The myosin head can bind two actin monomers

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

The DNase-I binding loop of actin may play a role in the regulation of actin-myosin interaction by tropomyosin/troponin

Various lines of evidence suggest that communication between tropomyosin and myosin in the regulation of vertebrate-striated muscle contraction involves yet unknown changes in actin conformation. Possible participation of loop 38-52 in this communication has recently been questioned based on unimpaired Ca(2+) regulation of myosin interaction, in the presence of the tropomyosin-troponin complex, with actin cleaved by subtilisin between Met(47) and Gly(48). We have compared the effects of actin cleavage by subtilisin and by protease ECP32, between Gly(42) and Val(43), on its interaction with myosin S1 in the presence and absence of tropomyosin or tropomyosin-troponin. Both individual modifications reduced activation of S1 ATPase by actin to a similar extent. The effect of ECP cleavage, but not of subtilisin cleavage, was partially reversed by stabilization of interprotomer contacts with phalloidin, indicating different pathways of signal transmission from the N- and C-terminal parts of loop 38-52 to myosin binding sites. ECP cleavage diminished the affinity to tropomyosin and reduced its inhibition of acto-S1 ATPase at low S1 concentrations, but increased the tropomyosin-mediated cooperative enhancement of the ATPase by S1 binding to actin. These effects were reversed by phalloidin. Subtilisin-cleaved actin more closely resembled unmodified actin than the ECP-modified actin. Limited proteolysis of the modified and unmodified F-actins revealed an allosteric effect of ECP cleavage on the conformation of the actin subdomain 4 region that is presumably involved in tropomyosin binding. Our results point to a possible role of the N-terminal part of loop 38-52 of actin in communication between tropomyosin and myosin through changes in actin structure.     

Analysis of turnover dynamics of the submembranous actin cortex

The cell cortex is a thin network of actin, myosin motors, and associated proteins that underlies the plasma membrane in most eukaryotic cells. It enables cells to resist extracellular stresses, perform mechanical work, and change shape. Cortical structural and mechanical properties depend strongly on the relative turnover rates of its constituents, but quantitative data on these rates remain elusive. Using photobleaching experiments, we analyzed the dynamics of three classes of proteins within the cortex of living cells: a scaffold protein (actin), a cross-linker (α-actinin), and a motor (myosin). We found that two filament subpopulations with very different turnover rates composed the actin cortex: one with fast turnover dynamics and polymerization resulting from addition of monomers to free barbed ends, and one with slow turnover dynamics with polymerization resulting from formin-mediated filament growth. Our data suggest that filaments in the second subpopulation are on average longer than those in the first and that cofilin-mediated severing of formin-capped filaments contributes to replenishing the filament subpopulation with free barbed ends. Furthermore, α-actinin and myosin minifilaments turned over significantly faster than F-actin. Surprisingly, only one-fourth of α-actinin dimers were bound to two actin filaments. Taken together, our results provide a quantitative characterization of essential mechanisms under­lying actin cortex homeostasis.     

Fluorescence depolarization of actin filaments in reconstructed myofibers: the effect of S1 or pPDM-S1 on movements of distinct areas of actin

Fluorescence polarization measurements were used to study changes in the orientation and order of different sites on actin monomers within muscle thin filaments during weak or strong binding states with myosin subfragment-1. Ghost muscle fibers were supplemented with actin monomers specifically labeled with different fluorescent probes at Cys-10, Gln-41, Lys-61, Lys-373, Cys-374, and the nucleotide binding site. We also used fluorescent phalloidin as a probe near the filament axis. Changes in the orientation of the fluorophores depend not only on the state of acto-myosin binding but also on the location of the fluorescent probes. We observed changes in polarization (i.e., orientation) for those fluorophores attached at the sites directly involved in myosin binding (and located at high radii from the filament axis) that were contrary to the fluorophores located at the sites close to the axis of thin filament. These altered probe orientations suggest that myosin binding alters the conformation of F-actin. Strong binding by myosin heads produces changes in probe orientation that are opposite to those observed during weak binding.     

Cooperativity of thiol-modified myosin filaments. ATPase and motility assays of myosin function.

The effects of chemical modifications of myosin's reactive cysteines on actomyosin adenosine triphosphatase (ATPase) activities and sliding velocities in the in vitro motility assays were examined in this work. The three types of modifications studied were 4-[N-[(iodoacetoxy)ethyl]-N-methylamino]-7-nitrobenz-2-oxa-1,3- diazole labeling of SH2 (based on Ajtai and Burghart. 1989. Biochemistry. 28:2204-2210.), phenylmaleimide labeling of SH1, and phenylmaleimide labeling of myosin in myofibrils under rigor conditions. Each type of modified myosin inhibited the sliding of actin in motility assays. The sliding velocities of actin over copolymers of modified and unmodified myosins in the motility assay were slowest with rigor-modified myosin and most rapid with SH2-labeled myosin. The actin-activated ATPase activities of similarly copolymerized myosins were lowest with SH2-labeled myosin and highest with rigor-modified myosin. The actin-activated ATPase activities of myosin subfragment-1 obtained from these modified myosins decreased in the same linear manner with the fraction of modified heads. These results are interpreted using a model in which the sliding of actin filaments over myosin filaments decreases the probability of myosin activation by actin. The sliding velocity of actin over monomeric rigor-modified myosin exceeded that over the filamentous form, which suggests for this myosin that filament structure is important for the inhibition of actin sliding in motility assays. The fact that all cysteine modifications examined inhibited the actomyosin ATPase activities and sliding velocities of actin over myosin poses questions concerning the information about the activated crossbridge obtained from probes attached to SH1 or SH2 on myosin.     

Tropomodulin 3 binds to actin monomers

Regulation of the actin cytoskeleton by filament capping proteins is critical to myriad dynamic cellular functions. The ability of these proteins to bind both filaments as well as monomers is often central to their cellular functions. The ubiquitous pointed end capping protein Tmod3 (tropomodulin 3) acts as a negative regulator of cell migration, yet mechanisms behind its cellular functions are not understood. Analysis of Tmod3 effects on kinetics of actin polymerization and steady state monomer levels revealed that Tmod3, unlike previously characterized tropomodulins, sequesters actin monomers with an affinity similar to its affinity for capping pointed ends. Furthermore, Tmod3 is found bound to actin in high speed supernatant cytosolic extracts, suggesting that Tmod3 can bind to monomers in the context of other cytosolic monomer binding proteins. The Tmod3-actin complex can be efficiently cross-linked with 1-ethyl-3-(dimethylaminopropyl)carbodiimide/N-hydroxylsulfosuccinimide in a 1:1 complex. Subsequent tryptic digestion and liquid chromatography/tandem mass spectrometry revealed two binding interfaces on actin, one distinct from other actin monomer binding proteins, and two potential binding sites in Tmod3, which are independent of the previously characterized leucine-rich repeat structure involved in pointed end capping. These data suggest that the Tmod3 isoform may regulate actin dynamics differently in cells than the previously described tropomodulin isoforms.     

Unidirectional movement of an actin filament taking advantage of temperature gradients

An actin filament with heat acceptors attached to its Cys374 residue in each actin monomer could move unidirectionally even under heat pulsation alone, while in the total absence of both ATP and myosin. The prime driver for the movement was temperature gradients operating between locally heated portions on an actin filament and its cooler surroundings. In this report, we investigated how the mitigation of the temperature gradients induces a unidirectional movement of an actin filament. We then observed the transversal fluctuations of the filament in response to heat pulsation and their transition into longitudinally unidirectional movement. The transition was significantly accelerated when Cys374 and Lys336 were simultaneously excited within an actin monomer. These results suggest that the mitigation of the temperature gradients within each actin monomer first went through the energy transformation to transversal fluctuations of the filament, and then followed by the transformation further down to longitudinal movements of the filament. The faster mitigation of temperature gradients within actin monomer helps build up the transition from the transversal to longitudinal movements of the filament by coordinating the interaction between the neighboring monomers.     

Caldesmon inhibits formation of strongly bound myosin cross-bridges and activates an ability of weakly bound cross-bridges to transform actin monomers to the off-conformation

The effect of caldesmon and its actin-binding C-terminal 35 kDa fragment on conformational alterations of actin in a muscle fiber at relaxation, rigor and at simulation of strong and weak binding of myosin heads to actin was studied by polarizational fluorimetry technique. The strong and weak binding forms were mimicked during binding of F-actin of ghost muscle fibers to myosin subfragment-1 modified with NEM (NEM-S1) or pPDM (pPDM-S1), respectively. As a test for alterations in actin conformation, changes in orientation and mobility of a fluorescent probe, TRITC-phalloidin, bound specifically to F-actin were used. The results obtained have shown that during transition of the muscle fiber from the relaxed state into the rigor and during binding of actin filaments to NEM-S1, changes of polarization parameters take place, which are characteristic of formation between actin and myosin of the strong binding and of transformation of actin subunits from the "turned-off" (inactive) to the "turned-on" (active) conformation. Binding of pPDM-S1 to actin and relaxation of the muscle fiber are accompanied, on the contrary, by the changes of orientation and of the fluorescent probe mobility, which are typical of formation of the weak ("non-force-producing") form of actin-myosin binding and of transformation of actin subunits from the active conformation into the inactive one. Caldesmon and its C-terminal fragment markedly inhibit formation of the strong binding at rigor and activate transition of actin monomers to the switched off conformation at relaxation of muscle fiber. In parallel experiments, these regulatory proteins have been shown to inhibit an active force developed at the transition of a muscle fiber from relaxation to rigor. Besides, caldesmon and its fragment decrease the rate of actin filament sliding over myosin in an in vitro motility assay. Caldesmon is suggested to regulate the smooth muscle contraction in an allosterical manner. The alterations in actin conformation inhibit formation of strong binding of myosin cross bridges to actin and activate the ability of weakly bound cross bridges to switch actin monomers from the "on" to the "off" conformation.     

Site-specific mutations in the myosin binding sites of actin affect structural transitions that control myosin binding.

We have examined the effects of actin mutations on myosin binding, detected by cosedimentation, and actin structural dynamics, detected by spectroscopic probes. Specific mutations were chosen that have been shown to affect the functional interactions of actin and myosin, two mutations (4Ac and E99A/E100A) in the proposed region of weak binding to myosin and one mutation (I341A) in the proposed region of strong binding. In the absence of nucleotide and salt, S1 bound to both wild-type and mutant actins with high affinity (K(d) < microM), but either ADP or increased ionic strength decreased this affinity. This decrease was more pronounced for actins with mutations that inhibit functional interaction with myosin (E99A/E100A and I341A) than for a mutation that enhances the interaction (4Ac). The mutations E99A/E100A and I341A affected the microsecond time scale dynamics of actin in the absence of myosin, but the 4Ac mutation did not have any effect. The binding of myosin eliminated these effects of mutations on structural dynamics; i.e., the spectroscopic signals from mutant actins bound to S1 were the same as those from wild-type actin. These results indicate that mutations in the myosin binding sites affect structural transitions within actin that control strong myosin binding, without affecting the structural dynamics of the strongly bound actomyosin complex.     

Role of actin C-terminus in regulation of striated muscle thin filament

In striated muscle, regulation of actin-myosin interactions depends on a series of conformational changes within the thin filament that result in a shifting of the tropomyosin-troponin complex between distinct locations on actin. The major factors activating the filament are Ca²⁺ and strongly bound myosin heads. Many lines of evidence also point to an active role of actin in the regulation. Involvement of the actin C-terminus in binding of tropomyosin-troponin in different activation states and the regulation of actin-myosin interactions were examined using actin modified by proteolytic removal of three C-terminal amino acids. Actin C-terminal modification has no effect on the binding of tropomyosin or tropomyosin-troponin + Ca²⁺, but it reduces tropomyosin-troponin affinity in the absence of Ca²⁺. In contrast, myosin S1 induces binding of tropomyosin to truncated actin more readily than to native actin. The rate of actin-activated myosin S1 ATPase activity is reduced by actin truncation both in the absence and presence of tropomyosin. The Ca²⁺-dependent regulation of the ATPase activity is preserved. Without Ca²⁺ the ATPase activity is fully inhibited, but in the presence of Ca²⁺ the activation does not reach the level observed for native actin. The results suggest that through long-range allosteric interactions the actin C-terminus participates in the thin filament regulation.     

Dynamic polymorphism of single actin molecules in the actin filament

Actin filament dynamics are critical in cell motility. The structure of actin filament changes spontaneously and can also be regulated by actin-binding proteins, allowing actin to readily function in response to external stimuli. The interaction with the motor protein myosin changes the dynamic nature of actin filaments. However, the molecular bases for the dynamic processes of actin filaments are not well understood. Here, we observed the dynamics of rabbit skeletal-muscle actin conformation by monitoring individual molecules in the actin filaments using single-molecule fluorescence resonance energy transfer (FRET) imaging with total internal reflection fluorescence microscopy (TIRFM). The time trajectories of FRET show that actin switches between low- and high-FRET efficiency states on a timescale of seconds. If actin filaments are chemically cross-linked, a state that inhibits myosin motility, the equilibrium shifts to the low-FRET conformation, whereas when the actin filament is interacting with myosin, the high-FRET conformation is favored. This dynamic equilibrium suggests that actin can switch between active and inactive conformations in response to external signals.     

Non-polymerizing long-pitch actin dimers that interact with myosin

The production of a soluble actomyosin complex would be a significant step toward elucidating molecular interactions responsible for biological movement. We took a systematic approach to producing soluble long-pitch actin dimers that are polymerization-deficient yet retain biological protein-protein interactions, including myosin binding. Actin mutant proteins and chemical crosslinking were combined with different polymerization inhibition strategies, including ADP-ribosylation, or the use of a polymerization-deficient actin mutant protein. While all of the long-pitch actin dimers retained interactions reflective of F-actin activity, each displayed different interactions with myosin. Myosin did not interact productively with long-pitch actin dimers capped with DNase-I, and led to filament formation of unmodified long-pitch actin dimers or dimers possessing a polymerization-deficient actin subunit. However, ADP-ribosylated long-pitch actin dimers interacted with myosin, giving this dimer great potential for producing a soluble actomyosin complex, which could greatly improve our understanding of the molecular basis of movement in cells, tissues, and organisms.     

D-loop of Actin Differently Regulates the Motor Function of Myosins II and V

To gain more information on the manner of actin-myosin interaction, we examined how the motile properties of myosins II and V are affected by the modifications of the DNase I binding loop (D-loop) of actin, performed in two different ways, namely, the proteolytic digestion with subtilisin and the M47A point mutation. In an in vitro motility assay, both modifications significantly decreased the gliding velocity on myosin II-heavy meromyosin due to a weaker generated force but increased it on myosin V. On the other hand, single molecules of myosin V “walked” with the same velocity on both the wild-type and modified actins; however, the run lengths decreased sharply, correlating with a lower affinity of myosin for actin due to the D-loop modifications. The difference between the single-molecule and the ensemble measurements with myosin V indicates that in an in vitro motility assay the non-coordinated multiple myosin V molecules impose internal friction on each other via binding to the same actin filament, which is reduced by the weaker binding to the modified actins. These results show that the D-loop strongly modulates the force generation by myosin II and the processivity of myosin V, presumably affecting actin-myosin interaction in the actomyosin-ADP·P_i state of both myosins.     

Disulfide cross-linking of caldesmon to actin.

Treatment of a solution of actin and smooth muscle caldesmon with 5,5'-dithiobis(2-nitrobenzoic acid) results in the formation of a disulfide cross-link between the C-terminal penultimate residue Cys-374 of actin and Cys-580 in caldesmon's C-terminal actin-binding region. Therefore, these 2 residues are close in the actin-caldesmon complex. Since myosin also binds to actin in the vicinity of Cys-374 and since caldesmon inhibits actomyosin ATPase activity by the reduction of myosin binding to actin, then the inhibition might be by caldesmon sterically hindering or blocking myosin's interaction with actin. [Ca2+]Calmodulin, which reverses the inhibition of the ATPase activity, decreases the yield of the cross-linked species, suggesting a weakening of the caldesmon-actin interaction in the cross-linked region. It is possible to maximally cross-link one caldesmon molecule/every three actin monomers, in the absence or presence of tropomyosin, clearly ruling out an elongated, end-to-end alignment of caldesmon on the actin filament in vitro, and raising the possibility that the N-terminal part of caldesmon projects out from the filament. Reaction of 5,5'-dithiobis(2-nitrobenzoic acid)-modified actin with caldesmon leads to the same disulfide cross-linked product between actin and caldesmon Cys-580, enabling the specific labeling of the other caldesmon cysteine, residue 153, in the N-terminal part of caldesmon with a spectroscopic probe.     

Molecular dynamics simulation of a myosin subfragment-1 docking with an actin filament

Myosins are typical molecular motor proteins, which convert the chemical energy of ATP into mechanical work. The fundamental mechanism of this energy conversion is still unknown. To explain the experimental results observed in molecular motors, Masuda has proposed a theory called the “Driven by Detachment (DbD)” mechanism for the working principle of myosins. Based on this theory, the energy used during the power stroke of the myosins originates from the attractive force between a detached myosin head and an actin filament, and does not directly arise from the energy of ATP. According to this theory, every step in the myosin working process may be reproduced by molecular dynamics (MD) simulations, except for the ATP hydrolysis step. Therefore, MD simulations were conducted to reproduce the docking process of a myosin subfragment-1 (S1) against an actin filament. A myosin S1 directed toward the barbed end of an actin filament was placed at three different positions by shifting it away from the filament axis. After 30 ns of MD simulations, in three cases out of ten trials on average, the myosin made a close contact with two actin monomers by changing the positions and the orientation of both the myosin and the actin as predicted in previous studies. Once the docking was achieved, the distance between the myosin and the actin showed smaller fluctuations, indicating that the docking is stable over time. If the docking was not achieved, the myosin moved randomly around the initial position or moved away from the actin filament. MD simulations thus successfully reproduced the docking of a myosin S1 with an actin filament. By extending the similar MD simulations to the other steps of the myosin working process, the validity of the DbD theory may be computationally demonstrated.     

Twirling of actin by myosins II and V observed via polarized TIRF in a modified gliding assay

The force generated between actin and myosin acts predominantly along the direction of the actin filament, resulting in relative sliding of the thick and thin filaments in muscle or transport of myosin cargos along actin tracks. Previous studies have also detected lateral forces or torques that are generated between actin and myosin, but the origin and biological role of these sideways forces is not known. Here we adapt an actin gliding filament assay to measure the rotation of an actin filament about its axis (“twirling”) as it is translocated by myosin. We quantify the rotation by determining the orientation of sparsely incorporated rhodamine-labeled actin monomers, using polarized total internal reflection microscopy. To determine the handedness of the filament rotation, linear incident polarizations in between the standard s- and p-polarizations were generated, decreasing the ambiguity of our probe orientation measurement fourfold. We found that whole myosin II and myosin V both twirl actin with a relatively long (∼1 μm), left-handed pitch that is insensitive to myosin concentration, filament length, and filament velocity.     

Structural studies of arthrin: monoubiquitinated actin

Here, we report on the structure and in situ location of arthrin (monoubiquitinated actin). Labelling of insect muscle thin filaments with a ubiquitin antibody reveals that every seventh subunit along the filament long-pitch helices is ubiquitinated. A three-dimensional reconstruction of frozen-hydrated arthrin filaments was produced. This was based on a novel algorithm that divides filament images into short segments that are used for single-particle image processing. Difference maps with an actin filament reconstruction locate ubiquitin at the side of actin sub-domain 1 opposite where myosin binds. Consistent with the reconstructions, peptide mapping places the ubiquitin linkage on lysine 118 in actin. Molecular modelling was used to generate arthrin monomers from ubiquitin and actin crystal structures. Filament models constructed from these monomers were compared with the arthrin reconstruction. The reconstruction suggests ubiquitin attached to Lys118 adopts one or a few conformers, stabilized by a small interface with actin. The function of actin ubiquitination is not known, but may involve regulation of muscle contractile activity.     

Orientation of actin filaments during motion in in vitro motility assay.

Rhodamine-phalloidin was added to F-actin, and the orientation of transition dipoles of the dye was measured in single actin filaments by polarization of fluorescence. Rhodamine-phalloidin was well immobilized on the surface of actin, indicating that changes in orientation of the dye reported changes in orientation of actin monomers. In stationary filaments the dipoles were inclined at 49.3 degrees with respect to the filament axis. The disorganization of dipoles in stationary filaments was insignificant. When the filaments were made to translate, the average orientation of the dye did not change, but disorganization slightly increased. Disorganization increased significantly when filaments were free in solution. We concluded that, within the accuracy of our measurements (approximately 18%), actin monomers did not undergo major reorientations during motion, but that binding of myosin heads deformed the structure of filaments.     

Tropomyosin prevents depolymerization of actin filaments from the pointed end

Regulation of the pointed, or slow-growing, end of actin filaments is essential to the regulation of filament length. The purpose of this study is to investigate the role of skeletal muscle tropomyosin (TM) in regulating pointed end assembly and disassembly in vitro. The effects of TM upon assembly and disassembly of actin monomers from the pointed filament end were measured using pyrenyl-actin fluorescence assays in which the barbed ends were capped by villin. Tropomyosin did not affect pointed end elongation; however, filament disassembly from the pointed end stopped in the presence of TM under conditions where control filaments disassembled within minutes. The degree of protection against depolymerization was dependent upon free TM concentration and upon filament length. When filaments were diluted to a subcritical actin concentration in TM, up to 95% of the filamentous actin remained after 24 h and did not depolymerize further. Longer actin filaments (150 monomers average length) were more effectively protected from depolymerization than short filaments (50 monomers average length). Although filaments stopped depolymerizing in the presence of TM, they were not capped as shown by elongation assays. This study demonstrates that a protein, such as TM, which binds to the side of the actin filament can prevent dissociation of monomers from the end without capping the end to elongation. In skeletal muscle, tropomyosin could prevent thin filament disassembly from the pointed end and constitute a mechanism for regulating filament length.     

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.