The myosin cross-bridge cycle and its control by twitchin phosphorylation in catch muscle

The anterior byssus retractor muscle of Mytilus edulis was used to characterize the myosin cross-bridge during catch, a state of tonic force maintenance with a very low rate of energy utilization. Addition of MgATP to permeabilized muscles in high force rigor at pCa > 8 results in a rapid loss of some force followed by a very slow rate of relaxation that is characteristic of catch. The fast component is slowed 3-4-fold in the presence of 1 mM MgADP, but the distribution between the fast and slow (catch) components is not dependent on [MgADP]. Phosphorylation of twitchin results in loss of the catch component. Fewer than 4% of the myosin heads have ADP bound in rigor, and the time course (0.2-10 s) of ADP formation following release of ATP from caged ATP is similar whether or not twitchin is phosphorylated. This suggests that MgATP binding to the cross-bridge and subsequent splitting are independent of twitchin phosphorylation, but detachment occurs only if twitchin is phosphorylated. A similar dependence of detachment on twitchin phosphorylation is seen with AMP-PNP and ATPgammaS. Single turnover experiments on bound ADP suggest an increase in the rate of release of ADP from the cross-bridge when catch is released by phosphorylation of twitchin. Low [Ca(2+)] and unphosphorylated twitchin appear to cause catch by 1) markedly slowing ADP release from attached cross-bridges and 2) preventing detachment following ATP binding to the rigor cross-bridge.     

Protein phosphatase 2B dephosphorylates twitchin, initiating the catch state of invertebrate smooth muscle

"Catch" is the state where some invertebrate muscles sustain high tension for long periods at low ATP hydrolysis rates. Physiological studies using muscle fibers have not yet fully provided the details of the initiation process of the catch state. The process was extensively studied by using an in vitro reconstitution assay with several phosphatase inhibitors. Actin filaments bound to thick filaments pretreated with the soluble protein fraction of muscle homogenate and Ca2+ (catch treatment) in the presence of MgATP at a low free Ca2+ concentration (the catch state). Catch treatment with > 50 microm okadaic acid, > 1 microm microcystin LR, 1 microm cyclosporin A, 1 microm FK506, or 0.2 mm calcineurin autoinhibitory peptide fragment produced almost no binding of the actin filaments, indicating protein phosphatase 2B (PP2B) was involved. Use of bovine calcineurin (PP2B) and its activator calmodulin instead of the soluble protein fraction initiated the catch state, indicating that only PP2B and calmodulin in the soluble protein fraction are essential for the initiation process. The initiation was reproduced with purified actin, myosin, twitchin, PP2B, and calmodulin. 32P autoradiography showed that only twitchin was dephosphorylated during the catch treatment with either the soluble protein fraction or bovine calcineurin and calmodulin. These results indicate that PP2B directly dephosphorylates twitchin and initiates the catch state and that no other component is required for the initiation process of the catch state.     

Regulation of catch bonds by rate of force application

The current paradigm for receptor-ligand dissociation kinetics assumes off-rates as functions of instantaneous force without impact from its prior history. This a priori assumption is the foundation for predicting dissociation from a given initial state using kinetic equations. Here we have invalidated this assumption by demonstrating the impact of force history with single-bond kinetic experiments involving selectins and their ligands that mediate leukocyte tethering and rolling on vascular surfaces during inflammation. Dissociation of bonds between L-selectin and P-selectin glycoprotein ligand-1 (PSGL-1) loaded at a constant ramp rate to a constant hold force behaved as catch-slip bonds at low ramp rates that transformed to slip-only bonds at high ramp rates. Strikingly, bonds between L-selectin and 6-sulfo-sialyl Lewis X were impervious to ramp rate changes. This ligand-specific force history effect resembled the effect of a point mutation at the L-selectin surface (L-selectinA108H) predicted to contact the former but not the latter ligand, suggesting that the high ramp rate induced similar structural changes as the mutation. Although the A108H substitution in L-selectin eliminated the ramp rate responsiveness of its dissociation from PSGL-1, the inverse mutation H108A in P-selectin acquired the ramp rate responsiveness. Our data are well explained by the sliding-rebinding model for catch-slip bonds extended to incorporate the additional force history dependence, with Ala-108 playing a pivotal role in this structural mechanism. These results call for a paradigm shift in modeling the mechanical regulation of receptor-ligand bond dissociation, which includes conformational coupling between binding pocket and remote regions of the interacting molecules.     

The N-terminal region of twitchin binds thick and thin contractile filaments: redundant mechanisms of catch force maintenance

Catch force maintenance in invertebrate smooth muscles is probably mediated by a force-bearing tether other than myosin cross-bridges between thick and thin filaments. The phosphorylation state of the mini-titin twitchin controls catch. The C-terminal phosphorylation site (D2) of twitchin with its flanking Ig domains forms a phosphorylation-sensitive complex with actin and myosin, suggesting that twitchin is the tether (Funabara, D., Osawa, R., Ueda, M., Kanoh, S., Hartshorne, D. J., and Watabe, S. (2009) J. Biol. Chem. 284, 18015-18020). Here we show that a region near the N terminus of twitchin also interacts with thick and thin filaments from Mytilus anterior byssus retractor muscles. Both a recombinant protein, including the D1 and DX phosphorylation sites with flanking 7th and 8th Ig domains, and a protein containing just the linker region bind to thin filaments with about a 1:1 mol ratio to actin and K(d) values of 1 and 15 μM, respectively. Both proteins show a decrease in binding when phosphorylated. The unphosphorylated proteins increase force in partially activated permeabilized muscles, suggesting that they are sufficient to tether thick and thin filaments. There are two sites of thin filament interaction in this region because both a 52-residue peptide surrounding the DX site and a 47-residue peptide surrounding the D1 site show phosphorylation-dependent binding to thin filaments. The peptides relax catch force, confirming the region's central role in the mechanism of catch. The multiple sites of thin filament interaction in the N terminus of twitchin in addition to those in the C terminus provide an especially secure and redundant mechanical link between thick and thin filaments in catch.     

Macrophage myosin. Regulation of actin-activated ATPase, activity by phosphorylation of the 20,000-dalton light chain.

Myosin was purified from rabbit alveolar macrophages in a form that could not be activated by actin. This myosin could be phosphorylated by an endogenous myosin light chain kinase, up to 2 mol of phosphate being incorporated/mol of myosin. The site phosphorylated was located on the 20,000-dalton myosin light chain. Phosphorylation of macrophage myosin was found to be necessary for actin activation of myosin ATPase activity. Moreover, the actin-activated ATPase activity was found to vary directly with the extent of myosin phosphorylation, maximal phosphorylation (2 mol of Pi/mol of myosin) resulting in an actin-activated MgATPase activity of approximately 200 nmol of Pi/mg of myosin/min at 37 degrees C. These results establish that phosphyoyration of the 20,000-dalton light chain of myosin is sufficient to regulate the actin-activated ATPase activity of macrophage myosin.     

The steady state intermediate of scallop smooth muscle myosin ATPase and effect of light chain phosphorylation. A molecular mechanism for catch contraction

The ATP-induced difference UV-absorption spectrum of myosin isolated from the opaque portion of scallop smooth muscle (opaque myosin) was Ca2+-sensitive at 40 mM KCl and 1.5 M sucrose. On adding sucrose to 1.5 M, the turbidity of myosin decreased to 24% and the characteristic two forms of the difference spectrum, the ATP-form and ADP-form (Morita, F. (1967) J. Biol. Chem. 242, 4501-4506), were distinguishable. In the presence of Ca2+, the difference spectrum was the ATP-form first and then decayed into the ADP-form with the depletion of ATP. In the absence of Ca2+, however, only the ADP-form was observed. The ADP-form observed in the absence of Ca2+ returned to the ATP-form when the regulatory light chain-a (RLC-a), one of the regulatory light chains of opaque myosin, was phosphorylated. These results suggest that the main intermediate at the steady state of opaque myosin ATPase is converted depending on the concentration of Ca2+, from EPADP in the presence of Ca2+ to EADP in the absence of Ca2+. It changes to EPADP in the absence of Ca2+ on the phosphorylation of RLC-a. Consistent results were obtained by measuring the ATP-induced Trp-fluorescence increase of opaque myosin in the absence of sucrose. Since the opaque portion of scallop smooth muscle is known to be responsible for catch contraction (Ruegg, J.C. (1961) Proc. R. Soc. London Ser. B 154, 224-249), these findings lead us to suppose that the opaque myosin in vivo may stay in the E.ADP complex during the catch state. It changes to EPADP by the phosphorylation of RLC-a, which may terminate the catch state.     

Mechanochemical coupling in muscle: attempts to measure simultaneously shortening and ATPase rates in myofibrils.

We studied the ATPase of shortening myofibrils at 4 degrees C by the rapid flow quench method. The progress curve has three phases: a P(i) burst, a fast linear phase kF of duration tB, and a deceleration to a slow kS. We propose that kF is the ATPase of myofibrils shortening under zero external load; at tB shortening and ATPase rates are reduced by passive resistance. The total ATP consumed during the rapid shortening is ATPc. Our purpose was to obtain information on the myofibrillar shortening velocity from their ATPase progress curves. We tested tB as an indicator of shortening velocity by determining the effects of different probes upon it and the other ATPase parameters. The dependence of tB upon the initial sarcomere length was linear, giving a shortening velocity close to that of muscle fibres (Vo). The Km of ATP was larger for tB than for kF, as found with fibers for Vo and their ATPase. ADP and 2,3-butanedione monoxime, but not P(i), inhibited tB to the same extent as Vo. The delta H for tB and Vo were similar. ATPc was independent of the sarcomere length, implying that the more the myofibrils shorten, the less ATP expended per myosin head per micron shortened. We propose that tB can be used as an indicator for myofibrillar shortening velocities.     

The dependence of isometric tension, isometric ATPase activity, and shortening velocity of limulus muscle on the MgATP concentration.

The dependence of the isometric tension, the velocity of unloaded shortening, and the steady-state rate of MgATP hydrolysis on the MgATP concentration (range 0.01-5 mM MgATP) was studied in Ca-activated skinned Limulus muscle fibers. With increasing MgATP concentration the isometric tension increased to a peak at approximately 0.1 mM, and slightly decreased in the range up to 5 mM MgATP. The velocity of unloaded shortening depended on the MgATP concentration roughly according to the Michaelis-Menten law of saturation kinetics with a Michaelis-Menten constant Kv = 95 microM and a maximum shortening velocity of 0.07 muscle lengths s-1; the detachment rate of the cross-bridges during unloaded shortening was 24 s-1. The rate of MgATP splitting also depended hyperbolically on the MgATP concentration with a Michaelis-Menten constant Ka = 129 microM and a maximum turnover frequency of 0.5-1 s-1. The results are discussed in terms of a cross-bridge model based on a biochemical scheme of ATP hydrolysis by actin and myosin in solution.     

Regulation of Drosophila myosin ATPase activity by phosphorylation of myosin light chains--I. Wild-type fly

1. Two types of myosins with phosphorylated and dephosphorylated myosin light chains were prepared from Drosophila flies. The former had ATPase (Ca2(+)- and Mg2(+)-activited) activities twice those of the latter. 2. The myosin phosphorylated with crude myosin light chain kinase from flies showed ATPase (Ca2(+)- and Mg2(+)-activated) activaties twice those of the dephosphorylated myosin. 3. It is suggested that phosphorylation of myosin light chains several hours after emergence stimulates myosin ATPase activity so as to facilitate the flight function of the fruitfly.     

Skeletal muscle force and actomyosin ATPase activity reduced by nitric oxide donor

Perkins, William J., Young-Soo Han, and Gary C. Sieck.Skeletal muscle force and actomyosin ATPase activity reduced bynitric oxide donor. J. Appl. Physiol.83(4): 1326-1332, 1997.Nitric oxide (NO) may exert directeffects on actin-myosin cross-bridge cycling by modulating criticalthiols on the myosin head. In the present study, the effects of the NOdonor sodium nitroprusside (SNP; 100 µM to 10 mM) on mechanicalproperties and actomyosin adenosinetriphosphatase (ATPase) activity ofsingle permeabilized muscle fibers from the rabbit psoas muscle weredetermined. The effects ofN-ethylmaleimide (NEM; 5-250µM), a thiol-specific alkylating reagent, on mechanical properties ofsingle fibers were also evaluated. Both NEM (25 µM) and SNP (1mM) significantly inhibited isometric force and actomyosin ATPaseactivity. The unloaded shortening velocity of SNP-treated single fiberswas decreased, but to a lesser extent, suggesting that SNP effects onisometric force and actomyosin ATPase were largely due to decreased cross-bridge recruitment. The calcium sensitivity of SNP-treated singlefibers was also decreased. The effects of SNP, but not NEM, on forceand actomyosin ATPase activity were reversed by treatment with 10 mMDL-dithiothreitol, athiol-reducing agent. We conclude that the NO donor SNP inhibitscontractile function caused by reversible oxidation of contractileprotein thiols.

     

Regulation of Drosophila myosin ATPase activity by phosphorylation of myosin light chains--II. Flightless mfd- fly

1. The Ca2(+)-activated and Mg2+ actin-activated myosin ATPase activities of flightless mfd- mutant Drosophila flight muscle myosin were one-half and one-third of those of the wild-type fly muscle myosin, respectively. 2. In the two-dimensional gel electrophoresis, the spots corresponding to phosphorylated myosin light chains, Lfl and Ltl, were hardly detected in mfd- mutant myosin. 3. These results support not only the conclusion that phosphorylation of myosin light chains regulates Drosophila myosin ATPase activity but also the assumption that the phosphorylation of myosin light chains is directly involved in flight function of the Drosophila fly.     

Substrate-concentration of dependences of tension, shortening velocity and ATPase activity of glycerinated single muscle fibers

Tension P0 and ATPase activity J0 of glycerinated single muscle fibers under isometric concentration as well as the velocity V0 of unloaded shortening were measured as a function of substrate concentration [S]. The stiffness of fibers with sinusoidal length changes at 1 kHz was used as a qualitative measure of the amount of rigor complex. P0 is an increasing function of [S] at low substrate concentrations and has a broad maximum at about 10-40 micrometers MgATP. In this concentration range, 10-40 micrometers, V0 still has a very small value. Then it increases and finally reaches at a plateau at about 1 mM MgATP. J0 increases as P0 does. However, it reaches at a saturated level at about the same concentration as V0. Either 0.5 mM 8-BrATP or 1 mM PPi was added to the substrate solutions to reduce the amount of rigor complex at low substrate concentrations. The addition of PPi of 8-BrATP decreases P0 dominantly at low concentrations of substrate and shifts the maximum to about 100 micrometers MgATP. 8-BrATP considerably increases V0 at low substrate concentrations while V0 is decreased by added PPi. The temperature coefficients, Q10 values were obtained for P0, J0, and V0. The values are essentially constant, 2.1-2.4, in the cases of P0 and J0, and about the same values were found for V0 at very low substrate concentrations. However, they become about 3.3 in the concentration range from 34 micrometers and 2.3 mM. The P-V relation was obtained at 11 micrometers and 2.3 micrometers MgATP. The normalized P-V relation at 11 micrometers was unchanged when 8-BrATP was added. The results are discussed in connection with the mechanism of actomyosin-ATPase activity as well as that of the elementary cycle of the motive force generation.     

Regulation of the Ca2+ pump ATPase by cAMP-dependent phosphorylation of phospholamban

Ca2+ transients in myocardial cells are modulated by cyclic AMP-dependent phosphorylation of a protein in the sarcoplasmic reticulum. This protein, termed phospholamban, serves to regulate the Ca2+ pump ATPase of this membrane, thus altering the mode of Ca2+ transients and the myocardial contractile response. Elucidating the structure of phospholamban and its intimate interaction with the Ca2+ pump ATPase should provide the basis for understanding, at the molecular level, how the cAMP system contributes to excitation-contraction coupling in muscle cells.     

Effects of shortening on stretch-induced force enhancement in single skeletal muscle fibers

The main purpose of this study was to evaluate the effects of shortening on the stretch-induced force enhancement in single muscle fibers, and indirectly test the hypothesis that force enhancement may be associated with the engagement of a passive element upon activation. Fibers were placed on the descending limb of the force-length relationship, and stretch and shortening contractions were performed. Fibers underwent two sets of shortening-stretch cycles. First, fibers were shortened by a fixed amplitude and speed (10% fiber length, and at 40% fiber length/s), and then were stretched (10% fiber length, and at 40% fiber length/s) immediately following shortening, or 500 or 1000 ms following the shortening. Second, fibers were shortened by varying amounts (5%, 10% and 15% fiber length) and at a constant speed (40% fiber length/s) immediately preceding a given fiber stretch (10% fiber length, and at 40% fiber length/s). When stretching was immediately preceded by shortening, force enhancement was decreased proportionally with the shortening magnitude. When intervals were introduced between shortening and stretch, the effects of shortening on the stretch-induced force enhancement became less prominent. We concluded that, in contrast to published suggestions, shortening affects the stretch-induced force enhancement in an amplitude-dependent manner in single fibers, as it does in whole muscles, but this effect is diminished by increasing the time period between the shortening and stretch phases.     

Influence of muscle geometry on shortening speed of fibre, aponeurosis and muscle.

The influence of muscle geometry on muscle shortening of the gastrocnemius medialis muscle (GM) of the rat was studied. Using cinematography, GM geometry was studied during isokinetic concentric activity at muscle lengths ranging from 85 to 105% of the optimum muscle length. The shortening speed of the distal fibre, the proximal aponeurosis and the muscle were determined, as well as the effect of rotation of the distal fibre and the proximal aponeurosis on the muscle speed of shortening. The results show that, due to the geometrical configuration, muscle shortening speed is not only determined by the speed of the fibre, but also to a large extent by the aponeurosis shortening speed. At optimum muscle length, the fibre and aponeurosis shortening speeds expressed relative to the muscle shortening speed amounted to 84% and 6%, respectively. At shorter muscle length, fibre speed relative to muscle speed decreased to values as low as 35%, whereas that of aponeurosis increased to values as high as 31%. Angular effects on the muscle speed of shortening can explain 10% of the muscle shortening speed at optimum muscle length and up to 34% of the muscle speed at shorter muscle length. In addition, a model was formulated to simulate the geometrical effects on muscle speed. This model, incorporating both fibre and aponeurosis length changes, contains a transfer function relating the shortening speeds of fibre and aponeurosis to muscle speed. The muscle shortening speed calculated using this transfer function demonstrated no significant differences with the speed measured experimentally.