity.     

Microsecond rotational dynamics of phosphorescent-labeled muscle cross-bridges

We have measured the microsecond rotational motions of myosin heads in muscle cross-bridges under physiological ionic conditions at 4 degrees C, by detecting the time-resolved phosphorescence of eosin-maleimide covalently attached to heads in skeletal muscle myofibrils. The anisotropy decay of heads in rigor (no ATP) is constant over the time range from 0.5 to 200 microsecond, indicating that they do not undergo rotational motion in this time range. In the presence of 5 mM MgATP, however, heads undergo complex rotational motion with correlation times of about 5 and 40 microsecond. The motion of heads in relaxed myofibrils is restricted out to 1 ms, as indicated by a nonzero value of the residual anisotropy. The anisotropy decay of eosin-labeled myosin, extracted from labeled myofibrils, also exhibits complex decay on the 200-microsecond time scale when assembled into synthetic thick filaments. The correlation times and amplitudes of heads in filaments (under the same ionic conditions as the myofibril experiments) are unaffected by MgATP and very similar to the values for heads in relaxed myofibrils. The larger residual anisotropy and longer correlation times seen in myofibrils are consistent with a restriction of rotational motion in the confines of the myofibril protein lattice. These are the first time-resolved measurements under physiological conditions of the rotational motions of cross-bridges in the microsecond time range.     

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.     

MgATP specifically controls in vitro self-assembly of vertebrate skeletal myosin in the physiological pH range

The appearances in the electron microscope of rat and rabbit skeletal muscle myosin filaments and rod aggregates, formed in the presence of variable amounts of MgATP, were compared at different pH values. It is shown that small amounts of MgATP, similar to those sufficient to trigger the dissociation of the actomyosin complex, were able to modify the geometry of myosin filaments profoundly in the physiological pH range, whereas the conformation of rod aggregates remained unchanged even in the presence of high concentrations of MgATP. Myosin filaments formed in the absence of MgATP displayed the classical spindle-shaped conformation and variable diameters at all pH values, whereas myosin filaments formed in the presence of MgATP in the physiological pH range had constant diameters, similar to those of natural thick filaments. These filaments of constant diameter frayed, rapidly and reversibly, into two types of subfilaments with respective diameters of 4 to 5 nm and 9 to 10 nm, when the pH of the medium was raised above 7.2. Spindle-shaped myosin filaments and rod aggregates remained unchanged by such small changes in pH. It was possible to change the conformation of preformed spindle-shaped filaments by simply adding MgATP to the medium, but this reaction was slow and took several hours to be completed. Relatively high concentrations of MgATP, similar to those in the living cell, increased the solubility of both myosin filaments and rod aggregates in the alkaline pH range (pH greater than or equal to 7.0). Low pH values (less than or equal to 6.5) and excess free Mg2+ (greater than or equal to 6 to 7 mM) abolished both the specific effect of MgATP on myosin filament conformation and its solubilizing effect on both myosin filaments and rod aggregates. The degree of purity of the myosin preparations and the level of phosphorylation of the LC-2 light chains did not influence filament behaviour noticeably and rat and rabbit myosins behaved similarly.     

Multiple structures of thick filaments in resting cardiac muscle and their influence on cross-bridge interactions.

Based on two criteria, the tightness of packing of myosin rods within the backbone of the filament and the degree of order of the myosin heads, thick filaments isolated from a control group of rat hearts had three different structures. Two of the structures of thick filaments had ordered myosin heads and were distinguishable from each other by the difference in tightness of packing of the myosin rods. Depending on the packing, their structure has been called loose or tight. The third structure had narrow shafts and disordered myosin heads extending at different angles from the backbone. This structure has been called disordered. After phosphorylation of myosin-binding protein C (MyBP-C) with protein kinase A (PKA), almost all thick filaments exhibited the loose structure. Transitions from one structure to another in quiescent muscles were produced by changing the concentration of extracellular Ca. The probability of interaction between isolated thick and thin filaments in control, PKA-treated preparations, and preparations exposed to different Ca concentrations was estimated by electron microscopy. Interactions were more frequent with phosphorylated thick filaments having the loose structure than with either the tight or disordered structure. In view of the presence of MgATP and the absence of Ca, the interaction between the myosin heads and the thin filaments was most likely the weak attachment that precedes the force-generating steps in the cross-bridge cycle. These results suggest that phosphorylation of MyBP-C in cardiac thick filaments increases the probability of cross-bridges forming weak attachments to thin filaments in the absence of activation. This mechanism may modulate the number of cross-bridges generating force during activation.     

Human platelet myosin. II. In vitro assembly and structure of myosin filaments

We have used electron microscopy and solubility measurements to investigate the assembly and structure of purified human platelet myosin and myosin rod into filaments. In buffers with ionic strengths of less than 0.3 M, platelet myosin forms filaments which are remarkable for their small size, being only 320 nm long and 10-11 nm wide in the center of the bare zone. The dimensions of these filaments are not affected greatly by variation of the pH between 7 and 8, variation of the ionic strength between 0.05 and 0.2 M, the presence or absence of 1 mM Mg++ or ATP, or variation of the myosin concentration between 0.05 and 0.7 mg/ml. In 1 mM Ca++ and at pH 6.5 the filaments grow slightly larger. More than 90% of purified platelet myosin molecules assemble into filaments in 0.1 M KC1 at pH 7. Purified preparations of the tail fragment of platelet myosin also form filaments. These filaments are slightly larger than myosin filaments formed under the same conditions, indicating that the size of the myosin filaments may be influenced by some interaction between the head and tail portions of myosin molecules. Calculations based on the size and shape of the myosin filaments, the dimensions of the myosin molecule and analysis of the bare zone reveal that the synthetic platelet myosin filaments consists of 28 myosin molecules arranged in a bipolar array with the heads of two myosin molecules projecting from the backbone of the filament at 14-15 nm intervals. The heads appear to be loosely attached to the backbone by a flexible portion of the myosin tail. Given the concentration of myosin in platelets and the number of myosin molecules per filament, very few of these thin myosin filaments should be present in a thin section of a platelet, even if all of the myosin molecules are aggregated into filaments.     

Kinetic rates of tryptic digestion of bovine cardiac myofibrils. An improved measurement of cross-bridge dissociation

The rates of tryptic digestion of the 50/20-kDa junction in myosin in cardiac myofibrils were determined under various solvent conditions. This cleavage reaction is slow in the rigor solvent and proceeds at a fast rate in the presence of MgATP. When the reaction solvent contains 50% ethylene glycol, the digestion of myosin in the presence of MgATP occurs at the same rate as in myofibrils relaxed by Mg adenyl-5'-yl imidodiphosphate (AMP-PNP). It is shown that with the help of two reference rates of digestion, for attached and dissociated myosin heads, the initial cleavage rates of myosin in the presence of nucleotides accurately measure the dissociation of cross-bridges from actin in myofibrils. Under physiological salt conditions and at 24 degrees C, MgADP, MgPPi, and MgAMP-PNP cause only small cross-bridge detachment (less than or equal to 15%) in cardiac myofibrils. The dissociation of myosin from actin is greatly increased by lowering the solvent temperature to 4 degrees C. Lowering the salt concentration of the solvent from 0.1 to 0.01 M NaCl has the most pronounced effect on the rates of myosin digestion in the presence of MgATP. In the low salt medium a substantial fraction of myosin heads (at least 30%) appears to be attached to actin in the presence of 5 mM MgATP.     

Characterizations of cross-bridges in the presence of saturating concentrations of MgAMP-PNP in rabbit permeabilized psoas muscle.

Several earlier studies have led to different conclusions about the complex of myosin with MgAMP-PNP. It has been suggested that subfragment 1 of myosin (S1)-MgAMP-PNP forms an S1-MgADP-like state, an intermediate between the myosin S1-MgATP and myosin S1-MgADP states or a mixture of cross-bridge states. We suggest that the different states observed result from the failure to saturate S1 with MgAMP-PNP. At saturating MgAMP-PNP, the interaction of myosin S1 with actin is very similar to that which occurs in the presence of MgATP. 1) At 1 degrees C and 170 mM ionic strength the equatorial x-ray diffraction intensity ratio I11/I10 decreased with an increasing MgAMP-PNP concentration and leveled off by approximately 20 mM MgAMP-PNP. The resulting ratio was the same for MgATP-relaxed fibers. 2) The two dimensional x-ray diffraction patterns from MgATP-relaxed and MgAMP-PNP-relaxed bundles are similar. 3) The affinity of S1-MgAMP-PNP for the actin-tropomyosin-troponin complex in solution in the absence of free calcium is comparable with that of S1-MgATP. 4) In the presence of calcium, I11/I10 decreased toward the relaxed value with increasing MgAMP-PNP, signifying that the affinity between cross-bridge and actin is weakened by MgAMP-PNP. 5) The degree to which the equatorial intensity ratio decreases as the ionic strength increases is similar in MgAMP-PNP and MgATP. Therefore, results from both fiber and solution studies suggest that MgAMP-PNP acts as a non hydrolyzable MgATP analogue for myosin.     

Polymerization of vertebrate non-muscle and smooth muscle myosins

We investigated how light chain phosphorylation controls the stability of filaments of vertebrate non-muscle myosins (from bovine thymocytes and chicken intestine epithelial brush border cells) and smooth muscle myosin (from chicken gizzard) in vitro. Using a sedimentation assay, the solubilities of the myosins were determined by measuring the amounts of myosin monomers (Cm) and filaments (Cp) present under a given set of conditions as a function of the total myosin concentration (Ct). Below 200 mM-NaCl, each myosin displayed distinct "critical monomer concentrations" (Cc) for polymerization, which were dependent on the salt concentration, the state of light chain phosphorylation and the presence of MgATP. At 150 mM-NaCl, MgATP increased the Cc of non-phosphorylated brush border myosin approximately five to tenfold, thymus myosin approximately 10 to 15-fold, and gizzard myosin approximately 25 to 50-fold. When these myosins were phosphorylated, MgATP had little effect on their solubilities, and their Cc values remained low. Analytical ultracentrifugation and electron microscopy demonstrated that the myosins were present in three different conformational states under the conditions used in the sedimentation assays, i.e. filaments, extended monomer (6 S) and folded monomer (10 S). Since at equilibrium only filaments and monomers were observed, we suggest that the polymerization pathway for these myosins can be analysed in terms of a dynamic monomer-polymer equilibrium (polymer in equilibrium 6 S monomer in equilibrium 10 S monomer). At roughly physiological ionic strength, light chain dephosphorylation (in the presence of MgATP) promotes the folded state (10 S), whereas phosphorylation promotes the extended state (6 S), and thereby favours filament assembly. The relevance of the monomer-polymer equilibrium to the state of organization of the myosin in vivo is discussed.     

Effects of MgATP, MgADP, and Pi on actin movement by smooth muscle myosin.

To test the idea that the in vitro motility assay is a simplified model system for muscle contraction, the MgATP-dependent movement of actin filaments by thiophosphorylated smooth muscle myosin was characterized in the presence of the products MgADP and inorganic phosphate. The dependence of actin filament velocity on MgATP concentration was hyperbolic with a maximum velocity of 0.6 micron/s and an apparent Km = 40 microM (30 degrees C). MgADP competitively inhibited actin movement by MgATP with a Ki = 0.25 mM. Inorganic phosphate did not affect actin filament velocity in the presence of 1 mM MgATP, but competitively inhibited movement in the presence of 50 microM MgATP with a Ki = 9.5 mM. The effects of ADP and Pi on velocity agree with fiber mechanical studies, confirming that the motility assay is an excellent system to investigate the molecular mechanisms of force generation and shortening in smooth muscle. The rate at which rigor cross-bridges can be recruited to move actin filaments was observed by initiating cross-bridge cycling from rigor by flash photolysis of caged MgATP. Following the flash, which results in a rapid increase in MgATP concentration, actin filaments experienced a MgATP-dependent delay prior to achieving steady state velocity. The delay at low MgATP concentrations was interpreted as evidence that motion generating cross-bridges are slowed by a load due to a transiently high percentage of rigor cross-bridges immediately following MgATP release.     

Electric birefringence study of the solution structure of chymotrypsin-cleaved Acanthamoeba myosin II

After removal of the 66 COOH-terminal amino acids from each of its two heavy chains by chymotrypsin digestion, Acanthamoeba myosin II forms only parallel dimers under conditions in which native myosin II forms bipolar filaments (Kuznicki, J., Cote, G. P., Bowers, B., and Korn, E. D. (1985) J. Biol. Chem. 260, 1967-1972). We have studied the solution structure of the chymotrypsin-cleaved myosin II by electric birefringence. Only two species, known to be monomer and parallel dimer from previous studies, were detected. The contribution to the birefringence decay from dimer increased from about 10 to 70% as the KCl concentration was lowered from 100 mM to 0 in 50% glycerol. At all ionic strengths, the monomer had a relaxation time corrected to water at 20 degrees C of 8.2 microseconds, whereas a relaxation time of 10.3 microseconds was expected for monomers with straight rigid rods. This strongly indicates that the myosin rod in solution is bent. On the assumption that there is a single bend 26 nm from the tip of the tail, as suggested by electron microscopy, it was calculated that the average bend angle would be 110 degrees, in solution, if as seems most likely, the average angle between the two globular heads were 180 degrees. The observed relaxation time of the dimer corrected to water at 20 degrees C was 25 microseconds, independent of ionic strength, which, if the motion of the heads were unrestricted, is consistent with a structure for a parallel dimer in which either the two monomer subunits have straight rigid rods and are staggered by about 28 nm or only one is bent and the stagger is 30 nm. As described in the accompanying Appendix, either of these dimers can be assembled into a bipolar filament compatible with the apparent structure of filaments of native myosin II (Pollard, T.D. (1982) J. Cell Biol. 95, 816-825).     

A protein friction model of the actin sliding movement generated by myosin in mixtures of MgATP and MgGTP in vitro.

The sliding movement of an actin filament generated by myosin heads with MgGTP bound is much slower than that by those with MgATP bound. Nonetheless, there is a report that the actin sliding velocity at low (11-21 microM) MgATP concentrations is increased by the addition of MgGTP in a range of 1-3 mM, although the actin sliding velocity at these MgATP concentrations is larger than the maximum sliding velocity attained in the presence of MgGTP alone. The convex rise in the velocity was called "mutual sensitization of MgATP and MgGTP" in the report. Here we propose a theoretical model to account for the mutual sensitization of MgATP and MgGTP. The model is an extension of a protein friction model, accommodating the presence of two different substrates and assuming the presence of motile and non-motile myosins. This new model is in accord with the characteristics of the actin/myosin sliding movement experimentally observed in mixtures of MgATP and MgGTP. Comparison of the model with the experimental results implies that the non-motile and motile myosins are those with the "converse and correct" orientations of their heads with respect to the direction of the actin sliding movement in vitro.     

Immunoelectron microscopic studies of the ultrastructure of myosin filaments in Dictyostelium discoideum

We have examined the characteristics of myosin in situ in Dictyostelium amoebae. By an improved immunofluorescence method, we previously found rod-like structures that contain myosin, which we call "myosin rods", in amoebae (Yumura. S., and Fukui, Y. (1985) Nature, 314: 194-196). Although we prepared samples for electron microscopy using conventional chemical fixation to clarify the ultrastructure of the myosin rods, we could not find any filamentous structures similar to myosin thick filaments. Therefore, we examined the effects of chemical fixatives on the myosin rods in situ by immunofluorescence staining. When cells were fixed in more than 0.05% glutaraldehyde or more than 1% osmium tetroxide at 4 degrees C, the myosin rods disappeared. These effects did not result from loss of the antigenicity, because a monoclonal myosin-specific antibody was able to react with synthetic myosin filaments treated with 0.5% glutaraldehyde or 2% osmium tetroxide. Cells fixed by the procedure used for immunofluorescence staining were post-fixed with permissible concentrations of chemical fixatives and prepared for examination by transmission electron microscopy. We found discrete filaments of about 12 nm thickness between the microfilaments. These filaments were shown to contain myosin by immunoelectron microscopy with an immunogold probe. These filaments were thinner than synthetic myosin thick filaments formed in vitro in the presence of 10 mM MgCl2, but they were similar to those formed in the presence of 2 mM MgCl2, or under nearly physiological ionic conditions. The images after immunofluorescence and immunogold labeling both suggested that these 12-nm-thick filaments in Dictyostelium amoebae were myosin filaments in situ.     

Class VI myosin moves processively along actin filaments backward with large steps.

Among a superfamily of myosin, class VI myosin moves actin filaments backwards. Here we show that myosin VI moves processively on actin filaments backwards with large ( approximately 36 nm) steps, nevertheless it has an extremely short neck domain. Myosin V also moves processively with large ( approximately 36 nm) steps and it is believed that myosin V strides along the actin helical repeat with its elongated neck domain that is critical for its processive movement with large steps. Myosin VI having a short neck cannot take this scenario. We found by electron microscopy that myosin VI cooperatively binds to an actin filament at approximately 36 nm intervals in the presence of ATP, raising a hypothesis that the binding of myosin VI evokes "hot spots" on actin filaments that attract myosin heads. Myosin VI may step on these "hot spots" on actin filaments in every helical pitch, thus producing processive movement with 36 nm steps.     

The two actin-binding regions on the myosin heads of cardiac muscle

In the presence of myosin S1 or myosin heads, actin filaments tend to form bundles. The biological meaning of the bundling of actin filaments has been unclear. In this study, we found that the cardiac myosin heads can form the bundles of actin filaments more rapidly than can skeletal S1, as monitored by light scattering and electron microscopy. Moreover, the actin bundles formed by cardiac S1 were found to be more stable against mechanical agitation. The distance between actin filaments in the bundles was approximately 20 nm, which is comparable to the length of a myosin head and two actin molecules. This suggests the direct binding of S1 tails to the adjacent actin filament. The "essential" light chain of cardiac myosin could be cross-linked to the actin molecule in the bundle. When monomeric actin molecules were added to the bundle, the bundles could be dispersed into individual filaments. The three-dimensional structure of the dispersed actin filaments was reconstructed from electron cryo-microscopic images of the single actin filaments dispersed by monomer actin. We were able to demonstrate that cardiac myosin heads bind to two actin molecules: one actin molecule at the conventional actin-binding region and the other at the essential light-chain-binding region. This capability of cardiac myosin heads to bind two actin molecules is discussed in view of lower ATPase activity and slower shortening velocity than those of skeletal ones.     

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.     

Binding of myosin to actin in myofibrils during ATP hydrolysis

Measurements of cross-bridge attachment to actin in myofibrils during ATP hydrolysis require prior fixation of myofibrils to prevent their contraction. The optimal cross-linking of myofibrils was achieved by using 10 mM carbodiimide (EDC) under rigor conditions and at 4 degrees C. The fixed myofibrils had elevated MgATPase activity (150%) and could not contract. As judged by chymotryptic digestions and subsequent SDS gel electrophoresis analysis, less than 25% of myosin heads were cross-linked in these myofibrils. The isolated, un-cross-linked myosin heads showed pH-dependent Ca2+- and EDTA(K+)-ATPase activities similar to those of standard intact S-1. For measurements of myosin binding to actin, the modified myofibrils were digested with trypsin at a weight ratio of 1:50 under rigor, relaxed, and active-state conditions. Aliquots of tryptic digestion reactions were then cleaved with chymotrypsin to yield isolated myosin heads and their fragments. Analysis of the decay of myosin heavy-chain bands on SDS gels yielded the rates of myosin cleavage under all conditions and enabled the measurements of actomyosin binding in myofibrils in the presence of MgATP. Using this approach, we detected rigorlike binding of 25 +/- 6% of myosin heads to actin in myofibrils during ATP hydrolysis.     

Subunit exchange between smooth muscle myosin filaments

Filaments formed from phosphorylated smooth muscle myosin are stable in the presence of MgATP, whereas dephosphorylated filaments are disassembled to a mixture of folded monomers and dimers. The stability of copolymers of phosphorylated and dephosphorylated myosin was, however, unknown. Gel filtration, sedimentation velocity, and pelleting assays were used to show that MgATP could dissociate dephosphorylated myosin from copolymers containing either rod and myosin or dephosphorylated and phosphorylated myosin. Copolymers were typically formed by dialyzing monomeric mixtures into filament-forming buffer but, unexpectedly, could also be formed within minutes of mixing preformed rod and myosin minifilaments. This result suggested that molecules can rapidly and extensively exchange between filaments, presumably via the monomeric pool of myosin in equilibrium with polymer. An exchange of molecules between filaments was demonstrated directly by electron microscopy using gold-labeled streptavidin or antibody to detect the exchanged species. By this approach it was shown that smooth muscle myosin filaments, like other macromolecular assemblies, are dynamic structures that can readily alter their composition in response to changing solvent conditions. Moreover, because folded monomeric myosin is unable to polymerize, these experiments suggest a mechanism for the disassembly of the filament by MgATP.     

MgATP binding changes neither the shape nor the flexibility of the heads of single myosin molecules.

The structural mechanism by which myosin heads exert force is unknown. One possibility is that the tight binding of the heads to actin drives them into a force-generating configuration. Another possibility is that the force-generating conformational change is inherent to the myosin heads. In this case the heads would make force by changing their shape according to the species of nucleotide in their active sites, the tight attachment to actin serving only to provide traction. To test this latter possibility, we used negative stain electron microscopy to search for a MgATP-induced shape change in the heads of single myosin molecules. We compared the heads of 10S smooth muscle myosin monomers (wherein MgATP is trapped at the active site) with the MgATP-free heads of 6S monomers. We found that to a resolution of about 2 nm, MgATP binding to the unrestrained myosin head does not drive it to change its shape or its flexibility. This result suggests that the head makes force by virtue of an induced fit to actin.