Muscle Myosin Motor Research Articles

Polarization-resolved microscopy reveals a muscle myosin motor-independent mechanism of molecular actin ordering during sarcomere maturation.

Sarcomeres are stereotyped force-producing mini-machines of striated muscles. Each sarcomere contains a pseudocrystalline order of bipolar actin and myosin filaments, which are linked by titin filaments. During muscle development, these three filament types need to assemble into long periodic chains of sarcomeres called myofibrils. Initially, myofibrils contain immature sarcomeres, which gradually mature into their pseudocrystalline order. Despite the general importance, our understanding of myofibril assembly and sarcomere maturation in vivo is limited, in large part because determining the molecular order of protein components during muscle development remains challenging. Here, we applied polarization-resolved microscopy to determine the molecular order of actin during myofibrillogenesis in vivo. This method revealed that, concomitantly with mechanical tension buildup in the myotube, molecular actin order increases, preceding the formation of immature sarcomeres. Mechanistically, both muscle and nonmuscle myosin contribute to this actin order gain during early stages of myofibril assembly. Actin order continues to increase while myofibrils and sarcomeres mature. Muscle myosin motor activity is required for the regular and coordinated assembly of long myofibrils but not for the high actin order buildup during sarcomere maturation. This suggests that, in muscle, other actin-binding proteins are sufficient to locally bundle or cross-link actin into highly regular arrays.

Interaction of isolated cross-linked short actin oligomers with the skeletal muscle myosin motor domain.

The cyclical interaction between F-actin and myosin in muscle cells generates contractile force. The myosin motor domain hydrolyses ATP, resulting in conformational changes that are amplified by the myosin lever arm that links the motor domain to the rod domain. Recent cryo-electron microscopic data have provided a clear picture of the myosin-ATP-F-actin complex, but structural insights into other stages of the myosin-actin interaction have been less forthcoming. To address this issue, we cross-linked F-actin subunits between Cys374 and Lys191, and separated them by gel filtration. Purified actin-dimers, -trimers and -tetramers retained the ability to polymerize and to stimulate myosin-subfragment 1 (myosin-S1) ATPase activity. To generate stable actin oligomer:myosin-S1 complexes, we blocked actin polymerization with gelsolin and Clostridium botulinum iota toxin-mediated ADP-ribosylation. After polymerization inhibition, actin-trimers and -tetramers retained the ability to stimulate the myosin-S1-ATPase, whereas the actin-dimer showed very little ATPase stimulation. We then analysed the stoichiometry and binding affinity of myosin-S1 to actin oligomers. Actin-trimers and -tetramers bound myosin-S1 in the absence of nucleotide; the trimer contains one myosin-S1 binding site. We calculated a dissociation constant (Kd ) of 1.1×10-10 m and 1.9×10-10 m for binding of native F-actin and the actin-trimer to myosin-S1, respectively. EM of the actin-trimer:myosin-S1 complex demonstrated the presence of single particles of uniform size. Image reconstruction allowed a reasonable fit of the actin-trimer and myosin-S1 into the obtained density clearly showing binding of one myosin-S1 molecule to the two long-pitch actins of the trimer, supporting the kinetic data.

The structure of the actin-smooth muscle myosin motor domain complex in the rigor state.

Myosin-based motility utilizes catalysis of ATP to drive the relative sliding of F-actin and myosin. The earliest detailed model based on cryo-electron microscopy (cryoEM) and X-ray crystallography postulated that higher actin affinity and lever arm movement were coupled to closure of a feature of the myosin head dubbed the actin-binding cleft. Several studies since then using crystallography of myosin-V and cryoEM structures of F-actin bound myosin-I, -II and -V have provided details of this model. The smooth muscle myosin II interaction with F-actin may differ from those for striated and non-muscle myosin II due in part to different lengths of important surface loops. Here we report a ∼6 Å resolution reconstruction of F-actin decorated with the nucleotide-free recombinant smooth muscle myosin-II motor domain (MD) from images recorded using a direct electron detector. Resolution is highest for F-actin and the actin-myosin interface (3.5-4 Å) and lowest (∼6-7 Å) for those parts of the MD at the highest radius. Atomic models built into the F-actin density are quite comparable to those previously reported for rabbit muscle actin and show density from the bound ADP. The atomic model of the MD, is quite similar to a recently published structure of vertebrate non-muscle myosin II bound to F-actin and a crystal structure of nucleotide free myosin-V. Larger differences are observed when compared to the cryoEM structure of F-actin decorated with rabbit skeletal muscle myosin subfragment 1. The differences suggest less closure of the 50 kDa domain in the actin bound skeletal muscle myosin structure.

Modeling Coordinated Kinetics in Large Groups of Muscle Myosin Motors

The kinetics of molecular motors are usually assessed for single or a few connected motors, or groups exceeding 100 motors. When we previously investigated coordinated kinetics of groups of 10 to 100 muscle myosin motors, we observed the emergence of group size-dependent patterns at the level of the whole motor group[1]. We used automated video analysis of in vitro motility assays, where fluorescent actin filaments were propelled by a surface coated with muscle myosins[2]. Here, actin motion showed two distinct modes: full arrest and phases of unidirectional sliding with a characteristic velocity[1]. The observation of either mode depended on the number of myosins maximally working as a coupled group on the same actin filament, which we calculated from myosin binding site distance (0.0355 µm) and filament length (L)[1]. Short actin filaments (L 1.0 µm) continuously slid forward[1]. We proposed a mathematical model, which monitors the coupled, load-dependent myosin kinetics at single myosin and single reaction resolution[1]. In the simulated myosin group kinetics, actin sliding and arrest corresponded to attractor-like-patterns “fixed point” and “limit cycle”, respectively; stochastic jumping between attractor-like-patterns explained sliding-arrest alternation[3]. We now extended this mathematical model by a spatial component: actin filament length is one spatial dimension, while myosin-to-myosin coupling is limited to ∼0.2 µm. In model simulations, arrested kinetics originated from both ends of the actin filament and could entrain global kinetics into arrest. Further, experimental velocity distributions recorded after addition of filamin crosslinker were reproduced, and explained by local perturbations by filamin crosslinking that spread to global extent along the filament. [1]Hilbert et al. Biophys J 2013 [2]Hilbert et al. PLoS Comp Biol 2013 [3]Hilbert et al. Biophys J 2015.

Phosphate and ADP Differently Inhibit Coordinated Smooth Muscle Myosin Groups

Actin filaments propelled in vitro by groups of skeletal muscle myosin motors exhibit distinct phases of active sliding or arrest, whose occurrence depends on actin length (L) within a range of up to 1.0 μm. Smooth muscle myosin filaments are exponentially distributed with ≈150 nm average length in vivo—suggesting relevance of the L-dependence of myosin group kinetics. Here, we found L-dependent actin arrest and sliding in in vitro motility assays of smooth muscle myosin. We perturbed individual myosin kinetics with varying, physiological concentrations of phosphate (Pi, release associated with main power stroke) and adenosine diphosphate (ADP, release associated with minor mechanical step). Adenosine triphosphate was kept constant at physiological concentration. Increasing [Pi] lowered the fraction of time for which actin was actively sliding, reflected in reduced average sliding velocity (ν) and motile fraction (fmot, fraction of time that filaments are moving); increasing [ADP] increased the fraction of time actively sliding and reduced the velocity while sliding, reflected in reduced ν and increased fmot. We introduced specific Pi and ADP effects on individual myosin kinetics into our recently developed mathematical model of actin propulsion by myosin groups. Simulations matched our experimental observations and described the inhibition of myosin group kinetics. At low [Pi] and [ADP], actin arrest and sliding were reflected by two distinct chemical states of the myosin group. Upon [Pi] increase, the probability of the active state decreased; upon [ADP] increase, the probability of the active state increased, but the active state became increasingly similar to the arrested state.

Erratum to: Identification of functional differences between recombinant human α and β cardiac myosin motors.

The myosin isoform composition of the heart is dynamic in health and disease and has been shown to affect contractile velocity and force generation. While different mammalian species express different proportions of α and β myosin heavy chain, healthy human heart ventricles express these isoforms in a ratio of about 1:9 (α:β) while failing human ventricles express no detectable α-myosin. We report here fast-kinetic analysis of recombinant human α and β myosin heavy chain motor domains. This represents the first such analysis of any human muscle myosin motor and the first of α-myosin from any species. Our findings reveal substantial isoform differences in individual kinetic parameters, overall contractile character, and predicted cycle times. For these parameters, α-subfragment 1 (S1) is far more similar to adult fast skeletal muscle myosin isoforms than to the slow β isoform despite 91% sequence identity between the motor domains of α- and β-myosin. Among the features that differentiate α- from β-S1: the ATP hydrolysis step of α-S1 is ~ten-fold faster than β-S1, α-S1 exhibits ~five-fold weaker actin affinity than β-S1, and actin·α-S1 exhibits rapid ADP release, which is >ten-fold faster than ADP release for β-S1. Overall, the cycle times are ten-fold faster for α-S1 but the portion of time each myosin spends tightly bound to actin (the duty ratio) is similar. Sequence analysis points to regions that might underlie the basis for this finding.

Differential Twitch Kinetics in Engineered Cardiac Tissue Expressing Human Cardiac Myosins

Congestive heart failure is a debilitating disease in which the principal pathology is impaired ventricular contractility leading to diminished cardiac output, and previous work indicates that reduced contractility is based in part on the ratio of myosin heavy chain (MyHC) isoforms, α- and β-MyHC, expressed in the ventricles. Normal human ventricles express ∼10% of the fast α-MyHC on a background of the slower β-MyHC, while in failing hearts α-MyHC is reduced to virtually undetectable levels with complete replacement by β-MyHC. Data from permeabilized myocardial preparations suggests that this isoform switch may be partly responsible for reduced myocardial twitch force and pressure development by failing ventricles since β-MyHC is a slower motor protein, yet most experiments have used non-human myosins and experimental conditions in which preparations were steadily activated, thus little is known about the response of human myosins to a time-varying Ca2+ transient. To address these limitations, we recently developed a human 3D engineered cardiac tissue (hECT) system in which we can express recombinant human muscle myosin motors. Using commercially available cloning and adenoviral expression systems, α- or β-MyHC isoform expressing adenoviral particles were used to transduce human cardiomyocytes produced from human iPS cells and construct hECTs. Preparations displayed well-defined cellular structure with elongated morphology aligned in the direction of preparation shortening during electrical pacing, while histological analysis of hECT revealed appropriate protein expression and localization within the sarcomere. In response to a Ca2+ transient, the time-course of twitch force development was accelerated in hECT expressing α-MyHC compared to β-MyHC, while peak twitch force was greater in hECT expressing α-MyHC. These results demonstrate the relative contribution of myosin isoforms to myocardial twitch kinetics in human engineered cardiac tissue constructs expressing a stable background of myofibrillar proteins.

Loop 1 dynamics in smooth muscle myosin: isoform specific differences modulate ADP release

Isoforms of the smooth muscle (SM) myosin motor domain differ in the presence or absence of a seven amino acid insert in a flexible surface loop spanning the nucleotide-binding pocket known as Loop 1. The presence of this insert leads to a two-fold increase in actin sliding velocity and ADP release rate between these isoforms, although the effect of Loop 1 on the kinetics of ADP release remains unclear. To further investigate the role of the Loop 1 insert in modulating ADP release in SM myosin we have inserted a single tryptophan residue into Loop 1 of both isoforms as a probe of local structural dynamics. By monitoring the dynamics of Loop 1 in relation to the release of ADP we have observed a unique movement of Loop 1 in the inserted isoform, preceding nucleotide release, which is absent in the non-inserted isoform. This movement is sequence dependent as alanine replacement of the insert residues abolishes the transition and slows ADP release. Thus movement of Loop 1 is a critical factor in increasing the ADP release rate in the inserted faster isoform of SM myosin.

Reconstitution of Contractile Actomyosin Bundles

Contractile actomyosin bundles are critical for numerous aspects of muscle and nonmuscle cell physiology. Due to the varying composition and structure of actomyosin bundles in vivo, the minimal requirements for their contraction remain unclear. Here, we demonstrate that actin filaments and filaments of smooth muscle myosin motors can self-assemble into bundles with contractile elements that efficiently transmit actomyosin forces to cellular length scales. The contractile and force-generating potential of these minimal actomyosin bundles is sharply sensitive to the myosin density. Above a critical myosin density, these bundles are contractile and generate large tensile forces. Below this threshold, insufficient cross-linking of F-actin by myosin thick filaments prevents efficient force transmission and can result in rapid bundle disintegration. For contractile bundles, the rate of contraction decreases as forces build and stalls under loads of ∼0.5 nN. The dependence of contraction speed and stall force on bundle length is consistent with bundle contraction occurring by several contractile elements connected in series. Thus, contraction in reconstituted actomyosin bundles captures essential biophysical characteristics of myofibrils while lacking numerous molecular constituents and structural signatures of sarcomeres. These results provide insight into nonsarcomeric mechanisms of actomyosin contraction found in smooth muscle and nonmuscle cells.

Correction for Resnicow et al., Functional diversity among a family of human skeletal muscle myosin motors

Correction for Resnicow et al., Functional diversity among a family of human skeletal muscle myosin motors

Functional diversity among a family of human skeletal muscle myosin motors

Human skeletal muscle fibers express five highly conserved type-II myosin heavy chain (MyHC) genes in distinct spatial and temporal patterns. In addition, the human genome contains an intact sixth gene, MyHC-IIb, which is thought under most circumstances not to be expressed. The physiological and biochemical properties of individual muscle fibers correlate with the predominantly expressed MyHC isoform, but a functional analysis of homogenous skeletal muscle myosin isoforms has not been possible. This is due to the difficulties of separating the multiple isoforms usually coexpressed in muscle fibers, as well as the lack of an expression system that produces active recombinant type II skeletal muscle myosin. In this study we describe a mammalian muscle cell expression system and the functional analysis of all six recombinant human type II skeletal muscle myosin isoforms. The diverse biochemical activities and actin-filament velocities of these myosins indicate that they likely have distinct functions in muscle. Our data also show that ATPase activity and motility are generally correlated for human skeletal muscle myosins. The exception, MyHC-IIb, encodes a protein that is high in ATPase activity but slow in motility; this is the first functional analysis of the protein from this gene. In addition, the developmental isoforms, hypothesized to have low ATPase activity, were indistinguishable from adult-fast MyHC-IIa and the specialized MyHC-Extraocular isoform, that was predicted to be the fastest of all six isoforms but was functionally similar to the slower isoforms.

An Integrative Analysis of the Muscle Myosin Motor Using Genetic and Transgenic Tools

We use Drosophila melanogaster to investigate the mechanisms by which myosin heavy chain isoforms contribute to muscle-specific cyto-architectures and contractile properties. We expressed various myosin isoforms in transgenic indirect flight muscles. Along with our collaborators, we examined 1) ATPase, in vitro actin sliding, step size and structure of the isolated myosin, 2) ultrastructure and mechanical properties of muscle fibers, and 3) locomotory abilities of the transgenic organisms. We found that isoform-specific differences in myosin cause relatively small structural variations in muscle assembly, but are critical to myofibril stability and function.

Unc45 Activates Hsp90-dependent Folding of the Myosin Motor Domain

Myosin folding and assembly in striated muscle are mediated by the general chaperones Hsc70 and Hsp90 and involve a myosin-specific co-chaperone related to the Caenorhabditis elegans gene unc-45. Two unc-45 genes are found in vertebrates, a general cell isoform, unc45a, and a striated muscle-specific isoform, unc45b. We have investigated the role of both isoforms of mouse Unc45 in myosin folding using an in vitro synthesis and folding assay. A smooth muscle myosin motor domain (MD) fused to green fluorescent protein (GFP) (MD::GFP) was used as substrate, and folding was measured by native gel electrophoresis and functional assays. In the absence of Unc45, the MD::GFP chimera folds poorly. Addition of either Unc45a or Unc45b dramatically enhances the folding in a reaction that is dependent on Hsp90 ATPase activity. Unc45a is more effective than Unc45b with a higher apparent affinity and greater extent of folding. The Unc45-Hsp90 chaperone complex acts late in the folding pathway and promotes motor domain maturation after release from the ribosome. Unc45a behaves kinetically as an activator of the folding reaction by stimulating the rate of the Hsp90-dependent folding by >20-fold with an apparent K(act) of 33 nm. This analysis of vertebrate Unc45 isoforms clearly demonstrates a direct role for Unc45 in Hsp90-mediated myosin motor domain folding and highlights major differences between the isoforms in substrate specificity and mechanism.

The Structural Basis for the Large Powerstroke of Myosin VI

Due to a unique addition to the lever arm-positioning region (converter), class VI myosins move in the opposite direction (toward the minus-end of actin filaments) compared to other characterized myosin classes. However, the large size of the myosin VI lever arm swing (powerstroke) cannot be explained by our current view of the structural transitions that occur within the myosin motor. We have solved the crystal structure of a fragment of the myosin VI motor in the structural state that represents the starting point for movement on actin; the pre-powerstroke state. Unexpectedly, the converter itself rearranges to achieve a conformation that has not been seen for other myosins. This results in a much larger powerstroke than is achievable without the converter rearrangement. Moreover, it provides a new mechanism that could be exploited to increase the powerstroke of yet to be characterized plus-end-directed myosin classes.

Myosin Mechanochemistry

Myosin Mechanochemistry

Expression and function of COOH-terminal myosin heavy chain isoforms in mouse smooth muscle

Isoforms of the smooth muscle myosin motor, SM1 and SM2, differ in length at the carboxy terminal tail region. Their proportion changes with development, hormonal status and disease, but their function is unknown. We developed mice carrying the myosin heavy chain (MyHC) transgenes SM1, cMyc-tagged SM1, SM2, and V5-tagged SM2, and all transgenes corresponded to the SMa NH(2)-terminal isoform. Transgene expression was targeted to smooth muscle by the smooth muscle alpha-actin promoter. Immunoblot analysis showed substantial expression of the cMyc-tagged SM1 and V5-tagged SM2 MyHC protein in aorta and bladder and transgene mRNA was expressed in mice carrying unlabeled SM1 or SM2 transgenes. Despite significant protein expression of tagged MyHCs we found only small changes in the SM1:SM2 protein ratio. Significant changes in functional phenotype were observed in mice carrying unlabeled SM1 or SM2 transgenes. Force in aorta and bladder was increased (72 +/- 14%, 92 +/- 11%) in SM1 and decreased to 57 +/- 1% and 80 +/- 3% in SM2 transgenic mice. SM1 transgenic bladders had faster (1.8 +/- 0.3 s) and SM2 slower (7.1 +/- 0.5 s) rates of force redevelopment following a rapid step shortening. We hypothesize that small changes in the SM1:SM2 ratio could be amplified if they are associated with changes in thick filament assembly and underlie the altered contractility. These data provide evidence indicating an in vivo function for the COOH-terminal isoforms of smooth muscle myosin and suggest that the SM1:SM2 ratio is tightly regulated in smooth muscle tissues.

Refined Model of the 10 S Conformation of Smooth Muscle Myosin by Cryo-electron Microscopy 3D Image Reconstruction

The actin-activated ATPase activity of smooth muscle myosin and heavy meromyosin (smHMM) is regulated by phosphorylation of the regulatory light chain (RLC). Complete regulation requires two intact myosin heads because single-headed myosin subfragments are always active. 2D crystalline arrays of the 10 S form of intact myosin, which has a dephosphorylated RLC, were produced on a positively charged lipid monolayer and imaged in 3D at 2.0 nm resolution by cryo-electron microscopy of frozen, hydrated specimens. An atomic model of smooth muscle myosin was constructed from the X-ray structures of the smooth muscle myosin motor domain and essential light chain and a homology model of the RLC was produced based on the skeletal muscle S1 structure. The initial model of the 10 S myosin, based on the previous reconstruction of smHMM, was subjected to real space refinement to obtain a quantitative fit to the density. The smHMM was likewise refined and both refined models reveal the same asymmetric interaction between the upper 50 kDa domain of the “blocked” head and parts of the catalytic, converter domains and the essential light chain of the “free” head observed previously. This observation suggests that this interaction is not simply due to crystallographic packing but is enforced by elements of the myosin heads. The 10 S reconstruction shows additional α-helical coiled-coil not seen in the earlier smHMM reconstruction, but the location of one segment of S2 is the same in both.

Modelling muscle motor conformations using low-angle X-ray diffraction

New results on myosin head organization using analysis of low-angle X-ray diffraction patterns from relaxed insect flight muscle (IFM) from a giant waterbug, building on previous studies of myosin filaments in bony fish skeletal muscle (BFM), show that the information content of such low-angle diffraction patterns is very high despite the 'crystallographically low' resolution limit (65 A) of the spacings of the Bragg diffraction peaks being used. This high information content and high structural sensitivity arises because: (i) the atomic structures of the domains of the myosin head are known from protein crystallography; and (ii) myosin head action appears to consist mainly of pivoting between domains which themselves stay rather constant in structure, thus (iii) the intensity distribution among diffraction peaks in even the low resolution diffraction pattern is highly determined by the high-resolution distribution of atomically modelled domain mass. A single model was selected among 5000+ computer-generated variations as giving the best fit for the 65 reflections recorded within the selected resolution limit of 65 A. Clear evidence for a change in shape of the insect flight muscle myosin motor between the resting (probably like the pre-powerstroke) state and the rigor state (considered to mimic the end-of-powerstroke conformation) has been obtained. This illustrates the power of the low-angle X-ray diffraction method. The implications of these new results about myosin motor action during muscle contraction are discussed.

Folding of the Striated Muscle Myosin Motor Domain

We have investigated the folding of the myosin motor domain using a chimera of an embryonic striated muscle myosin II motor domain fused on its COOH terminus to a thermal stable, fast folding variant of green fluorescent protein (GFP). In in vitro expression assays, the GFP domain of the chimeric protein, S1(795)GFP, folds rapidly enabling us to monitor the folding of the motor domain using fluorescence. The myosin motor domain folds very slowly and transits through multiple intermediates that are detectable by gel filtration chromatography. The distribution of the nascent protein among these intermediates is strongly dependent upon temperature. At 25 degrees C and above the predominant product is an aggregate of S1(795)GFP or a complex with other lysate proteins. At 0 degrees C, the motor domain folds slowly via an energy independent pathway. The unusual temperature dependence and slow rate suggests that folding of the myosin motor is highly susceptible to off-pathway interactions and aggregation. Expression of the S1(795)GFP in the C2C12 muscle cell line yields a folded and functionally active protein that exhibits Mg(2+)ATP-sensitive actin-binding and myosin motor activity. In contrast, expression of S1(795)GFP in kidney epithelial cell lines (human 293 and COS 7 cells) results in an inactive and aggregated protein. The results of the in vitro folding assay suggest that the myosin motor domain does not fold spontaneously under physiological conditions and probably requires cytosolic chaperones. The expression studies support this conclusion and demonstrate that these factors are optimized in muscle cells.

Myosin motor domain lever arm rotation is coupled to ATP hydrolysis.

We have investigated coupling of lever arm rotation to the ATP binding and hydrolysis steps for the myosin motor domain. In several current hypotheses of the mechanism of force production by muscle, the primary mechanical feature is the rotation of a lever arm that is a subdomain of the myosin motor domain. In these models, the lever arm rotates while the myosin motor domain is free, and then reverses the rotation to produce force while it is bound to actin. These mechanical steps are coupled to steps in the ATP hydrolysis cycle. Our hypothesis is that ATP hydrolysis induces lever arm rotation to produce a more compact motor domain that has stored mechanical energy. Our approach is to use transient electric birefringence techniques to measure changes in hydrodynamic size that result from lever arm rotation when various ligands are bound to isolated skeletal muscle myosin motor domain in solution. Results for ATP and CTP, which do support force production by muscle fibers, are compared to those of ATPgammaS and GTP, which do not. Measurements are also made of conformational changes when the motor domain is bound to NDP's and PP(i) in the absence and presence of the phosphate analogue orthovanadate, to determine the roles the nucleoside moieties of the nucleotides have on lever arm rotation. The results indicate that for the substrates investigated, rotation does not occur upon substrate binding, but is coupled to the NTP hydrolysis step. The data are consistent with a model in which only substrates that produce a motor domain-NDP-P(i) complex as the steady-state intermediate make the motor domain more compact, and only those substrates support force production.