Cryoenzymic studies on myosin: transient kinetic evidence for two types of head with different ATP binding properties

The two step tight binding of ATP to myosin, heavy meromyosin and myosin subfragment 1 was investigated, under cryoenzymic conditions by the unlabeled ATP chase method: M + ATP in equilibrium K1 M.ATP k2 in equilibrium k-2 M*.ATP where M is myosin. k-2 is close to zero. In multi-turnover experiments, one obtains the constants for the binding process together with the concentration of ATPase sites. Here the kinetics of the formation of M*.ATP are first order. Inversion of the reagent concentrations (i.e., single-turnover experiments) should give identical kinetics but such experiments often give biphasic curves. This biphasicity depends upon the myosin preparation used and it is directly related to the active site titration. The simplest explanation for these results is one involving 2 sites for ATP: one site hydrolyzes ATP by the Bagshaw-Trentham scheme (tight binding preceding hydrolysis) but the second site binds ATP loosely without significant hydrolysis. This heterogeneity in ATP binding may explain certain difficulties, such as questions concerning the non-identity of the myosin heads and the number of steps involved in nucleotide binding. Attempts were made to determine the cause of the head heterogeneity but these were unsuccessful. We cannot exclude the possibility that the heterogeneity is relevant to muscle contraction.     

Phosphorylation of a single head of smooth muscle myosin activates the whole molecule

Regulatory light chain (RLC) phosphorylation activates smooth and non-muscle myosin II, but it has not been established if phosphorylation of one head turns on the whole molecule. Baculovirus expression and affinity chromatography were used to isolate heavy meromyosin (HMM) containing one phosphorylated and one dephosphorylated RLC (1-P HMM). Motility and steady-state ATPase assays indicated that 1-P HMM is nearly as active as HMM with two phosphorylated heads (2-P HMM). Single-turnover experiments further showed that both the dephosphorylated and phosphorylated heads of 1-P HMM can be activated by actin. Singly phosphorylated full-length myosin was also an active species with two cycling heads. Our results suggest that phosphorylation of one RLC abolishes the asymmetric inhibited state formed by dephosphorylated myosin [Liu, J., et al. (2003) J. Mol. Biol. 329, 963-972], allowing activation of both the phosphorylated and dephosphorylated heads. These findings help explain how smooth muscles are able to generate high levels of stress with low phosphorylation levels.     

Transient interaction between the N-terminal extension of the essential light chain-1 and motor domain of the myosin head during the ATPase cycle

The molecular mechanism of muscle contraction is based on the ATP-dependent cyclic interaction of myosin heads with actin filaments. Myosin head (myosin subfragment-1, S1) consists of two major domains, the motor domain responsible for ATP hydrolysis and actin binding, and the regulatory domain stabilized by light chains. Essential light chain-1 (LC1) is of particular interest since it comprises a unique N-terminal extension (NTE) which can bind to actin thus forming an additional actin-binding site on the myosin head and modulating its motor activity. However, it remains unknown what happens to the NTE of LC1 when the head binds ATP during ATPase cycle and dissociates from actin. We assume that in this state of the head, when it undergoes global ATP-induced conformational changes, the NTE of LC1 can interact with the motor domain. To test this hypothesis, we applied fluorescence resonance energy transfer (FRET) to measure the distances from various sites on the NTE of LC1 to S1 active site in the motor domain and changes in these distances upon formation of S1-ADP-BeF_x complex (stable analog of S1¹-AТP state). For this, we produced recombinant LC1 cysteine mutants, which were first fluorescently labeled with 1,5-IAEDANS (donor) at different positions in their NTE and then introduced into S1; the ADP analog (TNP-ADP) bound to the S1 active site was used as an acceptor. The results show that formation of S1-ADP-BeF_x complex significantly decreases the distances from Cys residues in the NTE of LC1 to TNP-ADP in the S1 active site; this effect was the most pronounced for Cys residues located near the LC1 N-terminus. These results support the concept of the ATP-induced transient interaction of the LC1 N-terminus with the S1 motor domain.     

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.     

Mechanochemical coupling in actomyosin energy transduction studied by in vitro movement assay

In order to study the mechanochemical coupling in actomyosin energy transduction, the sliding distance of an actin filament induced by one ATP hydrolysis cycle was obtained by using an in vitro movement assay that permitted quantitative and simultaneous measurements of (1) the movements of single fluorescently labeled actin filaments on myosin bound to coverslip surfaces and (2) the ATPase rates. The sliding distance was determined as (the working stroke time in one ATPase cycle, tws) x (the filament velocity, v). tws was obtained from the ATPase turnover rate of myosin during the sliding (kt), the ATP hydrolysis time (delta t) and the ON-rate at which myosin heads enter into the working stroke state when they encounter actin (kON); tws approximately 1/kt-delta t-1/kON. kt was estimated from the ATPase rates of the myosin-coated surface during the sliding of actin filaments. delta t has been determined as less than 1/100 per second, kON was estimated by analyzing the movements of very short (40 nm) filaments. The resulting sliding distance during one ATP hydrolysis cycle near zero load was greater than 100 nm, which is about ten times longer than that expected for a single attachment-detachment cycle between an actin and a myosin head. This leads to the conclusion that the coupling between the ATPase and attachment-detachment cycles is not determined rigidly in a one-to-one fashion.     

The phosphorylated L2 light chain of skeletal myosin is a modifier of the actomyosin ATPase

Incubation of rabbit skeletal myosin with an extract of light chain kinase plus ATP phosphorylated the L2 light chain and modified the steady state kinetics of the actomyosin ATPase. With regulated actin, the ATPase activity of phosphorylated myosin (P-myosin) was 35 to 181% greater than that of unphosphorylated myosin when assayed with 0.05 to 5 micro M Ca2+. Phosphorylation had no effect on the Ca2+ concentration required for half-maximal activity, but it did increase the ATPase activity at low Ca2+. With pure actin, the percentage of increase in the actomyosin ATPase activity correlated with the percentage of phosphorylation of myosin. Steady state kinetic analyses of the actomyosin system indicated that 50 to 82% phosphorylation of myosin decreased significantly the Kapp of actin for myosin with no significant effect on the Vmax. Phosphorylaton of heavy meromyosin similarly modified the steady state kinetics of the acto-heavy meromyosin system. Both the K+/EDTA- and Mg-ATPase activities of P-myosin and phosphorylated heavy meromyosin were within normal limits indicating that phosphorylaiion had not altered significantly the hydrolytic site. Phosphatase treatment of P-myosin decreased both the level of phosphorylation of L2 and the actomyosin ATPase activity to control levels for unphosphorylated myosin. It is concluded levels for unphosphorylated myosin. It is concluded from these results that the ability of P-myosin to modify the steady state kinetics of the actomyosin ATPase was: 1) specific for phosphorylation; 2) independent of the thin filament regulatory proteins.     

Mechanism of nucleotide binding to actomyosin VI: evidence for allosteric head-head communication

We have examined the kinetics of nucleotide binding to actomyosin VI by monitoring the fluorescence of pyrene-labeled actin filaments. ATP binds single-headed myosin VI following a two-step reaction mechanism with formation of a low affinity collision complex (1/K(1)' = 5.6 mm) followed by isomerization (k(+2)' = 176 s-1) to a state with weak actin affinity. The rates and affinity for ADP binding were measured by kinetic competition with ATP. This approach allows a broader range of ADP concentrations to be examined than with fluorescent nucleotide analogs, permitting the identification and characterization of transiently populated intermediates in the pathway. ADP binding to actomyosin VI, as with ATP binding, occurs via a two-step mechanism. The association rate constant for ADP binding is approximately five times greater than for ATP binding because of a higher affinity in the collision complex (1/K(5b)' = 2.2 mm) and faster isomerization rate constant (k(+5a)' = 366 s(-1)). By equilibrium titration, both heads of a myosin VI dimer bind actin strongly in rigor and with bound ADP. In the presence of ATP, conditions that favor processive stepping, myosin VI does not dwell with both heads strongly bound to actin, indicating that the second head inhibits strong binding of the lead head to actin. With both heads bound strongly, ATP binding is accelerated 2.5-fold, and ADP binding is accelerated >10-fold without affecting the rate of ADP release. We conclude that the heads of myosin VI communicate allosterically and accelerate nucleotide binding, but not dissociation, when both are bound strongly to actin.     

Direct visualization by electron microscopy of the weakly bound intermediates in the actomyosin adenosine triphosphatase cycle.

We used a novel stopped-flow/rapid-freezing machine to prepare the transient intermediates in the actin-myosin adenosine triphosphatase (ATPase) cycle for direct observation by electron microscopy. We focused on the low affinity complexes of myosin-adenosine triphosphate (ATP) and myosin-adenosine diphosphate (ADP)-Pi with actin filaments since the transition from these states to the high affinity actin-myosin-ADP and actin-myosin states is postulated to generate the molecular motion that drives muscle contraction and other types of cellular movements. After rapid freezing and metal replication of mixtures of myosin subfragment-1, actin filaments, and ATP, the structure of the weakly bound intermediates is indistinguishable from nucleotide-free rigor complexes. In particular, the average angle of attachment of the myosin head to the actin filament is approximately 40 degrees in both cases. At all stages in the ATPase cycle, the configuration of most of the myosin heads bound to actin filaments is similar, and the part of the myosin head preserved in freeze-fracture replicas does not tilt by more than a few degrees during the transition from the low affinity to high affinity states. In contrast, myosin heads chemically cross-linked to actin filaments differ in their attachment angles from ordered at 40 degrees without ATP to nearly random in the presence of ATP when viewed by negative staining (Craig, R., L.E. Greene, and E. Eisenberg. 1985. Proc. Natl. Acad. Sci. USA. 82:3247-3251, and confirmed here), freezing in vitreous ice (Applegate, D., and P. Flicker. 1987. J. Biol. Chem. 262:6856-6863), and in replicas of rapidly frozen samples. This suggests that many of the cross-linked heads in these preparations are dissociated from but tethered to the actin filaments in the presence of ATP. These observations suggest that the molecular motion produced by myosin and actin takes place with the myosin head at a point some distance from the actin binding site or does not involve a large change in the shape of the myosin head.     

Structural changes accompanying phosphorylation of tarantula muscle myosin filaments

Electron microscopy has been used to study the structural changes that occur in the myosin filaments of tarantula striated muscle when they are phosphorylated. Myosin filaments in muscle homogenates maintained in relaxing conditions (ATP, EGTA) are found to have nonphosphorylated regulatory light chains as shown by urea/glycerol gel electrophoresis and [32P]phosphate autoradiography. Negative staining reveals an ordered, helical arrangement of crossbridges in these filaments, in which the heads from axially neighboring myosin molecules appear to interact with each other. When the free Ca2+ concentration in a homogenate is raised to 10(-4) M, or when a Ca2+-insensitive myosin light chain kinase is added at low Ca2+ (10(-8) M), the regulatory light chains of myosin become rapidly phosphorylated. Phosphorylation is accompanied by potentiation of the actin activation of the myosin Mg-ATPase activity and by loss of order of the helical crossbridge arrangement characteristic of the relaxed filament. We suggest that in the relaxed state, when the regulatory light chains are not phosphorylated, the myosin heads are held down on the filament backbone by head-head interactions or by interactions of the heads with the filament backbone. Phosphorylation of the light chains may alter these interactions so that the crossbridges become more loosely associated with the filament backbone giving rise to the observed changes and facilitating crossbridge interaction with actin.     

Kinetic model of regulation of muscle protein activity.

The widely accepted steric model of calcium regulation of actin-myosin interactions in vertebrate muscles has to be completed to fit the kinetic data. It should be supposed that: (1) the thin filaments consist of functionally independent units, containing seven actin sites regulated by one troponin-tropomyosin complex; (2) actin sites become available for myosin heads only due to fluctuations of tropomyosin position; (3) binding of calcium to troponin results either in the shift of the tropomyosin equilibrium position or in the weakening of its interactions with actin strand so that the probability of effective fluctuations increases; (4) link formation between myosin head and some of the available actin site fixates the tropomyosin in such a position that the other six actin sites of the same functional unit become available for myosin too.The model gives linear kinetic scheme for the transitions of a functional unit between nine states (a “turned off” state, and eight “turned on” ones with different occupancy by myosin heads). The dependences of the apparent rate constants of actomyosin formation and dissociation upon the myosin head and substrate concentrations are obtained from the Lymn-Taylor scheme. The frequency of the actomyosin complexes dissociation is assumed to give the ATPase rate.The model fits the kinetic data on the ATP hydrolysis by myosin subfragment-1 with regulated or unregulated actin as a cofactor under various conditions. It shows a sharp dependence of activation upon the apparent affinity of the actin and myosin sites. Therefore, the model appears to be applicable to myosin controlled systems.     

Random phosphorylation of the two heads of thymus myosin and the independent stimulation of their actin-activated ATPases

Like other vertebrate nonmuscle myosins, thymus myosin contains two phosphorylatable light chains. Phosphorylation of these light chains regulates the actin-activated ATPase of this myosin. The time courses for the phosphorylation of both monomeric and filamentous thymus myosin by gizzard myosin light chain kinase fitted single exponentials to greater than 85% phosphorylation. This indicates that the two heads of thymus myosin are phosphorylated at the same rate and suggests that these phosphorylations are random processes. The actin-activated ATPases of thymus myosins with different levels of light chain phosphorylation were also determined. A linear relationship was obtained between the extent of light chain phosphorylation and stimulation of the actin-activated ATPase. Since thymus myosin appears to be phosphorylated randomly, this linear relationship indicates that phosphorylation of one head of thymus myosin stimulates the actin-activated ATPase of that head independently of the phosphorylation of the second head. The apparent random phosphorylation of thymus myosin light chains contrasts with the reported ordered phosphorylation of the light chains of filamentous smooth (gizzard) muscle myosin. Also, while the actin-activated ATPases of the two heads of thymus myosin are regulated independently, both heads of gizzard myosin must be phosphorylated before the ATPase of either head is activated by actin.     

Reaction intermediates formed by myofibrils during the ATPase reaction under relaxed conditions

The species and amounts of intermediates formed by myosin in myofibrils during the ATPase reaction under relaxed conditions were examined. The amount of total nucleotides (ADP + ATP) bound to myofibrils, determined by a centrifugation method or a rapid filtration method, was 0.86 mol/mol myosin head. The amount of bound ADP, determined as the ADP remaining in the mixture after free ADP had been rapidly converted into ATP by an ATP-regenerating system, was found to be 0.67 mol/mol myosin head. We examined the time courses of free-Pi and total-Pi (TCA-Pi) formation after adding ATP to the myofibrils. The amount of Pi bound to myofibrils, calculated by subtracting the burst size of free Pi (0.23 mol/mol myosin head) from that of TCA-Pi (0.60 mol/mol myosin head), was found to be 0.37 mol/mol myosin head. The amount of tightly bound ATP determined by an ATP-quenching method was very low (0.03 mol/mol myosin head). If there is no myosin-phosphate complex, then the amounts of the myosin-phosphate-ADP complex, MADPP, and the tightly bound myosin-ATP complex, M*ATP, are 0.37 and 0.03 mol/mol myosin head, respectively, whereas the amounts of myosin-ADP and loosely bound myosin-ATP complexes are 0.30 and 0.16 mol/mol myosin head, respectively. Thus, half of the myosin heads forms MADPP or M*ATP, and the equilibrium between MADPP and M*ATP shifts to the MADPP side. These results agree with those obtained for myosin in solution (Inoue, A., Takenaka, H., Arata, T., & Tonomura, Y. (1979) Adv. Biophys. 13, 1-194). Therefore, in relaxed myofibrils the active site of myosin does not interact with actin.     

Two-headed binding of the unphosphorylated nonmuscle heavy meromyosin.ADP complex to actin

The enzymatic and motor function of smooth muscle and nonmuscle myosin II is activated by phosphorylation of the regulatory light chains located in the head portion of myosin. Dimerization of the heads, which is brought about by the coiled-coil tail region, is essential for regulation since single-headed fragments are active regardless of the state of phosphorylation. Utilizing the fluorescence signal on binding of myosin to pyrene-labeled actin filaments, we investigated the interplay of actin and nucleotide binding to thiophosphorylated and unphosphorylated recombinant nonmuscle IIA heavy meromyosin constructs. We show that both heads of either thiophosphorylated or unphosphorylated heavy meromyosin bind very strongly to actin (K(d) < 10 nM) in the presence or absence of ADP. The heads have high and indistinguishable affinities for ADP (K(d) around 1 microM) when bound to actin. These findings are in line with the previously observed unusually loose coupling between nucleotide and actin binding to nonmuscle myosin IIA subfragment-1 (Kovács et al. (2003) J. Biol. Chem. 278, 38132.). Furthermore, they imply that the structure of the two heads in the ternary actomyosin-ADP complex is symmetrical and that the asymmetrical structure observed in the presence of ATP and the absence of actin in previous investigations (Wendt et al. (2001) Proc. Natl. Acad. Sci. U.S.A. 98, 4361) is likely to represent an ATPase intermediate that precedes the actomyosin-ADP state.     

Smooth Muscle Heavy Meromyosin Phosphorylated on One of Its Two Heads Supports Force and Motion

Smooth muscle myosin is activated by regulatory light chain (RLC) phosphorylation. In the unphosphorylated state the activity of both heads is suppressed due to an asymmetric, intramolecular interaction between the heads. The properties of myosin with only one of its two RLCs phosphorylated, a state likely to be present both during the activation and the relaxation phase of smooth muscle, is less certain despite much investigation. Here we further characterize the mechanical properties of an expressed heavy meromyosin (HMM) construct with only one of its RLCs phosphorylated (HMM-1P). This construct was previously shown to have more than 50% of the ATPase activity of fully phosphorylated myosin (HMM-2P) and to move actin at the same speed in a motility assay as HMM-2P (Rovner, A. S., Fagnant, P. M., and Trybus, K. M. (2006) Biochemistry 45, 5280–5289). Here we show that the unitary step size and attachment time to actin of HMM-1P is indistinguishable from that of HMM-2P. Force-velocity measurements on small ensembles show that HMM-1P can generate approximately half the force of HMM-2P, which may relate to the observed duty ratio of HMM-1P being approximately half that of HMM-2P. Therefore, single-phosphorylated smooth muscle HMM molecules are active species, and the head associated with the unphosphorylated RLC is mechanically competent, allowing it to make a substantial contribution to both motion and force generation during smooth muscle contraction.Myosin motors are involved in a diverse array of actin-based cellular functions including muscle contraction, cargo transport, and cytokinesis. To accomplish any of these processes successfully, there needs to be strict control of when the motor is activated and when it is turned “off.” Smooth muscle myosin, which powers smooth muscle contraction in both vascular and visceral tissues, is no exception, and the mechanism by which it is regulated has been studied for many years (for review, see Ref. 2). Smooth muscle myosin is activated when the calcium-calmodulin-myosin light chain kinase complex phosphorylates Ser-19 of the regulatory light chain (RLC)² bound to the neck of the myosin head. In the unphosphorylated state, smooth muscle myosin is unable to move actin, and the actomyosin ATPase activity is rate-limited by phosphate release so that the motor can only weakly interact with actin in the M·ADP·P_i state (3).Early studies characterized the inhibited state of myosin at physiologic ionic strength as a species that sedimented at 10 S in the ultracentrifuge, indicating that the rod must adopt a compact conformation (4, 5). Consistent with the hydrodynamic studies, metal-shadowed images showed a structure with the rod bent into nearly equal thirds and heads bent back toward the rod (6). Higher resolution cryoelectron microscopic images of two-dimensional arrays of unphosphorylated HMM revealed an asymmetric intramolecular interaction between the heads called the “blocked” and “free” heads that proposed a molecular basis for inhibition (7). The actin binding domain of the blocked head interacts with the converter domain of the free head, so that the blocked head cannot bind actin and be actin-activated. The free head is prevented from progressing through its ATPase cycle because rotation of the converter domain cannot occur due to the binding of the blocked head, and thus, the free head is locked in a weak binding state (7). These asymmetric head interactions were also observed by single particle analysis of negatively stained images of smooth muscle myosin (8). This motif appears to be a general mechanism widely used by class II myosins to maintain a relaxed or inhibited state, as it was also observed in native striated muscle myosin thick filaments from tarantula, which are regulated by phosphorylation (9), as well as in striated myosins from both vertebrates and invertebrates (10).RLC phosphorylation abolishes these interactions, allowing both heads to freely interact with actin (7, 11). Although these two endpoints are well characterized, much less is agreed upon with regard to smooth muscle myosin that has only one of its two RLCs phosphorylated. RLC phosphorylation by myosin light chain kinase is random (12–14), so myosin with only one phosphorylated RLC is a predominant species during muscle activation and perhaps during relaxation. The hydrolytic and mechanical activity of this state has been investigated for decades. In the early studies, the activity of single-phosphorylated myosin was inferred from ensemble measurements in which it existed in a mixture with both unphosphorylated and double-phosphorylated myosin. Some of these studies suggested that it has less than half the actin-activated ATPase activity of the double-phosphorylated state (15, 16), whereas others suggested that both the hydrolytic and actin filament motility was approximately half (17, 18). The former studies imply that the activation of one head does not activate the whole molecule, whereas the latter was consistent with each head acting independently of its partner.Recently, the approach to this problem has been improved by employing various methods that allow isolation of a single-phosphorylated species (1, 19, 20). Single-phosphorylated heavy meromyosin (HMM) had much less than half the hydrolytic and mechanical activity of double-phosphorylated HMM when prepared using light chain exchange or stripping protocols (19, 20). Using differential tagging of constructs expressed in Sf9 cells followed by sequential affinity columns, the single-phosphorylated HMM (HMM-1P) had more than half the ATPase activity and actin filament speeds in the in vitro motility assay that were similar to double-phosphorylated HMM (1).Here, we further characterize the mechanical properties of the expressed HMM-1P construct. An optical trap assay was used to show that the unitary step size and attachment time of an expressed single HMM-1P molecule was indistinguishable from that of double-phosphorylated HMM (HMM-2P) (1), suggesting that at least one of the heads of HMM-1P is equivalent to a head of HMM-2P. The optical trap was further used to characterize the force-velocity relationship for a small ensemble of HMM-1P molecules (21). These data showed that HMM-1P can generate approximately half the force of HMM-2P, which may relate to the observed duty ratio of HMM-1P being approximately half that of HMM-2P. The results are discussed in terms of two mechanisms that cannot be distinguished from one another based on the current data. The ability of HMM-1P to generate motion and force implies that it likely contributes to smooth muscle contraction both during activation at low phosphorylation levels as well as in maintaining tension when phosphorylation levels start to decline.     

Kinetic mechanism and regulation of myosin VI.

Myosin VI is the only pointed end-directed myosin identified and is likely regulated by heavy chain phosphorylation (HCP) at the actin-binding site in vivo. We undertook a detailed kinetic analysis of the actomyosin VI ATPase cycle to determine whether there are unique adaptations to support reverse directionality and to determine the molecular basis of regulation by HCP. ADP release is the rate-limiting step in the cycle. ATP binds slowly and with low affinity. At physiological nucleotide concentrations, myosin VI is strongly bound to actin and populates the nucleotide-free (rigor) and ADP-bound states. Therefore, myosin VI is a high duty ratio motor adapted for maintaining tension and has potential to be processive. A mutant mimicking HCP increases the rate of P(i) release, which lowers the K(ATPase) but does not affect ADP release. These measurements are the first to directly measure the steps regulated by HCP for any myosin. Measurements with double-headed myosin VI demonstrate that the heads are not independent, and the native dimer hydrolyzes multiple ATPs per diffusional encounter with an actin filament. We propose an alternating site model for the stepping and processivity of two-headed high duty ratio myosins.     

Generation of force by single-headed myosin.

Myosin has two heads, each of which can interact with actin and ATP. We have investigated the possibility that co-operative interactions occur between the heads by measuring the force generated by single-headed myosin in reconstituted actomyosin threads. Myofibrils were digested with papain, actomyosin was extracted from the myofibrils, and one-headed myosin was purified by cycles of sedimentation with actin. The one-headed myosin was approximately 90 to 95% pure as determined by densitometer scans of polyacrylamide gels run in 20 mm-PP₁ (impurities consisted of 1 to 5% of myosin and 1 to 5% myosin rod). The ATPase activity per mole of single-headed myosin was one half that of myosin under conditions where the activity was activated by Ca²⁺, K⁺ or actin. One-headed myosin could also participate in superprecipitation, although with a rate that was at least one order of magnitude slower than that for myosin. Myosin or one-headed myosin was mixed with actin, threads were formed via extrusion into low ionic strength, and the isometric forces and isotonic velocities generated by the threads were measured. The ratio of the isometric tension produced per head by the one-headed myosin to the isometric tension produced per head by myosin was 1·0 ± 0·1. The maximum velocity of thread contraction for the one-headed myosin was also not different from the control myosin. Thus, the absence of one head does not appear to impair the generation of force or motion by the remaining head.     

Functional significance of the conserved residues in the flexible hinge region of the myosin motor domain.

Analysis of the three-dimensional crystal structure of the Dictyostelium myosin motor domain revealed that the myosin head is required to bend at residues Ile-455 and Gly-457 to produce the conformation changes observed in the ternary complexes that resemble the pre- and post-hydrolysis states (Fisher, A. J., Smith, C. A., Thoden, J. B., Smith, R., Sutoh, K., Holden, H. M., and Rayment, I. (1995) Biochemistry 34, 8960-8972). Asp-454, Ile-455, and Gly-457 of smooth muscle myosin were substituted by Ala, Met, and Ala, respectively, and the mechano-enzymatic activities were determined to study the role of these residues in myosin motor function. Whereas the basal steady-state Mg2+-ATPase activity of D454A was higher than that of the wild type, the rate of the hydrolytic step is reduced approximately 2,000-fold and becomes rate-limiting. M-ATP rather than M-ADP-P is the predominant steady-state intermediate, and the initial Pi burst and the ATP-induced enhancement of intrinsic tryptophan fluorescence are absent in D454A. D454A binds actin in the absence of ATP but is not dissociated from actin by ATP. Moreover, actin inhibits rather than activates the ATPase activity; consequently, D454A does not support actin translocating activity. I455M has normal actin-activated ATPase activity, Pi burst, and ATP-induced enhancement of intrinsic tryptophan fluorescence, suggesting that the enzymatic properties are normal. However, the actin translocating activity was completely inhibited. This suggests that the side chain at Ile-455 is critical for myosin motor activity but not for relatively normal enzymatic function, which indicates an apparent uncoupling between enzymatic activity and motile function. Although G457A has normal ATP-dependent actin dissociation, ATP hydrolytic step is reduced by approximately 10(5)-fold in the presence or absence of actin; consequently, G457A does not have actin translocating activity. These results indicate the importance of these conserved residues at the hinge region for normal myosin motor function.     

Nucleotide turnover rate measured in fully relaxed rabbit skeletal muscle myofibrils

Steady state measurements of the ATP turnover rate of myosin crossbridges in relaxed living mammalian muscle or in in vitro systems are complicated by other more rapid ATPase activities. To surmount these problems we have developed a technique to measure the nucleotide turnover rate of fully relaxed myosin heads in myofibrils using a fluorescent analogue of ATP (mant-ATP). Rabbit myofibrils, relaxed in 1.6 mM ATP, were rapidly mixed with an equal volume of solution containing 80 microM mant-ATP and injected into a fluorimeter. As bound ADP is released, a fraction of the myosin active sites bind mant-ATP and fluorescence emission rises exponentially, defining a rate of nucleotide turnover of 0.03 +/- 0.001 s-1 at 25 degrees C (n = 17). This rate was approximately equal to one half that of purified myosin. The turnover rates for myosin and myofibrils increased between 5 degrees and 42 degrees C, reaching 0.16 +/- 0.04 s-1 and 0.06 +/- 0.005 s-1, respectively, at 39 degrees C, the body temperature of the rabbit. If the rate observed for purified myosin occurred in vivo, it would generate more heat than is observed for resting living muscle. When myosin is incorporated into the myofilament lattice, its ATPase activity is inhibited, providing at least a partial explanation for the low rate of heat production by living resting muscle.     

Electron microscopic evidence for the myosin head lever arm mechanism in hydrated myosin filaments using the gas environmental chamber

Muscle contraction results from an attachment–detachment cycle between the myosin heads extending from myosin filaments and the sites on actin filaments. The myosin head first attaches to actin together with the products of ATP hydrolysis, performs a power stroke associated with release of hydrolysis products, and detaches from actin upon binding with new ATP. The detached myosin head then hydrolyses ATP, and performs a recovery stroke to restore its initial position. The strokes have been suggested to result from rotation of the lever arm domain around the converter domain, while the catalytic domain remains rigid. To ascertain the validity of the lever arm hypothesis in muscle, we recorded ATP-induced movement at different regions within individual myosin heads in hydrated myosin filaments, using the gas environmental chamber attached to the electron microscope. The myosin head were position-marked with gold particles using three different site-directed antibodies. The amplitude of ATP-induced movement at the actin binding site in the catalytic domain was similar to that at the boundary between the catalytic and converter domains, but was definitely larger than that at the regulatory light chain in the lever arm domain. These results are consistent with the myosin head lever arm mechanism in muscle contraction if some assumptions are made.     

The tail domain of myosin Va modulates actin binding to one head

Calcium activates full-length myosin Va steady-state enzymatic activity and favors the transition from a compact, folded "off" state to an extended "on" state. However, little is known of how a head-tail interaction alters the individual actin and nucleotide binding rate and equilibrium constants of the ATPase cycle. We measured the effect of calcium on nucleotide and actin filament binding to full-length myosin Va purified from chick brains. Both heads of nucleotide-free myosin Va bind actin strongly, independent of calcium. In the absence of calcium, bound ADP weakens the affinity of one head for actin filaments at equilibrium and upon initial encounter. The addition of calcium allows both heads of myosin Va.ADP to bind actin strongly. Calcium accelerates ADP binding to actomyosin independent of the tail but minimally affects ATP binding. Although 18O exchange and product release measurements favor a mechanism in which actin-activated Pi release from myosin Va is very rapid, independent of calcium and the tail domain, both heads do not bind actin strongly during steady-state cycling, as assayed by pyrene actin fluorescence. In the absence of calcium, inclusion of ADP favors formation of a long lived myosin Va.ADP state that releases ADP slowly, even after mixing with actin. Our results suggest that calcium activates myosin Va by allowing both heads to interact with actin and exchange bound nucleotide and indicate that regulation of actin binding by the tail is a nucleotide-dependent process favored by linked conformational changes of the motor domain.