Asymmetric photocross-linking of singly phosphorylated smooth muscle heavy meromyosin

Although activities of smooth muscle myosin are regulated by phosphorylation, the molecular mechanisms of regulation have not been fully established. Phosphorylation of both heads of myosin is known to activate ATPase and motor activities, but the effects of phosphorylation of only one of the heads have not been established. Such information on singly phosphorylated myosin can serve to elucidate the molecular mechanism of the phosphorylation-dependent regulation. To understand the structural properties of the singly phosphorylated state, we prepared singly phosphorylated heavy meromyosin (HMM) containing a photoreactive benzophenone-labeled RLC and examined its photocross-linking reactivity. The two heads in the singly phosphorylated HMM showed different reactivities. The dephosphorylated RLC in the singly phosphorylated HMM was cross-linked to a heavy chain, like that in the dephosphorylated HMM, whereas the phosphorylated RLC did not react, like that in the fully phosphorylated HMM. These results indicate that the two heads of the singly phosphorylated HMM have an asymmetric structure, suggesting that phosphorylation of one head can to some extent activate smooth muscle HMM.     

The interaction between the regulatory light chain domains on two heads is critical for regulation of smooth muscle myosin

Recent findings have suggested that the interaction between the two heads is critical for phosphorylation-dependent regulation of smooth muscle myosin. We hypothesized that the interaction between the two regulatory light chains on two heads of myosin dictates the regulation of myosin motor function. To evaluate this notion, we engineered and characterized smooth muscle heavy meromyosin (HMM), which is composed of one entire HMM heavy chain and one motor domain truncated heavy chain containing the S2 rod and regulatory light chain (RLC) binding site, as well as the bound RLC (SMDHMM). SMDHMM was inactive for both actin-translocating activity and actin-activated ATPase activity in the dephosphorylated state, demonstrating that the interaction between the two RLC domains on the two heads and/or a motor domain and a RLC domain in a distinct head is sufficient for the inhibition of smooth muscle myosin motor activity. When phosphorylated, SMDHMM was activated for both actin-translocating activity and actin-activated ATPase activity; however, these activities were lower than those of double-headed HMM, implying partial release of inhibition by phosphorylation in SMDHMM and/or cooperativity between the two heads of smooth muscle myosin. The present results indicate that the RLC domain is critical for phosphorylation-dependent regulation of smooth muscle myosin motor activity. On the other hand, similar to double-headed HMM, SMDHMM showed both "folded" and "extended" conformations, and the ratio of those conformations is dependent on ionic strength, suggesting that the RLC domain is sufficient to regulate the conformational transition in myosin.     

The apparently negatively cooperative phosphorylation of smooth muscle myosin at low ionic strength is related to its filamentous state

The correlation curve between phosphorylation and MgATPase activity suggests that the 20,000-dalton light chain of both heads of a smooth muscle myosin or heavy meromyosin (HMM) molecule must be phosphorylated before the MgATPase activity of either head can be activated by actin. The two heads of HMM appear to be phosphorylated randomly at equal rates, while those of myosin are phosphorylated in a negatively cooperative manner (Persechini, A., and Hartshorne, D.J. (1981) Science, 213, 1383-1385; Ikebe, M., Ogihara, S., and Tonomura, Y. (1982) J. Biochem. 91, 1809-1812). We have investigated the cause of this difference between HMM and myosin. We find that if myosin is first phosphorylated at high ionic strength (0.6 M KCl), where it is monomeric, and then assayed for MgATPase activity (in 0.05 M KCl), the data support a model where the two heads are phosphorylated randomly with equal rates (i.e. similarly to HMM). The correlation curves between MgATPase activity and dephosphorylation of fully phosphorylated myosin, both in a filamentous and monomeric state, are also best explained by a model where dephosphorylation of one head is sufficient to deactivate the entire molecule. With monomeric myosin, the dephosphorylation appears to occur randomly with equal rates, whereas with filamentous myosin the dephosphorylation appears to be negatively cooperative. The correlation between dephosphorylation of HMM and its MgATPase activity is more complex and is consistent with a positively cooperative dephosphorylation. Direct analyses of the time courses of phosphorylation of HMM and monomeric myosin show that a single exponential is sufficient to fit the data through greater than 90% of the reaction. However, when phosphorylation is carried out at low ionic strength (0.02 M KCl), where myosin is present as filaments, the time course consists of two exponential functions where the rate constant for the phosphorylation of one myosin head is 6-10 times greater than that for the other head which is located on the same molecule. This suggests that when myosin is polymerized into filaments the two previously indistinguishable heads either become nonequivalent or are subject to head-head interactions leading to a negatively cooperative phosphorylation reaction.     

Role of the essential light chain in the activation of smooth muscle myosin by regulatory light chain phosphorylation

The activity of smooth and non-muscle myosin II is regulated by phosphorylation of the regulatory light chain (RLC) at serine 19. The dephosphorylated state of full-length monomeric myosin is characterized by an asymmetric intramolecular head–head interaction that completely inhibits the ATPase activity, accompanied by a hairpin fold of the tail, which prevents filament assembly. Phosphorylation of serine 19 disrupts these head–head interactions by an unknown mechanism. Computational modeling (Tama et al., 2005. J. Mol. Biol. 345, 837–854) suggested that formation of the inhibited state is characterized by both torsional and bending motions about the myosin heavy chain (HC) at a location between the RLC and the essential light chain (ELC). Therefore, altering relative motions between the ELC and the RLC at this locus might disrupt the inhibited state. Based on this hypothesis we have derived an atomic model for the phosphorylated state of the smooth muscle myosin light chain domain (LCD). This model predicts a set of specific interactions between the N-terminal residues of the RLC with both the myosin HC and the ELC. Site directed mutagenesis was used to show that interactions between the phosphorylated N-terminus of the RLC and helix-A of the ELC are required for phosphorylation to activate smooth muscle myosin.     

Mechanism of smooth muscle myosin phosphorylation

In vertebrate smooth muscles, phosphorylation of the regulatory light chain appears to be necessary for actin activation of the Mg-ATPase activity and for the in vitro assembly of myosin into filaments. From a correlation between the degree of phosphorylation and enzymatic activity, it was suggested that both myosin heads must be phosphorylated before either head could be activated by actin, and that phosphorylation of filamentous myosin occurred in a negatively cooperative manner (Persechini, A., and Hartshorne, D. J. (1981) Science 213, 1383-1385; Ikebe, M., Ogihara, S., and Tonomura, Y. (1982) J. Biochem. (Tokyo) 91, 1809-1812; Sellers, J. R., Chock, P. B., and Adelstein, R. S. (1983) J. Biol. Chem. 258, 14181-14188). Here we have determined the mechanism of phosphorylation by separating dephosphorylated and phosphorylated myosin species based on their different structural properties in the minifilament buffer system (5 mM citrate, 22 mM Tris). Fully phosphorylated myosin remained assembled as minifilaments in 1 mM Mg-ATP, but dephosphorylated myosin dissociated to a mixture of folded monomers and dimers. Gel filtration was used to separate these two structures. At intermediate levels of phosphorylation, the relative amount of myosin that formed minifilament and dimer and the degree of phosphorylation of the separated species relative to the initial level of phosphorylation was measured. From these data, it was possible to deduce that singly and doubly phosphorylated myosin remained assembled in the presence of nucleotide. Myosin molecules with 0, 1, or 2 heads phosphorylated could also be separated by nondenaturing gel electrophoresis. The amount of myosin which formed each species was quantitated as a function of phosphorylation. Results from the combined approaches are consistent with a model in which light chain kinase randomly phosphorylates myosin, independent of the state of aggregation of the myosin.     

Comparison of Orientation and Rotational Motion of Skeletal Muscle Cross-bridges Containing Phosphorylated and Dephosphorylated Myosin Regulatory Light Chain

Calcium binding to thin filaments is a major element controlling active force generation in striated muscles. Recent evidence suggests that processes other than Ca²⁺ binding, such as phosphorylation of myosin regulatory light chain (RLC) also controls contraction of vertebrate striated muscle (Cooke, R. (2011) Biophys. Rev. 3, 33–45). Electron paramagnetic resonance (EPR) studies using nucleotide analog spin label probes showed that dephosphorylated myosin heads are highly ordered in the relaxed fibers and have very low ATPase activity. This ordered structure of myosin cross-bridges disappears with the phosphorylation of RLC (Stewart, M. (2010) Proc. Natl. Acad. Sci. U.S.A. 107, 430–435). The slower ATPase activity in the dephosporylated moiety has been defined as a new super-relaxed state (SRX). It can be observed in both skeletal and cardiac muscle fibers (Hooijman, P., Stewart, M. A., and Cooke, R. (2011) Biophys. J. 100, 1969–1976). Given the importance of the finding that suggests a novel pathway of regulation of skeletal muscle, we aim to examine the effects of phosphorylation on cross-bridge orientation and rotational motion. We find that: (i) relaxed cross-bridges, but not active ones, are statistically better ordered in muscle where the RLC is dephosporylated compared with phosphorylated RLC; (ii) relaxed phosphorylated and dephosphorylated cross-bridges rotate equally slowly; and (iii) active phosphorylated cross-bridges rotate considerably faster than dephosphorylated ones during isometric contraction but the duty cycle remained the same, suggesting that both phosphorylated and dephosphorylated muscles develop the same isometric tension at full Ca²⁺ saturation. A simple theory was developed to account for this fact.     

Refined model of the 10S conformation of smooth muscle myosin by cryo-electron microscopy 3D image reconstruction

The actin-activated ATPase activity of smooth muscle myosin and heavy meromyosin (smHMM) is regulated by phosphorylation of the regulatory light chain (RLC). Complete regulation requires two intact myosin heads because single-headed myosin subfragments are always active. 2D crystalline arrays of the 10S form of intact myosin, which has a dephosphorylated RLC, were produced on a positively charged lipid monolayer and imaged in 3D at 2.0 nm resolution by cryo-electron microscopy of frozen, hydrated specimens. An atomic model of smooth muscle myosin was constructed from the X-ray structures of the smooth muscle myosin motor domain and essential light chain and a homology model of the RLC was produced based on the skeletal muscle S1 structure. The initial model of the 10S myosin, based on the previous reconstruction of smHMM, was subjected to real space refinement to obtain a quantitative fit to the density. The smHMM was likewise refined and both refined models reveal the same asymmetric interaction between the upper 50 kDa domain of the "blocked" head and parts of the catalytic, converter domains and the essential light chain of the "free" head observed previously. This observation suggests that this interaction is not simply due to crystallographic packing but is enforced by elements of the myosin heads. The 10S reconstruction shows additional alpha-helical coiled-coil not seen in the earlier smHMM reconstruction, but the location of one segment of S2 is the same in both.     

Two new modes of smooth muscle myosin regulation by the interaction between the two regulatory light chains, and by the S2 domain

Previous studies indicated that single-headed smooth muscle myosin and S1 (a single head fragment) are not regulated through phosphorylation of the regulatory light chain (RLC). To investigate the importance of the double-headedness of myosin and of the S2 region for the phosphorylation-dependent regulation, we made three types of recombinant mutant smooth muscle HMMs with one intact head and an N-terminally truncated head. The truncated head of Delta MD lacked the motor domain, that of Delta(MD+ELC) lacked the motor and essential light chain binding domains, and single-headed HMM had one intact head alone. The basal ATPase activities of the three mutants decreased as the KCl concentration became less than 0.1 M. Such a decrease was not observed for S1, which had no S2 region, suggesting that S2 is necessary for this myosin behavior. This activity decrease also disappeared when RLCs of Delta MD and Delta(MD+ELC), but that of single-headed HMM, were phosphorylated. When their RLCs were unphosphorylated, the three mutants exhibited similar actin-activated ATPase levels. However, when they were phosphorylated, the actin-activated ATPase activities of Delta MD and Delta(MD+ELC) increased to the S1 level, while that of single-headed HMM remained unchanged. Even in the phosphorylated state, the actin-activated ATPase activities of the three mutants and S1 were much lower than that of wild-type HMM. We propose that S2 has an inhibitory function that is canceled by an interaction between two phosphorylated RLCs. We also propose that a cooperative interaction between two motor domains is required for a higher level of actin activation.     

Phosphorylation of the 20,000-dalton light chain of smooth muscle myosin by the calcium-activated, phospholipid-dependent protein kinase. Phosphorylation sites and effects of phosphorylation

Smooth muscle heavy meromyosin (HMM) is phosphorylated by the Ca2+-activated phospholipid-dependent protein kinase, i.e. protein kinase C, at three sites on each 20,000-dalton light chain. Phosphorylation of three sites also is observed with isolated 20,000-dalton light chain and HMM subfragment 1. The phosphorylation sites are serine 1, serine 2, and threonine 9. Threonine is phosphorylated most rapidly followed by either serine 1 or 2. Phosphorylation of the third site occurs only on prolonged incubation. Phosphorylation is a random process. HMM phosphorylated at two sites per light chain by protein kinase C can be dephosphorylated, as shown using two phosphatase preparations. Increasing levels of phosphorylation of HMM by protein kinase C causes a progressive inhibition of the subsequent rate of phosphorylation of serine 19 by myosin light chain kinase and causes a progressive inhibition of actin-activated ATPase activity of HMM, prephosphorylated by myosin light chain kinase. Inhibition of ATPase activity is due to a decreased affinity of HMM for actin rather than a change in Vmax. Previous results with HMM and protein kinase C (Nishikawa, M., Sellers, J. R., Adelstein, R. S., and Hidaka, H. (1984) J. Biol. Chem. 259, 8808-8814) examined effects induced by phosphorylation of the threonine residues. Our results confirm these and consider also the influence of higher levels of phosphorylation by protein kinase C.     

ADP binding induces an asymmetry between the heads of unphosphorylated myosin

Light chain phosphorylation is the key event that regulates smooth and non-muscle myosin II ATPase activity. Here we show that both heads of smooth muscle heavy meromyosin (HMM) bind tightly to actin in the absence of nucleotide, irrespective of the state of light chain phosphorylation. In striking contrast, only one of the two heads of unphosphorylated HMM binds to actin in the presence of ADP, and the heads have different affinities for ADP. This asymmetry suggests that phosphorylation alters the mechanical coupling between the heads of HMM. A model that incorporates strain between the two heads is proposed to explain the data, which have implications for how one head of a motor protein can gate the response of the other.     

Supramolecular regulation of the actin-activated ATPase activity of filaments of Acanthamoeba Myosin II

Acanthamoeba myosin II has three phosphorylation sites clustered near the end of the tail of each of its two heavy chains (six phosphorylation sites/molecule). Myosin II has little or no actin-activated ATPase activity when four to six of these sites are phosphorylated. Maximal actin-activated ATPase activity is obtained when all six sites are dephosphorylated. Under assay conditions, both phosphorylated and dephosphorylated myosin II form bipolar filaments. Filaments of dephosphorylated myosin II have larger sedimentation coefficients than filaments of phosphorylated myosin II but this difference does not explain the difference in their actin-activated ATPase activities. Heteropolymers, formed by mixing soluble dephosphorylated and phosphorylated myosins and then diluting the mixture into low ionic strength buffer containing MgCl2, have sedimentation coefficients close to those of the homopolymer of phosphorylated myosin. The actin-activated ATPase activities of heteropolymers are, under most conditions, lower than the equivalent mixtures of homopolymers of dephosphorylated and phosphorylated myosins. It is concluded, therefore, that the phosphorylation of myosin tails regulates the actin-activated ATPase activity of Acanthamoeba myosin II by affecting the myosin filament as a whole rather than specifically affecting the heads of the phosphorylated myosin molecules only.     

Constitutive Phosphorylation of Cardiac Myosin Regulatory Light Chain in Vivo

In beating hearts, phosphorylation of myosin regulatory light chain (RLC) at a single site to 0.45 mol of phosphate/mol by cardiac myosin light chain kinase (cMLCK) increases Ca²⁺ sensitivity of myofilament contraction necessary for normal cardiac performance. Reduction of RLC phosphorylation in conditional cMLCK knock-out mice caused cardiac dilation and loss of cardiac performance by 1 week, as shown by increased left ventricular internal diameter at end-diastole and decreased fractional shortening. Decreased RLC phosphorylation by conventional or conditional cMLCK gene ablation did not affect troponin-I or myosin-binding protein-C phosphorylation in vivo. The extent of RLC phosphorylation was not changed by prolonged infusion of dobutamine or treatment with a β-adrenergic antagonist, suggesting that RLC is constitutively phosphorylated to maintain cardiac performance. Biochemical studies with myofilaments showed that RLC phosphorylation up to 90% was a random process. RLC is slowly dephosphorylated in both noncontracting hearts and isolated cardiac myocytes from adult mice. Electrically paced ventricular trabeculae restored RLC phosphorylation, which was increased to 0.91 mol of phosphate/mol of RLC with inhibition of myosin light chain phosphatase (MLCP). The two RLCs in each myosin appear to be readily available for phosphorylation by a soluble cMLCK, but MLCP activity limits the amount of constitutive RLC phosphorylation. MLCP with its regulatory subunit MYPT2 bound tightly to myofilaments was constitutively phosphorylated in beating hearts at a site that inhibits MLCP activity. Thus, the constitutive RLC phosphorylation is limited physiologically by low cMLCK activity in balance with low MLCP activity.     

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.     

Calcium ions modulate regulation of smooth muscle contraction mediated by phosphorylation of myosin regulatory light chains

The effect of calcium ions on conformational changes of F-actin initiated by decoration of thin filaments with phosphorylated and dephosphorylated heavy meromyosin from smooth muscles was studied by fluorescence polarization spectroscopy. It is shown that heavy meromyosin with phosphorylated regulatory light chains (pHMM) promotes structural changes of F-actin which are typical for the "strong" binding of actin to the myosin heads. Heavy meromyosin with dephosphorylated regulatory light chains (dpHMM) causes conformational changes of F-actin which are typical for the "weak" binding of actin to the myosin heads. The presence of calcium enhances the pHMM effect and attenuates the dpHMM effect. We propose that a Ca2+-dependent mechanism exists in smooth muscles which modulates the regulation of actin--myosin interaction occurring via phosphorylation of myosin regulatory light chains.     

Phosphorylation of smooth muscle myosin heads regulates the head-induced movement of tropomyosin

It has been shown that skeletal and smooth muscle myosin heads binding to actin results in the movement of smooth muscle tropomyosin, as revealed by a change in fluorescence resonance energy transfer between a fluorescence donor on tropomyosin and an acceptor on actin (Graceffa, P. (1999) Biochemistry 38, 11984-11992). In this work, tropomyosin movement was similarly monitored as a function of unphosphorylated and phosphorylated smooth muscle myosin double-headed fragment smHMM. In the absence of nucleotide and at low myosin head/actin ratios, only phosphorylated heads induced a change in energy transfer. In the presence of ADP, the effect of head phosphorylation was even more dramatic, in that at all levels of myosin head/actin, phosphorylation was necessary to affect energy transfer. It is proposed that the regulation of tropomyosin position on actin by phosphorylation of myosin heads plays a key role in the regulation of smooth muscle contraction. In contrast, actin-bound caldesmon was not moved by myosin heads at low head/actin ratios, as uncovered by fluorescence resonance energy transfer and disulfide cross-linking between caldesmon and actin. At higher head concentration caldesmon was dissociated from actin, consistent with the multiple binding model for the binding of caldesmon and myosin heads to actin (Chen, Y., and Chalovich, J. M. (1992) Biophys. J. 63, 1063-1070).     

Phosphorylation kinetics of skeletal muscle myosin and the effect of phosphorylation on actomyosin adenosinetriphosphatase activity

Purified rabbit skeletal muscle myosin is phosphorylated on one type of light-chain subunit (P-light chain) by calmodulin-dependent myosin light chain kinase and dephosphorylated by phosphoprotein phosphatase C. Analyses of the time courses of both phosphorylation and dephosphorylation of skeletal muscle myosin indicated that both reactions, involving at least 90% of the P-light chain, were kinetically homogeneous. These results suggest that phosphorylation and dephosphorylation of rabbit skeletal muscle myosin heads are simple random processes in contrast to the sequential phosphorylation mechanism proposed for myosin from gizzard smooth muscle. We also examined the effect of phosphorylation of rabbit skeletal muscle myosin on the actin-activated ATPase activity. We observed an apparent 2-fold decrease in the Km for actin, from about 6 microM to about 2.5 microM, with no significant effect on the Vmax (1.8s-1) in response to P-light-chain phosphorylation. There was no significant effect of phosphorylation on the ATPase activity of myosin alone (0.045 s-1). ATPase activation could be fully reversed by addition of phosphatase catalytic subunit. The relationship between the extents of P-light-chain phosphorylation and ATPase activation (at 3.5 microM actin and 0.6 microM myosin) was essentially linear. Thus, in contrast to results obtained with myosin from gizzard smooth muscle, these results suggest that cooperative interactions between the myosin heads do not play an important role in the activation process in skeletal muscle. Since the effect of P-light-chain phosphorylation is upon the Km for actin, it would appear to be associated with a significant activation of ATPase activity only at appropriate concentrations of actin and salt.(ABSTRACT TRUNCATED AT 250 WORDS)     

Two functional heads are required for full activation of smooth muscle myosin

The motor activity of smooth muscle myosin II is regulated by the regulatory light chain phosphorylation, but it is not understood how phosphorylation activates motor activity. To address this question, we produced asymmetric heavy meromyosin (HMM), which is composed of a wild-type (WT) heavy chain and a mutant heavy chain having no motor activity (i.e. S236T or G457A). The actin-activated ATPase activities (Vmax) of asymmetric HMMs were only 21.8 and 8.4% of the wild-type HMM for S236A/WT HMM and G456A/WT HMM, respectively. If the two heads of HMM are independent for their ATPase activities, asymmetric HMM should show 50% of the activity of wild-type HMM; however, the activity of asymmetric HMM was much lower than the expected value. The results suggest that the activity of the wild-type head is attenuated by the presence of inactive head. Consistently, the actin-gliding velocity of the asymmetric HMM (i.e. S236T/WT or G457A/WT) was less than one-fifth of the wild-type HMM. The present study supports an idea that the two heads of smooth muscle myosin II interact with each other and the presence of two active heads is required for full activation.     

Binding of phosphorylated and dephosphorylated heavy meromyosin to F-actin

The effect of myosin light chain phosphorylation in skeletal muscle was investigated with respect to the binding affinity of phosphorylated and dephosphorylated heavy meromyosin (HMM) for F-actin in the absence of ATP. For phosphorylated HMM the affinity was 2.5-times weaker in the presence of Ca²⁺ as in its absence (HMM divalent binding sites saturated only with Mg). For dephosphorylated HMM the reverse was true, the binding being 2.4-times higher in the presence of Ca²⁺.     

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.     

Phosphorylation of light chains of myosin from rabbit skeletal muscles affects the type of conformation changes of F-actin induced by heavy meromyosin

The changes in F-actin conformation in myosin-free single ghost fiber induced by the binding of heavy meromyosin (HMM) with dephosphorylated or phosphorylated light chains-2 (LC2) have been studied by measuring intrinsic tryptophan polarized fluorescence of F-actin. It has been found that at low concentrations of Ca2+ (pCa greater than or equal to 8), the binding of HMM with dephosphorylated LC2 to F-actin in ghost fibres increases, whereas the binding of HMM with phosphorylated LC2 decreases the anisotropy of polarized tryptophan fluorescence. The effect is reversed at high concentrations of Ca2+ (pCa = 5). It has been assumed that this effect of myosin light chains phosphorylation may be due to its influence on the type of myosin head binding to F-actin.