Non-muscle actin filament elongation from complexes of profilin with nucleotide-free actin and divalent cation-free ATP-actin

Using vertebrate cytoplasmic actin consisting of a mixture of beta and gamma isoforms, we previously characterized profilin and nucleotide binding to monomeric actin (Kinosian, H. J., et al. (2000) Biochemistry 39, 13176-13188) and F-actin barbed end elongation from profilin-actin (PA) (Kinosian, H. J., et al. (2002) Biochemistry 41, 6734-6743). Our initial calculations indicated that elongation of F-actin from PA was more energetically favorable than elongation of F-actin from monomeric actin; therefore, the overall actin elongation reaction scheme described by these two linked reactions appeared to be thermodynamically unbalanced. However, we hypothesized that the profilin-induced weakening of MgATP binding by actin reduces the negative free energy change for the formation of profilin-MgATP-actin from MgATP-actin. When this was taken into account, the overall reaction scheme was calculated to be thermodynamically balanced. In our present work, we test this hypothesis by measuring actin filament barbed end elongation of nucleotide-free actin (NF-A) and nucleotide-free profilin-actin (NF-PA). We find that the free energy change for elongation of F-actin by NF-PA is equal to that for elongation of F-actin from NF-A, indicating energetic balance of the linked reactions. In the absence of actin-bound divalent cation, profilin has very little effect on ATP binding to actin; analysis of elongation experiments with divalent cation-free ATP-actin and profilin yielded an approximately energetically balanced reaction scheme. Thus, the data in this present report support our earlier hypothesis.     

Probing the structure of F-actin: cross-links constrain atomic models and modify actin dynamics.

Cross-links between protomers in F-actin can be used as a very sensitive probe of both the dynamics and structure of F-actin. We have characterized filaments formed from a previously described yeast actin Q41C mutant, where disulfide bonds can be formed between the Cys41 that is introduced into subdomain-2 and Cys374 on an adjacent protomer. We find that the distribution of cross-linked n-mers shows no cooperativity and corresponds to a random probability cross-linking reaction. The random distribution suggests that disulfide formation does not cause a significant perturbation of the F-actin structure. Consistent with this lack of perturbation, three-dimensional reconstructions of extensively cross-linked filaments, using a new approach to helical image analysis, show very small structural changes with respect to uncross-linked filaments. This finding is in conflict with refined models but in agreement with the original Holmes et al. model for F-actin. Under conditions where 94 % of the protomers are linked by disulfide bonds, the distribution of filament twist becomes more heterogeneous with respect to control filaments. A molecular model suggests that strain, introduced by the disulfide, is relieved by increasing the twist of the long-pitch actin helices. Disulfide formation makes yeast actin filaments approximately three times less flexible in terms of bending and similar, in this respect, to vertebrate skeletal muscle F-actin. These observations support previous reports that the rigidity of F-actin can be controlled by the position of subdomain-2, and that this region is more flexible in yeast F-actin than in skeletal muscle F-actin.     

The competitive interaction of actin and PIP2 with actophorin is based on overlapping target sites: design of a gain-of-function mutant

We studied the effect of mutations in an alpha-helical region of actophorin (residues 91-108) on F-actin and PIP(2) binding. As in cofilin, residues in the NH(2)-terminal half of this region are involved in F-actin binding. We show here also that basic residues in the COOH-terminal half of the region participate in this interaction whereby we extend the previously defined actin binding interface [Lappalainen, P., et al. (1997) EMBO J. 16, 5520-5530]. In addition, we demonstrate that some of the lysines in this alpha-helical region in actophorin are implicated in PIP(2) binding. This indicates that the binding sites of F-actin and PIP(2) on actophorin overlap, explaining the mutually exclusive binding of these ligands. The Ca(2+)-dependent F-actin binding of a number of actophorin mutants (carrying a lysine to glutamic acid substitution at the COOH-terminal positions of the actin binding helical region) may mimic the behavior of members of the gelsolin family. In addition, we show that PIP(2) binding, but not actin binding, of actophorin is strongly enhanced by a point mutation that leads to a reinforcement of the positive electrostatic potential of the studied alpha-helical region.     

Effects of tryptic digestion on myosin subfragment 1 and its actin-activated adenosinetriphosphatase

Myosin subfragment 1 (S-1) was fluorescently labeled at its rapidly reacting thiol ("SH1"). Short exposure to trypsin cuts the S-1 heavy chain into three still-associated fragments (20K, 50K, and 27K) [Balint, M., Wolf, L., Tarcsafalvi, A., Gergely, J., & Sreter, F.A. (1978) Arch. Biochem. Biophys. 190, 793-799] which bind F-actin to the same extent as does the uncut labeled S-1, as indicated by time-resolved fluorescence anisotropy decay (at 4 degrees C, pH 7, in 0.15 M KC1 and 5 mM MgC12, +/- 1 mM ADP). These results are thus in agreement with turbidity measurements on similar systems as reported by Mornet et al. [Mornet, D., Pantel, P., Audemard, E., & Kassab, R. (1979) Biochem. Biophys. Res. Commun. 89, 925-932]. The excited-state lifetime of the fluorescent label on cut S-1 is indistinguishable from that on normal S-1 (+/- ADP, +/- F-actin). F-Actin activation of MgATPase of cut S-1 is lower than that for normal S-1 at moderate concentrations of F-actin, as reported by Mornet et al. (1979). But as the F-actin concentration is increased, the MgATPase activities for cut S-1 approach those for uncut S-1. In terms of an eight-species steady-state kinetics scheme involving actin binding to free S-1, S-1 . ATP, S-1. ADP X P, and S-1 . ADP, actin affinity for the species S-1 . ADP X P was found to be 13.4 times greater for uncut S-1 than for cut S-1 [at 24 degrees C, pH 7.0, in 3 mM KC1, 1 mM ATP, 1 mM MgCl2, and 20 mM N-[tris(hydroxymethyl)methyl]-2-aminoethanesulfonic acid].     

Torsional motion of eosin-labeled F-actin as detected in the time-resolved anisotropy decay of the probe in the sub-millisecond time range

The internal motion of F-actin in the time range from 10(-6) to 10(-3) second has been explored by measuring the transient absorption anisotropy of eosin-labeled F-actin using laser flash photolysis. The transient absorption anisotropy of eosin-F-actin at 20 degrees C has a component that decays in the submicrosecond time scale to an anisotropy of about 0.3. This anisotropy then decays with a relaxation time of about 450 microseconds to a residual anisotropy of about 0.1 after 2 ms. When the concentration of eosin-F-actin was varied in the range from 7 to 28 microM, the transient absorption anisotropy curves obtained were almost indistinguishable from each other. These results show that the anisotropy decay arises from internal motion of eosin-F-actin. Analysis of the transient absorption anisotropy curves indicates that the internal motion detected by the decay in anisotropy is primarily a twisting of actin protomers in the F-actin helix; bending of the actin filament makes a minor contribution only to the measured decay. The torsional rigidity calculated from the transient absorption anisotropy is 0.2 X 10(-17) dyn cm2 at 20 degrees C, which is about an order of magnitude smaller than the flexural rigidity determined from previous studies. Thus, we conclude that F-actin is more flexible in twisting than in bending. The calculated root-mean-square fluctuation of the torsional angle between adjacent actin protomers in the actin helix is about 4 degrees at 20 degrees C. We also found that the torsional rigidity is approximately constant in the temperature range from 5 to approximately 35 degrees C, and that the binding of phalloidin does not appreciably affect the torsional motion of F-actin.     

Evidence for a gelsolin-rich, labile F-actin pool in human polymorphonuclear leukocytes.

Filamentous (F) actin is a major cytoskeletal element in polymorphonuclear leukocytes (PMNs) and other non-muscle cells. Exposure of PMNs to agonists causes polymerization of monomeric (G) actin to F-actin and activates motile responses. In vitro, all purified F-actin is identical. However, in vivo, the presence of multiple, diverse actin regulatory and binding proteins suggests that all F-actin within cells may not be identical. Typically, F-actin in cells is measured by either NBDphallacidin binding or as cytoskeletal associated actin in Triton-extracted cells. To determine whether the two measures of F-actin in PMNs, NBDphallacidin binding and cytoskeletal associated actin, are equivalent, a qualitative and quantitative comparison of the F-actin in basal, non-adherent endotoxin-free PMNs measured by both techniques was performed. F-actin as NBDphallacidin binding and cytoskeletal associated actin was measured in cells fixed with formaldehyde prior to cell lysis and fluorescent staining (PreFix), or in cells lysed with Triton prior to fixation (PostFix). By both techniques, F-actin in PreFix cells is higher than in PostFix cells (54.25 +/- 3.77 vs. 23.5 +/- 3.7 measured as mean fluorescent channel by NBDphallacidin binding and 70.3 +/- 3.5% vs. 47.2 +/- 3.6% of total cellular actin measured as cytoskeletal associated actin). These results show that in PMNs, Triton exposure releases a labile F-actin pool from basal cells while a stable F-actin pool is resistant to Triton exposure. Further characterizations of the distinct labile and stable F-actin pools utilizing NBDphallacidin binding, ultracentrifugation, and electron microscopy demonstrate the actin released with the labile pool is lost as filament. The subcellular localization of F-actin in the two pools is documented by fluorescent microscopy, while the distribution of the actin regulatory protein gelsolin is characterized by immunoblots with anti-gelsolin. Our studies show that at least two distinct F-actin pools coexist in endotoxin-free, basal PMNs in suspension: 1) a stable F-actin pool which is a minority of total cellular F-actin, Triton insoluble, resistant to depolymerization at 4 degrees C, gelsolin-poor, and localized to submembranous areas of the cell; and 2) a labile F-actin pool which is the majority of total cellular F-actin, Triton soluble, depolymerizes at 4 degrees C, is gelsolin-rich, and distributed diffusely throughout the cell. The results suggest that the two pools may subserve unique cytoskeletal functions within PMNs, and should be carefully considered in efforts to elucidate the mechanisms which regulate actin polymerization and depolymerization in non-muscle cells.     

Do the utrophin tandem calponin homology domains bind F-actin in a compact or extended conformation?

Tandem calponin-homology (CH) domains play an important role in the actin-binding function of many spectrin superfamily proteins. Crystal structures from several of these proteins have suggested a flexibility between these domains, and the manner in which these domains bind to F-actin has been the subject of some controversy. A recent paper has used electron microscopy and three-dimensional reconstruction to examine the complex of the utrophin tandem CH domain with F-actin. In contrast to our previously published study, a closed conformation of the two calponin-homology domains was suggested in the new work. We show here that the new results can be explained by incomplete binding of utrophin to actin, heterogeneity in the mode of binding, and angular disorder in F-actin. We conclude that helical averaging applied to disordered filaments is responsible for their results, and that approaches designed to separate out homogeneous subsets within such filamentous complexes offer many advantages.     

Yeast actin with a mutation in the "hydrophobic plug" between subdomains 3 and 4 (L266D) displays a cold-sensitive polymerization defect

Holmes et al. (Holmes, K. C., D. Popp, W. Gebhard, and W. Kabsch. 1990. Nature [Lond.] 347: 44-49) hypothesized that between subdomains 3 and 4 of actin is a loop of 10 amino acids including a four residue hydrophobic plug that inserts into a hydrophobic pocket formed by two adjacent monomers on the opposing strand thereby stabilizing the F- actin helix. To test this hypothesis we created a mutant yeast actin (L266D) by substituting Asp for Leu266 in the plug to disrupt this postulated hydrophobic interaction. Haploid cells expressing only this mutant actin were viable with no obvious altered phenotype at temperatures above 20 degrees C but were moderately cold-sensitive for growth compared with wild-type cells. The critical concentration for polymerization increased 10-fold at 4 degrees C compared with wild-type actin. The length of the nucleation phase of polymerization increased as the temperature decreased. At 4 degrees C nucleation was barely detectable. Addition of phalloidin-stabilized F-actin nuclei and phalloidin restored L266D actin''s ability to polymerize at 4 degrees C. This mutation also affects the overall rate of elongation during polymerization. Small effects of the mutation were observed on the exchange rate of ATP from G-actin, the G-actin intrinsic ATPase activity, and the activation of myosin S1 ATPase activity. Circular dichroism measurements showed a 15 degrees C decrease in melting temperature for the mutant actin from 57 degrees C to 42 degrees C. Our results are consistent with the model of Holmes et al. (Holmes, K. C., D. Popp, W. Gebhard, and W. Kabsch. 1990. Nature [Lond.]. 347:44-49) involving the role of the hydrophobic plug in actin filament stabilization.     

Heavy meromyosin induces sliding movements between antiparallel actin filaments

Suzuki et al. [Biochemistry 28, 6513-6518 (1989)] have shown that, when F-actin is mixed with inert high polymer, a large number of actin filaments closely align in parallel with overlaps to form a long and thick bundle. The bundle may be designated non-polar, as the constituent filaments are random in polarity (Suzuki et al. 1989). I prepared non-polar bundles of F-actin using methylcellulose (MC) as the high polymer, exposed them to heavy meromyosin (HMM) in the presence of ATP under a light microscope, and followed their morphological changes in the continuous presence of MC. It was found that bundles several tens of micrometers long contracted to about one-third the initial length, while becoming thicker, in half a minute after exposure to HMM. Subsequently, each bundle was split longitudinally into several bundles in a stepwise manner, while the newly formed ones remained associated together at one of the two ends. The product, an aster-like assembly of actin bundles, was morphologically quiescent; that is, individual bundles never contracted upon second exposure to HMM and ATP, although they were still longer than the F-actin used. Bundles in this state consisted of filaments with parallel polarity as examined by electron microscopy. This implies that non-polar bundles were transformed into assemblies of polar bundles with ATP hydrolysis by HMM. Importantly, myosin subfragment-1 caused neither contraction nor transformation. These results are interpreted as follows. In the presence of ATP, the two-headed HMM molecule was able to cross-bridge antiparallel actin filaments, as well as parallel ones.(ABSTRACT TRUNCATED AT 250 WORDS)     

Clearance of a Hirano body-like F-actin aggresome generated by jasplakinolide

We have reported in a variety of mammalian cells the reversible formation of a filamentous actin (F-actin)-enriched aggresome generated by the actin toxin jasplakinolide (Lázaro-Diéguez et al., J Cell Sci 2008; 121:1415-25). Notably, this F-actin aggresome (FAG) resembles in many aspects the pathological Hirano body, which frequently appears in some diseases such as Alzheimer's and alcoholism. Using selective inhibitors, we examined the molecular and subcellular mechanisms that participate in the clearance of the FAG. Chaperones, microtubules, proteasomes and autophagosomes all actively participate to eliminate the FAG. Here we compile and compare these results and discuss the involvement of each process. Because of its simplicity and high reproducibility, our cellular model could help to test pharmacological agents designed to interfere with the mechanisms involved in the clearance of intracellular bodies and, in particular, of those enriched in F-actin.     

Properties of two isoforms of human blood platelet alpha-actinin

The structural and functional properties of the aa (2 X 97 kDa) and cc (2 X 94 kDa) isoforms of platelet alpha-actinin have been compared. Structural differences between aa and cc are revealed by their peptide maps, obtained from limited proteolysis, and by their immunological cross-reactivity. Both isoforms stimulate the Mg ATPase activity of actomyosin, bind to F-actin (high-speed sedimentation) and cross-link or gel actin filaments (low-speed sedimentation and viscometry), in a calcium-dependent manner. The study of the interaction with F-actin indicates that the binding of 1 molecule of aa or cc alpha-actinin/9-11 actin monomers is sufficient to produce maximal gelation in the presence of EGTA. CaCl2 at 0.1 mM strongly inhibits the binding of aa to F-actin and weakly that of cc, while it inhibits similarly the cross-linking of either aa or cc. The cross-linking efficiency of cc is 9, 7, 1.7 and 1.3 times higher than that of aa at 4, 20, 30 and 37 degrees C, respectively. The bb form (2 X 96 kDa), which is a proteolytic product of aa [Y. Gache et al. (1984) Biochem. Biophys. Res. Commun. 124, 877-881], behaves roughly as aa, but the calcium sensitivity of its binding to F-actin is intermediate between that of aa and cc. These results suggest that the effect of Ca2+ concentration on the binding of platelet alpha-actinin to F-actin may be partly dissociated from the effect on the cross-linking.     

Cdc42-dependent actin polymerization during compensatory endocytosis in Xenopus eggs

The actin filament (F-actin) cytoskeleton associates dynamically with the plasma membrane and is thus ideally positioned to participate in endocytosis. Indeed, a wealth of genetic and biochemical evidence has confirmed that actin interacts with components of the endocytic machinery, although its precise function in endocytosis remains unclear. Here, we use 4D microscopy to visualize the contribution of actin during compensatory endocytosis in Xenopus laevis eggs. We show that the actin cytoskeleton maintains exocytosing cortical granules as discrete invaginated compartments, such that when actin is disrupted, they collapse into the plasma membrane. Invaginated, exocytosing cortical granule compartments are directly retrieved from the plasma membrane by F-actin coats that assemble on their surface. These dynamic F-actin coats seem to drive closure of the exocytic fusion pores and ultimately compress the cortical granule compartments. Active Cdc42 and N-WASP are recruited to exocytosing cortical granule membranes before F-actin coat assembly and coats assemble by Cdc42-dependent, de novo actin polymerization. Thus, F-actin may power fusion pore resealing and function in two novel endocytic capacities: the maintenance of invaginated compartments and the processing of endosomes.     

Filamentous actin is a substrate for protealysin, a metalloprotease of invasive Serratia proteamaculans

Homologous bacterial metalloproteases ECP32/grimelysin from Serratia grimesii and protealysin from Serratia proteamaculans are involved in the invasion of the nonpathogenic bacteria in eukaryotic cells and are suggested to translocate into the cytoplasm [Bozhokina ES et al. (2011) Cell Biol Int35, 111-118]. The proteases have been characterized as actin-hydrolyzing enzymes with a narrow specificity toward intact cell proteins. However, cleavage of filamentous actin (F-actin) (i.e. the main actin species in the cell) and the properties of the cleaved F-actin have not been investigated previously. In the present study, we revealed the presence of protealysin in the cytoplasm of 3T3-SV40 cells infected with S. proteamaculans or recombinant Escherichia coli expressing the protealysin gene. We also show for the first time that purified protealysin and the lysates of the recombinant E. coli producing protealysin cleave 20-40% of F-actin. Cleavage limited predominantly to the bond Gly42-Val43 efficiently increases the steady-state ATPase activity (dynamics) of F-actin. abolishes this effect and promotes the nucleation of protealysin-cleaved Mg-globular-actin even in the absence of 0.1 m KCl, most likely as a result of the stabilization of lateral intermonomer contacts of actin subunits. The results obtained in the present study suggest that F-actin can be a target for protealysin upon its translocation into the host cell.     

The experimental basis of some recent hypotheses on the mechanism of the polymerization of actin: a reappraisal

We have studied the effect of sonication on the fluorescence of N-(1-pyrenyl)iodoacetamide-labeled F-actin as well as of native actin-pyrenyl-actin mixed oligomers in which the subunits were covalently attached to each other by phenylenebismaleimide. In both cases the fluorescence of the solution was largely decreased by sonication. We have found that this effect is due (a) to a 20-30% decrease of the specific fluorescence of the polymers. These results question the validity of the novel mechanism for the polymerization of actin recently proposed (D. Pantaloni et al. (1984) J. Biol. Chem. 259, 6274-6283). In these studies, in fact, the implicit assumption was made that the quenching of the fluorescence of the solution under sonication was due exclusively to the conversion of F-actin into G-actin.     

Compartmentalization and actin binding properties of ABP-50: the elongation factor-1 alpha of Dictyostelium.

ABP-50 is the elongation factor-1 alpha (EF-1 alpha) of Dictyostelium discoideum (Yang et al.: Nature 347:494-496, 1990). ABP-50 is also an actin filament binding and bundling protein (Demma et al.: J. Biol. Chem. 265:2286-2291, 1990). In the present study we have investigated the compartmentalization of ABP-50 in both resting and stimulated cells. Immunofluorescence microscopy shows that in addition to being colocalized with F-actin in surface extensions in unstimulated cells, ABP-50 exhibits a diffuse distribution throughout the cytosol. Upon addition of cAMP, a chemoattractant, ABP-50 becomes localized in the filopodia that are extended as a response to stimulation. Quantification of ABP-50 in Triton-insoluble and -soluble fractions of resting cells indicates that 10% of the total ABP-50 is recovered in the Triton cytoskeleton, while the remainder is in the soluble cytosolic fraction. Stimulation with cAMP increases the incorporation of ABP-50 into the Triton cytoskeleton. The peak of incorporation of ABP-50 at 90 sec is concomitant with filopod extension. Immunoprecipitation of the cytosolic ABP-50 from unstimulated cells using affinity-purified polyclonal anti ABP-50 results in the coprecipitation of non-filamentous actin with ABP-50. Purified ABP-50 binds to G-actin with a Kd of approximately 0.09 microM. The interaction between ABP-50 and G-actin is inhibited by GTP but not by GDP, while the bundling of F-actin by ABP-50 is unaffected by guanine nucleotides. We conclude that a significant amount of ABP-50 is bound to either G- or F-actin in vivo and that the interaction between ABP-50 and F-actin in the cytoskeleton is regulated by chemotactic stimulation.     

Two opposite effects of cofilin on the thermal unfolding of F-actin: a differential scanning calorimetric study

Differential scanning calorimetry was used to examine the effects of cofilin on the thermal unfolding of actin. Stoichiometric binding increases the thermal stability of both G- and F-actin but at sub-saturating concentrations cofilin destabilizes F-actin. At actin:cofilin molar ratios of 1.5-6 the peaks corresponding to stabilized (66-67 degrees C) and destabilized (56-57 degrees C) F-actin are observed simultaneously in the same thermogram. Destabilizing effects of sub-saturating cofilin are highly cooperative and are observed at actin:cofilin molar ratios as low as 100:1. These effects are abolished by the addition of phalloidin or aluminum fluoride. Conversely, at saturating concentrations, cofilin prevents the stabilizing effects of phalloidin and aluminum fluoride on the F-actin thermal unfolding. These results suggest that cofilin stabilizes those actin subunits to which it directly binds, but destabilizes F-actin with a high cooperativity in neighboring cofilin-free regions.     

Expression of the 53 kD forked protein rescues F-actin bundle formation and mutant bristle phenotypes in Drosophila.

forked mutations affect bristle development in Drosophila pupae, resulting in short, thick, gnarled bristles in the adult. The forked proteins are components of 200-300-microm-long actin fiber bundles that are present transiently during pupal development [Petersen et al., 1994: Genetics 136:173-182]. These bundles are composed of segments of 3-10 microm long, and forked protein is localized along the actin fiber bundle segments and accumulates at the junctions connecting them longitudinally. In the forked mutants, f(36a) and f(hd), F-actin bundles are greatly reduced in number and size, and bundle segmentation is absent. The p-element, P[w(+), falter] contains a 5.3-kb fragment of the forked gene that encodes the 53-kD forked protein [Lankenau et al., 1996: Mol Cell Biol 16:3535-3544]. Expression of only the 53-kD forked protein is sufficient to rescue the actin bundle and bristle phenotypes of f(36a) and f(hd) mutant flies. The 5.3-kb forked sequence, although smaller than the 13-kb region previously shown to rescue forked mutants [Petersen et al., 1994: Genetics 136:173-182], does contain the core forked sequence that encodes actin binding and bundling domains in cultured mammalian cells [Grieshaber and Petersen, 1999: J Cell Sci 112:2203-2211]. These data show that the 53-kD forked protein is sufficient for normal bristle development and that the domains shown previously to be important for actin bundling in cell culture may be all that are required for normal actin bundle formation in developing Drosophila bristles.     

Nucleotide exchange between cytosolic ATP and F-actin-bound ADP may be a major energy-utilizing process in unstimulated platelets

About 40% of the cytosolic ADP of human platelets is tightly bound to protein and the complex is precipitated from the cells by 43% ethanol. We show here that this ADP is bound to F-actin by three criteria (a) copurification with F-actin, (b) specific extraction with water and (c) by specific interaction with DNase I. Platelets contain 0.3 mumol/10(11) cells of this F-actin--ADP complex compared to the total actin content of 0.8 mumol/10(11) cells, which is consistent with the view that actin is maintained in different pools (F-actin--ADP, profilactin, G-actin). In intact platelets the F-actin-bound ADP turns over rapidly and we have determined a turnover rate at 37 degrees C of 0.1 +/- 0.025 s-1 by using a double-labelling procedure. This rapid turnover indicates that F-actin in intact platelets is in a very dynamic state, which may be necessary for rapid responses to stimuli. If it is assumed that the source of the ADP bound to F-actin is cytosolic ATP, the turnover of F-actin ADP measured represents an ATP-consuming process that would account for up to 50% of total ATP consumption in resting platelets.     

Modulation of actin mechanics by caldesmon and tropomyosin

The ability of cells to sense and respond to physiological forces relies on the actin cytoskeleton, a dynamic structure that can directly convert forces into biochemical signals. Because of the association of muscle actin-binding proteins (ABPs) may affect F-actin and hence cytoskeleton mechanics, we investigated the effects of several ABPs on the mechanical properties of the actin filaments. The structural interactions between ABPs and helical actin filaments can vary between interstrand interactions that bridge azimuthally adjacent actin monomers between filament strands (i.e. by molecular stapling as proposed for caldesmon) or, intrastrand interactions that reinforce axially adjacent actin monomers along strands (i.e. as in the interaction of tropomyosin with actin). Here, we analyzed thermally driven fluctuations in actin's shape to measure the flexural rigidity of actin filaments with different ABPs bound. We show that the binding of phalloidin increases the persistence length of actin by 1.9-fold. Similarly, the intrastrand reinforcement by smooth and skeletal muscle tropomyosins increases the persistence length 1.5- and 2- fold respectively. We also show that the interstrand crosslinking by the C-terminal actin-binding fragment of caldesmon, H32K, increases persistence length by 1.6-fold. While still remaining bound to actin, phosphorylation of H32K by ERK abolishes the molecular staple (Foster et al. 2004. J Biol Chem 279;53387-53394) and reduces filament rigidity to that of actin with no ABPs bound. Lastly, we show that the effect of binding both smooth muscle tropomyosin and H32K is not additive. The combination of structural and mechanical studies on ABP-actin interactions will help provide information about the biophysical mechanism of force transduction in cells.     

Three-dimensional image reconstruction of insect flight muscle. II. The rigor actin layer

The averaged structure of rigor cross-bridges in insect flight muscle is further revealed by three-dimensional reconstruction from 25-nm sections containing a single layer of thin filaments. These exhibit two thin filament orientations that differ by 60 degrees from each other and from myac layer filaments. Data from multiple tilt views (to +/- 60 degrees) was supplemented by data from thick sections (equivalent to 90 degrees tilts). In combination with the reconstruction from the myac layer (Taylor et al., 1989), the entire unit cell is reconstructed, giving the most complete view of in situ cross-bridges yet obtained. All our reconstructions show two classes of averaged rigor cross-bridges. Lead bridges have a triangular shape with leading edge angled at approximately 45 degrees and trailing edge angled at approximately 90 degrees to the filament axis. We propose that the lead bridge contains two myosin heads of differing conformation bound along one strand of F-actin. The lead bridge is associated with a region of the thin filament that is apparently untwisted. We suggest that the untwisting may reflect the distribution of strain between myosin and actin resulting from two-headed, single filament binding in the lead bridge. Rear bridges are oriented at approximately 90 degrees to the filament axis, and are smaller and more cylindrical, suggesting that they consist of single myosin heads. The rear bridge is associated with a region of apparently normal thin filament twist. We propose that differing myosin head angles and conformations consistently observed in rigor embody different stages of the power stroke which have been trapped by a temporal sequence of rigor cross-bridge formation under the constraints of the intact filament lattice.