Myosin light chain phosphorylation inhibits muscle fiber shortening velocity in the presence of vanadate

We have shown that myosin light chain phosphorylation inhibits fiber shortening velocity at high temperatures, 30 degrees C, in the presence of the phosphate analog vanadate. Vanadate inhibits tension by reversing the transition to force-generating states, thus mimicking a prepower stroke state. We have previously shown that at low temperatures vanadate also inhibits velocity, but at high temperatures it does not, with an abrupt transition in inhibition occurring near 25 degrees C (E. Pate, G. Wilson, M. Bhimani, and R. Cooke. Biophys J 66: 1554-1562, 1994). Here we show that for fibers activated in the presence of 0.5 mM vanadate, at 30 degrees C, shortening velocity is not inhibited in dephosphorylated fibers but is inhibited by 37 +/- 10% in fibers with phosphorylated myosin light chains. There is no effect of phosphorylation on fiber velocity in the presence of vanadate at 10 degrees C. The K(m) for ATP, defined by the maximum velocity of fibers partially inhibited by vanadate at 30 degrees C, is 20 +/- 4 microM for phosphorylated fibers and 192 +/- 40 microM for dephosphorylated fibers, showing that phosphorylation also affects the binding of ATP. Fiber stiffness is not affected by phosphorylation. Inhibition of velocity by phosphorylation at 30 degrees C depends on the phosphate analog, with approximately 12% inhibition in fibers activated in the presence of 5 mM BeF(3) and no inhibition in the presence of 0.25 mM AlF(4). Our results show that myosin phosphorylation can inhibit shortening velocity in fibers with large populations of myosin heads trapped in prepower stroke states, such as occurs during muscle fatigue.     

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.     

Kinetics of tryptophan fluorescence enhancement in myofibrils during ATP hydrolysis

The mechanism of ATP hydrolysis in myofibrils can be studied by following the time course of tryptophan fluorescence. Stoichiometric quantities of ATP produce an enhancement of the tryptophan fluorescence in stirred suspensions of rabbit psoas myofibrils at pCa greater than 7. Approximately 1 mol of ATP/myosin head is required to obtain the maximum fluorescence enhancement of 4-6%. Upon the addition of quantities of ATP greater than 1 mol/mol of myosin head, the fluorescence rapidly increases to a steady state, which lasts for a period that is proportional to the amount of ATP added. The fluorescence then decays to the initial level with a half-time of approximately 40 s at 20 degrees C. Hydrolysis of [gamma-32P]ATP at pCa greater than 7 in myofibrils has an initial burst of approximately 0.7 mol/mol of myosin head that is followed by a constant rate of hydrolysis. The duration of the steady state hydrolysis is identical to the duration of the enhancement of tryptophan fluorescence. A lower limit of 5 X 10(5) M-1 S-1 was obtained for the second order rate constant of the fluorescence enhancement by ATP. At pCa of 4, the duration of the fluorescence enhancement is one-tenth to one-twentieth as long as at pCa greater than 7; this is consistent with the increased steady state rate of ATP hydrolysis at higher calcium concentrations. The time course of the fluorescence enhancement observed in myofibrils during ATP hydrolysis is qualitatively and quantitatively similar to that observed with actomyosin-S1 in solution. These results suggest that the kinetic mechanism of ATP hydrolysis that has been well established by studies of actomyosin-S1 in solution also occurs in myofibrils.     

Heterogeneity in the actin activation of myosin

The soluble proteolytic fragments of myosin, heavy meromyosin and subfragment 1, were prepared with varying amounts of the proteases chymotrypsin and papain, respectively. The actin-activated ATP hydrolysis were examined with oxygen-18-labeled ATP. Each preparation of heavy meromyosin and subfragments 1 displayed two pathways of ATP hydrolysis, called respectively the high and low oxygen exchange mechanisms. The contributions of the two mechanisms were found to be sensitive to the potassium chloride concentration. With a fixed concentration of actin (300 microM), the contribution of the low-exchange mechanism decreased from a maximum of 90% of the ATP hydrolysis at 10 and 20 mM KCl to 12% at 180 mM KCl. The results suggested that the two mechanisms were competing reactions catalyzed by a single species of myosin.     

Twirling Motion of Actin Filaments in Gliding Assays with Nonprocessive Myosin Motors

We present a model study of gliding assays in which actin filaments are moved by nonprocessive myosin motors. We show that even if the power stroke of the motor protein has no lateral component, the filaments will rotate around their axis while moving over the surface. Notably, the handedness of this twirling motion is opposite from that of the actin filament structure. It stems from the fact that the gliding actin filament has target zones, where its subunits point toward the surface and are therefore more accessible for myosin heads. Each myosin head has a higher binding probability before it reaches the center of the target zone than afterwards, which results in a left-handed twirling. We present a stochastic simulation and an approximative analytical solution. The calculated pitch of the twirling motion depends on the filament velocity (ATP concentration). It reaches ∼400 nm for low speeds and increases with higher speeds.     

Myosin step size. Estimation from slow sliding movement of actin over low densities of heavy meromyosin

We have estimated the step size of the myosin cross-bridge (d, displacement of an actin filament per one ATP hydrolysis) in an in vitro motility assay system by measuring the velocity of slowly moving actin filaments over low densities of heavy meromyosin on a nitrocellulose surface. In previous studies, only filaments greater than a minimum length were observed to undergo continuous sliding movement. These filaments moved at the maximum speed (Vo), while shorter filaments dissociated from the surface. We have now modified the assay system by including 0.8% methylcellulose in the ATP solution. Under these conditions, filaments shorter than the previous minimum length move, but significantly slower than Vo, as they are propelled by a limited number of myosin heads. These data are consistent with a model that predicts that the sliding velocity (v) of slowly moving filaments is determined by the product of vo and the fraction of time when at least one myosin head is propelling the filament, that is, v = vo [1-(1-ts/tc)N], where ts is the time the head is strongly bound to actin, tc is the cycle time of ATP hydrolysis, and N is the average number of myosin heads that can interact with the filament. Using this equation, the optimum value of ts/tc to fit the measured relationship between v and N was calculated to be 0.050. Assuming d = vots, the step size was then calculated to be between 10nm and 28 nm per ATP hydrolyzed, the latter value representing the upper limit. This range is within that of geometric constraint for conformational change imposed by the size of the myosin head, and therefore is not inconsistent with the swinging cross-bridge model tightly coupled with ATP hydrolysis.     

Purealin, a novel stabilizer of smooth muscle myosin filaments that modulates ATPase activity of dephosphorylated myosin

Effects of purealin isolated from a sea sponge, Psammaplysilla purea, on the enzymatic and physiochemical properties of chicken gizzard myosin were studied. At 0.15 M KCl, 40 microM purealin increased the Ca2+- and Mg2+-ATPase activity of dephosphorylated gizzard myosin to 2.5- and 3-fold, respectively, but decreased the K+-EDTA-ATPase activity of the myosin to 0.25-fold. In contrast, purealin had little effect on the ATPase activities of phosphorylated gizzard myosin. The ATP-induced decrease in light scattering of dephosphorylated gizzard myosin at 0.15 M KCl was lessened by 40 microM purealin. Electron microscopic observations indicated that thick filaments of dephosphorylated myosin were disassembled immediately by addition of 1 mM ATP at 0.15 M KCl, although they were preserved by purealin for a long time even after addition of ATP. Upon ultracentrifugation, dephosphorylated myosin sedimented as two components, the 10 S species and myosin filaments, in the solution containing 0.18 M KCl and 1 mM Mg X ATP in the presence of 60 microM purealin. These results suggest that purealin modulates the ATPase activities of dephosphorylated gizzard myosin by enhancing the stability of myosin filaments against the disassembling action of ATP.     

Diffusion-limited kinetics of immobilized myosin ATPase

To test the possibility that ATP diffusion limits the kinetics of myosin ATPase (EC. 3.6.1.3) in situ, myosin was covalently bound to the surface of 2 kinds of films: collagen and Immunodyne. On collagen films, it was bound either with 1-ethyl-3 (3 dimethyl-aminopropyl)carbodiimide (EDC) or with dimethyl-3,3'-dithiobis(propionimidate) (DTP). The apparent Km for K+-ATP rose from 0.26 mM for free myosin in solution to 2-5 mM for covalently bound myosin, and maximum K+-ATPase activity was very low. With the other film, Immunodyne from Pall, the maximum activity of bound myosin was 170 nmol per min per 1.5 cm2 film. The apparent Km for K+-ATP was 2.1 mM when the incubation mixture was vigorously stirred, and the effect of stirring indicated that the kinetics of K+-ATP hydrolysis are limited by external diffusion. The large amount of myosin bound per unit of Immunodyne film surface permitted the study of Mg2+-ATPase activity, although it was 400-500 times less than the K+-ATPase activity. The apparently non-Michaelian kinetics of Mg2+-ATP hydrolysis are attributable to the external diffusion. The apparent Michaelis constant observed at low Mg2+-ATP concentrations rose from 0.27 microM for myosin in solution to 5 microM for myosin bound to Immunodyne film.     

In vitro motility of skeletal muscle myosin and its proteolytic fragments

We have compared actin-activated myosin ATPase activity, myosin binding to actin, and the velocity of myosin-induced actin sliding in order to understand the mechanism of myosin motility. In our in vitro assay, F-actin slides at a constant velocity, regardless of length. The F-actin could slide over myosin heads at KCl concentrations below a critical value (60 mM with myosin and HMM, 100 mM with S-1), and the sliding velocities were quite similar below the critical KCl concentration. However, at KCl concentrations close to the critical value, the sliding F-actin is attached to only one or a few particular points on the surface, each of which perhaps consists of a single head of myosin. The KATPase values for actin-activated ATPase were approximately 300 microM for S-1 and approximately 200 microM with HMM below the critical KCl concentration, and approximately 5,000 microM above the critical KCl concentration. This increase in KATPase is due to a drastic reduction in the binding affinity of myosin heads to F-actin, as determined by a proteolytic digestion method and direct observation by fluorescence microscopy. We also show that the Vmax of actin-activated myosin ATPase activity decreases steadily with increasing KCl concentration, even though the velocity of F-actin sliding remains unchanged. This result provides evidence that the ATPase activity is not necessarily linked to motility. We discuss possible models that do not require a tight coupling between myosin ATPase and motility.     

Relationship between myosin phosphorylation and contractile capability of canine airway smooth muscle.

To better understand excitation-contraction coupling in smooth muscle, myosin phosphorylation and force-velocity properties of canine tracheal muscle were compared during the rise and early plateau of force in electrically stimulated tetani. Velocity reached a peak of approximately 1.5 times plateau value when force had risen to approximately 45% of its maximum value and then declined progressively. Except early in the tetanus, when phosphorylation rose rapidly, maximum power and phosphorylation had nearly parallel time courses, reaching peaks of 1.2-1.3 times reference at 6-8 s before declining to the plateau level at approximately 12 s. Force, velocity, maximum power, and phosphorylation fell somewhat during the plateau, with the closest correlation between phosphorylation and power. These results suggest that 1) early velocity slowing is not associated with light chain dephosphorylation and 2) maximum power, which we use to signal changes in activation, is closely correlated with the degree of light chain phosphorylation, at least when phosphorylation level is not changing rapidly. Dissociation of these two properties would be expected early in the tetanus if phosphorylation precedes mechanical activity.     

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.     

Reaction of two heads of gizzard myosin with ATP

The reaction intermediates formed by the two heads of smooth muscle myosin were studied. The amount of myosin-phosphate-ADP complex, MPADP, formed was measured from the Pi-burst size over a wide range of ATP concentrations. At low concentrations of ATP, the Pi-burst size was 0.5 mol/mol myosin head, and the apparent Kd value was about 0.15 microM. However, at high ATP concentrations, the Pi burst size increased from 0.5 to 0.75 mol/mol myosin head with an observed Kd value of 15 microM. The binding of nucleotides to gizzard myosin during the ATPase reaction was directly measured by a centrifugation method. Myosin bound 0.5 mol of nucleotides (ATP and ADP) with high affinity (Kd congruent to 1 microM) and 0.35 mol of nucleotides with low affinity (Kd = 24 microM) for ATP. These results indicate that gizzard myosin has two kinds of nucleotide binding sites, one of which forms MPADP with high affinity for ATP while the other forms MPADP and MATP with low affinity for ATP. We studied the correlation between the formation of MPADP and the dissociation of actomyosin. The amount of Pi-burst size was not affected by the existence of F-actin, and when 0.5 mol of ATP per mol of myosin head was added to actomyosin (1 mg/ml F-actin, 5 microM myosin at 0 degrees C) most (93%) of the added ATP was hydrolyzed in the Pi-burst phase. All gizzard actomyosin dissociated when 1 mol of ATP per mol myosin head was added to actomyosin.(ABSTRACT TRUNCATED AT 250 WORDS)     

Selective perturbation of the myosin recovery stroke by point mutations at the base of the lever arm affects ATP hydrolysis and phosphate release

After ATP binding the myosin head undergoes a large structural rearrangement called the recovery stroke. This transition brings catalytic residues into place to enable ATP hydrolysis, and at the same time it causes a swing of the myosin lever arm into a primed state, which is a prerequisite for the power stroke. By introducing point mutations into a subdomain interface at the base of the myosin lever arm at positions Lys(84) and Arg(704), we caused modulatory changes in the equilibrium constant of the recovery stroke, which we could accurately resolve using the fluorescence signal of single tryptophan Dictyostelium myosin II constructs. Our results shed light on a novel role of the recovery stroke: fine-tuning of this reversible equilibrium influences the functional properties of myosin through controlling the effective rates of ATP hydrolysis and phosphate release.     

Direct observation of the myosin Va recovery stroke that contributes to unidirectional stepping along actin

Myosins are ATP-driven linear molecular motors that work as cellular force generators, transporters, and force sensors. These functions are driven by large-scale nucleotide-dependent conformational changes, termed "strokes"; the "power stroke" is the force-generating swinging of the myosin light chain-binding "neck" domain relative to the motor domain "head" while bound to actin; the "recovery stroke" is the necessary initial motion that primes, or "cocks," myosin while detached from actin. Myosin Va is a processive dimer that steps unidirectionally along actin following a "hand over hand" mechanism in which the trailing head detaches and steps forward ～72 nm. Despite large rotational Brownian motion of the detached head about a free joint adjoining the two necks, unidirectional stepping is achieved, in part by the power stroke of the attached head that moves the joint forward. However, the power stroke alone cannot fully account for preferential forward site binding since the orientation and angle stability of the detached head, which is determined by the properties of the recovery stroke, dictate actin binding site accessibility. Here, we directly observe the recovery stroke dynamics and fluctuations of myosin Va using a novel, transient caged ATP-controlling system that maintains constant ATP levels through stepwise UV-pulse sequences of varying intensity. We immobilized the neck of monomeric myosin Va on a surface and observed real time motions of bead(s) attached site-specifically to the head. ATP induces a transient swing of the neck to the post-recovery stroke conformation, where it remains for ～40 s, until ATP hydrolysis products are released. Angle distributions indicate that the post-recovery stroke conformation is stabilized by ≥ 5 k(B)T of energy. The high kinetic and energetic stability of the post-recovery stroke conformation favors preferential binding of the detached head to a forward site 72 nm away. Thus, the recovery stroke contributes to unidirectional stepping of myosin Va.     

Myosin head mechanical performance under different conformational change mechanisms

The present paper puts forward a mathematical approach to model the conformational changes of the myosin head due to ATP hydrolysis, which determine the head swinging and consequent sliding of the actin filament. Our aim is to provide a simple but effective model simulating myosin head performance to be integrated into the overall model of sarcomere mechanics under development at our Laboratory (J. Biomech. 34 (2001) 1607). We began by exploring myosin head mechanics in recent findings about myosin ultrastructure, morphology and energetics in order to calculate the working stroke distance (WS) and the force transmitted to the actin filament during muscle contraction. Two different working stroke mechanisms were investigated, assuming that the swinging of the myosin head occurs either as a consequence of purely conformational changes (Science 261 (1993a) 58) or by thermally driven motion (ratchet mechanism) followed by conformational changes (Cell 99 (1999) 421). Our results show that force and WS values vary markedly between the two models. The maximum force generated is about 10 pN for the first model and 31 pN for the second model, and the WSs are about 13 and 4 nm, respectively. These results are then discussed and compared with published data. The experimental data used for comparison are scarce and non-homogeneous; hence, the final remarks do not lead to definite conclusions. In any event, relatively speaking, the first model is more coherent with experimental findings.     

Actin-activated Mg-ATPase activity of Dictyostelium myosin II. Effects of filament formation and heavy chain phosphorylation.

The actin-activated Mg-ATPase activities of unphosphorylated and heavy chain phosphorylated Dictyostelium myosin II and of a Dictyostelium myosin II heavy meromyosin (HMM) fragment were examined at different Mg2+ and KCl concentrations. The Mg-ATPase activity of HMM displayed a maximum rate, Vmax, of about 4.0/s and a Kapp (actin concentration required to achieve 1/2 Vmax) that increased from 8 to 300 microM as the KCl concentration increased from 0 to 120 mM. When assayed with greater than 5 mM Mg2+ and 0 mM KCl the unphosphorylated Dictyostelium myosin II yielded a Kapp of 0.25 microM and a Vmax of 2.8/s. At lower Mg2+ concentrations or with 50 mM KCl the data were not fit well by a single hyperbolic curve and Kapp increased to 25-100 microM. The increase in Kapp did not correlate with the loss of sedimentable filaments. At KCl concentrations above 100 mM Vmax increased to greater than 4/s. Heavy chain phosphorylated myosin (3.5 mol of phosphate/mol myosin) displayed a Vmax of about 5/s and a Kapp of 50 microM under all conditions tested. Thus, heavy chain phosphorylation inhibited the actin-activated Mg-ATPase activity of Dictyostelium myosin II in 5-10 mM Mg2+ and low ionic strength through an increase in Kapp.     

Simulations of the myosin II motor reveal a nucleotide-state sensing element that controls the recovery stroke

During the recovery stroke, the myosin motor is primed for the next power stroke by a 60° rotation of its lever arm. This reversible motion is coupled to the activation of the ATPase function of myosin through conformational changes along the relay helix, which runs from the Switch-2 loop near the ATP to the converter domain carrying the lever arm. Via a hydrogen bond between the side-chain of Asn475 on the relay helix and the Gly457/Ser456 peptide group on the Switch-2, the rotation of the converter domain is coupled to the formation of a hydrogen bond between Gly457 and γ-phosphate that is essential for ATP hydrolysis. Here, molecular dynamics simulations of Dictyostelium discoideum myosin II in the two end conformations of the recovery stroke with different nucleotide states (ATP, ADP·Pi, ADP) reveal that the side-chain of Asn475 breaks away from Switch-2 upon ATP hydrolysis to make a hydrogen bond with Tyr573. This sensing of the nucleotide state is achieved by a small displacement of the cleaved γ-phosphate towards Gly457 which in turn pushes Asn475 away. The sensing plays a dual role by (i) preventing the wasteful reversal of the recovery stroke while the nucleotide is in the ADP·Pi state, and (ii) decoupling the relay helix from Switch-2, thus allowing the power stroke to start upon initial binding to actin while Gly457 of Switch-2 keeps interacting with the Pi (known to be released only later after tight actin binding). A catalytically important salt bridge between Arg238 (on Switch-1) and Glu459 (on Switch-2), which covers the hydrolysis site, is seen to form rapidly when ATP is added to the pre-recovery stroke conformer and remains stable after the recovery stroke, indicating that it has a role in shaping the ATP binding site by induced fit.     

Detection of the swings of the lever arm of a myosin motor by fluorescence resonance energy transfer of green and blue fluorescent proteins

The "lever-arm" model of a myosin motor predicts that the lever-arm domain in the myosin head tilts and swings against the catalytic domain during ATP hydrolysis, resulting in force generation. To investigate if this "swing" of the lever arm really occurs during the hydrolysis of ATP, we employed fluorescence resonance energy transfer (FRET) between two fluorescent proteins [green (GFP) and blue (BFP)] fused to the N and C termini of the Dictyostelium myosin-motor domain. FRET measurements showed that the C-terminal BFP in the fusion protein first swings against the N-terminal GFP at the isomerization step of the ATP hydrolysis cycle and then swings back at the phosphate-release step. Because the C-terminal BFP mimics the motion of the lever arm, the result indicates that the lever arm swings at the specific steps of the ATP hydrolysis cycle, i.e., at the isomerization and phosphate-release steps. The latter swing may correspond to the power stroke of myosin, while the former may be related to the recovery stroke.     

ATP consumption and efficiency of human single muscle fibers with different myosin isoform composition

Chemomechanical transduction was studied in single fibers isolated from human skeletal muscle containing different myosin isoforms. Permeabilized fibers were activated by laser-pulse photolytic release of 1.5 mM ATP from p(3)-1-(2-nitrophenyl)ethylester of ATP. The ATP hydrolysis rate in the muscle fibers was determined with a fluorescently labeled phosphate-binding protein. The effects of varying load and shortening velocity during contraction were investigated. The myosin isoform composition was determined in each fiber by sodium dodecyl sulfate-polyacrylamide gel electrophoresis. At 12 degrees C large variations (three- to fourfold) were found between slow and fast (2A and 2A-2B) fibers in their maximum shortening velocity, peak power output, velocity at which peak power is produced, isometric ATPase activity, and tension cost. Isometric tension was similar in all fiber groups. The ATP consumption rate increased during shortening in proportion to shortening velocity. At 12 degrees C the maximum efficiency was similar (0.21-0.27) for all fiber types and was reached at a higher speed of shortening for the faster fibers. In all fibers, peak efficiency increased to approximately 0.4 when the temperature was raised from 12 degrees C to 20 degrees C. The results were simulated with a kinetic scheme describing the ATPase cycle, in which the rate constant controlling ADP release is sensitive to the load on the muscle. The main difference between slow and fast fibers was reproduced by increasing the rate constant for the hydrolysis step, which was rate limiting at low loads. Simulation of the effect of increasing temperature required an increase in the force per cross-bridge and an acceleration of the rate constants in the reaction pathway.     

Characterization of regulatory light chain-a myosin kinase from smooth muscle of scallop, Patinopecten yessoensis

The protein kinase that phosphorylates the regulatory light chain-a (RLC-a) of scallop smooth muscle myosin was isolated from scallop smooth muscle (Sohma, H. & Morita, F. (1986) J. Biochem. 100, 1155-1163). The enzymatic properties of this kinase (aMK) were investigated using RLC-a as the substrate. The Km value for ATP was 6.5 microM in the presence of 27 microM RLC-a at pH 7.0, and that for RLC-a was 133 microM in the presence of 1 mM ATP. The Vm value at saturation of both RLC-a and ATP was 0.25 s-1 at pH 7.0. The pH activity curve for aMK was bell-shaped with a maximum at around pH 7.8. The aMK activity was inhibited strongly by an increase in the KCl concentration. aMK required Mg2+, but was inhibited by high concentrations of Mg2+. The optimum activity was seen at 3 mM MgCl2. The mode of inhibition of the aMK activity by Ca2+ was studied. Assuming that the binding of Ca2+ to aMK induces the inhibition, the dissociation constant of Ca2+ was estimated to be 64 microM. aMK also phosphorylated LC20 of chicken gizzard myosin at a similar rate to that for RLC-a and the DTNB light chain of rabbit skeletal muscle myosin at a more lower rate. The helix and beta-sheet contents of aMK were estimated to be 19 and 30%, respectively, from the CD spectrum.