Crowded surfaces change annealing dynamics of actin filaments

Changes in cell shape that occur in many cellular processes are thought to arise from polymerization of actin filaments near the cell membrane. End-to-end annealing of actin filaments is believed to play only a minor role in this process, as annealing in solution was shown to be a slow process, which is not typical for a bimolecular reaction, its rate constant decreasing over time, being inversely proportional to the filament length. Furthermore, in vitro studies on f-actin solutions were found to display an exponential steady-state length distribution. In the cell, many physiologically important parameters, such as mechanical strength or viscoelastic response are a direct function of the physical properties of the underlying actin cytoskeleton, such as actin filament length distribution and dynamics. How the underlying physical parameters of the actin cytoskeleton may be influenced by the cell surface or molecular crowding remains poorly understood. Using total internal reflection fluorescence (TIRF) microscopy we reinvestigated actin end-to-end annealing in vitro in a more realistic environment. We studied the process near a hydrophilic surface together with crowding agents, in order to mimic the physiological media near the cell membrane, which has substantial amounts of macromolecules present. We find that actin end-to-end annealing changes in three ways near a crowded hydrophilic surface as compared to solution. First the annealing rate becomes a factor of 20 faster than in solution. Second the rate of annealing becomes typical of a bimolecular reaction, shows no length dependence and is basically just a function of the square of the concentration of ends. Lastly the length distribution is Gaussian throughout the entire annealing process. This implicates that dynamic rearrangement of actin filaments by annealing near the leading edge of the cell, could change physical parameters like the mechanical response and contribute significantly to cell motility.     

Intermediate filaments exchange subunits along their length and elongate by end-to-end annealing

Actin filaments and microtubules lengthen and shorten by addition and loss of subunits at their ends, but it is not known whether this is also true for intermediate filaments. In fact, several studies suggest that in vivo, intermediate filaments may lengthen by end-to-end annealing and that addition and loss of subunits is not confined to the filament ends. To test these hypotheses, we investigated the assembly dynamics of neurofilament and vimentin intermediate filament proteins in cultured cells using cell fusion, photobleaching, and photoactivation strategies in combination with conventional and photoactivatable fluorescent fusion proteins. We show that neurofilaments and vimentin filaments lengthen by end-to-end annealing of assembled filaments. We also show that neurofilaments and vimentin filaments incorporate subunits along their length by intercalation into the filament wall with no preferential addition of subunits to the filament ends, a process which we term intercalary subunit exchange.     

Kinetic analysis of actin assembly suggests that tropomyosin inhibits spontaneous fragmentation of actin filaments

The time-course of actin assembly was measured in the absence and in the presence of tropomyosin. The polymerization was followed by the fluorescence enhancement of a 7-chloro-4-nitrobenzeno-2-oxa-1,3-diazole label attached to actin molecules or by light-scattering. The kinetic curves measured in the absence and in the presence of tropomyosin revealed characteristic differences. Tropomyosin was found to retard actin polymerization and to cause the final constant actin monomer concentration to be reached slowly. In the absence of tropomyosin, the final constant actin monomer concentration was approached considerably faster. The time-course of polymerization was interpreted quantitatively in terms of inhibition of actin filament fragmentation by tropomyosin molecules bound along the filaments. Within the limits of this model, actin monomers are consumed slowly in the presence of tropomyosin because the creation of new filament ends by spontaneous fragmentation is inhibited by tropomyosin.     

Single molecule polymerization, annealing and bundling dynamics of SipA induced actin filaments

Salmonella bacteria cause more than three million deaths each year. They hijack cells and inject among other proteins SipA via a "molecular syringe" into the cell, which can tether actin subunits in opposing strands to form mechanically stabilized filaments which rapidly reshape the cells surface into extended ruffles, leading to bacterial internalization. Exactly how these ruffles form at a single filament level remains unknown. Our real time total internal fluorescence microscopy observations show that both bidirectional elongation of actin by SipA as well as end-to-end annealing of SipA-actin filaments are rapid processes. Complementary electron microscopy investigations demonstrate that crowding agents in vitro readily induce stiff bundles of SipA-actin filaments. Taken together these three effects, rapid SipA induced actin polymerization, filament annealing and bundle formation due to molecular crowding can explain how Salmonella invades cells at molecular level.     

Rate and mechanism of the assembly of tropomyosin with actin filaments

The rate of assembly of tropomyosin with actin filaments was measured by stopped-flow experiments. Binding of tropomyosin to actin filaments was followed by the change of the fluorescence intensity of a (dimethylamino)naphthalene label covalently linked to tropomyosin and by synchrotron radiation X-ray solution scattering. Under the experimental conditions (2 mM MgCl2, 100 mM KCl, pH 7.5, 25 degrees C) and at the protein concentrations used (2.5-24 microM actin, 0.2-3.4 microM tropomyosin) the half-life time of assembly of tropomyosin with actin filaments was found to be less than 1 s. The results were analyzed quantitatively by a model in which tropomyosin initially binds to isolated sites. Further tropomyosin molecules bind contiguously to bound tropomyosin along the actin filaments. Good agreement between the experimental and theoretical time course of assembly was obtained by assuming a fast preequilibrium between free and isolatedly bound tropomyosin.     

Effect of ATP removal and inorganic phosphate on length redistribution of sheared actin filament populations. Evidence for a mechanism of end-to-end annealing

The effect of inorganic phosphate (Pi) on the depolymerization of F-actin has been measured. Pi inhibits disassembly of pyrene-labelled F-actin at steady-state induced either by dilution, or by shearing, suggesting that Pi decreases the off rate constant, k-, for dissociation. This effect of Pi is maximal at 20 mM, unlike the effect of Pi in reducing the critical concentration at the pointed end (maximal at 2 mM). This difference in concentration dependence for the two effects is interpreted as different affinities of Pi for the barbed and pointed ends, presumably as ADP-Pi-actin species. The contribution of ATP/ADP phase changes at filament ends (i.e. "dynamic instability") to length redistribution in sheared polymer steady-state actin filament populations was determined by (1) converting ATP to ADP in the system to prevent phase changes, or (2) adding 20 mM-Pi to the system to inhibit depolymerization. The observed absence of effect of these treatments on length redistribution excludes all mechanisms which involve phase change-driven disassembly or monomer exchange at filament ends, and appears to constrain the mechanism to one of end-to-end annealing under these conditions.     

Formin-induced nucleation of actin filaments

Formins are proteins best defined by the presence of the unique, highly conserved formin homology domain 2 (FH2). FH2 is necessary and sufficient to nucleate an actin filament in vitro. The FH2 domain also binds to the filament's barbed end, modulating its elongation and protecting it from capping proteins. FH2 itself appears to be a processive cap that walks with the barbed end as it elongates.     

Heavy-meromyosin-decorated actin filaments: a simple method to preserve actin filaments for rotary shadowing

It has become accepted that deep-freeze-drying at or below -90 degrees C is necessary to preserve the structure of supramolecular assemblies such as actin filaments (AFs) for metal shadowing. This has kept the metal shadowing technique from widespread use in the study of proteins complexed with AFs because of the limited availability of the apparatus for deep-freeze-drying. I report here that adsorption to freshly cleaved mica, treatment with buffered uranyl acetate in glycerol solution, rinsing, and removal of liquid eliminate the need of freeze-drying to preserve the structure of AFs. This technique, in combination with metal shadowing, was applied to the study of AFs decorated with heavy meromyosin (HMM). It was observed that (1) when HMM molecules are associated with single AFs in the majority of cases only one head of each HMM molecule makes contact at the point furthest from the neck region; (2) binding of HMM causes bundling of AFs, probably by the two heads of each molecule binding different filaments; and (3) the binding of HMM to the bundled AFs appears to be more stable than that to a single AF. This method of specimen preparation requires no freeze-drying and is therefore easily applicable to other large protein complexes.     

Formation and destabilization of actin filaments with tetramethylrhodamine-modified actin

Actin labeling at Cys(374) with tethramethylrhodamine derivatives (TMR-actin) has been widely used for direct observation of the in vitro filaments growth, branching, and treadmilling, as well as for the in vivo visualization of actin cytoskeleton. The advantage of TMR-actin is that it does not lock actin in filaments (as rhodamine-phalloidin does), possibly allowing for its use in investigating the dynamic assembly behavior of actin polymers. Although it is established that TMR-actin alone is polymerization incompetent, the impact of its copolymerization with unlabeled actin on filament structure and dynamics has not been tested yet. In this study, we show that TMR-actin perturbs the filaments structure when copolymerized with unlabeled actin; the resulting filaments are more fragile and shorter than the control filaments. Due to the increased severing of copolymer filaments, TMR-actin accelerates the polymerization of unlabeled actin in solution also at mole ratios lower than those used in most fluorescence microscopy experiments. The destabilizing and severing effect of TMR-actin is countered by filament stabilizing factors, phalloidin, S1, and tropomyosin. These results point to an analogy between the effects of TMR-actin and severing proteins on F-actin, and imply that TMR-actin may be inappropriate for investigations of actin filaments dynamics.     

Yeast actin patches are networks of branched actin filaments

Cortical actin patches are the most prominent actin structure in budding and fission yeast. Patches assemble, move, and disassemble rapidly. We investigated the mechanisms underlying patch actin assembly and motility by studying actin filament ultrastructure within a patch. Actin patches were partially purified from Saccharomyces cerevisiae and examined by negative-stain electron microscopy (EM). To identify patches in the EM, we correlated fluorescence and EM images of GFP-labeled patches. Patches contained a network of actin filaments with branches characteristic of Arp2/3 complex. An average patch contained 85 filaments. The average filament was only 50-nm (20 actin subunits) long, and the filament to branch ratio was 3:1. Patches lacking Sac6/fimbrin were unstable, and patches lacking capping protein were relatively normal. Our results are consistent with Arp2/3 complex-mediated actin polymerization driving yeast actin patch assembly and motility, as described by a variation of the dendritic nucleation model.     

ADP-ribosylated actin caps the barbed ends of actin filaments

The mode of action on actin polymerization of skeletal muscle actin ADP-ribosylated on arginine 177 by perfringens iota toxin was investigated. ADP-ribosylated actin decreased the rate of nucleated actin polymerization at substoichiometric ratios of ADP-ribosylated actin to monomeric actin. ADP-ribosylated actin did not tend to copolymerize with actin. Actin filaments were depolymerized by the addition of ADP-ribosylated actin. The maximal monomer concentration reached by addition of ADP-ribosylated actin was similar to the critical concentration of the pointed ends of actin filaments. ADP-ribosylated actin had no effect on the rate of polymerization of gelsolin-capped actin filaments which polymerize at the pointed ends. The results suggest that ADP-ribosylated actin acts as a capping protein which binds to the barbed ends of actin filaments to inhibit polymerization. Based on an analysis of the depolymerizing effect of ADP-ribosylated actin, the equilibrium constant for binding of ADP-ribosylated actin to the barbed ends of actin filaments was determined to be about 10(8) M-1. As actin is ADP-ribosylated by perfringens iota toxin and by botulinum C2 toxin, it appears that conversion of actin into a capping protein by ADP-ribosylation is a pathophysiological reaction catalyzed by bacterial toxins which ultimately leads to inhibition of actin assembly.     

Binding of actin filaments to connectin

The binding of actin filaments to connectin, a muscle elastic protein, was investigated by means of turbidity and sedimentation measurements and electron microscopy. In the presence of less than 0.12 M KCl at pH 7.0, actin filaments bound to connectin. Long actin filaments formed bundles. Short actin filaments also aggregated into irregular bundles or a meshwork, and were frequently attached perpendicularly to long bundles. The binding of F-actin to connectin was saturated at an equal weight ratio (molar ratio, 50 : 1), as determined by a cosedimentation assay. Larger amounts of sonicated short actin filaments appeared to bind to connectin than intact F-actin. Myosin S1-decorated actin filaments did not bind to connectin. The addition of S1 to connectin-induced actin bundles resulted in partial disaggregation. Thus, connectin does not appear to interfere with actin-myosin interactions, since myosin S1 binds to actin more strongly than connectin.     

Interaction of tropomyosin-troponin with actin filaments

The assembly of actin filaments with tropomyosin-troponin was investigated by means of light scattering. Binding curves of tropomyosin-troponin [consisting of all three subunits (holotroponin)] and of tropomyosin-troponin-T-I to actin filaments were analyzed by separating the affinity of tropomyosin-troponin for actin filaments and the affinity for the end-to-end contact of tropomyosin molecules. Under the experimental conditions (42.4 degrees C, 300 mM KCl), tropomyosin-holotroponin in the absence of calcium and tropomyosin-troponin-T-I had similar affinities for actin filaments whereas tropomyosin-holotroponin in the presence of calcium was found to bind more weakly. Tropomyosin-holotroponin and tropomyosin-troponin-T-I bound about 200-300-fold more strongly to binding sites with adjacent tropomyosin-troponin units than to isolated sites on actin filaments. The equilibrium constant for isolated association with actin filaments was more than 2-fold higher for tropomyosin-holotroponin in the absence of calcium (15 400 M-1) and tropomyosin-troponin-T-I (17 500 M-1) than for tropomyosin-holotroponin in the presence of calcium (6600 M-1). Binding curves of mixtures of tropomyosin-holotroponin in the presence of calcium and of tropomyosin-troponin-T-I were measured and analyzed on the basis of a model of cooperative binding of two types of large ligands to a one-dimensional homogeneous lattice. The results provided information on the strength of the end-to-end contacts of tropomyosin-troponin units in different positions on an actin filament. It was found that a tropomyosin-troponin unit binds adjacently to another unit in a different position on an actin filament about 2-fold more weakly than adjacent to a unit in the same position. With the aid of these results, it was possible to obtain information of the equilibrium distribution of tropomyosin-troponin in the two positions on actin filaments. Generation of a sequence of tropomyosin-troponin units in a different position on actin filaments was found to be 4-fold less favored than elongation of an existing sequence (cooperativity parameter sigma = 1/4). Shifting of tropomyosin-troponin on actin filaments appears to be accompanied by small free-energy changes in the various interactions of the components of actin-tropomyosin-troponin filaments and not to be an all-or-none reaction     

A mechanochemical model of actin filaments

In eukaryotic cells, actin filaments are involved in important processes such as motility, division, cell shape regulation, contractility, and mechanosensation. Actin filaments are polymerized chains of monomers, which themselves undergo a range of chemical events such as ATP hydrolysis, polymerization, and depolymerization. When forces are applied to F-actin, in addition to filament mechanical deformations, the applied force must also influence chemical events in the filament. We develop an intermediate-scale model of actin filaments that combines actin chemistry with filament-level deformations. The model is able to compute mechanical responses of F-actin during bending and stretching. The model also describes the interplay between ATP hydrolysis and filament deformations, including possible force-induced chemical state changes of actin monomers in the filament. The model can also be used to model the action of several actin-associated proteins, and for large-scale simulation of F-actin networks. All together, our model shows that mechanics and chemistry must be considered together to understand cytoskeletal dynamics in living cells.     

Dynamics of actin filaments during tension-dependent formation of actin bundles

The actin cytoskeleton stress fiber is an actomyosin-based contractile structure seen as a bundle of actin filaments. Although tension development in a cell is believed to regulate stress fiber formation, little is known for the underlying biophysical mechanisms. To address this question, we examined the effects of tension on the behaviors of individual actin filaments during stress fiber (actin bundle) formation using cytosol-free semi-intact fibroblast cells that were pre-treated with the Rho kinase inhibitor Y-27632 to disassemble stress fibers into a meshwork of actin filaments. These filaments were sparsely labeled with quantum dots for live tracking of their motions. When ATP and Ca(2+) were applied to the semi-intact cells to generate actomyosin-based forces, actin meshwork in the protruded lamellae was dragged toward the cell body, while the periphery of the meshwork remained in the original region, indicating that centripetally directed tension developed in the meshwork. Then the individual actin filaments in the meshwork moved towards the cell body accompanied with sudden changes in the direction of their movements, finally forming actin bundles along the direction of tension. Dragging the meshwork by externally applied mechanical forces also exerted essentially the same effects. These results suggest the existence of tension-dependent remodeling of cross-links within the meshwork during the rearrangement of actin filaments, thus demonstrating that tension is a key player to regulate the dynamics of individual actin filaments that leads to actin bundle formation.     

Mechanotransduction down to individual actin filaments

The actin cytoskeleton plays an essential role in a cell's ability to generate and sense forces, both internally and in interaction with the outside world. The transduction of mechanical cues into biochemical reactions in cells, in particular, is a multi-scale process which requires a variety of approaches to be understood. This review focuses on understanding how mechanical stress applied to an actin filament can affect its assembly dynamics. Today, experiments addressing this issue at the scale of individual actin filaments are emerging and bring novel insight into mechanotransduction. For instance, recent data show that actin filaments can act as mechanosensors, as an applied tension or curvature alters their conformation and their affinity for regulatory proteins. Filaments can also transmit mechanical tension to other proteins, which consequently change the way they interact with the filaments to regulate their assembly. These results provide evidence for mechanotransduction at the scale of individual filaments, showing that forces participate in the regulation of filament assembly and organization. They bring insight into the elementary events coupling mechanics and biochemistry in cells. The experiments presented here are linked to recent technical developments, and certainly announce the advent of more exciting results in the future.