Structural dynamics of actin during active interaction with myosin: different effects of weakly and strongly bound myosin heads

We have used optical spectroscopy (transient phosphorescence anisotropy, TPA, and fluorescence resonance energy transfer, FRET) to detect the effects of weakly bound myosin S1 on actin during the actomyosin ATPase cycle. The changes in actin were reported by (a) a phosphorescent probe (ErIA) attached to Cys 374 and (b) a FRET donor-acceptor pair, IAEDANS attached to Cys 374 and a nucleotide analogue (TNPADP) in the nucleotide-binding cleft. Strong interactions were detected in the absence of ATP, and weak interactions were detected in the presence of ATP or its slowly hydrolyzed analogue ATP-gamma-S, under conditions where a significant fraction of weakly bound acto-S1 complex was present and the rate of nucleotide hydrolysis was low enough to enable steady-state measurements. The results show that actin in the weakly bound complex with S1 assumes a new structural state in which (a) the actin filament has microsecond rotational dynamics intermediate between that of free actin and the strongly bound complex and (b) S1-induced changes are not propagated along the actin filament, in contrast to the highly cooperative changes due to the strongly bound complex. We propose that the transition on the acto-myosin interface from weak to strong binding is accompanied by transitions in the structural dynamics of actin parallel to transitions in the dynamics of interacting myosin heads.     

Mechanism of formation of actomyosin interface

Force generation in muscle results from binding of myosin to F-actin. ATP binding to myosin provides energy to dissociate actomyosin complex while the hydrolysis of ATP is needed for re-binding of myosin to F-actin. At the end of each cycle myosin and actin form a tight complex with a substantial interface area. We investigated the dynamics of formation of actomyosin interface in presence and absence of nucleotides by quenched flow cross-linking technique. We showed previously that myosin head (subfragment 1, S1) directly interacts with at least two monomers in the actin filament. The quenched flow cross-linking experiments revealed that the initial contact (in presence or absence of nucleotides) occurs between loop 635-647 of S1 and 1-12 N-terminal residues of one actin and, then, the second contact forms between loop 567-574 of S1 and the N terminus of the second actin. The distance between these two loops in S1 corresponds to the distance between N termini of two actins in the same strand (53 A) but is smaller than that between two actins from the different strands (102 A). The formation of the actomyosin complex proceeds in ordered sequence: S1 initially binds to one actin then binds with the second actin located in the same strand but probably closer to the barbed end of F-actin. The presence of nucleotides slows down the interaction of S1 with the second actin, which correlates with recently proposed cleft movement in a 50 kDa domain of S1. The sequential mechanism of formation of actomyosin interface starting from one end and developing towards the barbed end might be involved in force generation and directional movement in actin-myosin system.     

Structural characterization of the binding of Myosin*ADP*Pi to actin in permeabilized rabbit psoas muscle

When myosin is attached to actin in a muscle cell, various structures in the filaments are formed. The two strongly bound states (A*M*ADP and A*M) and the weakly bound A*M*ATP states are reasonably well understood. The orientation of the strongly bound myosin heads is uniform ("stereospecific" attachment), and the attached heads exhibit little spatial fluctuation. In the prehydrolysis weakly bound A*M*ATP state, the orientations of the attached myosin heads assume a wide range of azimuthal and axial angles, indicating considerable flexibility in the myosin head. The structure of the other weakly bound state, A*M*ADP*P(i), however, is poorly understood. This state is thought to be the critical pre-power-stroke state, poised to make the transition to the strongly binding, force-generating states, and hence it is of particular interest for understanding the mechanism of contraction. However, because of the low affinity between myosin and actin in the A*M*ADP*P(i) state, the structure of this state has eluded determination both in isolated form and in muscle cells. With the knowledge recently gained in the structures of the weakly binding M*ATP, M*ADP*P(i) states and the weakly attached A*M*ATP state in muscle fibers, it is now feasible to delineate the in vivo structure of the attached state of A*M*ADP*P(i). The series of experiments presented in this article were carried out under relaxing conditions at 25 degrees C, where approximately 95% of the myosin heads in the skinned rabbit psoas muscle contain the hydrolysis products. The affinity for actin is enhanced by adding polyethylene glycol (PEG) or by lowering the ionic strength in the bathing solution. Solution kinetics and binding constants were determined in the presence and in the absence of PEG. When the binding between actin and myosin was increased, both the myosin layer lines and the actin layer lines increased in intensity, but the intensity profiles did not change. The configuration (mode) of attachment in the A*M*ADP*P(i) state is thus unique among the intermediate attached states of the cross-bridge ATP hydrolysis cycle. One of the simplest explanations is that both myosin filaments and actin filaments are stabilized (e.g., undergo reduced spatial fluctuations) by the attachment. The alignment of the myosin heads in the thick filaments and the alignment of the actin monomers in the thin filaments are improved as a result. The compact atomic structure of M*ADP*P(i) with strongly coupled domains may contribute to the unique attachment configuration: the "primed" myosin heads may function as "transient struts" when attached to the thin filaments.     

New states of actomyosin

Unstained frozen hydrated samples of myosin subfragment 1 (S-1) cross-linked to actin with the zero-length cross-linker 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide have been examined by electron microscopy in an effort to probe structural states of the attached cross-bridge. The cross-linked complex in the absence of ATP has a rigor-like appearance. In contrast, both in the presence of ATP and after the N, N'-p-phenylenedimaleimide (pPDM) bridging of the reactive thiols of S-1, the covalently attached cross-bridges of the acto X S-1 complex appear more disordered and no longer assume the characteristic rigor 45 degrees angle with the actin filaments. The images both in the presence and absence of ATP bear a striking resemblance to those obtained by negative staining of the cross-linked acto X S-1 complex (Craig, R., Greene, L. E. & Eisenberg, E. (1985) Proc. Natl. Acad. Sci. U.S. A. 82, 3247-3251). The actin-bound pPDM S-1 complex, formed by treating the cross-linked complex with pPDM in the presence of ATP, is an expected analog of the weakly bound cross-bridge state. The disordered appearance of S-1 molecules of the cross-linked complex in the presence of ATP and after pPDM treatment may reflect the structural state of the weakly bound cross-bridge.     

Rotational dynamics of spin-labeled F-actin during activation of myosin S1 ATPase using caged ATP.

The most probable source of force generation in muscle fibers in the rotation of the myosin head when bound to actin. This laboratory has demonstrated that ATP induces microsecond rotational motions of spin-labeled myosin heads bound to actin (Berger, C. L. E. C. Svensson, and D. D. Thomas. 1989. Proc. Natl. Acad. Sci. USA. 86:8753-8757). Our goal is to determine whether the observed ATP-induced rotational motions of actin-bound heads are accompanied by changes in actin rotational motions. We have used saturation transfer electron paramagnetic resonance (ST-EPR) and laser-induced photolysis of caged ATP to monitor changes in the microsecond rotational dynamics of spin-labeled F-actin in the presence of myosin subfragment-1 (S1). A maleimide spin label was attached selectively to cys-374 on actin. In the absence of ATP (with or without caged ATP), the ST-EPR spectrum (corresponding to an effective rotational time of approximately 150 microseconds) was essentially the same as observed for the same spin label bound to cys-707 (SH1) on S1, indicating that S1 is rigidly bound to actin in rigor.(ABSTRACT TRUNCATED AT 250 WORDS)     

Submillisecond rotational dynamics of spin-labeled myosin heads in myofibrils.

The rotational motion of crossbridges, formed when myosin heads bind to actin, is an essential element of most molecular models of muscle contraction. To obtain direct information about this molecular motion, we have performed saturation transfer EPR experiments in which spin labels were selectively and rigidly attached to myosin heads in purified myosin and in glycerinated myofibrils. In synthetic myosin filaments, in the absence of actin, the spectra indicated rapid rotational motion of heads characterized by an effective correlation time of 10 microseconds. By contrast, little or no submillisecond rotational motion was observed when isolated myosin heads (subfragment-1) were attached to glass beads or to F-actin, indicating that the bond between the myosin head and actin is quite rigid on this time scale. A similar immobilization of heads was observed in spin-labeled myofibrils in rigor. Therefore, we conclude that virtually all of the myosin heads in a rigor myofibril are immobilized, apparently owing to attachment of heads to actin. Addition of ATP to myofibrils, either in the presence or absence of 0.1 mM Ca2+, produced spectra similar to those observed for myosin filaments in the absence of actin, indicating rapid submillisecond rotational motion. These results indicate that either (a) most of the myosin heads are detached at any instant in relaxed or activated myofibrils or (b) attached heads bearing the products of ATP hydrolysis rotate as rapidly as detached heads.     

Changes in actin structural transitions associated with oxidative inhibition of muscle contraction

We have used transient phosphorescence anisotropy (TPA) to detect changes in actin structural dynamics associated with oxidative inhibition of muscle contraction. Contractility of skinned rabbit psoas muscle fibers was inhibited by treatment with 50 mM H 2O 2, which induced oxidative modifications in the myosin head and in actin, as previously reported. Using proteins purified from oxidized and unoxidized muscle, we used TPA to measure the effects of weakly (+ATP) and strongly (no ATP) bound myosin heads (S1) on the microsecond dynamics of actin labeled at Cys374 with erythrosine iodoacetamide. Oxidative modification of S1 had no effect on actin dynamics in the absence of ATP (strong binding complex), but restricted the dynamics in the presence of ATP (weakly bound complex). In contrast, oxidative modification of actin did not have a significant effect on the weak-to-strong transitions. Thus, we concluded that (1) the effects of oxidation on the dynamics of actin in the actomyosin complex are predominantly determined by oxidation-induced changes in S1, and (2) changes in weak-to-strong structural transitions in actin and myosin are coupled to each other and are associated with oxidative inhibition of muscle contractility.     

Comparative structural and enzymatic properties of skeletal muscle myosin from neonatal and adult rabbits

Several structural and enzymatic properties of myosin from skeletal muscles of neonatal and adult rabbits were compared. Electrophoretic analyses and proteolysis experiments indicated that differences between the two myosin types could be attributed to their heavy subunits. Circular dichroism measurements of subfragment-1 species, and trypsin-digested derivatives showed that the neonatal protein contained less alpha-helices than the adult form. The Mg2(+)-ATPase activity of neonatal myosin was lower than that of adult myosin, especially in the presence of actin. In comparison with adult subfragment-1, it was found that the binding of ATP analogues such as adenosine 5'-[beta, gamma-imino]triphosphate and PPi, or that of ATP (as deduced from the apparent KmATP) to neonatal subfragment-1 in the presence of actin was enhanced, while that of ADP was decreased. On the other hand, the association of actin with the ADP - neonatal-subfragment-1 complex was weaker. These features must be expressed in the cyclical actin-myosin association/dissociation steps occurring in ATP hydrolysis, and more particularly in the reassociation of actin with the ATP-hydrolysis-products - myosin complex.     

Dynamic quenching studies of fluorophore-labelled myosin subfragment 1 and its alkali light chain subunits

The technique of fluorescence quenching by the non-ionic quenchers acrylamide and nicotinamide has been used to probe the accessibility of the environmentally sensitive N-(bromoacetyl)-N'-(1-sulpho-5-naphthyl) ethylenediamine (1,5-Br-AEDANS) fluorophore attached to either Cys-177 of the A1-light chain or the SH1 thiol (Cys-707) of the myosin subfragment (S1) heavy chain. Neither quencher caused any detrimental effects to the ATPase activities of S1 under the conditions of the experiments. It was found that the fluorophore on the isolated light chain was highly exposed to solvent and although this exposure was reduced on hybridization into S1(A1-AEDANS), the probe was still accessible to solvent. This exposure was unaltered by formation of binary complexes with either Mg.ATP or actin or by the formation of a weakly associated acto-S1 complex (in which the Cys-697 and Cys-707 residues of S1 were crosslinked with p-phenylenedimaleimide). The lack of corresponding change in lambda max of emission and quantum yield supported the quenching date and indicated that actin neither binds directly to this region nor induces any significant conformational changes in this locality despite the observation that the A1-Cys-707 moves some 3 nm closer to a point on actin in the weak-binding state (Trayer, H.R. and Trayer, I.P. (1988) Biochemistry, 27, 5718-5727). Parallel experiments with the fluorophore attached to the Cys-707 of the S1 indicated that this region was less accessible to solvent than the light chain thiol despite its ease of labelling. This exposure was not significantly altered by binary complex formation with actin and Mg.ATP, although spectral changes in the absence of quencher support the notion that some conformational change is occurring in this region.     

The effects of various nucleotides on the structure of actin-attached myosin subfragment-1 studied by quick-freeze deep-etch electron microscopy

Stereo electron microscopy of negatively stained images showed that myosin heads in acto-subfragment-1 (S1) covalently cross-linked with 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide were predominantly short and round when ATP was added, in contrast to their uniform tilted appearance in the rigor state. As an attempt to exclude molecules which were actually dissociated but still tethered to actin by artificial cross-links, quick-freeze deep-etch electron microscopy was coupled with the mica flake method to observe uncross-linked native acto-S1 in the presence of ATP. To maintain the low affinity S1 associated to actin in the presence of ATP, a high concentration of acto-S1 was applied to mica flakes whose absorption had been chemically modified. The image of acto-S1 with added ATP agreed well with the expected time-course of reversible dissociation and reassociation, confirming the applicability of this approach to examination of the structural changes of acto-S1. S1 molecules attached to F-actin under rigor conditions or in the presence of ADP were elongated, with the long axis tilted to F-actin. Actin-attached S1 became short and round upon addition of ATP or ADP-inorganic vanadate. Adenyl-5'-yl imidodiphosphate and inorganic pyrophosphate each partially dissociated S1 from actin, as expected.     

Interaction of myosin subfragment 1 with forms of monomeric actin

The ability of myosin subfragment 1 to interact with monomeric actin complexed to sequestering proteins was tested by a number of different techniques such as affinity absorption, chemical cross-linking, fluorescence titration, and competition procedures. For affinity absorption, actin was attached to agarose immobilized DNase I. Both chymotryptic subfragment 1 isoforms (S1A1 and S1A2) were retained by this affinity matrix. Fluorescence titration employing pyrenyl-actin in complex with deoxyribonuclease I (DNase I) or thymosin beta4 demonstrated S1 binding to these actin complexes. A K(D) of 5 x 10(-8) M for S1A1 binding to the actin-DNase I complex was determined. Fluorescence titration did not indicate binding of S1 to actin in complex with gelsolin segment 1 (G1) or vitamin D-binding protein (DBP). However, fluorescence competition experiments and analysis of tryptic cleavage patterns of S1 indicated its interaction with actin in complex with DBP or G1. Formation of the ternary DNase I-acto-S1 complex was directly demonstrated by sucrose density sedimentation. S1 binding to G-actin was found to be sensitive to ATP and an increase in ionic strength. Actin fixed in its monomeric state by DNase I was unable to significantly stimulate the Mg2+-dependent S1-ATPase activity. Both wild-type and a mutant of Dictyostelium discoideum myosin II subfragment 1 containing 12 additional lysine residues within an insertion of 20 residues into loop 2 (K12/20-Q532E) were found to also interact with actin-DNase I complex. Binding of the K12/20-Q532E mutant to the actin-DNase I complex occurred with higher affinity than wild-type S1 and was less sensitive to mono- and divalent cations.     

Interaction of F-actin-AMPPNP with myosin subfragment-1 and troponin-tropomyosin: influence of an extra phosphate at the nucleotide binding site in F-actin on its function

An unsplitable analogue of ATP (adenylyl imidodiphosphate; AMPPNP) was incorporated into F-actin [Cooke, R. (1975) Biochemistry 14, 3250-3256]. The resulting polymers (F-actin-AMPPNP) activated the ATPase activity of myosin subfragment-1 (S1) as efficiently as normal F-actin; neither the maximum velocity at infinite actin concentration (Vmax) nor the affinity of actin to S1 in the presence of ATP (1/KATPase) changed, which indicates that the terminal phosphate of the bound nucleotide at the cleft region between the two domains of the actin molecule [Kabsch, W., Mannherz, H.G., & Suck, D. (1985) EMBO J. 4, 2113-2118] is not directly involved in a myosin binding site. However, the interaction of F-actin with troponin-tropomyosin was strongly modulated by the replacement of ADP with AMPPNP. The troponin-tropomyosin complex strongly enhanced the activation of S1-ATPase activity by F-actin-AMPPNP in the presence of Ca2+, although it has no effect on the activation by normal F-actin-ADP. KATPase was enhanced about threefold by troponin-tropomyosin in the presence of Ca2+, while Vmax was not markedly changed. F-actin-AMPPNP is highly potentiated by troponin-tropomyosin even with low S1 to actin ratios and at high ATP conditions. In the absence of Ca2+, the activation by F-actin-AMPPNP was inhibited normally by troponin-tropomyosin. The results suggest that the terminal beta-phosphate of the bound nucleotide in F-actin is located in a region which is important for regulation of the interaction with myosin.     

Energetics of the actomyosin bond in the filament array of muscle fibers.

The interaction between actin and myosin in the filament array of glycerinated muscle fibers has been monitored using paramagnetic probes and mechanical measurements. Both fiber stiffness and the spectra of probes bound to a reactive sulfydral on the myosin head were measured as the actomyosin bond was weakened by addition of magnesium pyrophosphate (MgPPi) and glycerol. In the absence of MgPPi, all myosin heads are attached to actin with oriented probes. When fibers were incubated in buffers containing MgPPi, a fraction of the probes became disordered, and this effect was greater in the presence of glycerol. To determine whether the heads with disordered probes were detached from actin, spin-labeled myosin subfragment-1 (MSL-S1) was diffused into unlabeled fibers, and the fractions bound to actin and free in the medium were correlated with the oriented and disordered spectral components. These experiments showed that the label was oriented when MSL-S1 was attached to actin in a ternary complex with the ligand and that all heads with disordered probes were detached from actin. Thus the fraction of oriented labels could be used to determine the fraction of heads attached to actin in a fiber in the presence of ligand. The fraction of myosin heads attached to actin decreased with increasing [MgPPi], and in the absence of glycerol approximately 50% of the myosin heads were dissociated at 3.3 mM ligand with little change in fiber stiffness. In the presence of 37% glycerol plus ligand, up to 80% of the heads could be detached with a 50% decrease in fiber stiffness. The data indicate that there are two populations of myosin heads in the fiber. All the data could be fit with a model in which one population of myosin heads (comprising approximately 50% of the total) sees an apparent actin concentration of 0.1 mM and can be released from actin with little change in fiber stiffness. A second population of myosin heads (approximately 50%) sees a higher actin concentration (5 mM) and is only released in the presence of both glycerol and ligand.     

Decavanadate as a biochemical tool in the elucidation of muscle contraction regulation

Recently reported decameric vanadate (V(10)) high affinity binding site in myosin S1, suggests that it can be used as a tool in the muscle contraction regulation. In the present article, it is shown that V(10) species induces myosin S1 cleavage, upon irradiation, at the 23 and 74 kDa sites, the latter being prevented by actin and the former blocked by the presence of ATP. Identical cleavage patterns were found for meta- and decavanadate solutions, indicating that V(10) and tetrameric vanadate (V(4)) have the same binding sites in myosin S1. Concentrations as low as 50 muM decavanadate (5 muM V(10) species) induces 30% of protein cleavage, whereas 500 muM metavanadate is needed to attain the same extent of cleavage. After irradiation, V(10) species is rapidly decomposed, upon protein addition, forming vanadyl (V(4+)) species during the process. It was also observed by NMR line broadening experiments that, V(10) competes with V(4) for the myosin S1 binding sites, having a higher affinity. In addition, V(4) interaction with myosin S1 is highly affected by the products release during ATP hydrolysis in the presence or absence of actin, whereas V(10) appears to be affected at a much lower extent. From these results it is proposed that the binding of vanadate oligomers to myosin S1 at the phosphate loop (23 kDa site) is probably the cause of the actin stimulated myosin ATPase inhibition by the prevention of ATP/ADP exchange, and that this interaction is favoured for higher vanadate anions, such as V(10).     

The kinetic mechanism of mouse myosin VIIA

Myosin VIIa is crucial in hearing and visual processes. We examined the kinetic and association properties of the baculovirus expressed, truncated mouse myosin VIIa construct containing the head, all 5IQ motifs and the putative coiled coil domain (myosin VIIa-5IQ). The construct appears to be monomeric as determined by analytical ultracentrifugation experiments, and only single headed molecules were detected by negative stain electron microscopy. The relatively high basal steady-state rate of 0.18 s(-1) is activated by actin only by ～3.5-fold resulting in a V(max) of 0.7 s(-1) and a K(ATPase) of 11.5 μM. There is no single rate-limiting step of the ATP hydrolysis cycle. The ATP hydrolysis step (M·T M·D·P) is slow (12 s(-1)) and the equilibrium constant (K(H)) of 1 suggests significant reversal of hydrolysis. In the presence of actin ADP dissociates with a rate constant of 1.2 s(-1). Phosphate dissociation is relatively fast (>12 s(-1)), but the maximal rate could not be experimentally obtained at actin concentrations ≤ 50 μM because of the weak binding of the myosin VIIa-ADP-P(i) complex to actin. At higher actin concentrations the rate of attached hydrolysis (0.4 s(-1)) becomes significant and partially rate-limiting. Our findings suggest that the myosin VIIa is a "slow", monomeric molecular motor with a duty ratio of 0.6.     

Time-resolved electron microscopic analysis of the behavior of myosin heads on actin filaments after photolysis of caged ATP

The interaction between myosin subfragment 1 (S1) and actin filaments after the photolysis of P3-1-(2-nitrophenyl)ethyl ester of ATP (caged ATP) was analyzed with a newly developed freezing system using liquid helium. Actin and S1 (100 microM each) formed a ropelike double-helix characteristic of rigor in the presence of 5 mM caged ATP at room temperature. At 15 ms after photolysis, the ropelike double helix was partially disintegrated. The number of S1 attached to actin filaments gradually decreased up to 35 ms after photolysis, and no more changes were detected from 35 to 200 ms. After depletion of ATP, the ropelike double helix was reformed. Taking recent analyses of actomyosin kinetics into consideration, we concluded that most S1 observed on actin filaments at 35-200 ms are so called "weakly bound S1" (S1.ATP or S1.ADP.Pi) and that the weakly bound S1 under a rapid association- dissociation equilibrium with actin filaments can be captured by electron microscopy by means of our newly developed freezing system. This enabled us to directly compare the conformation of weakly and strongly bound S1. Within the resolution of deep-etch replica technique, there were no significant conformational differences between weakly and strongly bound S1, and neither types of S1 showed any positive cooperativity in their binding to actin filaments. Close comparison revealed that the weakly and strongly bound S1 have different angles of attachment to actin filaments. As compared to strongly bound S1, weakly bound S1 showed a significantly broader distribution of attachment angles. These results are discussed with special reference to the molecular mechanism of acto-myosin interaction in the presence of ATP.     

Antibody against the amino terminus of alpha-actin inhibits actomyosin interactions in the presence of ATP

Actomyosin interactions in the presence of ATP were examined by using site-specific antibodies directed against the first seven N-terminal residues on skeletal alpha-actin. Fab fragments of these antibodies (S alpha N Fab) inhibited effectively the actin-activated ATPase of myosin subfragment 1 (S-1) at both 5 and 25 degrees C. Binding experiments carried out in the presence of ATP at 5 degrees C revealed that the catalytic inhibition was related to the inhibition of S-1 binding to actin by Fab. At equimolar ratios of Fab to actin, the binding of S-1 to actin and the activated ATPase were inhibited by 75 and 82%, respectively. These results, when contrasted with the small effect of Fab on rigor actomyosin binding, suggest ATP-induced changes at the interface of actin and myosin.     

Structure of the actin-myosin complex produced by crosslinking in the presence of ATP

The structure of the actin-myosin complex during ATP hydrolysis was studied by covalently crosslinking myosin subfragment 1 (S1) to F-actin in the presence of nucleotides (especially ATP) using 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide. The fluorescence energy transfer was measured between N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine and 6-(iodoacetamide)fluorescein bound to the SH1 thiol of S1 and the Cys374 thiol of actin. The covalent acto-S1, produced by crosslinking in the absence of nucleotide or in the presence of ADP, showed transfer efficiency of 0.50 to 0.52 and intersite distance of 4.5 to 4.7 nm, which were equal to those obtained with non-crosslinked acto-S1 in the absence of nucleotide. However, the covalent acto-S1, produced by crosslinking in the presence of either 5'-adenylyl imidodiphosphate (AMPPNP) at high ionic strength or ATP, showed a significant decrease in the efficiency to 0.26 to 0.34 and hence an increase in the distance to 5.2 to 5.5 nm. These results suggest that AM-ATP and/or AM-ADP-P (formed during ATP hydrolysis) and AM-AMPPNP have a very different conformation from AM and AM-ADP (in which A is actin and M is myosin).     

Fluorimetric studies of actin labeled with dansyl aziridine.

F-actin has been specifically labeled with a fluorescent probe, dansyl aziridine, at cysteine-373 of the protein. The fluorescence property of the conjugated probe serves as a spectroscopic indicator of several processes in which actin participates. The sulfhydryl modification does not impair the G-F transformation of actin, nor does it affect the complex formation of actin and myosin or the dissociation of the complex by ATP as judged by viscosity measurements. However, both labeled actin and actin modified by N-ethylmaleimide, which also reacts at cysteine-373, stimulate the Mg²⁺-ATPase of myosin only about 75% as well as unmodified actin. The probe attached to actin exhibits a 65-nm blue shift of its emission maximum from 560 to 495 nm and a sixfold fluorescence enhancement indicating that it is located in a hydrophobic environment. The excitation spectrum of labeled actin indicates that a tryptophan and a tyrosine residue are close to the probe and transfer excitation energy to the dansyl fluorophore. Upon depolymerization of F-actin, the fluorescence intensity of labeled actin increases about 20%. The fluorescence of labeled actin is also enhanced by the addition of EDTA, ATP, and pyrophosphate, but Mg²⁺ antagonizes this effect reversibly. However, in the presence of 10 mm orthophosphate buffer (pH 7.4) these effects disappear. When labeled F-actin binds with myosin subfragment-1 (SF-1) or heavy meromyosin (HMM), the fluorescence of the actin adduct is enhanced. The fluorescence properties of labeled acto-SF-1 and acto-HMM become insensitive to EDTA and polyphosphates even in the absence of orthophosphate. These results suggest that the two-stranded helical structure of the F-actin filament is stabilized by the presence of phosphate and/or the binding of the myosin “head”.     

Myosin subfragment-1 interacts with two G-actin molecules in the absence of ATP

The interaction between G-actin and myosin subfragment-1 (S1) has been monitored by pyrenyl-actin fluorescence and light scattering. In low ionic strength buffer and in the absence of ATP the polymerization of G-actin induced by myosin subfragment-1 is preceded by the formation of binary GS and ternary G2S complexes in which S1 interacts tightly in rapid equilibrium (K greater than 10(7) M-1) with one and two G-actin molecules, respectively. Pyrenyl fluorescence of G-actin is enhanced 4-fold in GS and 3-fold in G2S. At concentrations of G-actin and S1 in the micromolar range and above, G2S is the predominant species at G-actin/S1 ratios equal to or greater than 1. The isomer of myosin subfragment-1 carrying the A1 light chain, S1(A1), forms a tighter ternary complex than the isomer S1(A2). Actin-bound ATP is not hydrolyzed upon formation of GS and G2S. In the presence of one molar equivalent or more of myosin subfragment-1/mol of G-actin, in low ionic strength buffer containing no nucleotides, G-actin polymerizes faster in the presence of S1(A1) than in the presence of S1(A2). The interaction of S1 with G-actin is inhibited by the binding of ATP or ADP to S1, ATP having a higher affinity for S1 than ADP. The possible structural similarity of the G2S complex to the F-acto-S1 complex in the rigor state and the potential significance of a ternary (actin)2-myosin interaction for actomyosin-based motility are discussed.