Role of magnesium binding to myosin in controlling the state of cross-bridges in skeletal rabbit muscle

The effect of Mg2+ on the disposition of myosin cross-bridges was studied on myofibrils and synthetic myosin and rod filaments by employing chymotryptic digestion and chemical cross-linking methods. In the presence of low Mg2+ concentrations (0.1 mM), the proteolytic susceptibility at the heavy meromyosin/light meromyosin (HMM/LMM) junction in these three systems sharply increases over the pH range from 7.0 to 8.2. Such a change has been previously associated with the release of myosin cross-bridges from the filament surface [Ueno, H., & Harrington, W.F. (1981) J. Mol. Biol. 149, 619-640]. Millimolar concentrations of Mg2+ block or reverse this charge-dependent transition. Rod filaments show the same behavior as myosin filaments, indicating that the low-affinity binding sites for Mg2+ are located on the rod portion of myosin. The interpretation of these results in terms of Mg2+-mediated binding of cross-bridges to the filament backbone is supported by cross-linking experiments. The normalized rate of S-2 cross-linking in rod filaments at pH 8.0, kS-2/kLMM, increases upon addition of Mg2+ from 0.30 to 0.65 and approaches the cross-linking rate measured at pH 7.0 (0.75), when the cross-bridges are close to the filament surface. In rod filaments prepared from oxidized rod particles, chymotryptic digestion proceeds both at the S-2/LMM junction and at a new cleavage site located in the N-terminal portion of the molecule. Kinetic analysis of digestion rates at these two sites reveals that binding of Mg2+ to oxidized myosin rods has a similar effect at both sites over the pH range from 7.0 to 8.0.(ABSTRACT TRUNCATED AT 250 WORDS)     

The tail of myosin reduces actin filament velocity in the in vitro motility assay

It has been observed that heavy meromyosin (HMM) propels actin filaments to higher velocities than native myosin in the in vitro motility assay, yet the reason for this difference has remained unexplained. Since the major difference between these two proteins is the presence of the tail in native myosin, we tested the hypothesis that unknown interactions between actin and the tail (LMM) slow motility in native myosin. Chymotryptic HMM and LMM were mixed in a range of molar ratios (0-5 LMM/HMM) and compared to native rat skeletal myosin in the in vitro motility assay at 30 degrees C. Increasing proportions of LMM to HMM slowed actin filament velocities, becoming equivalent to native myosin at a ratio of 3 LMM/HMM. NH4+ -ATPase assays demonstrated that HMM concentrations on the surface were constant and independent of LMM concentration, arguing against a simple displacement mechanism. Relationships between velocity and the number of available heads suggested that the duty cycle of HMM was not altered by the presence of LMM. HMM prepared with a lower chymotrypsin concentration and with very short digestion times moved actin at the same high velocity. The difference between velocities of actin filament propelled by HMM and HMM/LMM decreased with increasing ionic strength, suggesting that ionic bonds between myosin tail and actin filaments may play a role in slowing filament velocity. These data suggest the high velocities of actin filaments over HMM result from the absence of drag generated by the myosin tail, and not from proteolytic nicking of the motor domain.     

Studies of myosin and its proteolytic fragments by laser Raman spectroscopy.

Two bands in the Raman spectrum of myosin, at 1,304 cm-1 and 1,270 cm-1, are attributable to alpha-helical structure. The first of these, also present in the spectrum of light meromyosin (LMM) but not in that of subfragment-1 (S-1), is assigned to the coiled-coil tail region of myosin; the second, seen in spectra of S-1 or heavy meromyosin (HMM), is largely absent from the spectrum of light meromyosin and is likely to correspond to the alpha-helical segments of the head region. When myosin or LMM aggregates, spectral bands attributable to backbone and sidechain groups sharpen suggesting a reduction in motional freedom. This sharpening is particularly apparent in the 902 cm-1 C--C stretching mode. Mg2+ broadens and shifts the peak at 1,244 cm-1 to 1,237 cm-1 and diminishes the intensity from 1,230 to 1,240 cm-1, changes which appear to be associated the S-1 region. MgPPi produces changes in the 1,300 cm-1 region attributable to alpha-helical regions in coiled-coil structures suggesting that MgPPi affects not only S-1, but also some part of the myosin rod.     

Conformational stability of the myosin rod

Chymotryptic cleavage patterns of myosin rods from pig stomach, chicken gizzard, and rabbit skeletal muscle indicate that short (approximately 45 nm) heavy meromyosin subfragment 2 (SF2) is a consistent product of all three rods, whereas long (approximately 60 nm) SF2 is derived only from skeletal muscle myosin. Differential scanning calorimetry was used to follow the thermally induced melting transition of the rods and certain of their subfragments. In 0.12 M KCl, sodium phosphate buffer, pH 6.2-7.6, the light meromyosin (LMM) and SF2 domains of each rod had essentially identical conformational stabilities. Temperature midpoints for the melting transitions were 54-56 degrees C for the two smooth muscle myosin rods and 50-53 degrees C for the skeletal muscle myosin rod. In 0.6 M K Cl buffer, melting transitions for the smooth muscle myosin rods were essentially unchanged, but skeletal muscle myosin rods showed multiphase melting, with major transitions at 43 degrees C and 52 degrees C. The first of these was tentatively attributed to LMM, and the second to SF2. In 0.12 M K Cl buffer, the LMM transition was stabilised so that it superimposed on that of SF2. No melting was observed in any of the rods at physiological temperature. These results indicate that, excluding a possible but only narrow hinge region, the entire myosin rod has essentially uniform conformational stability at physiological pH and ionic strength, and thus that the contractile and elastic properties of the cross-bridge exist in the heavy meromyosin subfragment 1 (SF1) domains of the molecule.     

Effect of the integrity of the myofibrillar structure on the tryptic accessibility of a hinge region of the myosin rod

Limited proteolysis has been used to study the influence of actin, in the absence or presence of regulatory proteins of the thin filament (tropomyosin and troponin), as well as that of the myofibrillar structure on the tryptic cleavage of the heavy meromyosin (HMM)/light meromyosin (LMM) hinge region in myosin heavy chain. Cleavage at the HMM/LMM hinge is almost absent in myofibrils, whereas this hinge is accessible to tryptic digestion in actomyosin, in native thin filaments attached to myosin and in myosin heavy chain alone. This observation indicates that it is the myofibrillar structure which profoundly affects the tryptic accessibility of this specific hinge region of myosin. This provides a good example of the manner by which a highly organized supramolecular structure might affect the chemical properties of a specific site in a macromolecule.     

Coiled-coil unwinding at the smooth muscle myosin head-rod junction is required for optimal mechanical performance

Myosin II has two heads that are joined together by an alpha-helical coiled-coil rod, which can separate in the region adjacent to the head-rod junction (Trybus, K. M. 1994. J. Biol. Chem. 269:20819-20822). To test whether this flexibility at the head-rod junction is important for the mechanical performance of myosin, we used the optical trap to measure the unitary displacements of heavy meromyosin constructs in which a stable coiled-coil sequence derived from the leucine zipper was introduced into the myosin rod. The zipper was positioned either immediately after the heads (0-hep zip) or following 15 heptads of native sequence (15-hep zip). The unitary displacement (d) decreased from d = 9.7 +/- 0.6 nm for wild-type heavy meromyosin (WT HMM) to d = 0.1 +/- 0.3 nm for the 0-hep zip construct (mean +/- SE). Native values were restored in the 15-hep zip construct (d = 7.5 +/- 0.7 nm). We conclude that flexibility at the myosin head-rod junction, which is provided by an unstable coiled-coil region, is essential for optimal mechanical performance.     

Electric birefringence study of rabbit skeletal myosin subfragments HMM, LMM, and rod in solution.

Electric birefringence measurements and depolarized light scattering experiments were performed with HMM, LMM, and rod, the three fragments of myosin, under conditions (0.3 M KCl, 0.02 M PO4, pH 7.3) the medium currently used for biochemical assays of myosin in its native state as well as of its subfragments. The comparison of myosin and rod relaxation times (17.2 and 22.8 microseconds, respectively) suggests that the average bend angle in the tail is sharper in intact myosin (90 degrees) whereas rod, when detached from the heads, is a more elongated species with an average bend angle of 120-135 degrees. The LMM relaxation time (6.4 microseconds) is consistent with a rigid linear stick model of length 78 nm. Flexibility in myosin tail is thus confirmed as located in the HMM-LMM hinge. LMM and rod did not exhibit any significant variation of their apparent relaxation times with concentration and the decay curves were best fitted by a single exponential, evidence that the concentration of parallel staggered dimers was negligible in the concentration range studied here (0-7 g/l). This observation lends support to previous results obtained with myosin. Respective HMM, LMM, and rod molecular weights and homogeneity as evaluated by SDS-PAGE analysis were correlated to the Kerr constants of their solutions. Large variations in LMM Kerr constants could be related to the loss of a COOH-terminal peptide on prolonged chymotryptic digestion. Electric birefringence combined with depolarized light scattering is presented as a potential method for net charge distribution studies.     

Electron paramagnetic resonance and nanosecond fluorescence depolarization studies on creatine-phosphokinase interaction with myosin and its fragments

Recent reports in the literature have indicated a physical association of creatinephosphokinase (CPK) with the tail portion of the myosin molecule. The present paper describes further studies on the interaction of CPK with myosin and myosin fragments, using the techniques of electron paramagnetic resonance (EPR) and nanosecond fluorescence depolarization. From EPR work, spin-labeled CPK appears to interact with myosin, tail-less myosin (heavy meromyosin [HMM]), and myosin heads (subfragment-1 [S1]), the extent of interaction being proportional to the S1 content of myosin or its fragments. Spin-labeled CPK did not evidence interaction with the headless myosin “rods”, with myosin tails (light meromyosin [LMM]), with S2 necks (which connect S1 to the rest of the myosin molecule), or with actin. When a fluorescent dye is directed to the essential ϵ-amino group of CPK, nanosecond fluorescence depolarization studies indicate a substantial interaction with myosin, HMM, and S1, but very little with F-actin. When the “fast-reacting” thiol of the S1 moiety or the “essential thiol” of CPK was labeled with either a fluorescent dye or a spin label, no interaction between CPK and myosin (or S1) was detected.     

Internal motions in myosin.

High-resolution proton nuclear magnetic resonance (1H NMR) measurements were made on myosin, heavy meromyosin (HMM), myosin subfragment 1 (S1), light meromyosin (LMM), and actin. A strong signal from amino acid side chains undergoing motions too fast to be accounted for by simple rotations of groups on a rigid backbone was obtained from myosin. Comparison of myosin, HMM, S1, and LMM showed that the mobile region is located almost entirely in S1 and accounts for approximately 22% of its structure. Adenosine triphosphate (ATP) and ATP analogues had no measurable effect on the S1 spectrum. Actin, on the other hand, quenched the internal motions of S1. When S1 was titrated with actin, an association was obtained which was in agreement with other measured values. The actin effect was reversed by adding magnesium pyrophosphate (MgPPi) or adenyl-5'-yl imidophosphate (MgAMPPNP). Quantitative treatment of the broad signals from myosin and its subfragments substantiated the existence of two flexible regions in myosin. The highly mobile portion of myosin may be located in the "swivel" between S1 and the rest of myosin or in the actin binding site or in both. These possibilites are discussed, and a new possible mechanism for muscle cross bridge elasticity is proposed.     

Effect of myosin DTNB light chain on the actin-myosin interaction in the presence of ATP.

The influence of the DTNB light chain of myosin on its enzymatic activities was examined by studying the superprecipitation of actomyosin and the actin-activated ATPase of heavy meromyosin (HMM) [EC 3.6.1.3]. Although the Ca2+-, Mg2+-, and EDTA-ATPase activities of control and DTNB myosin were practically the same, the superprecipitation of actomyosin prepared from actin and DTNB myosin occurred more slowly than that of control myosin. The apparent binding constant obtained from double-reciprocal plots of actin-activated ATPase of DTNB HMM was lower than that of control HMM. Recombination of DTNB myosin and HMM with DTNB light chains restored the original properties of myosin and HMM. The removal of DTNB light chain from myosin had no effect on the formation of the rigor complex between actin and myosin. These results suggest that the DTNB light chain participates in the interaction of myosin with actin in the presence of ATP.     

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 actomyosin ATPase of synthetic myosin minifilaments, filaments, and heavy meromyosin

The actin-activated ATPase activities of myosin minifilaments and heavy meromyosin are similar at high actin concentrations. Under low ionic strength conditions, the minifilaments in Tris citrate buffer yield the same maximal turnover rate (Vmax) and apparent dissociation constant of actin from myosin (Kapp) as heavy meromyosin in standard low salt conditions. The time course of actin-activated ATP hydrolysis of minifilaments is similar to that observed for standard myosin preparations. Depending on the exact protein composition of the assay mixture, either the ATPase activity declines continuously with time, or is accelerated at the onset of superprecipitation. In analogy with myosin filaments, the ATPase of minifilaments shows a biphasic dependence on actin concentration. Super-precipitation of minifilaments follows a well resolved clearing phase during which their structural integrity appears to be fully preserved. These results indicate that minifilaments or similar small assemblies of myosin can fulfill contractile functions.     

Crossbridge release and alpha-helix-coil transition in myosin and rod minifilaments

The relationship between crossbridge release and alpha-helix-coil transition in myosin has been investigated by employing synthetic myosin and rod minifilaments prepared in 10 mM-citrate/Tris buffer at pH 7.0 and 8.0. Initial sedimentation velocity and turbidity measurements have established that the minifilament structures obtained at pH 7.0 and 8.0 are relatively similar in size and homogeneity, and can be used in comparative circular dichroism studies. Chemical crosslinkings and proteolytic digestions carried out at pH 7.0 and 8.0 verify that myosin and rod minifilaments undergo the same pH-induced changes as myosin filaments, i.e. a decrease in the rate of subfragment-2 crosslinking to the filament surface, and an increase in proteolytic susceptibility of the light meromyosin-heavy meromyosin hinge at alkaline pH. These results suggest charge-induced release of the S-2 element from the myosin and rod minifilament surface. Circular dichroism measurements reveal a reduced alpha-helical content of myosin (5%) and rod minifilaments (10%) at pH 8.0 compared to the respective pH 7.0 structures. These results establish a direct link between crossbridge release and alpha-helix-coil transition in myosin.     

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⁺.     

Solubility properties of a 65-kDa peptide prepared by restricted digestion of myosin with astacin-like squid metalloprotease

Substructure of the myosin rod and its correlation to filament formation is largely based on studies of proteolytic digests and expressed proteins. However, tryptic digestion of myosin always produces polymorphous peptides. Consequently, it is difficult to determine the relation between myosin substructure and filament formation. Similarly, filament formation with recombinant myosin protein is also difficult to interpret because it is never clear whether the recombinant protein folds like the native protein. We recently reported a novel metal protease isolated from squid liver, astacin-like squid metalloprotease (ALSM), which can specifically hydrolyze in vitro myosin heavy chain. In the present study, we examined the solubility properties of the 65-kDa peptide and light meromyosin (LMM) prepared by ALSM isoform II and trypsin digestion, respectively. The 65-kDa peptide is much less soluble than LMM under physiological conditions, even though the length of 65-kDa peptide is shorter than that of LMM. These results suggest that a novel substructure of myosin drives filament assembly.     

Hinging of rabbit myosin rod

The question of hinging in myosin rod from rabbit skeletal muscle has been reexamined. Elastic light scattering and optical rotation have been used to measure the radius of gyration and fraction helix, respectively, as a function of temperature for myosin rod, light meromyosin (LMM), and long subfragment 2 (long S-2). The radius of gyration vs temperature profile of myosin rod is shifted with respect to the optical rotation melting curve by about -5 degrees C. Similar studies on both LMM and long S-2 show virtually superimposable profiles. To correlate changes in the secondary structure with the overall conformation, plots of radius of gyration vs fraction helix are presented for each myosin subfragment. Myosin rod exhibits a marked decrease in the radius of gyration from 43 nm to approximately 35 nm, while the fraction helix remains at nearly 100%. LMM and long S-2 did not show this behavior. Rather, a decrease in the radius of gyration of these fragments occurred with comparable changes in fraction helix. These results are interpreted in terms of hinging of the myosin rod within the LMM/S-2 junction.     

Crosslinking by thiol disulfide interchange of 5,5'-dithiobis(2-nitrobenzoic acid)-treated light chain and heavy chain of rabbit skeletal myosin

Interchain disulfide crosslinks between the heavy-chain fragment in heavy meromyosin and myosin light chain 2, generated by 5,5'-dithiobis(2-nitrobenzoic acid (Nbs2), are formed under appropriate ionic conditions at neutral pH as revealed by liberation of the chromogenic 2-nitro-5-thiobenzoic acid. The presence of the original or of a slightly digested light chain 2 reduces the rate of the reaction of heavy meromyosin with Nbs2-modified light chain 2 by 32 - 39%, if Ca2+ is present. Dodecyl sulfate/polyacrylamide gel electrophoresis in absence of reducing agents shows that Nbs2-modified light chain 2 attaches to the heavy chain in the region of the 21-kDa fragment of heavy meromyosin, which contains the essential thiol groups and which has been located at the subfragment 1/subfragment 2 junction of myosin [Balint, M., Wolf, I., Tarcsafalvi, A., Gergely, J. and Sreter, F. A. (1978) Arch. Biochem. Biophys. 190, 793-799]. Modification of thiol-1 groups with iodoacetamide as well as crosslinking the thiol-1 and thiol-2 groups by the bifunctional reagent p-N,N'-phenylenedimaleimide prior to incubation with Nbs2-modified light chain 2 has no substantial effect on the crosslinking reaction. This indicates that other thiol groups are involved in the binding of Nbs2-modified light chain 2 to the heavy chain. An examination of K+, Ca2+, Mg2+ and actin-activated Mg2+ ATPase activities of heavy meromyosin that had been crosslinked with Nbs2-modified light chain 2 shows only a slight change in comparison with intact heavy meromyosin, indicating that crosslinking had not altered significantly the hydrolytic site. Crosslinking of Nbs2-modified light chain 2 to light-chain-2-deficient heavy meromyosin restored the original light-chain-2-dependent Ca2+ sensitivity of the tryptic fragmentation of heavy meromyosin, suggesting that crosslinking takes place at the proper binding site for light 2.     

A spin-label study of phosphatidylcholine exchange protein. Regulation of the activity by phosphatidylserine and calcium ion.

The effects of the divalent cations Mg2+, Mn2+ and Ca2+ on the Brownian rotational motion of fluorescently labeled myosin, heavy meromyosin and myosin subfragment-1 were measured by the method of time-resolved fluorescence depolarization. When Mg2+ was added to solutions of myosin or heavy meromyosin and EDTA, their rotational mobility increased. Ca2+ had no effect. Mn2+ increased the mobility of heavy meromyosin but decreased that of myosin. None of these divalent cations effected the mobility of subfragment-1. The binding of heavy meromyosin to actin was affected very little by Mg2+ or EDTA over a wide range of conditions. Divalent cations appear to change the swivel about which the heads of myosin rotate, presumably by binding to light chain 2 (also called DTNB light chain). However, the heads are still able to bind actin in nearly the same way whether Mg2+ is present or not. The concentration of free Mg2+ for the mid-point of the change in heavy meromyosin mobility is in good agreement with that for EDTA activation of ATPase activity. This suggests that EDTA activation is due to removal of Mg2+ bound to myosin itself.     

Effects of phosphorylation of light chain residues threonine 18 and serine 19 on the properties and conformation of smooth muscle myosin

Smooth muscle myosin can be phosphorylated by myosin light chain kinase at the serine 19 and threonine 18 residues of the two 20,000-dalton light chains (Ikebe, M., Hartshorne, D. J., and Elizinga, M. (1986) J. Biol. Chem. 261, 36-39). These studies with myosin and heavy meromyosin (HMM) compare the effects induced by phosphorylation of serine 19 (M2P and HMM2P) and serine 19 plus threonine 18 (M4P and HMM4P). Formation of M4P altered the KCl dependence of viscosity and Mg2+-ATPase and higher values were maintained at lower ionic strengths, compared to M2P or dephosphorylated myosin (Mo). This is consistent with the stabilization of the 6 S conformation. The tendency for aggregation, as judged by light scattering, followed the sequence M4P greater than M2P greater than Mo. Filaments formed with M4P were more resistant to dissociation by ATP compared to filaments of M2P. Phosphorylation of HMM2P doubled Vmax of actin-activated ATPase with little effect on the apparent affinity for actin. The Mg2+-ATPase of HMM4P exhibited a higher activity at low ionic strength compared to HMM2P and HMMo. Hydrodynamic differences were detected at low ionic strength in the presence of ATP by sedimentation velocity measurements with HMM4P, HMM2P, and HMMo. Proteolysis by papain indicated an increased susceptibility of the head-neck junction of HMM4P compared to HMM2P. These data suggest that the phosphorylation of threonine 18 in addition to serine 19 change the conformation of myosin and HMM and this is associated with altered biological properties.     

Structural changes in synthetic myosin minifilaments and their dissociation by adenosine triphosphate and pyrophosphate

Morphologically similar short myosin and rod filaments (minifilaments) have been prepared in 10 mM Tris--citrate buffer, pH 8.0, in the absence of other myosin or rod forms. Both minifilament systems are dissociated in the same manner in the presence of ATP or pyrophosphate. Identical binding of these ligands to myosin and rod minifilaments suggests that myosin heads play no role in substrate-induced destabilization of the minifilaments. The effects of ATP and pyrophosphate on minifilaments are similar to their dissociating effect on synthetic filaments [Harrington, W. F., & Himmelfarb, S. (1972) Biochemistry 11, 2945--2952], thus justifying their use in conformational studies in lieu of filaments. In view of their small size and homogeneity, the minifilaments constitute an appropriate material for such studies. The binding of pyrophosphate to myosin and rod minifilaments decreases their alpha-helical content, as measured by circular dichroism. No change in the secondary structure of subfragment 1 and light meromyosin is observed upon binding of pyrophosphate, but substantial changes (10%) are detected in subfragment 2. The structural changes in myosin, possibly relevant to contraction, are localized in the subfragment 2 region of the molecule. These results emphasize the importance of charge interactions in the functional behavior of thick filaments.