On the origin and transmission of force in actomyosin subfragment 1

40-kDa protein from thin filaments of the mussel Crenomytilus grayanus changes the conformation of F-actin during the ATPase cycle

Polarized fluorimetry was used to study in ghost muscle fibers the influence of a 40-kDa protein from the thin filaments of the mussel Crenomytilus grayanus on conformational changes of F-actin modified by the fluorescent probes 1,5-IAEDANS and FITC-phalloidin during myosin subfragment (S1) binding in the absence of nucleotides and in the presence of MgADP or MgATP. The fluorescence probes were rigidly bound with actin, which made the absorption and emission dipoles of the probes sensitive to changes in the orientation and mobility of both actin monomer and its subdomain-1 in thin filaments of the muscle fiber. On modeling different intermediate states of actomyosin, the orientation and mobility of oscillators of the dyes were changed discretely, which suggests multistep changes in the actin conformation during the cycle of ATP hydrolysis. The 40-kDa protein influenced the orientation and mobility of the fluorescent probes markedly, suppressing changes in their orientation and mobility in the absence of nucleotides and in the presence of MgADP, but enhancing these changes in the presence of MgATP. The calponin-like 40-kDa protein is supposed to prevent formation of the strong binding state of actomyosin in the absence of nucleotides and in the presence of MgADP but to activate formation of this state in the presence of MgATP.

The use of FRET in the analysis of motor protein structure

Fluorescence resonance energy transfer (FRET) is a spectroscopic phenomenon that consists of long-range dipole-dipole interaction between two chromophores. This method can be employed to gain quantitative distance information on macromolecules. FRET is particularly useful to characterize structural states of motor proteins, because the spatial relationship between various mechanical elements of the motor undergoing its mechanical cycle is essential to understand how force and movement are generated. In this chapter, we describe the technique, including the equations, methods of introducing fluorescence probes in specific loci of the protein, and data analysis. Practical guidelines and hints are also provided for protein preparation, labeling, and measuring FRET efficiency. The protocol is presented for interhead distance measurements in the dimeric kinesin-like motor, Ncd. However, it can easily be adapted to many other motor proteins.

The calcium-saturated cTnI/cTnC complex: structure of the inhibitory region of cTnI

The contiguous inhibitory and regulatory regions of troponin I in the heterotrimeric troponin complex play a critical role in Ca(2+) activation of striated muscle. Knowledge of the structure of this critical region within the complex will enhance efforts toward understanding regulatory mechanisms. Toward this goal, we have used simulated annealing to study the structure of the inhibitory and regulatory regions of cardiac muscle troponin I in the calcium-saturated complex formed between cardiac troponin C and cardiac troponin I. We have incorporated distances determined experimentally by Förster resonance energy transfer in the full-length complex, rather than using peptides derived from cTnI. For these models, we assume a helix-loop-helix conformation for the inhibitory region. We have found several structures that satisfy the experimental constraints fairly well. Although it is not possible to eliminate any of these models at this time, future studies with additional experimental restraints will yield insights on the mechanisms of calcium regulation in cardiac muscle.

Conformational changes of contractile proteins and their role in muscle contraction

The review summarizes the results of studies on conformational changes in contractile proteins that occur during muscle contraction. Polarized fluorescence of tryptophan residues in actin and of fluorescent probes bound specifically to different sites on actin, myosin, or tropomyosin in muscle fibers was measured. The results show that the transition of actomyosin complex from the weak to the strong-binding state is accompanied by a change in the orientation of F-actin subunits with the C and N termini moving opposite to a large part of the subunit. Myosin light chains and some areas in the 20-kDa domain of myosin head move in the same direction as the C- and N-terminal regions of actin. It is established that troponin, caldesmon, calponin, and myosin systems of regulation of muscle contraction modify intramolecular actomyosin rearrangements in a Ca(2+)-dependent manner. The role of intramolecular movements of contractile proteins in muscle contraction is discussed.

Crossbridge head detachment rate constants determined from a model that explains the behavior of both weakly- and strongly-binding crossbridges

Experimentally it is observed that the head regions of weakly-binding myosin crossbridges (crossbridges with ATP or ADP.Pi at the nucleotide binding site) are mobile while attached to actin, while strongly-binding crossbridge heads, such as those with PPi or AMP-PNP at the nucleotide binding site, are immobile (Pate and Cooke, Biophys. J., 1988; Fajer et al., Biophys. J., 1988). I postulate that the fundamental difference between weakly- and strongly-binding crossbridges is not their difference in affinity for actin, but the difference in mobility of the myosin heads attached to actin. Because the heads of weakly-binding crossbridges are mobile while attached to actin, the heads function independently and their behavior can be described by a simple independent-head model. With strongly-binding crossbridges, when one head detaches, it cannot re-attach in a position of lesser strain while the other is attached immobile; both heads must be detached concurrently before the crossbridge can relocate to a position of less strain and relax any tension it supports. This makes the heads appear to act cooperatively. A double-headed crossbridge model is presented which takes into account the difference between weakly- and strongly-binding crossbridges. The model is quite successful at describing the experimental data. In particular, for weakly-binding crossbridges the time constant of the response to stretch is shown to be relatively insensitive to ionic strength and for strongly-binding crossbridges, the model predicts with great accuracy the large ionic strength dependence of the rate constant for force decay. When the experimental results are interpreted according to the model, an important conclusion that emerges is that in all cases (for both weakly- and strongly-binding crossbridges) unstrained crossbridge heads in the muscle fiber detach from actin with approximately the same rate constant as myosin subfragment-1 detaches from actin in solution.

Localization of Cys133 of rabbit skeletal troponin-I with respect to troponin-C by resonance energy transfer

We have used the technique of resonance energy transfer in conjunction with distance geometry analysis to localize Cys133 of troponin-I (TnI) with respect to troponin-C (TnC) in the ternary troponin complex and the binary TnC.TnI complex in the presence and absence of Ca2+. Cys133 of TnI was chosen because our previous work has shown that the region of TnI containing this residue undergoes Ca2+-dependent movements between actin and TnC, and may play an important role in the regulatory function of troponin. For this purpose, a TnI mutant with a single Cys at position 133, and TnC mutants, each with a single Cys at positions 5, 12, 21, 41, 49, 89, 98, 133, and 158, were constructed by site-directed mutagenesis. The distances between TnI Cys133 and each of the nine residues in TnC were then measured. Using a least-squares minimization procedure, we determined the position of TnI Cys133 in the coordinate system of the crystal structure of TnC. Our results show that in the presence of Ca2+, TnI Cys133 is located near residue 12 beneath the N-terminal lobe of TnC, and moves away by 12.6 A upon the removal of Ca2+. TnI Cys133 and the region of TnC that undergoes major change in conformation in response to Ca2+ are located roughly on opposite sides of TnC's central helix. This suggests that the region in TnI that undergoes Ca2+-dependent interaction with TnC is distinct from that interacting with actin.

Structural studies on myosin II: communication between distant protein domains

Understanding how chemical energy is converted into directed movement is a fundamental problem in biology. In higher organisms this is accomplished through the hydrolysis of ATP by three families of motor proteins: myosin, dynein and kinesin. The most abundant of these is myosin, which operates against actin and plays a central role in muscle contraction. As summarized here, great progress has been made towards understanding the molecular basis of movement through the determination of the three-dimensional structures of myosin and actin and through the establishment of systems for site-directed mutagenesis of this motor protein. It now appears that the generation of movement is coupled to ATP hydrolysis by a series of domain movements within myosin.

Effect of complexes of ADP and phosphate analogs on the conformation of the Cys707-Cys697 region of myosin subfragment 1

Recent crystallographic studies have suggested structural differences between the complexes of S1.Mg.ADP with the phosphate analogs aluminium fluoride (AlF4-), vanadate (VO(4)3-) and beryllium fluoride (BeFx) [Fisher, A. J., Smith, C. A., Thoden, J. B., Smith, R., Sutoh, K., Holden, H. M. & Rayment, I. (1995) Biochemistry 34, 8960-8972; Smith, R. & Rayment, I. (1996) Biochemistry 35, 5404-5417]. In this work, chemical modifications, namely labeling of Cys707 (the reactive SH1 thiol) and Cys707-Cys697 (SH1-SH2) cross-linking, were used to compare the S1.ADP.BeFx, S1.ADP. AlF4- and S1.ADP-VO(4)3- complexes with specific states of the myosin-ATPase pathway. Modification of Cys707 with the fluorescent monofunctional reagents 7-diethylamino-3-(4'-maleimidylphenyl)-4-methylcoumarin and N-iodoacetyl-N'-(5-sulfo-1-naphtyl)ethylenediamine has shown that the reactivity of the SH1 group depends on the nucleotide bound to S1. The observed rates of Cys707 modification at 20 degrees C lead to the conclusion that S1.ADP.BeFx is similar to S1*.ATP, while S1.ADP.AlF4- and S1.ADP.VO(4)3- are more similar to S1**.ADP.Pi. The conformations of the analog states were also compared by monitoring the dissociation of the fluorescent nucleotide analog 1-N6-ethenoadenosine diphosphate (ADP[C2H2]) from the active site of Cys707-modified (by N-ethylmaleimide) and Cys707-Cys697-cross-linked (by N,N'-p-phenylene dimaleimide) S1.ADP[C2H2].AlF4- and S1.ADP[C2H2]. BeFx. Our results suggest that the conformations of the S1.ADP.AlF4-, S1.ADP.VO(4)3- and S1.ADP.BeFx complexes in the Cys707-Cys697 region are distinct from each other, with the former two at least partially resembling the S1**.ADP.Pi state, while the latter is similar to the prehydrolyzed S1*.ATP state.

Differential scanning calorimetric study of the complexes of modified myosin subfragment 1 with ADP and vanadate or beryllium fluoride

The effects of various modifications of rabbit skeletal myosin subfragment 1 on the thermal denaturation of subfragment 1 in ternary complexes with Mg-ADP and orthovanadate (V1) or beryllium fluoride (BeFx) have been studied by differential scanning calorimetry. It has been shown that specific modifications of SH1 group of Cys-707 by different sulfhydryl reagents, trinitrophenylation of Lys-83, and reductive methylation of lysine residues promote the decomposition of the S1.ADP.Vi complex and change the character of structural transitions of the subfragment 1 molecule induced by the formation of this complex, but they have much less or no influence on subfragment 1 thermal stability in the S1.ADP.BeFx complex. Thus, the differential scanning calorimetric studies on modified subfragment 1 preparations reveal a significant difference between S1.ADP.Vi and S1.ADP.BeFx complexes. It is suggested that S1.ADP.Vi and S1.ADP.BeFx complexes represent structural analogues of different transition states of the ATPase cycle, namely the intermediate states S1**.ADP.Pi and S1*.ATP, respectively. It is also proposed that during formation of the S1.ADP.Vi complex the region containing both Cys-707 and Lys-83 plays an important role in the spread of conformational changes from the active site of subfragment 1 ATPase throughout the structure of the entire subfragment 1 molecule. In such a case, the effects of reductive methylation of lysine residues on the subfragment 1 structure in the S1.ADP.Vi complex are related to the modification of Lys-83.

Structure-function studies of the myosin motor domain: importance of the 50-kDa cleft

We used random mutagenesis to create 21 point mutations in a highly conserved region of the motor domain of Dictyostelium myosin and classified them into three distinct groups based on the ability to complement myosin null cell phenotypes: wild type, intermediate, and null. Biochemical analysis of the mutated myosins also revealed three classes of mutants that correlated well with the phenotypic classification. The mutated myosins that were not fully functional showed defects ranging from ATP nonhydrolyzers to myosins whose enzymatic and mechanical properties are uncoupled. Placement of the mutations onto the three-dimensional structure of myosin showed that the mutated region lay along the cleft that separates the active site from the actin-binding domain and that has been shown to move in response to changes at the active site. These results demonstrate that this region of myosin plays a key role in transduction of chemical energy to mechanical displacement.

The putative actin-binding role of hydrophobic residues Trp546 and Phe547 in chicken gizzard heavy meromyosin

In the course of myosin-catalyzed ATP hydrolysis, certain amino acid residues in myosin interact with counterparts in actin to produce the relational changes that underlie muscle contraction; some of these interactions are ionic, but the stronger interactions are hydrophobic. In an effort to identify myosin residues participating in hydrophobic interactions, myosin (from smooth muscle) fragments with mutations at suspected sites were engineered and compared with wild-type fragments. It was found that the ATPase of doubly mutated (Trp546Ser and Phe547His) fragments was minimally activated by actin and did not decorate actin well to form the regular arrowhead pattern characteristic of myosin binding to actin filaments. Thus, we suggest that Trp546 and Phe547 are important participants in the hydrophobic actin-myosin interaction.

Fluorescence polarization study of the rigor complexes formed at different degrees of saturation of actin filaments with myosin subfragment-1

A serine residue located in the active site of myosin head (S1) was labelled by 9-anthroylnitrile, an amino group located in the central domain of S1 was labelled by 7-diethylamino-3-(4'-isothio-cyanato-phenyl)-4-methylcoumari n, a cysteine residue located near the C-terminus of S1 was labelled by 5-[2-((iodoacetyl)-amino)ethyl]-amino-naphthalene-1-sulfonic acid (1,5-IAEDANS) and a cysteine residue located near the C-terminus of the alkali light chain 1 was labelled with iodoacetamido-tetramethyl-rhodamine. Polarization of fluorescence of S1 was measured in solution (where it indicated the mobility of actin-bound S1) and in myofibrils (where it indicated orientation of probes) to check whether the anisotropy of S1 labelled at different positions depended on the molar ratio S1:actin. In solution, when increasing amounts of actin were added to a fixed amount of labelled S1 (i.e. when myosin heads were initially in excess over actin), anisotropy saturated at 1 mol of S1 per 1 mol of actin. When increasing amounts of S1 were added to a fixed amount of F-actin (i.e. when actin was initially in excess over S1), the anisotropy saturated at 1 mol of S1 per 2 mols of actin. In myofibrils, orientation of S1 was different when S1 was added at nanomolar concentration (intrinsic actin was in excess over extrinsic S1) then when it was added at micromolar concentration (excess of S1 over actin). The fact that the anisotropy of S1 labelled at different positions depended on the molar ratio excluded the possibility that changes were confined to one part of the cross-bridge and supports our earlier proposal that the two rigor complexes which S1 can form with F-actin differ globally in conformation.

Production and properties of skeletal myosin subfragment 1 selectively labeled with fluorescein at lysine-553 proximal to the strong actin-binding site

We describe, for the first time, the reaction of skeletal myosin subfragment 1 (S-1) with the succinimido ester of 6-[fluorescein-5(and 6)-carboxamido]hexanoic acid (FHS), which takes place at pH 7.0, 20 degrees C, within a 15 min period, in the presence of 1.5-1.8-fold molar excess of reagent over protein. As a result, 0.9-1.0 mol of fluorescyl group/mol of S-1 was covalently incorporated exclusively into the 95 kDa heavy chain as monitored by spectroscopic measurements. The central 50 kDa segment included the main site of fluorescence attachment as assessed by gel electrophoresis. The extent of S-1--FHS conjugation is strongly sensitive to F-actin binding but not to the interaction of nucleotides. The formation of the rigor F-actin--S-1 complex decreased the level of S-1 labeling to 20% without any competition between actin and S-1 for FHS binding. The derivatization of S-1 did not alter the K(+)-ATPase activity, but it enhanced the Ca(2+)-ATPase and Mg(2+)-ATPase to 150% and 225%, respectively, whereas it lowered the actin-activated ATPase to only 75% of the original activity. A double-reciprocal plot of the ATPase rate against actin concentration indicated a 2-fold decrease of the Vmax value for modified S-1, while the Km for actin was unchanged. Cosedimentation experiments did not reveal disruption of the rigor acto-S-1 interaction by the bound fluorophore. The labeled S-1 heavy chain was isolated, and its total tryptic digest was fractionated by reverse-phase HPLC.(ABSTRACT TRUNCATED AT 250 WORDS)

Structural interpretation of the mutations in the beta-cardiac myosin that have been implicated in familial hypertrophic cardiomyopathy

In 10-30% of hypertrophic cardiomyopathy kindreds, the disease is caused by > 29 missense mutations in the cardiac beta-myosin heavy chain (MYH7) gene. The amino acid sequence similarity between chicken skeletal muscle and human beta-cardiac myosin and the three-dimensional structure of the chicken skeletal muscle myosin head have provided the opportunity to examine the structural consequences of these naturally occurring mutations in human beta-cardiac myosin. This study demonstrates that the mutations are related to distinct structural and functional domains. Twenty-four are clustered around four specific locations in the myosin head that are (i) associated with the actin binding interface, (ii) around the nucleotide binding site, (iii) adjacent to the region that connects the two reactive cysteine residues, and (iv) in close proximity to the interface of the heavy chain with the essential light chain. The remaining five mutations are in the myosin rod. The locations of these mutations provide insight into the way they impair the functioning of this molecular motor and also into the mechanism of energy transduction.

A single myosin head can be cross-linked to the N termini of two adjacent actin monomers

Myosin subfragment-1 (S1) can be cross-linked to two actin monomers by 1-ethyl-3-[3-(dimethylamino)-propyl]-carbodiimide only when F-actin is in excess over S1. Electron micrographs of the covalent actin2-S1 complex showed that S1 was cross-linked to two adjacent monomers of the same actin filament. Cross-linking experiments with pre-proteolyzed S1 derivatives in combination with a proteolytic dissection of the intact covalent actin2-S1 adduct (m = 265 kDa), revealed that two N-terminal segments of actin (residues 1-28) were covalently attached to a single S1 molecule. One was cross-linked to either the 20-kDa or the 50-kDa heavy chain fragments of S1, and the other only to the 50-kDa region. The doubly cross-linked product was formed under physiological ionic strength with S1 or with reconstituted myosin filaments, regardless of the presence of ADP or the regulatory proteins, tropomyosin and troponin. Finally, we found that this cross-linking could also take place within myofibrils in the rigor state. These results demonstrate that under nonsaturating conditions, the actin-S1 interface encompasses a much larger region than that recently proposed for the nonphysiological, fully saturated actin filaments.

Intracellular signaling through long-range linked functions in the Ca2+ transport ATPase

The Ca2+ transport ATPases of intracellular membranes exhibit an intracellular long-range functional linkage which is the basic mechanistic device for Ca2+ transport through ATP utilization. The functional linkage operates between a phosphorylation (catalytic) domain located in the extramembranous region, and a Ca2+ binding domain located in the membrane bound region of the enzyme. The two domains are separated by a distance of approximately 50 A, and are both affected by binding of a single molecule of the highly specific inhibitor, thapsigargin, to the enzyme. Functional and structural features are here described to explain the long-range linkage through the protein structure.

Mapping of the actomyosin interfaces

Recombinant DNA methods were used to obtain soluble, undenatured fragments of the heavy chain of myosin subfragment 1 (S-1). These fragments were of preselected lengths and could include protease-sensitive segments that are destroyed when other preparation methods are used. Actin binding by each of the three contiguous segments (residues 1-248, 249-524, and 518-722, essentially spanning the entire S-1 heavy chain) was demonstrated. ATP binding, comparable to that of native S-1, was obtained only with a segment consisting of residues 1-524. Competition among the various fragments for actin was also studied. The data are discussed in relation to the recently reported resolved structure of S-1 [Rayment, I., Rypnieski, R. W., Schmidt-Bäse, K., Smith, R., Tomchick, D. R., Benning, M. M., Winkelmann, D. A., Wesenberg, G. & Holden, H. M. (1993) Science 261, 50-58].

Transient kinetics of the interaction of actin with myosin subfragment-1 in the absence of nucleotide

The kinetics of the association of actin with myosin subfragment-1 (S1) has been studied by using S1 labeled at the sulfhydryl group SH1 with 5-(iodoacetamido)fluorescein (S1-AF). Upon rapid mixing in a stopped-flow apparatus, the fluorescence intensity of the fluorescein moiety increased by 50%, followed by a slower increase that was well resolved. This slow phase of the fluorescence change could not be fitted to either a monoexponential or a biexponential function, but it could be fitted to a sum of three exponential terms yielding three observed first-order rate constants (lambda i). The dissociation of acto.-(S1-AF) was studied by displacement of S1-AF from the complex with native S1. The dissociation kinetics was characterized by a single rate constant (approximately 0.012 s-1 at 20 degrees C), and this constant was independent of S1 concentration. Together with previous equilibrium data that were obtained under identified conditions for formation of acto-subfragment-1 (Lin, S.-H., and H. C. Cheung. 1991. Biochemistry. 30:4317-4323), a six-state two-pathway model is proposed as a minimum kinetic scheme for formation of rigor acto.S1. In this model, unbound subfragment-1 exists in two conformational states (S1' and S1) which are in equilibrium with each other, one corresponding to the previously established low-temperature state and the other to the high-temperature state. Each subfragment-1 state can interact with actin to form a collision complex, followed by two isomerizations to form two acto-subfragment-1 states (A.S1' and A.S1). Both isomerizations were visible in stopped-flow experiments. Two special cases of the model were considered: 1) a rapid pre-equilibration of the initial collision complex with actin and S1, and 2) trace accumulation of the collision complex. The first case required that the three combinations of the three observed rate constants be independent of actin concentration. The data were incompatible with this approximation. The other special case required that the sum of the lambda i vary linearly with actin concentration and the other two combinations of lambda i vary with actin concentration in a quadratic fashion. The present data were in agreement with the second case. At 20 degrees C and in 60 mM KCl, 2 mM MgCl2, 30 mM 2-([-hydroxy-1,1-bis(hydroxymethyl)ethyl]amino)ethanesulfonic acid, and pH 7.5, the biomolecular association rate constants for the interaction of actin with S1' and S1 were 8.58 x 10(5) and 1.11 x 10(6) M-1 s-1, respectively.

Interaction and polymerization of the G-actin-myosin head complex: effect of DNase I

The properties of polymerization and interaction of the G-actin-myosin S1 complexes (formed with either the S1(A1) or the S1(A2) isoform) have been studied by light-scattering and fluorescence measurements in the absence and in the presence of DNase I. In the absence of DNase I, the G-actin-S1(A1) and G-actin-S1(A2) complexes were found to be characterized by different limiting concentrations (l.c.), defined as the complex concentrations above which the polymerization occurs spontaneously within 20 h at 20 degrees C in a "no salt" buffer (l.c. = 0.42 and 8.8 microM for G-actin-S1(A1) and G-actin-S1(A2), respectively). The occurrence of a limiting concentration for either complex together with the kinetic properties of the polymerization led us to conclude that the G-actin-S1 polymerization occurs via a nucleation-elongation process. Fluorescence titrations and proteolysis experiments revealed that G-actin interacts with S1 with a 1:1 stoichiometry (independently of the presence of ATP) with dissociation constants, in the absence of nucleotide, of 20 and 50 nM for the G-actin-S1(A1) and G-actin-S1(A2) complexes, respectively. In the presence of at least a 1.5-fold excess of DNase I, the polymerization of the G-actin-S1 complexes was blocked even at high protein concentration or in the presence of salts. In addition, the affinity of either S1 isoform to actin was reduced 4-5-fold by DNase I, while the stoichiometry of the G-actin-S1 complexes was not changed. However, since the dissociation constants remain in the submicromolar range, we could demonstrate the existence of ternary DNase I-G-actin-S1 complexes stable under polymerizing conditions. Finally, the study of the effect of nucleotides and of various salts on the G-actin-S1 interaction further showed significant differences between the G-actin-S1 and F-actin-S1 interactions.

On how a myosin tryptophan may be perturbed

A well-known indication that a nucleotide has bound to myosin is the enhancement of the fluorescence of a specific tryptophan in the "subfragment 1" segment of the protein. Empirically the effect has been enormously useful in myosin enzymology. But beyond an early suggestion that it arises from a purine-tryptophan charge-transfer complex, the mechanism of the effect has not been considered. Here we consider the alternative that it arises from an ionizable group (either another residue or the phosphate of the nucleotide) whose proximity to the tryptophan is altered by substrate binding. We study this possibility by studying the interaction of an ionizable residue and tryptophan when both are incorporated in a diketopiperazine structure. The geometry of the situation is inferred from molecular mechanics simulations. Unexpectedly, the best explanation seems to be that the field of the imposed charge, acting across space, affects events in the excited state of the indole.

[2-3H]ATP synthesis and 3H NMR spectroscopy of enzyme-nucleotide complexes: ADP and ADP.Vi bound to myosin subfragment 1

The synthesis of [2-3H]ATP with specific activity high enough to use for 3H NMR spectroscopy at micromolar concentrations was accomplished by tritiodehalogenation of 2-Br-ATP. ATP with greater than 80% substitution at the 2-position and negligible tritium levels at other positions had a single 3H NMR peak at 8.20 ppm in 1D spectra obtained at 533 MHz. This result enables the application of tritium NMR spectroscopy to ATP utilizing enzymes. The proteolytic fragment of skeletal muscle myosin, called S1, consists of a heavy chain (95 kDa) and one alkali light chain (16 or 21 kDa) complex that retains myosin ATPase activity. In the presence of Mg2+, S1 converts [2-3H]ATP to [2-3H]ADP and the complex S1.Mg[2-3H]ADP has ADP bound in the active site. At 0 degrees C, 1D 3H NMR spectra of S1.Mg[2-3H]ADP have two broadened peaks shifted 0.55 and 0.90 ppm upfield from the peak due to free [2-3H]ADP. Spectra with good signal-to-noise for 0.10 mM S1.Mg[2-3H]ADP were obtained in 180 min. The magnitude of the chemical shift caused by binding is consistent with the presence of an aromatic side chain being in the active site. Spectra were the same for S1 with either of the alkali light chains present, suggesting that the alkali light chains do not interact differently with the active site. The two broad peaks appear to be due to the two conformations of S1 that have been observed previously by other techniques. Raising the temperature to 20 degrees C causes small changes in the chemical shifts, narrows the peak widths from 150 to 80 Hz, and increases the relative area under the more upfield peak. Addition of orthovanadate (Vi) to produce S1.Mg[2-2H]ADP.Vi shifts both peaks slightly more upfield without changing their widths or relative areas.

The region in myosin S-1 that may be involved in energy transduction

Newly-reported structural information about certain proximities between points on bound nucleotide and points on the heavy chain of myosin S-1 are incorporated into a previously-reported [Botts, J. Thomason, J.F. & Morales, M.F. Proc. Nat. Acad. Sci. USA, 86, 2204-2208 (1989)] structure of S-1. The resulting, enhanced structure is then used to identify some functionalities (e.g., the ATP-perturbable tryptophans), and to explain certain observations (e.g., some concerning the role of bound Mg2+ in the spectral response of TNBS-labelled Lys-83, and some concerning the response of the S-1 CD signal to nucleotide binding and to temperature change). These considerations lead to the suggestion that a strand of the 50 kDa "domain" (residues 510 to 540), and a strand of the 20 kDa 'domain' (residues 697-719) are involved in transmitting the effects of nucleotide binding and hydrolysis to the loop (constituted from the same "domain") that reaches a major (S-1)-actin interface.

Interaction between two myosin heads in acto-smooth muscle heavy meromyosin rigor complex

Muscle contraction occurs as a result of the cyclic interaction between actin and myosin, coupled with the hydrolysis of ATP by the myosin heads. A myosin molecule consists of two globular heads and a rod-shaped tail. It is thought that each myosin head functions as a contractile machinery unit, because each head shows ATPase activity and binds to F-actin. A still unsolved question is whether or not the two heads of a myosin molecule interact with each other during their cyclic interaction with F-actin. Here we report that when chicken gizzard heavy meromyosin (HMM) in its rigor complex with F-actin is reacted with the zero-length cross-linker 1-ethyl-3-[3-(dimethylamino)propyl] carbodiimide (EDC), the two heads of the HMM molecule are cross-linked. This result suggests that the two heads of smooth muscle myosin are in contact with each other when myosin is attached to F-actin. It is thus possible that the two myosin heads interact with each other when cross-bridges are formed.

Structure of the myosin head in solution and the effect of light chain 2 removal

Structural properties of rabbit skeletal myosin head (S1) and the influence of the DTNB light chain (LC2) on the size and shape of myosin heads in solution were investigated by small angle x-ray scattering. The LC2 deficient myosin head, S1 (-LC2), and the S1 containing LC2 light chain, S1 (+LC2) were studied in parallel. The respective values of the radius of gyration were found to be (40.2 +/- 0.5) A and (46.7 +/- 1) A, while the maximum dimension was (190 +/- 15) A for both species. The large difference between the two Rg values suggest that LC2 is located close to one extremity of the myosin head, in agreement with most electron microscopy observations. All models derived from the x-ray scattering pattern of the native myosin head share a common overall morphology, showing two main regions, an asymmetric globular portion which tapers smoothly into a thinner domain of roughly equivalent length making an angle of approximately 60 degrees, with a contour length of approximately 210 A.

Antibody and peptide probes of interactions between the SH1-SH2 region of myosin subfragment 1 and actin's N-terminus

The negatively charged residues in the N-terminus of actin and the 697-707 region on myosin subfragment 1 (S-1), containing the reactive cysteines SH1 and SH2, are known to be important for actin-activated myosin ATPase activity. The relationship between these two sites was first examined by monitoring the rates of SH1 and SH2 modification with N-ethylmaleimide in the presence of actin and, secondly, by testing for direct binding of SH1 peptides to the N-terminal segment on actin. While actin alone protected SH1 from N-ethylmaleimide modification, this effect was abolished by an antibody against the seven N-terminal amino acids on actin, F(ab)(1-7), and was greatly reduced when the charge of acidic residues at actin's N-terminus was altered by carbodiimide coupling of ethylenediamine. Neither F(ab)(1-7) nor ethylenediamine treatment reversed the effect of F-actin on SH2 reactivity in SH1-modified S-1. These results show a communication between the SH1 region on S-1 and actin's N-terminus in the acto-S-1 complex. To test whether such a communication involves the binding of the SH1 site on S-1 to the N-terminal segment of actin, the SH1 peptide IRICRKG-NH2(4+) was used. Cosedimentation experiments revealed the binding of three to six peptides per actin monomer. Peptide binding to actin was affected slightly, if at all, by F(ab)(1-7). The antibody also did not change the polymerization of G-actin by the peptides. The peptides caused a small reduction in the binding of S-1 to actin and did not change the binding of F(ab)(1-7).(ABSTRACT TRUNCATED AT 250 WORDS)

Two different acto-S1 complexes

Based on change in anisotropy of fluorescently labelled S1 and on increase in turbidity of acto-S1 complex when S1 bound to F-actin, we reported previously that depending on the molar ratio of S1 to actin two different complexes of actin monomer (A) and myosin subfragment 1 (S1) could be formed: A1*S1 (one actin with one S1) and A2*S1 (two actins with one S1). Here we extend these findings to F-actin labelled with pyrene and cross-linked to S1 with 1-ethyl-3-(3-dimethyl-aminopropyl)carbodiimide (EDC). The fluorescence of pyrene F-actin decreased with increase in S1 concentration and reached saturation at a molar ratio of S1 to actin of either 0.5 or 1.0, depending on whether S1 was added slowly (5 min) or quickly (10-20 s between additions). Incubation of A2*S1 complex in excess of S1 for > 1 h caused a shift in equilibrium towards the A1*S1 complex. The A2*S1 complexes were not formed at high S1 to actin ratios (> 1.0) owing to competition between heads. Crosslinking experiments showed that the formation of EDC crosslinked products, 175-185 kDa doublet and 265 kDa band, depended on the ratio S1 to actin. To assess the relative ratio of S1 and actin in crosslinked products, we labelled S1 and F-actin with different fluorescent probes (5-IAF and IATR). The S1 to actin ratio was proportional to the ratio of intensities of fluorescence of labelled S1 and actin. The S1 to actin ratio in 265 kDa product was two times smaller than in 175-185 kDa doublet (which is believed to be A1*S1 complex) and therefore 265 kDa band corresponded to A2*S1. Transition between two types of binding may be important to understanding how muscle contracts.

Models of the actin monomer and filament from fluorescence resonance-energy transfer

We have developed algorithms for combining fluorescence resonance-energy transfer (FRET) efficiency measurements into structural models which predict the relative positions of the chemical groups used in FRET. We used these algorithms to construct models of the actin monomer and filament derived solely from FRET measurements based on seven distinct loci. We found a mirror-image pair of monomer models which best fit the FRET data. One of these models agrees well with the atomic-resolution crystal structure recently published by Kabsch et al. in Heidelberg [Kabsch, W., Mannherz, H. G., Suck, D., Pai, E. F. & Holmes, K. C. (1990) Nature 347, 37-44]. The root-mean-square deviation between this FRET model and the crystal structure was about 0.9 nm. Other macromolecular models assembled from FRET measurements are likely to have a similar resolution. The largest discrepancy was for the Cys10 locus which deviated 1.44 nm from the crystal position. We discuss the limitations of the FRET method that may have contributed to this discrepancy, and conclude that the Cys10 FRET data have probably located Cys10 incorrectly in the FRET monomer model. Using the FRET monomer models, we found three orientations in the filament which best fit the intermonomer FRET data. These orientations differ substantially from the atomic-resolution filament model proposed by the Heidelberg group [Holmes, K., Popp, D., Gebhard, W. & Kabsch, W. (1990) Nature 347, 44-49], largely because of the discrepancies in the Cys10 data. These data should probably be excluded from the analysis; however, this would leave too few measurements to assemble a filament model. In the near future, we hope to obtain additional FRET measurements to other actin loci so that the filament modelling can be done without the Cys10 data.

Inactivation, subunit dissociation, aggregation, and unfolding of myosin subfragment 1 during guanidine denaturation

The effect of guanidine hydrochloride on ATPase activity, gel filtration, turbidity, exposure of thiol groups, far-UV circular dichroism, and the fluorescence emission intensity of myosin subfragment 1 (S-1) was studied under equilibrium conditions. It was found that the denaturation process involves several intermediate states. The enzymatic activity of S-1 is at first lost at very low concentrations of GdnHCl (lower than 0.5 M). At a slightly higher GdnHCl concentration (about 0.5 M), the light chains dissociate and this dissociation is closely followed by the formation of aggregates between the naked heavy chains of S-1 molecules in the guanidine hydrochloride range of concentrations 0.5-1 M. At GdnHCl concentrations above 1 M, aggregates gradually disappear and S-1 loses its secondary and tertiary structures. These phenomena are partly reversible, and ATPase activity is only partially recovered under highly limited conditions. These results are discussed in relation to the nature of myosin subunit assembly. The head fragment of 20 kDa is thus suggested to be implicated in the binding of light chain to heavy chain and in the self-association of free heavy chains.

Diffusion of heavy meromyosin in the presence of F-actin and ATP

We looked for evidence that the diffusion of heavy meromyosin is modified by its interaction with actin. To be able to observe diffusion in one dimension, we electrophoresed the complex of F-actin and heavy meromyosin in agarose gels in thin capillaries. The intensity profile of the electrophoretic band of the complex showed a sharp peak, which in 1% agarose in the electric field of 17.8 V cm-1 at room temperature migrated at 3.2 cm h-1. The time evolution of the profile after the electrophoresis ended was a measure of the diffusion of heavy meromyosin. After 10 min the intensity profile of heavy meromyosin diffusing in the presence of F-actin and ATP had undergone as much change as the profile of free heavy meromyosin. Modelling of the diffusion process showed that the mean diffusion coefficient of heavy meromyosin moving over actin in the presence of ATP was 7.2 x 10(-7) cm2 s-1 and that it was not statistically different from the diffusion coefficient of free heavy meromyosin. This data is interpreted to show that the diffusion of heavy meromyosin is not modified by its interaction with actin.

Regulatory light chain influences alterations of myosin head induced by actin

The effect of magnesium-for-calcium exchange and phosphorylation of regulatory light chain (LC2) on structural organization of rabbit skeletal myosin head was studied by limited tryptic digestion. In the presence of actin, exchange of magnesium bound to LC2 by calcium in dephosphorylated myosin accelerates the digestion of myosin and heavy meromyosin heavy chain and increases the accumulation of a 50 kDa fragment. This effect is significantly diminished in the case of phosphorylated myosin. Thus, both phosphorylation and cation exchange influences the effect of actin binding on the structural organization of myosin head.

A search for protein structural changes accompanying the contractile interaction

It appears that small movements (detected hitherto only by fluorescence resonance energy transfer measurements and crosslinking studies) in a region of the myosin S-1 particle may mediate chemomechanical energy transduction in the contractile system. Here we find under conditions of high precision at 10 degrees C and 20 degrees C that ATP binding to S-1 causes small (0.4%) changes in CD signal, delta epsilon 222, as do temperature changes in the regime below 16 degrees C. ATP binding perturbs tryptophan residues that we now think are in the mobile region, and we find here that temperature affects tryptophan fluorescence in much the same way that it affects the CD signal, so we believe that the CD signal reports transduction-related movements in S-1. If S-1 is exposed to the range 16-30 degrees C, CD signal falls with temperature; ATP counteracts this fall. Analysis of vacuum-UV CD spectra yields 42% alpha-helix, 9% antiparallel beta-sheet, 7% parallel beta-sheet, 14% beta-turns, and 29% other structures.

Effects of ions on vanadate-induced photocleavage of myosin subfragment 1

Myosin subfragment 1 (S1) is cleaved by near-ultraviolet irradiation in the presence of vanadate at three sites located at 23, 31 and 74 kDa from the N-terminus. Since vanadate is considered to be a good structural analogue of phosphate, it is assumed that the cleavage sites participate in forming the phosphate-binding site(s) of S1. In this work, the effect of various ions on the vanadate-induced photocleavage of S1 was studied. Monovalent anions were found to inhibit photocleavage in the 50-200 mM range. The inhibition is more expressed at a site 74 kDa from the N-terminus than at the 23-kDa and 31-kDa sites. The inhibitory effect of the monovalent anions increases in the order acetate = F- less than Cl- less than Br- less than I- = SCN-. The order of the inhibitory effect is identical to the protein-structure-damaging effect of monovalent anions in the von Hippel series [von Hipel, P. H. & Wong, K. Y. (1964) Science 145, 577-581]. Therefore, it is assumed that decreased photocleavage is due to local perturbations of structure, especially at the 74-kDa site, in addition to increased ionic strength. Divalent anions, sulfate and thiosulfate, strongly inhibit photocleavage at 2 mM. The inhibition is very pronounced at the 23-kDa and 31-kDa sites, while the 74-kDa site is hardly affected. Since photocleavage at the 23-kDa and 31-kDa sites is regulated jointly and independently from cleavage at the 74-kDa site, it is assumed that S1 has two distinct phosphate-binding sites: the regions of the 23-kDa and 31-kDa cleavage sites, which are proximal to each other in the spatial structure, participate in forming the first phosphate-binding site, while the 74-kDa site is part of the second binding site. Sulfate was also found to inhibit the trapping of vanadate and to facilitate its release from the S1-MgADP-Vi (Vi, inorganic vanadate) complex. Photocleavage of S1 takes place at all three sites, both in the presence or absence of divalent cations, indicating that these, including Mg2+, are not essential for cleavage.

Molecular charge dominates the inhibition of actomyosin in skinned muscle fibers by SH1 peptides

It is not definitively known whether the highly conserved region of myosin heavy chain around SH1 (Cys 707) is part of the actin-binding site. We tested this possibility by assaying for competitive inhibition of maximum Ca-activated force production of skinned muscle fibers by synthetic peptides which had sequences derived from the SH1 region of myosin. Force was inhibited by a heptapeptide (IRICRKG) with an apparent K0.5 of about 4 mM. Unloaded shortening velocity of fibers, determined by the slack test, and maximum Ca-activated myofibrillar MgATPase activity were also inhibited by this peptide, but both required higher concentrations. We found that other cationic peptides also inhibited force in a manner that depended on the charge of the peptide; increasing the net positive charge of the peptide increased its efficacy. The inhibition was not significantly affected by altering solution ionic strength (100-200 mM). Disulfide bond formation was not involved in the inhibitory mechanism because a peptide with Thr substituted for Cys was inhibitory in the presence or absence of DTT. Our data demonstrate that the net charge was the predominant molecular characteristic correlated with the ability of peptides from this region of myosin heavy chain to inhibit force production. Thus, the hypothesis that the SH1 region of myosin is an essential part of the force-producing interaction with actin during the cross-bridge cycle (Eto, M., R. Suzuki, F. Morita, H. Kuwayama, N. Nishi, and S. Tokura., 1990, J. Biochem. 108:499-504; Keane et al., 1990, Nature (Lond.). 344:265-268) is not supported.

Cryoenzymic studies on actomyosin ATPase: kinetic evidence for communication between the actin and ATP sites on myosin

The post-ATP binding steps of myosin subfragment 1 (S1) and actomyosin subfragment 1 (actoS1) ATPases were studied at -15 degrees C with 40% ethylene glycol as antifreeze. The cleavage and release of Pi steps were studied by the rapid-flow quench method and the interaction of actin with S1 plus ATP by light scattering in a stopped-flow apparatus. At -15 degrees C, the interaction of actin with S1 remains tight, and the Km for the activation of S1 ATPase is very small (0.3 microM). The chemical data were interpreted by E + ATP----E*.ATP----E**.ADP.Pi----E*.ADP----products, where E is S1 or actoS1. In Pi burst experiments with S1, there was a large Pi burst of free Pi, but E**.ADP.Pi could not be detected. Here the predominant complex in the seconds time range is E*.ATP and in the steady-state E*.ADP. With actoS1, there was a small Pi burst of E**.ADP.Pi, evidence that the cleavage steps for S1 and actoS1 are different. From the stopped-flow experiments, the dissociation of actoS1 by ATP was complete, even at actin concentrations 60X its Km. Further, no interaction of actin with the key intermediate M*.ATP could be detected. Therefore, at -15 degrees C, actoS1 ATPase occurs by a dissociative pathway; in particular, the cleavage step appears to occur in the absence of actin.(ABSTRACT TRUNCATED AT 250 WORDS)

Conformational flexibility of the Cys 697-Cys 707 segment of myosin subfragment-1. Distance distributions by frequency-domain fluorometry

The separation between Cys 697 (SH1) and Cys 707 (SH2) of the heavy chain of myosin subfragment-1 was previously measured by fluorescence resonance energy transfer with a donor linked to SH1 and an acceptor to SH2. In the present study the distribution of the distances between the two thiols was recovered from frequency-domain fluorometry. In the native state and in the presence of ligands such as MgADP, pyrophosphate, orthovanadate (Vi) and actin, we found wide distributions of the separations between SH1 and SH2 (11-16 A) comparable to that found in the random-coil state (20 A). These results suggest that the SH1-SH2 segment has a high degree of conformational flexibility even in native S1. The flexibility is not much affected by the physiological state of S1. However, the ligands MgADP, Vi and MgADP + Vi decrease significantly the mean SH1-SH2 distance from 27 to 17 A with the effect of MgADP+ Vi being the most pronounced. The anisotropy decay of donor-labeled S1 is biphasic with two rotational correlation times. The long component is decreased by these ligands from 289 to 93 ns, suggesting a more compact symmetric structure of S1 in the presence of the ligands. The complex S1(MgADP)Vi has been shown to be a stable analogue of S1(MgADP)Pi, an unstable intermediate that is generated in the actomyosin ATPase cycle during muscle contraction. Since the power stroke of muscle is accompanied by release of Pi from S1(MgADP)Pi, the present results are consistent with a model in which force generation can be accompanied by transition of S1 from a highly symmetric or compact structure to a more extended structure.

Expression of human beta-myosin heavy chain fragments in Escherichia coli; localization of actin interfaces on cardiac myosin

A cDNA clone coding for an internal fragment of slow-cardiac beta-myosin heavy chain was isolated from a lambda gt10 human skeletal muscle library. Six overlapping cDNA subclones, which span myosin heavy chain subregions and presumably interact with actin, were derived from this clone, fused to a beta-galactosidase vector and expressed in Escherichia coli. Three of the subclones were obtained by PCR (polymerase chain reaction) which enables gene or cDNA fragments to be amplified independently of preexisting restriction sites. Initially, various experiments were carried out using a long MHC (myosin heavy chain) fusion protein containing the 50 kDa-20 kDa connecting region, the whole 20 kDa region and the short subfragment 2 region. This MHC fusion protein was chemically or proteolytically cleaved in the same conditions as the native myosin molecule. Whole and truncated forms of the MHC fusion protein were separated on polyacrylamide gels, electroblotted on nitrocellulose sheets and renatured. They were then assayed in overlay experiments with F-actin and/or myosin light chains in solution. Specific antibodies were used to detect interactions between heavy chain fragments and F-actin or light chains. We thus observed that one long heavy chain fragment synthesized by E. coli behaved like proteolytic or chemical MHC preparations made from native myosin molecules. Two chymotryptic fragments of the MHC fusion protein, which are soluble at low ionic strength, cosedimented with F-actin in solution. Our results demonstrate that, in actin overlay experiments with whole fusion proteins, interactions seem to be due to the heavy chain fragment, not to the bacterial component. All interactions were non ATP-sensitive. We further investigated the possible participation of the six recombinant MHC fragments in contributing to the actomyosin interfaces on the 50 kDa-20 kDa regions of the human cardiac beta-MHC. The present procedure, which enables the synthesis of any MHC fragment independent of any protease site, is a powerful new tool for studying structure-function relationships within the myosin molecule family.

51V NMR study of vanadate binding to myosin and its subfragment 1

The binding of various forms of vanadate to myosin and myosin subfragment 1 (S-1) was studied by 51V NMR at increasing vanadate concentrations between 0.06 and 1.0 mM. The distribution of the various forms of vanadate in the solution depended on the total concentration of vanadate. At low concentrations, the predominant vanadate form was monomeric, while at high concentration, it was tetrameric. The presence of myosin or S-1 in the solution produced a significant broadening of the signal of each form of vanadate, indicating that all of them bind to the protein. Addition of ATP, which does not affect the 51V NMR spectra in the absence of proteins, causes their significant alteration in the presence of myosin or S-1. The changes, which include the broadening of the signal of the monomeric and the narrowing of the signal of the oligomeric vanadate forms, indicate that more monomeric and less oligomeric vanadate binds to the proteins in the presence than in the absence of ATP. Irradiation by near-UV light in the presence of vanadate cleaves S-1 at three specific sites--at 23, 31, and 74 kDa from the N-terminus. The cleavages at 23 and 31 kDa are specifically inhibited by the addition of ATP. The vanadate-associated photocleavage of S-1 also depends on the total concentration of vanadate; it is observed only when the concentration of vanadate is at least 0.2 mM. This was also the lowest concentration at which oligomeric vanadate was detected in the 51V NMR spectra. From the parallel concentration dependence of the photocleavage and the appearance of the tetrameric vanadate, it is concluded that photocleavage occurs only when tetrameric vanadate binds to S-1.

Conformational transitions within the head and at the head-rod junction in smooth muscle myosin studied with a limited proteolysis method

It was previously shown that tryptic digestion of subfragment 1 (S1) of skeletal muscle myosins at 0 degree C results in cleavage of the heavy chain at a specific site located 5 kDa from the NH2-terminus. This cleavage is enhanced by nucleotides and suppressed by actin and does not occur at 25 degrees C, except in the presence of nucleotide. Here we show a similar temperature sensitivity and protection by actin of an analogous chymotryptic cleavage site in the heavy chain of gizzard S1. The results support the view that the myosin head, in general, can exist in two different conformational states even in the absence of nucleotides and actin, and indicate that the heavy chain region 5 kDa from the NH2-terminus is involved in the communication between the sites of nucleotide and actin binding. We also show here for the first time that the S1-S2 junction in gizzard myosin can be cleaved by chymotrypsin and that this cleavage (observed in papain-produced S1 devoid of the regulatory light chain) is also temperature-dependent but insensitive to nucleotides and actin. It is suggested that the temperature-dependent alteration in the flexibility of the head-rod junction, which is apparent from these and similar observations on skeletal muscle myosin [Miller, L. & Reisler, E. (1985) J. Mol. Biol. 182, 271-279; Redowicz, M.J. & Strzelecka-Gołaszewska, H. (1988) Eur. J. Biochem. 177, 615-624], may contribute to the temperature dependence of some steps in the cross-bridge cycle.

Effect of nucleotides, actin and temperature on thermolysin digestion of myosin subfragment-1

Myosin subfragment-1 from rabbit skeletal muscle was digested by thermolysin at 25 degrees, 12 degrees and 0 degree C. Thermolysin cleaves subfragment-1 heavy chain into two stable fragments, 28 kDa and 70 kDa, aligned in this order from the N-terminus [Applegate, D. & Reisler, E. (1983) Proc. Natl Acad. Sci. USA 80, 7109-7112]. The rate of digestion at 25 degrees C was significantly increased in the presence of MgATP and somewhat less in the presence of MgADP, or magnesium pyrophosphate. This activating effect of the nucleotides was decreased at 12 degrees C and completely eliminated at 0 degrees C. The results can be explained by assuming that there are two subfragment-1 conformers [Shriver, J. W. & Sykes, B. D. (1981) Biochemistry 20, 2004-2012], and that both the addition of ATP or its analogs, and lowering the temperature, shift the conformational equilibrium in the direction that is more susceptible to thermolysin. Actin inhibited thermolysin digestion of subfragment-1 at all three temperatures studied. Actin inhibition can be explained either by shifting the equilibrium of the conformers in the direction of the less susceptible form or by direct interference of actin with the binding of thermolysin to subfragment-1. Actin inhibition of thermolysin digestion also prevailed when subfragment-1 was in a ternary complex with nucleotide and actin, in both the strongly and weakly attached states. Similarly, actin inhibited the digestion of subfragment-1 modified by 4-phenylenedimaleimide [corrected], which also forms a weakly attached complex with actin. No difference could be found in the accessibility of the thermolysin-susceptible site of subfragment-1 at the 28-70 kDa junction in either rigor, strongly or weakly attached states, which indicates the similarity of the structure proximal to this specific site in the three attached states.

Localization of epitopes and functional effects of two novel monoclonal antibodies against skeletal muscle myosin

Two skeletal myosin monoclonal antibodies, raised against human skeletal myosin, were used to study the correlation between function, primary and tertiary structure of S-1 prepared from rabbit skeletal myosin. The heavy chain of S-1 is cleaved into three fragments by trypsin--27 kDa, 50 kDa and 20 kDa--aligned in this order from the N-terminus. The epitope of the first antibody was assigned to the N-terminal 1-23 amino acid stretch of S-1, since it reacted with the 27 kDa N-terminal tryptic fragment of S-1 but not with a derivative of the 27 kDa fragment, which lacks the above amino acid stretch. The epitope of the second antibody was assigned to the 3 kDa N-terminal region of the central 50 kDa domain of S-1. This assignment was based on proteolytic and photochemical cleavage of S-1 and on the labelling of its N-terminus by a specific antibody. The antibodies were visualized binding to the myosin head on electron micrographs of rotary-shadowed complexes of antibodies with myosin. Measurements on the micrographs indicated that the distances between the head-tail junction of myosin and the 'anti-27 K' and 'anti-50 K' epitopes are 14 nm and 17 nm, respectively. Both antibodies have a high affinity to S-1. The affinity of the 'anti-50 K' to S-1 decreased upon actin binding, while that of the 'anti-27 K' was not affected by binding of S-1 to F-actin. The 'anti-50 K' antibody inhibited the K+ (EDTA) and the actin-activated ATPase activity of S-1, while the 'anti-27 K' had no effect. The results indicate that either the epitope of the 'anti-50 K' is near to the actin or to the ATP-binding sites of S-1, or that there is communication, expressed as propagated conformational changes, between these sites and the epitope.

MgADP-induced changes in the structure of myosin S1 near the ATPase-related thiol SH1 probed by cross-linking

The structural consequences of MgADP binding at the vicinity of the ATPase-related thiol SH1 (Cys-707) have been examined by subjecting myosin subfragment 1, premodified at SH2 (Cys-697) with N-ethylmaleimide (NEM), to reaction with the bifunctional reagent p-phenylenedimaleimide (pPDM) in the presence and absence of MgADP. By monitoring the changes in the Ca2(+)-ATPase activity as a function of reaction time, it appears that the reagent rapidly modifies SH1 irrespective of whether MgADP is present or not. In the absence of nucleotide, only extremely low levels of cross-linking to the 50-kDa middle segment of S1 can be detected, while in the presence of MgADP substantial cross-linking to this segment is observed. A similar cross-link is also formed if MgADP is added subsequent to the reaction of the SH2-NEM-pre-modified S1 with pPDM in the absence of nucleotide. Isolation of the labeled tryptic peptide from the cross-linked adduct formed with [14C]pPDM, and subsequent partial sequence analyses, indicates that the cross-link is made from SH1 to Cys-522. Moreover, it appears that this cross-link results in the trapping of MgADP in this S1 species. These data suggest that the binding of MgADP results in a change in the structure of S1 in the vicinity of the SH1 thiol relative to the 50-kDa "domain" which enables Cys-522 to adopt the appropriate configuration to enable it to be cross-linked to SH1 by pPDM.

A second consensus sequence of ATP-requiring proteins resides in the 21-kDa C-terminal segment of myosin subfragment 1

Previous comparisons of sequence homologies of ATP-requiring enzymes have defined three consensus sequences which appear to be involved in the binding of the nucleotide. One of these was identified in the N-terminal 27-kDa segment of the myosin heavy chain but the other two sequences have not hitherto been located in myosin. The present paper proposes that one of these other two consensus sequences is in the 21-kDa C-terminal portion of S1 and that it may contribute to the ATP binding domain.

New subfragment 1 of skeletal muscle myosin obtained by thrombin cleavage

The head of the myosin molecule (i.e., subfragment 1 with a heavy chain of 95 kDa) is usually obtained by chymotryptic cleavage in the presence of a divalent cation chelator. In the present work, we used another specific proteolytic enzyme, thrombin, to produce a limited cut within the myosin molecule, resulting in a new species of N-terminal fragment. Treatment of skeletal muscle myosin yielded a 97-kDa split heavy chain associated with intact light chains, corresponding to a single cut. The ATPase activities of this new S-1 derivative were slightly affected by the breakdown. It recognized actin in an ATP-dependent manner, as expected, with an affinity 2-5 times higher than that of the usual chymotryptic S-1 preparation but with a very different electron microscopic pattern. Functional differences are noted, and we involve them more precisely in relation to possible structural aspects of the additional C-terminal segment extending the usual S-1 heavy chain from 95 to 97 kDa.