Contraction and polymerization cooperate to assemble and close actomyosin rings around Xenopus oocyte wounds

Xenopus oocytes assemble an array of F-actin and myosin 2 around plasma membrane wounds. We analyzed this process in living oocytes using confocal time-lapse (four-dimensional) microscopy. Closure of wounds requires assembly and contraction of a classic "contractile ring" composed of F-actin and myosin 2. However, this ring works in concert with a 5-10-microm wide "zone" of localized actin and myosin 2 assembly. The zone forms before the ring and can be uncoupled from the ring by inhibition of cortical flow and contractility. However, contractility and the contractile ring are required for the stability and forward movement of the zone, as revealed by changes in zone dynamics after disruption of contractility and flow, or experimentally induced breakage of the contractile ring. We conclude that wound-induced contractile arrays are provided with their characteristic flexibility, speed, and strength by the combined input of two distinct components: a highly dynamic zone in which myosin 2 and actin preferentially assemble, and a stable contractile actomyosin ring.     

The cortical microfilament system of lymphoblasts displays a periodic oscillatory activity in the absence of microtubules: implications for cell polarity

For an understanding of the role of microtubules in the definition of cell polarity, we have studied the cell surface motility of human lymphoblasts (KE37 cell line) using video microscopy, time-lapse photography, and immunofluorescent localization of F-actin and myosin. Polarized cell surface motility occurs in association with a constriction ring which forms on the centrosome side of the cell: the cytoplasm flows from the ring zone towards membrane veils which keep protruding in the same general direction. This association is ensured by microtubules: in their absence the ring is conspicuous and moves periodically back and forth across the cell, while a protrusion of membrane occurs alternately at each end of the cell when the ring is at the other. This oscillatory activity is correlated with a striking redistribution of myosin towards a cortical localization and appears to be due to the alternate flow of cortical myosin associated with the ring and to the periodic assembly of actin coupled with membrane protrusion. The ring cycle involves the progressive recruitment of myosin from a polar accumulation, or cap, its transportation across the cell and its accumulation in a new cap at the other end of the cell, suggesting an assembly-disassembly process. Inhibition of actin assembly induces, on the other hand, a dramatic microtubule-dependent cell elongation with definite polarity, likely to involve the interaction of microtubules with the cell cortex. We conclude that the polarized cell surface motility in KE37 cells is based on the periodic oscillatory activity of the actin system: a myosin-powered equatorial contraction and an actin-based membrane protrusion are concerted at the cell level and occur at opposite ends of the cell in absence of microtubules. This defines a polarity which reverses periodically as the ring moves across the cell. Microtubules impose a stable cell polarity by suppressing the ring movement. A permanent association of the myosin-powered contraction and the membrane protrusion is established which results in the unidirectional activity of the actin system. Microtubules exert their effect by controlling the recruitment of cytoplasmic myosin into the cortex, probably through their direct interaction with the cortical microfilament system.     

Relative distribution of myosin, actin, and alpha-actinin in adherent monocytes.

The characteristic amoeboid movement of human leucocytes uses mechanical energy derived from the hydrolysis of adenosine triphosphate through a mechanochemical system of the contractile proteins myosin, actin, and the actin-associated protein alpha-actinin. We observed the relative distribution of myosin, actin, and alpha-actinin in adherent monocytes during movement by a double-fluorescence staining procedure. The results indicate that myosin and alpha-actinin are closely associated with the actin cable network, and that alpha-actinin is in close association with the plasma membrane and anchors filamentous actin (F-actin) beneath the plasma membrane; F-actin and alpha-actinin play an important role at the leading edge during the formation of lamellipodia. These findings should be helpful in clarifying the mechanism of leucocyte movement from a morphologic standpoint.     

The Association of Myosin IB with Actin Waves in Dictyostelium Requires Both the Plasma Membrane-Binding Site and Actin-Binding Region in the Myosin Tail

F-actin structures and their distribution are important determinants of the dynamic shapes and functions of eukaryotic cells. Actin waves are F-actin formations that move along the ventral cell membrane driven by actin polymerization. Dictyostelium myosin IB is associated with actin waves but its role in the wave is unknown. Myosin IB is a monomeric, non-filamentous myosin with a globular head that binds to F-actin and has motor activity, and a non-helical tail comprising a basic region, a glycine-proline-glutamine-rich region and an SH3-domain. The basic region binds to acidic phospholipids in the plasma membrane through a short basic-hydrophobic site and the Gly-Pro-Gln region binds F-actin. In the current work we found that both the basic-hydrophobic site in the basic region and the Gly-Pro-Gln region of the tail are required for the association of myosin IB with actin waves. This is the first evidence that the Gly-Pro-Gln region is required for localization of myosin IB to a specific actin structure in situ. The head is not required for myosin IB association with actin waves but binding of the head to F-actin strengthens the association of myosin IB with waves and stabilizes waves. Neither the SH3-domain nor motor activity is required for association of myosin IB with actin waves. We conclude that myosin IB contributes to anchoring actin waves to the plasma membranes by binding of the basic-hydrophobic site to acidic phospholipids in the plasma membrane and binding of the Gly-Pro-Gln region to F-actin in the wave.     

Contractile ring formation in Xenopus egg and fission yeast

How actin filaments (F-actin) and myosin II (myosin) assemble to form the contractile ring was investigated with fission yeast and Xenopus egg. In fission yeast cells, an aster-like structure composed of F-actin cables is formed at the medial cortex of the cell during prophase to metaphase, and a single F-actin cable(s) extends from this structure, which seems to be a structural basis of the contractile ring. In early mitosis, myosin localizes as dots in the medial cortex independently of F-actin. Then they fuse with each other and are packed into a thin contractile ring. At the growing ends of the cleavage furrow of Xenopus eggs, F-actin at first assembles to form patches. Next they fuse with each other to form short F-actin bundles. The short bundles then form long bundles. Myosin seems to be transported by the cortical movement to the growing end and assembles there as spots earlier than F-actin. Actin polymerization into the patches is likely to occur after accumulation of myosin. The myosin spots and the F-actin patches are simultaneously reorganized to form the contractile ring bundles. The idea that a Ca signal triggers cleavage furrow formation was tested with Xenopus eggs during the first cleavage. We could not detect any Ca signals such as a Ca wave, Ca puffs or even Ca blips at the growing end of the cleavage furrow. Furthermore, cleavages are not affected by Ca-chelators injected into the eggs at concentrations sufficient to suppress the Ca waves. Thus we conclude that formation of the contractile ring is not induced by a Ca signal at the growing end of the cleavage furrow.     

Nonmedially assembled F-actin cables incorporate into the actomyosin ring in fission yeast

In many eukaryotes, cytokinesis requires the assembly and constriction of an actomyosin-based contractile ring. Despite the central role of this ring in cytokinesis, the mechanism of F-actin assembly and accumulation in the ring is not fully understood. In this paper, we investigate the mechanism of F-actin assembly during cytokinesis in Schizosaccharomyces pombe using lifeact as a probe to monitor actin dynamics. Previous work has shown that F-actin in the actomyosin ring is assembled de novo at the division site. Surprisingly, we find that a significant fraction of F-actin in the ring was recruited from formin-Cdc12p nucleated long actin cables that were generated at multiple nonmedial locations and incorporated into the ring by a combination of myosin II and myosin V activities. Our results, together with findings in animal cells, suggest that de novo F-actin assembly at the division site and directed transport of F-actin cables assembled elsewhere can contribute to ring assembly.     

Coupled myosin VI motors facilitate unidirectional movement on an F-actin network

Unconventional myosins interact with the dense cortical actin network during processes such as membrane trafficking, cell migration, and mechanotransduction. Our understanding of unconventional myosin function is derived largely from assays that examine the interaction of a single myosin with a single actin filament. In this study, we have developed a model system to study the interaction between multiple tethered unconventional myosins and a model F-actin cortex, namely the lamellipodium of a migrating fish epidermal keratocyte. Using myosin VI, which moves toward the pointed end of actin filaments, we directly determine the polarity of the extracted keratocyte lamellipodium from the cell periphery to the cell nucleus. We use a combination of experimentation and simulation to demonstrate that multiple myosin VI molecules can coordinate to efficiently transport vesicle-size cargo over 10 µm of the dense interlaced actin network. Furthermore, several molecules of monomeric myosin VI, which are nonprocessive in single molecule assays, can coordinate to transport cargo with similar speeds as dimers.     

Germinal center-specific protein human germinal center associated lymphoma directly interacts with both myosin and actin and increases the binding of myosin to actin

Human germinal center associated lymphoma (HGAL) is a germinal center-specific gene whose expression correlates with a favorable prognosis in patients with diffuse large B-cell and classic Hodgkin lymphomas. HGAL is involved in negative regulation of lymphocyte motility. The movement of lymphocytes is directly driven by actin polymerization and actin-myosin interactions. We demonstrate that HGAL interacts directly and independently with both actin and myosin and delineate the HGAL and myosin domains responsible for the interaction. Furthermore, we show that HGAL increases the binding of myosin to F-actin and inhibits the ability of myosin to translocate actin by reducing the maximal velocity of myosin head/actin movement. No effects of HGAL on actomyosin ATPase activity and the rate of actin polymerization from G-actin to F-actin were observed. These findings reveal a new mechanism underlying the inhibitory effects of germinal center-specific HGAL protein on lymphocyte and lymphoma cell motility.     

Myosin VI stabilizes an actin network during Drosophila spermatid individualization

Here, we demonstrate a new function of myosin VI using observations of Drosophila spermatid individualization in vivo. We find that myosin VI stabilizes a branched actin network in actin structures (cones) that mediate the separation of the syncytial spermatids. In a myosin VI mutant, the cones do not accumulate F-actin during cone movement, whereas overexpression of myosin VI leads to bigger cones with more F-actin. Myosin subfragment 1-fragment decoration demonstrated that the actin cone is made up of two regions: a dense meshwork at the front and parallel bundles at the rear. The majority of the actin filaments were oriented with their pointed ends facing in the direction of cone movement. Our data also demonstrate that myosin VI binds to the cone front using its motor domain. Fluorescence recovery after photobleach experiments using green fluorescent protein-myosin VI revealed that myosin VI remains bound to F-actin for minutes, suggesting its role is tethering, rather than transporting cargo. We hypothesize that myosin VI protects the actin cone structure either by cross-linking actin filaments or anchoring regulatory molecules at the cone front. These observations uncover a novel mechanism mediated by myosin VI for stabilizing long-lived actin structures in cells.     

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.     

The mechanism of the movement of leucocytes

In a study of the movement of human leucocytes it was clarified that characteristic contraction waves were observed on the cell surface during movement and an initial morphological change directly related to the appearance of the wave originated in the surface of the granuloplasm and not in the cell membrane. From these findings, together with physicochemical properties of the contractile protein from equine leucocytes, it was proposed that the wave observed in moving leucocytes might be conducted, in some way, by contraction and relaxation of the contractile protein in the cells. Myosin A and actin as constituents of the contractile protein were extracted separately from leucocytes in polymerized form, which resemble myosin aggregate and F-actin from muscle, respectively. The thick and thin filaments of about 150 and 80 Å in diameter were observed in glycerinated leucocytes with electron microscopy. When glycerinated leucocytes were incubated with heavy meromyosin (HMM) from rabbit skeletal myosin A, the thin filaments developed a structure resembling the ‘arrowhead structure’ of the HMM F-actin complex in vitro. The thick filaments seemed to correspond to myosin aggregates and the thin ones to filaments containing F-actin.     

Effect of actin filament length and filament number concentration on the actin-activated ATPase activity of Acanthamoeba myosin I

The actin-activated Mg2+-ATPase activities of phosphorylated Acanthamoeba myosins IA and IB were previously found to have a highly cooperative dependence on myosin concentration (Albanesi, J. P., Fujisaki, H., and Korn, E. D. (1985) J. Biol. Chem. 260, 11174-11179). This behavior is reflected in the requirement for a higher concentration of F-actin for half-maximal activation of the myosin Mg2+-ATPase at low ratios of myosin:actin (noncooperative phase) than at high ratios of myosin:actin (cooperative phase). These phenomena could be explained by a model in which each molecule of the nonfilamentous myosins IA and IB contains two F-actin-binding sites of different affinities with binding of the lower affinity site being required for expression of actin-activated ATPase activity. Thus, enzymatic activity would coincide with cross-linking of actin filaments by myosin. This theoretical model predicts that shortening the actin filaments and increasing their number concentration at constant total F-actin should increase the myosin concentration required to obtain the cooperative increase in activity and should decrease the F-actin concentration required to reach half-maximal activity at low myosin:actin ratios. These predictions have been experimentally confirmed by shortening actin filaments by addition of plasma gelsolin, an F-actin capping/severing protein. In addition, we have found that actin "filaments" as short as the 1:2 gelsolin-actin complex can significantly activate Acanthamoeba myosin I.     

A kinetic model for the molecular basis of the contractile activity of Acanthamoeba myosins IA and IB

Acanthamoeba myosins IA and IB are single-headed, monomeric molecules consisting of one heavy chain and one light chain. Both have high actin-activated Mg2+-ATPase activity, when the heavy chain is phosphorylated, but neither seems to be able to form the bipolar filaments that are generally thought to be required for actomyosin-dependent contractility. In this paper, we show that, at fixed F-actin concentration, the actin-activated Mg2+-ATPase activities of myosins IA and IB increase about 5-fold in specific activity in a cooperative manner as the myosin concentration is increased. The myosin concentration range over which this cooperative change occurs depends on the actin concentration. More myosin I is required for the cooperative increase in activity at high concentrations of F-actin. The cooperative increase in specific activity at limiting actin concentrations is caused by a decrease in the KATPase for F-actin. The high and low KATPase states of the myosin have about the same Vmax at infinite actin concentration. Both myosins are completely bound to the F-actin long before the Vmax values are reached. Therefore, much of the actin activation must be the result of interactions between F-actin and actomyosin. These kinetic data can be explained by a model in which the cooperative shift of myosin I from the high KATPase to the low KATPase state results from the cross-linking of actin filaments by myosin I. Cross-linking might occur either through two actin-binding sites on a single molecule or by dimers or oligomers of myosin I induced to form by the interaction of myosin I monomers with the actin filaments. The ability of Acanthamoeba myosins IA and IB to cross-link actin filaments is demonstrated in the accompanying paper (Fujisaki, H., Albanesi, J.P., and Korn, E.D. (1985) J. Biol. Chem. 260, 11183-11189).     

Protein phosphorylation regulates actomyosin-driven vesicle movement in cell extracts isolated from the green algae,Chara corallina

In Characean cells endoplasmic streaming stops upon membrane depolarization accompanied by Ca(2+) entry. We investigated the mechanism of this cessation of endoplasmic streaming by reconstituting the vesicle movement in vitro. In a living cell of Chara corallina, there are a number of vesicles moving along actin cables. Vesicles in the endoplasm squeezed out of the cell into a medium containing Mg-ATP showed directional movements under a dark field microscope. When the extracted endoplasm was treated with 20 nM okadaic acid, vesicles showed only movements like the Brownian motion. When it was treated with 50 nM staurosporine, directional movements of vesicles were activated. These movements were analyzed by image processing of videomicroscopic records. Vesicle movements along F-actin filaments were also observed by merging both images of the same field by dark field microscopy and fluorescence microscopy, indicating that myosin on the vesicle surface was responsible for vesicle movements. We also examined the effects of okadaic acid and staurosporine on in vitro sliding of F-actin on Chara myosin. When Chara myosin was treated with 20 nM okadaic acid in the cell extract, the number of sliding F-actin filaments was greatly reduced. In contrast, it increased when Chara myosin was treated with 50 nM staurosporine. In addition, Chara myosin treated with protein kinase C greatly diminished its motility. These results suggest that inactivation of Chara myosin via its phosphorylation is responsible for cessation of endoplasmic streaming.     

Immobilization of the type XIV myosin complex in Toxoplasma gondii

The substrate-dependent movement of apicomplexan parasites such as Toxoplasma gondii and Plasmodium sp. is driven by the interaction of a type XIV myosin with F-actin. A complex containing the myosin-A heavy chain, a myosin light chain, and the accessory protein GAP45 is attached to the membranes of the inner membrane complex (IMC) through its tight interaction with the integral membrane glycoprotein GAP50. For the interaction of this complex with F-actin to result in net parasite movement, it is necessary that the myosin be immobilized with respect to the parasite and the actin with respect to the substrate the parasite is moving on. We report here that the myosin motor complex of Toxoplasma is firmly immobilized in the plane of the IMC. This does not seem to be accomplished by direct interactions with cytoskeletal elements. Immobilization of the motor complex, however, does seem to require cholesterol. Both the motor complex and the cholesterol are found in detergent-resistant membrane domains that encompass a large fraction of the inner membrane complex surface. The observation that the myosin XIV motor complex of Toxoplasma is immobilized within this cholesterol-rich membrane likely extends to closely related pathogens such as Plasmodium and possibly to other eukaryotes.     

The utrophin actin-binding domain binds F-actin in two different modes: implications for the spectrin superfamily of proteins

Utrophin, like its homologue dystrophin, forms a link between the actin cytoskeleton and the extracellular matrix. We have used a new method of image analysis to reconstruct actin filaments decorated with the actin-binding domain of utrophin, which contains two calponin homology domains. We find two different modes of binding, with either one or two calponin-homology (CH) domains bound per actin subunit, and these modes are also distinguishable by their very different effects on F-actin rigidity. Both modes involve an extended conformation of the CH domains, as predicted by a previous crystal structure. The separation of these two modes has been largely dependent upon the use of our new approach to reconstruction of helical filaments. When existing information about tropomyosin, myosin, actin-depolymerizing factor, and nebulin is considered, these results suggest that many actin-binding proteins may have multiple binding sites on F-actin. The cell may use the modular CH domains found in the spectrin superfamily of actin-binding proteins to bind actin in manifold ways, allowing for complexity to arise from the interactions of a relatively few simple modules with actin.     

Membrane Phospholipid Redistribution in Cytokinesis： A Theoretical Model

In cell mitosis, cytokinesis is a major deformation process, during which the site of the contractile ring is determined by the biochemical stimulus from asters of the mitotic apparatus, actin and myosin assembly is related to the motion of membrane phospholipids, and local distribution and arrangement of the microfilament cytoskeleton are different at different cytokinesis stages. Based on the Zinemanas-Nir model, a new model is proposed in this study to simulate the entire process by coupling the biochemical stimulus with the mechanical actions. There were three assumptions in this model： the movements of phospholipid proteins are driven by gradients of biochemical stimulus on the membrane surface; the local assembly of actin and myosin filament depends on the amount of phospholipid proteins at the same location; and the surface tension includes membrane tensions due to both the passive deformation of the membrane and the active contraction of actin filament, which is determined by microfilament redistribution and rearrangement. This model could explain the dynamic movement of microfilaments during cytokinesis and predict cell deformation. The calculated results from this model demonstrated that the reorientation of phospholipid proteins and the redistribution and reorientation of microfilaments may play a crucial role in cell division. This model may better represent the cytokinesis process by the introduction of biochemical stimulus.     

Parking problem and negative cooperativity of binding of myosin subfragment 1 to F-actin

Previously we provided evidence that myosin subfragment 1 (S1) can bind either one (state 1) or two actin monomers (state 2) in solution and in muscle fiber. Here we present results of the kinetics study of binding of S1 to F-actin labeled with fluorescent dye pyrene. A transition from state 1 to state 2 depends on probability that the second actin is free, which is high when molar ratio of S1/actin (R) is less than 0.5, and it decreases dramatically when R>2.0 due to the parking problem. The kinetics data obtained at different molar ratios were well fitted by two binding states model. The sequential binding of myosin head initially with one actin monomer and then with the second actin monomer in F-actin can play a key role in force generation by actin-myosin and their directed movement.     

Two components of actin-based retrograde flow in sea urchin coelomocytes

Sea urchin coelomocytes represent an excellent experimental model system for studying retrograde flow. Their extreme flatness allows for excellent microscopic visualization. Their discoid shape provides a radially symmetric geometry, which simplifies analysis of the flow pattern. Finally, the nonmotile nature of the cells allows for the retrograde flow to be analyzed in the absence of cell translocation. In this study we have begun an analysis of the retrograde flow mechanism by characterizing its kinetic and structural properties. The supramolecular organization of actin and myosin II was investigated using light and electron microscopic methods. Light microscopic immunolocalization was performed with anti-actin and anti-sea urchin egg myosin II antibodies, whereas transmission electron microscopy was performed on platinum replicas of critical point-dried and rotary-shadowed cytoskeletons. Coelomocytes contain a dense cortical actin network, which feeds into an extensive array of radial bundles in the interior. These actin bundles terminate in a perinuclear region, which contains a ring of myosin II bipolar minifilaments. Retrograde flow was arrested either by interfering with actin polymerization or by inhibiting myosin II function, but the pathway by which the flow was blocked was different for the two kinds of inhibitory treatments. Inhibition of actin polymerization with cytochalasin D caused the actin cytoskeleton to separate from the cell margin and undergo a finite retrograde retraction. In contrast, inhibition of myosin II function either with the wide-spectrum protein kinase inhibitor staurosporine or the myosin light chain kinase-specific inhibitor KT5926 stopped flow in the cell center, whereas normal retrograde flow continued at the cell periphery. These differential results suggest that the mechanism of retrograde flow has two, spatially segregated components. We propose a "push-pull" mechanism in which actin polymerization drives flow at the cell periphery, whereas myosin II provides the tension on the actin cytoskeleton necessary for flow in the cell interior.     

Inhibition of sliding movement of F-actin by crosslinking emphasizes the role of actin structure in the mechanism of motility

The effects of crosslinking of monomeric and polymeric actin with 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide (EDC), disuccinimidyl suberate (DSS) and glutaraldehyde on the interaction with heavy meromyosin (HMM) in solution and on the sliding movement on glass-attached HMM were examined. The Vmax values of actin-activated HMM ATPase decreased in the following order: intact actin = EDC F-actin greater than DSS actin greater than glutaraldehyde F-actin = glutaraldehyde G-actin greater than EDC G-actin. The affinity of actin for HMM in the presence of ATP decreased in the following order: DSS actin greater than glutaraldehyde F-actin = glutaraldehyde G-actin greater than intact actin greater than EDC F-actin greater than EDC G-actin. However, sliding movement was inhibited only in the case of glutaraldehyde-crosslinked F and G-actin and EDC-crosslinked G-actin. Interestingly, after copolymerization of "non-motile" glutaraldehyde or EDC-crosslinked monomers with "motile" monomers of intact actin sliding of the copolymers was observed and its rate was independent of the type of crosslinked monomer, i.e. of the manner of their interaction with HMM. These data strongly indicate that inhibition of the sliding of actin by crosslinking cannot be explained entirely by changes in the Vmax value or affinity for myosin heads. We conclude that movement is generated by interaction of myosin with segments of F-actin containing a number of intact monomers, and the mechanism of inhibition involves an effect of the crosslinkers on the structure of F-actin itself.