Substructure of the myosin molecule. IV. Interactions of myosin and its subfragments with adenosine triphosphate and F-actin

Synergistic protection of MLC 1 against cardiac ischemia/reperfusion-induced degradation: a novel therapeutic concept for the future

Cardiovascular diseases are a major burden to society and a leading cause of morbidity and mortality in the developed world. Despite clinical and scientific advances in understanding the molecular mechanisms and treatment of heart injury, novel therapeutic strategies are needed to prevent morbidity and mortality due to cardiac events. Growing evidence reported over the last decade has focused on the intracellular targets for proteolytic degradation by MMP-2. Of particular interest is the establishment of MMP-2-dependent degradation of cardiac contractile proteins in response to increased oxidative stress conditions, such as ischemia/reperfusion. The authors' laboratory has identified a promising preventive therapeutic target using the classical pharmacological concept of synergy to target MMP-2 activity and its proteolytic action on a cardiac contractile protein. This manuscript provides an overview of the body of evidence that supports the importance of cardiac contractile protein degradation in ischemia/reperfusion injury and the use of synergy to protect against it.

Molecular mechanism of actin-myosin motor in muscle

The interaction of actin and myosin powers striated and smooth muscles and some other types of cell motility. Due to its highly ordered structure, skeletal muscle is a very convenient object for studying the general mechanism of the actin-myosin molecular motor. The history of investigation of the actin-myosin motor is briefly described. Modern concepts and data obtained with different techniques including protein crystallography, electron microscopy, biochemistry, and protein engineering are reviewed. Particular attention is given to X-ray diffraction studies of intact muscles and single muscle fibers with permeabilized membrane as they give insight into structural changes that underlie force generation and work production by the motor. Time-resolved low-angle X-ray diffraction on contracting muscle fibers using modern synchrotron radiation sources is used to follow movement of myosin heads with unique time and spatial resolution under near physiological conditions.

Tropomyosin: double helix from the protein world

This review concerns the structure and functions of tropomyosin (TM), an actin-binding protein that plays a key role in the regulation of muscle contraction. The TM molecule is a dimer of α-helices, which form a coiled-coil. Recent views on the TM structure are analyzed, and special attention is concentrated on those structural traits of the TM molecule that distinguish it from the other coiled-coil proteins. Modern data are presented on TM functional properties, such as its interaction with actin and ability to move on the surface of actin filaments, which underlies the regulation of the actin-myosin interaction upon contraction of skeletal and cardiac muscles. Also, part of the review is devoted to analysis of the effects of mutations in TM genes associated with muscle diseases (myopathies) on the structure and functions of TM.

Myofibrillar myopathy caused by a mutation in the motor domain of mouse MyHC IIb

Ariel is a mouse mutant that suffers from skeletal muscle myofibrillar degeneration due to the rapid accumulation of large intracellular protein aggregates. This fulminant disease is caused by an ENU-induced recessive mutation resulting in an L342Q change within the motor domain of the skeletal muscle myosin protein MYH4 (MyHC IIb). Although normal at birth, homozygous mice develop hindlimb paralysis from Day 13, consistent with the timing of the switch from developmental to adult myosin isoforms in mice. The mutated myosin (MYH4(L342Q)) is an aggregate-prone protein. Notwithstanding the speed of the process, biochemical analysis of purified aggregates showed the presence of proteins typically found in human myofibrillar myopathies, suggesting that the genesis of ariel aggregates follows a pathogenic pathway shared with other conformational protein diseases of skeletal muscle. In contrast, heterozygous mice are overtly and histologically indistinguishable from control mice. MYH4(L342Q) is present in muscles from heterozygous mice at only 7% of the levels of the wild-type protein, resulting in a small but significant increase in force production in isolated single fibres and indicating that elimination of the mutant protein in heterozygotes prevents the pathological changes observed in homozygotes. Recapitulation of the L342Q change in the functional equivalent of mouse MYH4 in human muscles, MYH1, results in a more aggregate-prone protein.

Modeling smooth muscle myosin's two heads: long-lived enzymatic roles and phosphorylation-dependent equilibria

Smooth muscle myosin has two heads, each capable of interacting with actin to generate force and/or motion as it hydrolyzes ATP. These heads are inhibited when their associated regulatory light chain is unphosphorylated (0P), becoming active and hydrolyzing ATP maximally when phosphorylated (2P). Interestingly, with only one of the two regulatory light chains phosphorylated (1P), smooth muscle myosin is active but its ATPase rate is <2P. To explain published 1P single ATP turnover and steady-state ATPase activities, we propose a kinetic model in which 1P myosin exists in an equilibrium between being fully active (2P) and inhibited (0P). Based on the single ATP turnover data, we also propose that each 2P head adopts a hydrolytic role distinct from its partner at any point in time, i.e., one head strongly binds actin and hydrolyzes ATP at its actin-activated rate while the other weakly binds actin. Surprisingly, the heads switch roles slowly (<0.1 s(-1)), suggesting that their activities are not independent. The phosphorylation-dependent equilibrium between active and inhibited states and the hydrolytic role that each head adopts during its interaction with actin may have implications for understanding regulation and mechanical performance of other members of the myosin family of molecular motors.

On the attribution and additivity of binding energies

It can be useful to describe the Gibbs free energy changes for the binding to a protein of a molecule, A-B, and of its component parts, A and B, in terms of the "intrinsic binding energies" of A and B, DeltaG(A) (i) and DeltaG(B) (i), and a "connection Gibbs energy," DeltaG(s) that is derived largely from changes in translational and rotational entropy. This empirical approach avoids the difficult or insoluble problem of interpreting observed DeltaH and TDeltaS values for aqueous solutions. The DeltaG(i) and DeltaG(s) terms can be large for binding to enzymes and other proteins.

Alternative exon 9-encoded relay domains affect more than one communication pathway in the Drosophila myosin head

We investigated the biochemical and biophysical properties of one of the four alternative regions within the Drosophila myosin catalytic domain: the relay domain encoded by exon 9. This domain of the myosin head transmits conformational changes in the nucleotide-binding pocket to the converter domain, which is crucial to coupling catalytic activity with mechanical movement of the lever arm. To study the function of this region, we used chimeric myosins (IFI-9b and EMB-9a), which were generated by exchange of the exon 9-encoded domains between the native embryonic body wall (EMB) and indirect flight muscle isoforms (IFI). Kinetic measurements show that exchange of the exon 9-encoded region alters the kinetic properties of the myosin S1 head. This is reflected in reduced values for ATP-induced actomyosin dissociation rate constant (K(1)k(+2)) and ADP affinity (K(AD)), measured for the chimeric constructs IFI-9b and EMB-9a, compared to wild-type IFI and EMB values. Homology models indicate that, in addition to affecting the communication pathway between the nucleotide-binding pocket and the converter domain, exchange of the relay domains between IFI and EMB affects the communication pathway between the nucleotide-binding pocket and the actin-binding site in the lower 50-kDa domain (loop 2). These results suggest an important role of the relay domain in the regulation of actomyosin cross-bridge kinetics.

Mechanoenzymatic characterization of human myosin Vb

There are three isoforms of class V myosin in mammals. While myosin Va has been studied well, little is known about the function of other myosin V isoforms (Vb and Vc) at a molecular level. Here we report the mechanoenzymatic function of human myosin Vb (HuM5B) for the first time. Electron microscopic observation showed that HuM5B has a double-headed structure with a long neck like myosin Va. V(max) and K(actin) of the actin-activated ATPase activity of HuM5B were 9.7 +/- 0.4 s(-)(1) and 8.5 +/- 0.1 microM, respectively. K(actin) and K(ATP) of the actin-activated ATPase activity were significantly higher than those of myosin Va. ADP markedly inhibited the ATPase activity. The rate of release of ADP from acto-HuM5B was 12.2 +/- 0.5 s(-)(1), which was comparable to the V(max) of the actin-activated ATPase activity. These results suggest that ADP release is the rate-limiting step for the actin-activated ATPase cycle; thus, HuM5B is a high duty ratio myosin. Consistently, the actin gliding velocity (0.22 +/- 0.03 microm/s) remained constant at a low motor density. The actin filament landing assay revealed that a single HuM5B molecule is sufficient to move the actin filament continuously, indicating that HuM5b is a processive motor.

A mutant heterodimeric myosin with one inactive head generates maximal displacement

Each of the heads of the motor protein myosin II is capable of supporting motion. A previous report showed that double-headed myosin generates twice the displacement of single-headed myosin (Tyska, M.J., D.E. Dupuis, W.H. Guilford, J.B. Patlak, G.S. Waller, K.M. Trybus, D.M. Warshaw, and S. Lowey. 1999. Proc. Natl. Acad. Sci. USA. 96:4402-4407). To determine the role of the second head, we expressed a smooth muscle heterodimeric heavy meromyosin (HMM) with one wild-type head, and the other locked in a weak actin-binding state by introducing a point mutation in switch II (E470A). Homodimeric E470A HMM did not support in vitro motility, and only slowly hydrolyzed MgATP. Optical trap measurements revealed that the heterodimer generated unitary displacements of 10.4 nm, strikingly similar to wild-type HMM (10.2 nm) and approximately twice that of single-headed subfragment-1 (4.4 nm). These data show that a double-headed molecule can achieve a working stroke of approximately 10 nm with only one active head and an inactive weak-binding partner. We propose that the second head optimizes the orientation and/or stabilizes the structure of the motion-generating head, thereby resulting in maximum displacement.

The two heads of smooth muscle myosin are enzymatically independent but mechanically interactive

The interaction between the two heads of myosin II during motion and force production is poorly understood. To examine this issue, we developed an expression and purification strategy to isolate homogeneous populations of heterodimeric smooth muscle heavy meromyosins containing heads with different properties. As an extreme example, we characterized a heterodimer containing one native head and one head locked in a "weak binding" state by a point mutation in switch 2 (E470A). The in vitro actin filament motility of this heterodimer was the same as the homodimeric control with two cycling heads, suggesting that only one head of a pair actively interacts with actin to generate maximal velocity. A second naturally occurring heterodimer contained two cycling heads with 2-fold different activity, due to the presence or absence of a 7-amino acid insert near the active site. Enzymatically this (+/-) insert heterodimer was indistinguishable from a (50:50) mixture of the two homodimers, but its motility averaged 17% less than that of the mixture. These data suggest that one head of a heterodimer can disproportionately affect the mechanics of double-headed myosin, a finding relevant to our understanding of heterozygous mutant myosins found in disease states like familial hypertrophic cardiomyopathy.

The myosin power stroke

Optical trapping technology now allows investigators in the motility field to measure the forces generated by single motor molecules. A handful of research groups have exploited this approach to further develop our understanding of the actin-based motor, myosin, an ATPase that is capable of converting chemical energy into mechanical work during a cyclical interaction with filamentous actin. In this regard, myosin-II from muscle is the most well-characterized myosin superfamily member. By combining the data obtained from optical trap assays with that from ensemble biochemical and mechanical assays, this review discusses the fundamental properties of the myosin-II power stroke and, perhaps more significantly, how these properties are governed by this molecule's atomic structure and the biochemical transitions that define its catalytic cycle.

A model for regulation of the Mg(2+)-stimulated acto-myosin-ATPase activity: inhibition of the formation of actin-myosin complex and the Mg( 2+)-stimulated acto-myosin-ATPase activity by IMP and AMP

Previously, we showed that the decrease in force output during continuous isometric contractions in rat skeletal muscle was related to an increase in the concentration of IMP. In this paper we report on additional experiments in which the effect of IMP on the Mg(2+)-stimulated acto-myosin-ATPase activity of isolated actin and myosin is measured at 35 degrees C. The results show that 1) the binding of actin to myosin is co-operative (Hill coefficient = 3.82); 2) in the presence of IMP or AMP the Mg(2+)-stimulated acto-myosin-ATPase activity is inhibited up to 60% at 10 mM; 3) in the presence of IMP or AMP not only the Mg(2+)-stimulated acto-myosin-ATPase activity decreases, but also K(50). From these results we conclude that IMP and AMP may be considered as uncompetitive inhibitors. Our results suggest that IMP and AMP can prevent an 'energy crisis' during exhaustive exercise of short duration by down-regulating the contractile machinery.

Structural mechanism of muscle contraction

X-ray crystallography shows the myosin cross-bridge to exist in two conformations, the beginning and end of the "power stroke." A long lever-arm undergoes a 60 degrees to 70 degrees rotation between the two states. This rotation is coupled with changes in the active site (OPEN to CLOSED) and phosphate release. Actin binding mediates the transition from CLOSED to OPEN. Kinetics shows that the binding of myosin to actin is a two-step process which affects ATP and ADP affinity. The structural basis of these effects is not explained by the presently known conformers of myosin. Therefore, other states of the myosin cross-bridge must exist. Moreover, cryoelectronmicroscopy has revealed other angles of the cross-bridge lever arm induced by ADP binding. These structural states are presently being characterized by site-directed mutagenesis coupled with kinetic analysis.

The structural basis of muscle contraction

The myosin cross-bridge exists in two conformations, which differ in the orientation of a long lever arm. Since the lever arm undergoes a 60 degree rotation between the two conformations, which would lead to a displacement of the myosin filament of about 11 nm, the transition between these two states has been associated with the elementary 'power stroke' of muscle. Moreover, this rotation is coupled with changes in the active site (CLOSED to OPEN), which probably enable phosphate release. The transition CLOSED to OPEN appears to be brought about by actin binding. However, kinetics shows that the binding of myosin to actin is a two-step process which affects both ATP and ADP affinity and vice versa. The structural basis of these effects is only partially explained by the presently known conformers of myosin. Therefore, additional states of the myosin cross-bridge should exist. Indeed, cryoelectron microscopy has revealed other angles of the lever arm induced by ADP binding to a smooth muscle actin-myosin complex.

Dystrophin and utrophin complexed with different associated proteins in cardiac Purkinje fibres

Abnormal dystrophin expression is directly responsible for Duchenne and Becker muscular dystrophies. In skeletal muscle, dystrophin provides a link between the actin network and the extracellular matrix via the dystrophin-associated protein complex. In mature skeletal muscle, utrophin is a dystrophin-related protein localized mainly at the neuromuscular junction, with the same properties as dystrophin in terms of linking the protein complex. Utrophin could potentially overcome the absence of dystrophin in dystrophic skeletal muscles. In cardiac muscle, dystrophin and utrophin were both found to be present with a distinct subcellular distribution in Purkinje fibres, i.e. utrophin was limited to the cytoplasm, while dystrophin was located in the cytoplasmic membrane. In this study, we used this particular characteristic of cardiac Purkinje fibres and demonstrated that associated proteins of dystrophin and utrophin are different in this structure. We conclude, contrary to skeletal muscle, dystrophin-associated proteins do not form a complex in Purkinje fibres. In addition, we have indirect evidence of the presence of two different 400 kDa dystrophins in Purkinje fibres.

Two heads of myosin are better than one for generating force and motion

Several classes of the myosin superfamily are distinguished by their "double-headed" structure, where each head is a molecular motor capable of hydrolyzing ATP and interacting with actin to generate force and motion. The functional significance of this dimeric structure, however, has eluded investigators since its discovery in the late 1960s. Using an optical-trap transducer, we have measured the unitary displacement and force produced by double-headed and single-headed smooth- and skeletal-muscle myosins. Single-headed myosin produces approximately half the displacement and force (approximately 6 nm; 0.7 pN) of double-headed myosin (approximately 10 nm; 1.4 pN) during a unitary interaction with actin. These data suggest that muscle myosins require both heads to generate maximal force and motion.

Utrophin and dystrophin-associated glycoproteins in normal and dystrophin deficient cardiac muscle

In this study, various members of the dystrophin family (dystrophin, the short dystrophin product Dp 71, utrophin and DRP2), and different members of the dystrophin-associated glycoprotein (DAG) complex (beta-dystroglycan, alpha-, beta-, gamma- and delta-sarcoglycans) were localized in bovine cardiac muscle using a battery of specific antibodies. We have established that dystrophin is exclusively associated with beta-dystroglycan and both alpha- and delta-sarcoglycans in cardiac muscle cell membranes. In contrast, utrophin is a specific component of intercalated disks together with beta- and gamma-sarcoglycans, while beta-dystroglycan, alpha- and delta-sarcoglycans are not present. Dp 71 is mainly localized at the T tubule transverse area. In dystrophin deficient cardiac muscle, utrophin and beta-sarcoglycan were observed in intercalated disks and at the sarcolemma of each cardiocyte. Our results revealed that complexes of associated glycoproteins differ in cardiac muscle when associated with dystrophin or utrophin. Despite the described sequence homologies between dystrophin and utrophin, the present results indicate that these proteins have different roles in some specific cardiac cell areas.

Cooperativity between two heads of dictyostelium myosin II in in vitro motility and ATP hydrolysis

To elucidate the significance of the two-headed structure of myosin II, we have engineered and characterized recombinant single-headed myosin II. A tail segment of a myosin II heavy chain fused with a His-tag was expressed in wild-type Dictyostelium cells. Single-headed myosin, which consists of a full length myosin heavy chain and a tagged tail, was isolated on the basis of the affinities for Nickel agarose and actin. Actin sliding velocity by the single-headed myosin was about half of the two-headed, whereas the minimum density of the heads to support continuous movement was twofold higher. Actin-activated MgATPase activity of the single-headed myosin in solution in the presence of 24 microM actin was less than half of the two headed. This decrease is primarily because of fourfold-elevated Kapp for actin and secondary to 40% lower Vmax. These results suggest that the two heads of a Dictyostelium myosin II molecule act cooperatively on an actin filament. We propose a mechanism by which two heads move actin efficiently based on the cooperativity.

Pathway of ATP hydrolysis by monomeric and dimeric kinesin

The ATPase mechanism for a monomeric Drosophila kinesin construct, K341, was determined by pre-steady-state kinetic methods and compared to dimeric kinesin, K401. We directly measured the kinetics of binding mantATP (a fluorescent ATP analog) to the microtubule K341 complex, the dissociation of K341 from the microtubule, and release of phosphate and ADP from K341. Measurements of phosphate release kinetics at low salt concentration show that K341 hydrolyzes 18 molecules of ATP per kinesin monomer prior to release from the microtubule. At a higher salt concentration the amplitude of the pre-steady-state burst of phosphate release was reduced to 8 molecules per kinesin monomer. The maximum rate of dissociation of K341 from the microtubule following the addition of ATP was 22 s-1. The rate of mantADP release from the M.K341.mantADP complex increased as a function of tubulin concentration with a second-order rate constant of 11 microM-1 s-1 for K341 binding to the microtubule and reached a maximum rate of mantADP release of 303 s-1. ADP release kinetics were also determined by monitoring the binding of mantATP to K341.ADP and K401.ADP after mixing with microtubules. We show that monomeric kinesin remains associated with the microtubule through multiple rounds of ATP hydrolysis. This apparent processivity implies that one of the functions of the cooperative interaction between the two kinesin heads in dimeric kinesin is for the reactions occurring on one kinesin head to facilitate the release of the adjacent head from the microtubule.

Myosin regulatory light chain and nucleotide modulation of actin binding site electric charge

The ionic strength dependence of skeletal muscle myosin subfragment 1 (S1) binding to actin in the presence of ADP and ATP was measured for S1 with either only an essential light chain [S1(elc)] or with both an essential and the regulatory light chains [S1(elc,rlc)] bound. The data were analyzed to determine the apparent association constant, K(A), for actin binding and the absolute value of the product of the net effective electric charges at the actin-myosin interface, /ZMZA/. When MgADP is bound at the myosin active site, K(A) values at 0 M ionic strength for S1(elc) and S1(elc,rlc) are 12 and 4.9 x 10(6) M(-1), respectively, and /ZMZA/ values are 3.9 +/- 0.3 and 3.6 +/- 0.2 esu2. In the presence of ATP, K(A) values at 0 M ionic strength for S1(elc) and S1(elc,rlc) are 81 and 7.3 x 10(4) M(-1), respectively, and /ZMZA/ values are 14.7 esu2 for S1(elc) but only 6.4 esu2 for S1(elc,rlc). The Michaelis constant, K(M), for the actin activation of S1 steady-state MgATPase activity was significantly smaller for S1(elc), consistent with its greater K(A) and /ZMZA/. These data indicate that the regulatory light chain can allosterically regulate the interactions of myosin and actin by modulating the electric charge at the actin binding site. K(A) and /ZMZA/ were also measured at 25 degrees C for S1(elc,rlc) binding to actin in the presence of the ATP analog ATPgammaS. At 0 M ionic strength, K(A) is 8.0 x 10(4) M(-1), and /ZMZA/ is 0, within experimental uncertainty, suggesting that for S1 x MgATP the electric charge at the actin binding site is abolished. The results are interpreted in terms of possible roles of electrostatic interactions in mechanisms for S1 x MgATP dissociating from one actin and S1 x MgADP x Pi being guided electrostatically to bind to another.

Kinetics of association of myosin subfragment-1 to unlabeled and pyrenyl-labeled actin

The kinetics of reaction of myosin subfragment-1 (S1) with F-actin have been monitored by the changes in light scattering and in pyrenyl-actin fluorescence at 20 degrees C, pH 7.5, and physiological ionic strength. The association rate constant of S1 to F-actin decreases about 10-fold as the molar ratio of bound S1 increases from 0 to 1. This decrease in k+ is most likely due to the steric hindrance of available binding sites by initially bound S1. The apparent rate constant for association of S1 to bare filaments is 9 microM-1 s-1, a value 1 order of magnitude higher than the one previously estimated from experiments in which S1 was in excess over F-actin. The anticooperative binding kinetics of S1 to F-actin are consistent with the negative cooperativity displayed in the equilibrium binding curves of S1 to pyrenyl-F-actin. Fluorescence titration curves of partially labeled pyrenyl-F-actin by S1 are sigmoidal, consistent with a 4-fold higher affinity of S1 for unlabeled than for labeled action. This conclusion is strengthened by kinetic data of S1 binding to partially labeled F-actin, which exhibit a biphasic behavior due to the slower dissociation of S1 from unlabeled than from labeled actin.

Compliance of thin filaments in skinned fibers of rabbit skeletal muscle

The mechanical compliance (reciprocal of stiffness) of thin filaments was estimated from the relative compliance of single, skinned muscle fibers in rigor at sarcomere lengths between 1.8 and 2.4 micron. The compliance of the fibers was calculated as the ratio of sarcomere length change to tension change during imposition of repetitive cycles of small stretches and releases. Fiber compliance decreased as the sarcomere length was decreased below 2.4 micron. The compliance of the thin filaments could be estimated from this decrement because in this range of lengths overlap between the thick and thin filaments is complete and all of the myosin heads bind to the thin filament in rigor. Thus, the compliance of the overlap region of the sarcomere is constant as length is changed and the decrease in fiber compliance is due to decrease of the nonoverlap length of the thin filaments (the I band). The compliance value obtained for the thin filaments implies that at 2.4-microns sarcomere length, the thin filaments contribute approximately 55% of the total sarcomere compliance. Considering that the sarcomeres are approximately 1.25-fold more compliant in active isometric contractions than in rigor, the thin filaments contribute approximately 44% to sarcomere compliance during isometric contraction.

Single-headed myosin II acts as a dominant negative mutation in Dictyostelium

Conventional myosin II is an essential protein for cytokinesis, capping of cell surface receptors, and development of Dictyostelium cells. Myosin II also plays an important role in the polarization and movement of cells. All conventional myosins are double-headed molecules but the significance of this structure is not understood since single-headed myosin II can produce movement and force in vitro. We found that expression of the tail portion of myosin II in Dictyostelium led to the formation of single-headed myosin II in vivo. The resultant cells contain an approximately equal ratio of double- and single-headed myosin II molecules. Surprisingly, these cells were completely blocked in cytokinesis and capping of concanavalin A receptors although development into fruiting bodies was not impaired. We found that this phenotype is not due to defects in myosin light chain phosphorylation. These results show that single-headed myosin II cannot function properly in vivo and that it acts as a dominant negative mutation for myosin II function. These results suggest the possibility that cooperativity of myosin II heads is critical for force production in vivo.

A minimal motor domain from chicken skeletal muscle myosin

The myosin head (S1) consists of a wide, globular region that contains the actin- and nucleotide-binding sites and an alpha-helical, extended region that is stabilized by the presence of two classes of light chains. The essential light chain abuts the globular domain, whereas the regulatory light chain lies near the head-rod junction of myosin. Removal of the essential light chain by a mild denaturant exposes the underlying heavy chain to proteolysis by chymotrypsin. The cleaved fragment, or "motor domain" (MD), migrates as a single band on SDS-polyacrylamide gel electrophoresis, with a slightly greater mobility than S1 prepared by papain or chymotrypsin. Three-dimensional image analysis of actin filaments decorated with MD reveals a structure similar to S1, but shorter by an amount consistent with the absence of a light chain-binding domain. The actin-activated MgATPase activity of MD is similar to that of S1 in Vmax and Km. But the ability of MD to move actin filaments in a motility assay is considerably reduced relative to S1. We conclude that the globular, active site region of the myosin head is a stable, independently folded domain with intrinsic motor activity, but the coupling efficiency between ATP hydrolysis and movement declines markedly as the light chain binding region is truncated.

Movement of single myosin filaments and myosin step size on an actin filament suspended in solution by a laser trap

Movement of single myosin filaments, synthesized by copolymerization of intact myosin and fluorescently labeled light meromyosin, were observed along a single actin filament suspended in solution by a dual laser trap in a fluorescence microscope. The sliding velocity of the myosin filaments was 11.0 +/- 0.2 micron/s at 27 degrees C. This is similar to that of actin moving toward the center from the tip (the physiological direction) of myosin filaments bound to a glass surface but several times larger than that in the opposite direction (Ishijima and Yanagida, 1991; Yanagida, 1993). This indicates that the movement of myosin filaments is dominated by the myosin heads on one side of the myosin filament, which are correctly oriented relative to the actin filament. The incorrectly oriented myosin heads on the other side do not interfere with the fast movement. The step size (displacement produced during one ATPase cycle) of correctly oriented myosin was estimated from the minimum number of myosin heads necessary to produce the maximum velocity. This was determined by measuring the velocities of various lengths of myosin filaments. The minimum length of the myosin filaments moving near the maximum velocity was 0.30-0.40 microns, which contains 20 +/- 5 correctly oriented myosin heads. This number leads to a myosin step size of 71 +/- 22 nm. This value probably represents the lower limit, because all of the myosin heads on the filament would not always interact with the actin filament. Thus, the myosin step size is considerably larger than the length of a power stroke expected from the physical size of a myosin head, 10-20 nm (Huxley, 1957, 1969).

A functional recombinant myosin II lacking a regulatory light chain-binding site

Myosin II, which converts the energy of adenosine triphosphate hydrolysis into the movement of actin filaments, is a hexamer of two heavy chains, two essential light chains, and two regulatory light chains (RLCs). Dictyostelium myosin II is known to be regulated in vitro by phosphorylation of the RLC. Cells in which the wild-type myosin II heavy chain was replaced with a recombinant form that lacks the binding site for RLC carried out cytokinesis and almost normal development, processes known to be dependent on functional myosin II. Characterization of the purified recombinant protein suggests that a complex of RLC and the RLC binding site of the heavy chain plays an inhibitory role for adenosine triphosphatase activity and a structural role for the movement of myosin along actin.

Binding of myosin subfragment-1 to F-actin

During a part of the hydrolytic cycle, myosin head (S1) carries no nucleotide and binds strongly to an actin filament forming a rigor bond. At saturating concentration of S1 in rigor, S1 is well known to form 1:1 complex with actin. However, we have provided evidence that under certain conditions S1 could also form a complex with 2 actin monomers in a filament (Andreev, O.A. & Borejdo, J. (1991) Biochem. Biophys. Res. Comm. 177, 350-356). This view was recently challenged by Carlier & Didry (Carlier, M-F. & Didry, D. (1992) Biochem. Biophys. Res. Comm. 183, 970-974) who interpreted our data by suggesting that F-actin underwent a simple depolymerization and implied that, when only actin in the F-form was scored, the real stoichiometry in our experiments was 1:1. We show here that under conditions of our experiments less than 8% of actin was depolymerized. Moreover, we have repeated the experiments in the presence of phalloidin and show that under these conditions too, when S1 was added slowly to a fixed concentration of F-actin, it formed a different complex with F-actin than when it was added quickly. This confirms our original conclusion that S1 can bind actin in two different ways and shows that depolymerization of F-actin is not responsible for this finding.

Three-dimensional structure of myosin subfragment-1 from electron microscopy of sectioned crystals

Image analysis of electron micrographs of thin-sectioned myosin subfragment-1 (S1) crystals has been used to determine the structure of the myosin head at approximately 25-A resolution. Previous work established that the unit cell of type I crystals of myosin S1 contains eight molecules arranged with orthorhombic space group symmetry P212121 and provided preliminary information on the size and shape of the myosin head (Winkelmann, D. A., H. Mekeel, and I. Rayment. 1985. J. Mol. Biol. 181:487-501). We have applied a systematic method of data collection by electron microscopy to reconstruct the three-dimensional (3D) structure of the S1 crystal lattice. Electron micrographs of thin sections were recorded at angles of up to 50 degrees by tilting the sections about the two orthogonal unit cell axes in sections cut perpendicular to the three major crystallographic axes. The data from six separate tilt series were merged to form a complete data set for 3D reconstruction. This approach has yielded an electron density map of the unit cell of the S1 crystals of sufficient detail. to delineate the molecular envelope of the myosin head. Myosin S1 has a tadpole-shaped molecular envelope that is very similar in appearance to the pear-shaped myosin heads observed by electron microscopy of rotary-shadowed and negatively stained myosin. The molecule is divided into essentially three morphological domains: a large domain on one end of the molecule corresponding to approximately 60% of the total molecular volume, a smaller central domain of approximately 30% of the volume that is separated from the larger domain by a cleft on one side of the molecule, and the smallest domain corresponding to a thin tail-like region containing approximately 10% of the volume. This molecular organization supports models of force generation by myosin which invoke conformational mobility at interdomain junctions within the head.

Influence of the cardiac myosin hinge region on contractile activity

The participation of cardiac myosin hinge in contractility was investigated by in vitro motility and ATPase assays and by measurements of sarcomere shortening. The effect on contractile activity was analyzed using an antibody directed against a 20-amino acid peptide within the hinge region of myosin. This antibody bound specifically at the hinge at a distance of 55 nm from the S1/S2 junction, was specific to human, dog, and rat cardiac myosins, did not crossreact with gizzard or skeletal myosin, and had no effect on ATPase activity of purified S1 and myofibrils. However, it completely suppressed the movement of actin filaments in in vitro motility assays and reduced active shortening of sarcomeres of skinned cardiac myocytes by half. Suppression of motion by the anti-hinge antibody may reflect a mechanical constraint imposed by the antibody upon the mobility of the S2 region of myosin. The results suggest that the steps in the mechanochemical energy transduction can be separately influenced through S2.

The myosin head can bind two actin monomers

Force impulse is thought to be generated in muscle when myosin head (S-1), while weakly bound to actin filament, undergoes orientational change to form a strong (rigor) bond with actin. There is ample evidence that this bond involves interaction of 1 myosin head with 1 actin monomer. However, X-ray diffraction data of muscle decorated with S-1, as well as recently proposed model of the thin filaments, suggested that each S-1 molecule interacted with two actin monomers. We reinvestigated this controversy and found that the stoichiometry of acto-S-1 bond depended on the relative amounts of actin and myosin present during titrations: when increasing amounts of actin were added to a fixed amount of S-1 (i.e. when myosin heads were initially in excess over actin), the saturating stoichiometry was 1 mol of S-1 per 1 mol of actin. However, when increasing amounts of S-1 were added slowly to a fixed amount of F-actin (i.e. when actin was initially in excess over S-1), the stoichiometry at saturation was 1 mol of S-1 per 2 mols of actin. The ability of S-1 to bind either one or two actin monomers suggests a way that force could be generated during muscle contraction.

Temperature dependence of the release of ATP hydrolysis products from the 10S conformation of smooth muscle myosin

The transition of smooth muscle myosin to the folded 10S monomeric conformation dramatically inhibits the release of the ATP hydrolysis products, ADP and Pi. In this work, we examined the influence of temperature on the time course of product release from the 10S conformer of chicken gizzard smooth muscle myosin. Release was monitored by single turnover assays, using either [gamma-32P]ATP or the fluorescent ATP analog, formycin triphosphate (FTP). For all temperatures over the range 15-35 degrees C, single exponential kinetics described the observed product release from 10S myosin. A 10 degrees C increase in temperature resulted in a fourfold increase in the rate constant for the observed product release. Using single turnover analysis, we found a similar temperature dependence for the apparent rate constants for product release from the extended 6S monomeric conformation of myosin. However, at any given temperature, the rate constant for 6S myosin was approximately 1.5 orders of magnitude greater than that for the 10S. These results are consistent with a kinetic scheme in which 10S myosin must undergo transition to the 6S conformation prior to product release.

The influence of substoichiometric concentrations of myosin subfragment 1 on the state of aggregation of actin under depolymerizing conditions

In 3 mM KCl, 2 mM Tris/HCl pH 7.5, 22 degrees C, 0.38 microM myosin subfragment 1 delays the depolymerization of F-actin (7.2 microM measured as monomer). The depolymerization proceeds rapidly for a few minutes and then slows down suddenly when the ratio between the monomers in the actin filaments and myosin subfragment 1 reaches the value of 11. At this time myosin subfragment 1 is substantially all bound to the actin polymers which form an irregular and discontinuous network of filaments running in doublets and in triplets, perhaps cross-linked by myosin subfragment 1. Depolymerization proceeds then for several hours, apparently ending up with the formation of the 1:1 actin-S1 heteropolymer. The ratio between the monomers in the actin filaments and myosin subfragment 1 at the end of the rapid depolymerization process is different for different protein preparations and may be as low as 5.5. In 2 mM Tris/HCl pH 7.5, 25 degrees C, 1 microM myosin subfragment 1 is able to induce the formation of undecorated actin filaments from 12 microM ATP--G-actin. These filaments probably originate by redistribution of myosin subfragment 1 between the newly formed 1/1 actin-S1 heteropolymer and G-actin in the medium, a process which allows the transient formation of undecorated actin filaments.

Temporal and tissue-specific expression of myosin heavy chain isoforms in developing and adult avian muscle

We have raised monoclonal antibodies (Mabs) to myosin heavy chain isoforms (MHCs) that have specific patterns of temporal expression during the development of quail pectoral muscle and that are expressed in very restricted, tissue-specific patterns in adult birds. We find that an early embryonic, a perinatal, and an adult-specific, fast myosin heavy chain are co-expressed at different levels in the pectoral muscle of 8-12 day quail embryos. The early embryonic MHC disappears from the pectoral muscle at approximately 14 days in ovo, whereas the perinatal MHC persists until 26 days post-hatching. The adult-specific MHC accumulates preferentially and eventually completely replaces the other isoforms. These Mabs cross-react with the homologous isoforms of the chick and detect a similar pattern of MHC expression in the pectoral muscle of developing chicks. Although the early embryonic and perinatal MHC isoforms recognized by our Mabs are expressed in the pectoral muscle only during distinct developmental stages, our Mabs also recognize MHC isoforms present in the heart and extraocular muscle of adult quail. Immunofingerprinting using Staphylococcus aureus protease V8 suggests that the early embryonic and perinatal MHC isoforms that we see are strongly homologous with the adult ventricular and extraocular muscle isoforms, respectively. These observations suggest that at least three distinct MHC isoforms, which are normally expressed in adult muscles, are co-expressed during the early development of the pectoral muscle in birds. In this respect, the pattern of expression of the MHCs recognized by our Mabs in developing, fast muscle is very similar to the patterns described for other muscle contractile proteins.

Force measurements by micromanipulation of a single actin filament by glass needles

Single actin filaments (approximately 7 nm in diameter) labelled with fluorescent phalloidin can be clearly seen by video-fluorescence microscopy. This technique has been used to observe motions of single filaments in solution and in several in vitro movement assays. In a further development of the technique, we report here a method to catch and manipulate a single actin filament (F-actin) by glass microneedles under conditions in which external force on the filament can be applied and measured. Using this method, we directly measured the tensile strength of a filament (the force necessary to break the bond between two actin monomers) and the force required for a filament to be moved by myosin or its proteolytic fragment bound to a glass surface in the presence of ATP. The first result shows that the tensile strength of the F-actin-phalloidin complex is comparable with the average force exerted on a single thin filament in muscle fibres during isometric contraction. This force is increased only slightly by tropomyosin. The second measurement shows that the myosin head (subfragment-1) can produce the same ATP-dependent force as intact myosin. The magnitude of this force is comparable with that produced by each head of myosin in muscle during isometric contraction.

The 110-kD protein-calmodulin complex of the intestinal microvillus is an actin-activated MgATPase

The microvillus 110-kD protein-calmodulin complex (designated 110K-CM) shares several properties with all myosins. In addition to its well-defined ATP-dependent binding interaction with F-actin, 110K-CM is an ATPase with diagnostically myosin-like divalent cation sensitivity. It exhibits maximum enzymatic activity in the presence of K+ and EDTA (0.24 mumol P1/mg per min) or in the presence of Ca++ (0.40 mumol P1/mg per min) and significantly less activity in physiological ionic conditions of salt and Mg++ (0.04 mumol P1/mg per min). This MgATPase is activated by F-actin in an actin concentration-dependent manner (up to 2.5-3.5-fold). The specific MgATPase activity of 110K-CM is also enhanced by the addition of 5-10 microM Ca++, but in the isolated complex, there is often also a decrease in the extent of actin activation in this range of free Ca++. Actin activation is maintained, however, in samples with exogenously added calmodulin; under these conditions, there is an approximately sevenfold stimulation of 110K-CM's enzymatic activity in the presence of 5-10 microM Ca++ and actin. 110K-CM is relatively indiscriminant in its nucleoside triphosphate specificity; in addition to ATP, GTP, CTP, UTP, and ITP are all hydrolyzed by the complex in the presence of either Mg++ or Ca++. Neither AMP nor the phosphatase substrate p-nitrophenyl phosphate are substrates for the enzymatic activity. The pH optimum for CaATPase activity is 6.0-7.5; maximum actin activation of MgATPase occurs over a broad pH range of 6.5-8.5. Finally, like myosins, purified 110K-CM crosslinks actin filaments into loosely ordered aggregates in the absence of ATP. Collectively these data support the proposal of Collins and Borysenko (1984, J. Biol. Chem., 259:14128-14135) that the 110K-CM complex is functionally analogous to the mechanoenzyme myosin.

Physico-chemical properties of rat and dog cardiac alpha-actinin

alpha-Actinin exists in several polymorphic forms which appear to be characteristic of the muscle type from which it is isolated. In order to determine the possible physiological role of this structural protein in cardiac muscle, we describe and compare here the physico-chemical properties of cardiac alpha-actinin from two different mammalian species, rat (fast contracting muscle) and dog (slow contracting muscle). Purification of cardiac alpha-actinin was achieved by chromatography on DEAE-cellulose and hydroxyapatite columns. The alpha-actinins isolated were different in their electrophoretic mobility (SDS-polyacrylamide gel electrophoresis), molecular size and alpha-helical content. However, their shape as revealed by electron microscopy and their activating effect on Mg2+-ATPase activity of actomyosin appear to be similar. These studies suggest that the rat and dog cardiac alpha-actinin are structurally different but functionally similar proteins.

Analysis of the self-association of human red cell spectrin

The self-association equilibrium of spectrin has been studied by separating the molecular species present in the cooled reaction mixture by gel electrophoresis. The association constant for formation of the hexamer from dimer and tetramer is lower by an order of magnitude than that for the association of two dimers. The association constant for the formation of the octamer from the hexamer is appreciably larger, and the value appears to reach a constant level for higher oligomers. These observations are explained in terms of conformational strain due to formation of cyclic structures, the distortion being greatest on passing from the tetramer to the hexamer. The association for a single-site interaction between the dimer and a univalent fragment has also been analyzed. The results show that the free energy generated by a single-point interaction is much greater than that obtained by averaging over all pairwise interactions within the oligomers, correcting for the effect of cratic entropy. The results are related to the association state of the spectrin prevailing in the cell. Phosphorylation at the physiological sites in the dimer does not appreciably change the thermodynamics of self-association, at least up to the hexamer.

Probing myosin head structure with monoclonal antibodies

Monoclonal antibodies that react with defined regions of the heavy and light chains of chicken skeletal muscle myosin have been used to provide a correlation between the primary and the tertiary structures of the head. Electron microscopy of rotary shadowed antibody-myosin complexes shows that the sites for three epitopes in the 25,000 Mr tryptic fragment (25k) of subfragment-1, including one within 4000 Mr of the amino terminus of the myosin heavy chain, are clustered 145(+/- 20) A from the head-rod junction. An epitope in the 50,000 Mr fragment maps even further out on the head. These antibodies bind to the head in several orientations, suggesting that each of the heads can rotate can rotate 180 degrees about the head-rod junction. The epitopes are accessible on subfragment-1 bound to actin when they were probed with Fab fragments; therefore, none of these heavy chain sites is is on the contact surface between the head and actin. Two of the anti-25k antibodies affect the K+-EDTA-and Ca2+-ATPase activities of myosin in a manner that mimics the effect on activity of the modification of the reactive thiol, SH-1. These two antibodies also inhibit the actin-activated ATPase non-competitively with respect to actin. None of the other eight antibodies tested had any marked effect on activity. A monoclonal antibody that reacts with an epitope in the amino-terminal third of myosin light chain 2 maps close to the head-rod junction. A polyclonal antibody specific for the amino terminus of light chain 3 binds further up in the "neck region" of the head, indicating that these portions of the two classes of light chains are located at different sites.

Reflective densitometry of Western blots to quantitate the developmentally regulated accumulation of myosin light chain 3

We have employed a monoclonal antibody to fast myosin alkali light chains to study the accumulation of myosin light chain 3 (MLC3f) in the breast and limb musculature of developing quail embryos using quantitative densitometry of Western blots. Our analyses reveal that MLC3f is first detected in the breast muscle of 11 day embryos and accumulates at a constant rate until hatching at day 16. This data suggests, by extrapolation, that MLC3f accumulation is initiated at day 10 in embryonic breast muscle. MLC3f is also first detected in the limb muscle of 11 day embryos, but does not accumulate rapidly until after day 13. These results demonstrate the effective use of reflective densitometry in the study of developmental problems and in the quantitation of Western blots in general.

Identification of amino acid substitutions differentiating actin isoforms in their interaction with myosin

Various aspects of actin--myosin interaction were studied with actin preparations from two types of smooth muscle: bovine aorta and chicken gizzard, and from two types of sarcomeric muscle: bovine cardiac and rabbit skeletal. All four preparations activated the Mg2+-ATPase activity of skeletal muscle myosin to the same Vmax, but the Kapp for the smooth muscle preparations was higher. At low KCl, pH 8.0 and millimolar substrate concentrations the Kapp values differed by a factor of 2.5. This differential behaviour of the four actin preparations correlates with amino acid substitutions at positions 17 and 89 of actin polypeptide chain, differentiating the smooth-muscle-specific gamma and alpha isomers from cardiac and skeletal-muscle-specific alpha isomers. This correlation provides evidence for involvement of the NH2-terminal portion of the actin polypeptide chain in the interaction with myosin. The differences in the activation of myosin ATPase by various actins were sensitive to changes in the substrate and KCl concentration and pH of the assay medium. Addition of myosin subfragment-1 or heavy meromyosin in the absence of nucleotide produced similar changes in the fluorescence of a fluorescent reagent N-(1-pyrenyl)-iodoacetamide, attached at Cys-374, or 1,N6-ethenoadenosine 5'-diphosphate substituted for the bound ADP in actin protomers in gizzard and skeletal muscle F-actin. The results are consistent with an influence of the amino acid substitutions on ionic interactions leading to complex formation between actin and myosin intermediates in the ATPase cycle but not on the associated states.

Rabbit skeletal myosin heads in solution, as observed by ultracentrifugation and freeze-fracture electron microscopy: dimerization and maximum chord

The use of analytical ultracentrifugation and freeze-fracture electron microscopy in solution allowed us to observe the monomeric and dimeric forms of Mg.71. This subfragment of the myosin molecule contains the LC2 light chain and is comparable to a "native" myosin head. Sedimentation-diffusion equilibrium ultracentrifugation shows that it is necessary to use slightly different conditions in order to obtain a pure Mg.S1 dimer, as compared to the case of chymotryptic S1 (LC2-free S1). For example, in a buffer leading to a complete dimerization of chymotryptic S1, Mg.S1 is only in the form of a monomer-dimer mixture, with comparable proportions of monomer and dimer. The freeze-fracture technique, applied to solutions containing Mg.S1 or chymotryptic S1, revealed that the monomeric species both have the same maximum chord (about 120 A) and that both dimeric species also have the same maximum chord (about 250 A). The maximum chord of the monomer is comparable to the surface-to-surface spacing between the myosin and actin filaments, in a fiber at the slack length. In sharp contrast this chord is higher than this spacing in a stretched fiber. The consequences of this fact are discussed, with particular reference to the sarcomere length-tension relationship.

Muscle contraction and free energy transduction in biological systems

Muscle contraction occurs when the actin and myosin filaments in muscle are driven past each other by a cyclic interaction of adenosine triphosphate (ATP) and actin with cross-bridges that extend from myosin. Current biochemical studies suggest that, during each adenosine triphosphatase cycle, the myosin cross-bridge alternates between two main conformations, which differ markedly in their strength of binding to actin and in their overall structure. Binding of ATP to the cross-bridge induces the weak-binding conformation, whereas inorganic phosphate release returns the cross-bridge to the strong-binding conformation. This cross-bridge cycle is similar to the kinetic cycle that drives active transport and illustrates the general principles of free energy transduction by adenosine triphosphatase systems.

Packing analysis of crystalline myosin subfragment-1. Implications for the size and shape of the myosin head

Crystals of myosin subfragment-1 have been examined by X-ray diffraction and electron microscopy to determine how the molecules pack in the unit cell and to gain preliminary information on the size and shape of the myosin head. Subfragment-1 crystallizes in space group P212121. Analysis of the X-ray diffraction photographs shows that there are eight molecules in the unit cell with two in the asymmetric unit related by a non-crystallographic or local 2-fold axis. It also indicates that in projection down the a axis, two molecules of myosin subfragment-1 lie almost directly on top of one another except for a translation of about 9 A along c. Small crystals were fixed and embedded in the presence of tannic acid, and thin sections were cut perpendicular to each of the three crystallographic axes. Image analysis of micrographs recorded from these sections confirm the packing arrangement deduced from X-ray diffraction, and give the approximate size and shape of the molecule in the crystal lattice. They show that the molecule is at least 160 A long with a maximum thickness of about 60 A, and that it has marked curvature in the unit cell.

Effect of the filamentous structure of myosin on the actomyosin ATPase activity

The ATPase activities of acto-heavy meromyosin and of acto-myosin minifilaments have been compared under the same conditions at low ATP (0.1 mM) and at several KC1 concentrations. The activities, which are strongly salt-dependent in both systems, have been found to be similar at high ionic strength (about 0.16 M) but different at lower ionic strength (0.06-0.07 M). Under this last condition, the catalytic constants kcat and Km are lower for acto-myosin minifilaments than for acto-heavy meromyosin ATPase. In addition, at low ionic strength, any decrease in the concentration of any of the ionic species (ATP, citrate, etc.) induces an increase in the interaction strength between myosin and actin filaments, as revealed by the Km changes. The presence of the troponintropomyosin complex and of Ca2+ also enhances the strength of this interaction. On the other hand, the occurrence of particular interactions between F-actin and myosin minifilaments is further substantiated by the phenomenon of superprecipitation which occurs when the ATP concentration decreases. The favourable effect of the organized structure of the myosin minifilaments on the ATPase activity of actomyosin is discussed.