Fluorescence energy transfer between Cys-10 residues in F-actin filaments

Fluorescence energy transfer was measured between Cys-10 residues in an F-actin filament using 5-[2-((iodoacetyl)amino)-ethyl]aminonaphthalene-1-sulphonic acid (1,5-IAEDANS) as a fluorescence energy donor and 4-dimethylaminophenylazophenyl-4'-maleimide (DABMI) as the acceptor. Both labels were covalently attached to Cys-10 residues in an F-actin filament. Taking the helical structure of the F-actin filament into consideration, the radial coordinate of Cys-10 was calculated to be 23 A. This corresponds to a distance between adjacent sites along the long pitch helix of 56.1 A and along the genetic helix of 53.3 A.     

The structure of the C-terminal actin-binding domain of talin

Talin is a large dimeric protein that couples integrins to cytoskeletal actin. Here, we report the structure of the C-terminal actin-binding domain of talin, the core of which is a five-helix bundle linked to a C-terminal helix responsible for dimerisation. The NMR structure of the bundle reveals a conserved surface-exposed hydrophobic patch surrounded by positively charged groups. We have mapped the actin-binding site to this surface and shown that helix 1 on the opposite side of the bundle negatively regulates actin binding. The crystal structure of the dimerisation helix reveals an antiparallel coiled-coil with conserved residues clustered on the solvent-exposed face. Mutagenesis shows that dimerisation is essential for filamentous actin (F-actin) binding and indicates that the dimerisation helix itself contributes to binding. We have used these structures together with small angle X-ray scattering to derive a model of the entire domain. Electron microscopy provides direct evidence for binding of the dimer to F-actin and indicates that it binds to three monomers along the long-pitch helix of the actin filament.     

Binding mode of cytochalasin B to F-actin is altered by lateral binding of regulatory proteins

The binding of cytochalasin B (CB) to F-actin was studied using a trace amount of [3H]-cytochalasin B. F-Actin-bound CB was separated from free CB by ultracentrifugation and the amount of F-actin-bound CB was determined by comparing the radioactivity both in the supernatant and in the precipitate. A filament of pure F-actin possessed one high-affinity binding site for CB (Kd = 5.0 nM) at the B-end. When the filament was bound to native tropomyosin (complex of tropomyosin and troponin), two low-affinity binding sites for CB (Kd = 230 nM) were created, while the high-affinity binding site was reserved (Kd = 3.4 nM). It was concluded that the creation of low-affinity binding sites was primarily due to binding of tropomyosin to F-actin, as judged from the following two observations: (1) a filament of F-actin/tropomyosin complex possessed one high-affinity binding site (Kd = 3.9 nM) plus two low-affinity binding sites (Kd = 550 nM); (2) the Ca2(+)-receptive state of troponin C in F-actin/native tropomyosin complex did not affect CB binding.     

Cardiomyopathy Mutation Alters End-to-End Junction of Tropomyosin and Reduces Calcium Sensitivity

Muscle contraction is governed by tropomyosin (Tpm) shifting azimuthally between three states on F-actin (B-, C-, and M-states) in response to calcium binding to troponin and actomyosin cross-bridge formation. The Tpm coiled coil polymerizes head to tail along the long-pitch helix of F-actin to form continuous superhelical cables that wrap around the actin filaments. The end-to-end bonds formed between the N- and C-terminus of adjacent Tpm molecules define Tpm continuity and play a critical role in the ability of Tpm to cooperatively bind to actin, thus facilitating Tpm conformational switching to cooperatively propagate along F-actin. We expect that a missense mutation in this critical overlap region associated with dilated cardiomyopathy, A277V, will alter Tpm binding and thin filament activation by altering the overlap structure. Here, we used cosedimentation assays and in vitro motility assays to determine how the mutation alters Tpm binding to actin and its ability to regulate actomyosin interactions. Analytical viscometry coupled with molecular dynamics simulations showed that the A277V mutation results in enhanced Tpm end-to-end bond strength and a reduced curvature of the Tpm overlap domain. The mutant Tpm exhibited enhanced actin-Tpm binding affinity, consistent with overlap stabilization. The observed A277V-induced decrease in cooperative activation observed with regulated thin filament motility indicates that increased overlap stabilization is not correlated with Tpm-Tpm overlap binding strength or mechanical rigidity as is often assumed. Instead, A277V-induced structural changes result in local and delocalized increases in Tpm flexibility and prominent coiled-coil twisting in pseudorepeat 4. An A277V-induced decrease in Ca²⁺ sensitivity, consistent with a mutation-induced bolstering of the B-state Tpm-actin electrostatic contacts and an increased Tpm troponin T1 binding affinity, was also observed.     

Synthesis of nonlinear DNA-binding peptide with binding specificity determinants close to those of 434 Cro-repressor

Design, synthesis and DNA binding activity of a nonlinear 102 residue peptide are reported. The peptide contains four sequence-specific DNA binding domains of 434 Cro protein. These four domains were linked covalently to a symmetrical carboxyterminal crosslinker that contains four arms each ending with an aliphatic aminogroup. From CD studies we have found that in aqueous buffer in the presence of 20% trifluoroethanol the peptide residues assume alpha helical, beta-sheet and random coiled conformations with an alpha helical content of about 16% at room temperature. The alpha helicity is increased up to 40% in the presence of 40% trifluoroethanol. Upon complex formation between the peptide and DNA a change in the peptide conformation takes place which is consistent with an alpha-beta transition in the DNA binding, helix-turn-helix motif of 434 Cro repressor. Evidently residues present in helices alpha(2) and alpha(3) form a beta hairpin which is inserted in the minor DNA groove. The latter inference is supported by our observations that the peptide can displace minor groove binding antibiotic distamycin A from a complex with poly(dA).poly(dT). As revealed from DNase protection studies the peptide exhibits preferences for binding to operator and pseudooperator sites recognized by 434 Cro repressor. It binds strongly to operator sites OR1, OR2 and OR3 and exhibits a greater affinity for pseudooperator site Op1. From analysis of nucleotide sequences in the strong affinity binding sites for the peptide on DNA a conclusion is drawn that it binds to pseudosymmetrical nucleotide sequences 5'-ACAA(W)nCTGT-3', where W is an arbitrary nucleotide. n is equal to six or seven. In the strongest affinity binding site for the peptide on DNA (Op1) motif 5'-ACAA-3' is replaced by sequence 5'-ACCA-3'. A difference in binding specificity shown by the peptide and 434 Cro protein could be attributed to a flexibility of the connecting chains between DNA-binding domains in the peptide molecule as well as to a replacement of Thr - Ala in the alpha 2 helix. Removal of two residues from the N-terminal end of helix alpha 2 in each of the four DNA binding domains of 434 Cro present in the peptide leads to a loss of binding specificity, although the modified peptide binds to DNA unspecifically.     

Structural mapping of chloroplast coupling factor

Fluorescence resonance energy transfer measurements have been used to investigate the spatial relationships between the nucleotide binding sites and the gamma-subunit of the H+-ATPase from chloroplasts and the orientation of these sites with respect to the membrane surface. Fluorescent maleimides reacted covalently at specific sulfhydryl sites on the gamma-subunit served as energy donors. One sulfhydryl site can be labeled only under energized conditions on the thylakoid membrane surface (light site). The two gamma-sulfhydryls exposed after catalytic activation served as a second donor site (disulfide site). In one set of experiments, the nucleotide analogue 2'(3')-(trinitrophenyl)adenosine triphosphate, selectively bound at each of the three nucleotide binding sites of the solubilized coupling factor, was used as an energy acceptor; in another, octadecylrhodamine with its acyl chain inserted in the vesicle bilayer and the rhodamine fluorophore exposed along the membrane surface was the energy acceptor. The distance between the sulfhydryl and disulfide sites was also obtained by sequentially labeling the sites with coumarin (donor) and fluorescein (acceptor) maleimide derivatives, respectively. The results indicate that all three nucleotide sites are approximately equal to 50 A from the light-labeled gamma-sulfhydryl. Two of the nucleotide sites are very far from the gamma-disulfide (greater than 74 A), while the third site, which binds nucleotides reversibly under all conditions, is 62 A from this sulfhydryl. The light-labeled sulfhydryl and disulfide sites are about 42-47 A apart. Finally, the distance of closest approach between the membrane surface of the reconstituted system and the gamma-disulfide is 31 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structural mapping of nucleotide binding sites on chloroplast coupling factor

Fluorescence resonance energy transfer was used to measure the distances between three nucleotide binding sites on solubilized chloroplast coupling factor from spinach and between each nucleotide site and two tyrosine residues which are important for catalytic activity. The nucleotide energy donor was 1,N6-ethenoadenosine di- or triphosphate, and the nucleotide energy acceptor was 2'(3')-(trinitrophenyl)adenosine diphosphate. The tyrosine residues were specifically labeled with 7-chloro-4-nitro-2,1,3-benzoxadiazole, which served as an energy acceptor. The results obtained indicate the three nucleotide binding sites form a triangle with sides of 44, 48, and 36 A. (The assumption has been made in calculating these distances that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime.) Two of the nucleotide sites are approximately equidistant from each of the two tyrosines: one of the nucleotide sites is about 37 A and the other about 41 A from each tyrosine. The third nucleotide site is about 41 A from one of the tyrosines and greater than or equal to 41 A from the other tyrosine.     

Bundling of actin filaments by alpha-actinin depends on its molecular length

Cross-linking of actin filaments (F-actin) into bundles and networks was investigated with three different isoforms of the dumbbell-shaped alpha-actinin homodimer under identical reaction conditions. These were isolated from chicken gizzard smooth muscle, Acanthamoeba, and Dictyostelium, respectively. Examination in the electron microscope revealed that each isoform was able to cross-link F-actin into networks. In addition, F-actin bundles were obtained with chicken gizzard and Acanthamoeba alpha-actinin, but not Dictyostelium alpha-actinin under conditions where actin by itself polymerized into disperse filaments. This F-actin bundle formation critically depended on the proper molar ratio of alpha-actinin to actin, and hence F-actin bundles immediately disappeared when free alpha-actinin was withdrawn from the surrounding medium. The apparent dissociation constants (Kds) at half-saturation of the actin binding sites were 0.4 microM at 22 degrees C and 1.2 microM at 37 degrees C for chicken gizzard, and 2.7 microM at 22 degrees C for both Acanthamoeba and Dictyostelium alpha-actinin. Chicken gizzard and Dictyostelium alpha-actinin predominantly cross-linked actin filaments in an antiparallel fashion, whereas Acanthamoeba alpha-actinin cross-linked actin filaments preferentially in a parallel fashion. The average molecular length of free alpha-actinin was 37 nm for glycerol-sprayed/rotary metal-shadowed and 35 nm for negatively stained chicken gizzard; 46 and 44 nm, respectively, for Acanthamoeba; and 34 and 31 nm, respectively, for Dictyostelium alpha-actinin. In negatively stained preparations we also evaluated the average molecular length of alpha-actinin when bound to actin filaments: 36 nm for chicken gizzard and 35 nm for Acanthamoeba alpha-actinin, a molecular length roughly coinciding with the crossover repeat of the two-stranded F-actin helix (i.e., 36 nm), but only 28 nm for Dictyostelium alpha-actinin. Furthermore, the minimal spacing between cross-linking alpha-actinin molecules along actin filaments was close to 36 nm for both smooth muscle and Acanthamoeba alpha-actinin, but only 31 nm for Dictyostelium alpha-actinin. This observation suggests that the molecular length of the alpha-actinin homodimer may determine its spacing along the actin filament, and hence F-actin bundle formation may require "tight" (i.e., one molecule after the other) and "untwisted" (i.e., the long axis of the molecule being parallel to the actin filament axis) packing of alpha-actinin molecules along the actin filaments.     

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

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

Effect of tropomyosin on the interactions of actin with actin-binding proteins isolated from pig platelets

Several non-muscle tropomyosins have been reported to lack the ability to polymerize in a head-to-tail manner [Dabrowska, R. et al. (1983) J. Muscle Res. Cell Motil. 1, 83-92; C?té, G.P. (1983) Mol. Cell. Biochem. 57, 127-146]. Unlike rabbit skeletal muscle tropomyosin, these proteins could therefore not protect the F-actin microfilaments neither from disassembly or from cross-linking by the other actin-associating factors. However, we have provided evidence that, in vitro, pig platelet tropomyosin, although shorter in molecular length, exhibits the same properties as the muscle protein: it self-associates and forms a 1:6 complex with platelet filamentous actin under physiological conditions [Prulière et al. (1984) J. Muscle Res. Cell Motil. 6, 126]. In this paper, we examine the effects of several other actin-binding proteins on the microfilaments saturated with this non-muscle tropomyosin. Since contractile proteins often vary with the cell type and may require different conditions for their interactions, we have developed a procedure which allows the parallel purification of actin-binding protein (ABP), vinculin, alpha-actinin, gelsolin as well as actin and tropomyosin from the same batch of cells. Thus, using an homogeneous system, we show by viscometry, sedimentation and densitometry, and by electron microscopy, that pig platelet tropomyosin can protect the structure of the microfilaments from the action of the modulating factors to the same extent as rabbit skeletal muscle alpha-tropomyosin. Our data suggest that interaction of ABP, vinculin or alpha-actinin can occur only with the ends of the filaments when F-actin is saturated with tropomyosin, while cross-linking takes place by interactions with sites localized along the entire length of F-actin in the absence of tropomyosin. Moreover, the presence of tropomyosin on F-actin leads to the total inhibition of gelsolin severing activity, although it did not prevent the binding of gelsolin to the F-actin--tropomyosin complex. This suggests that pig platelet as well as skeletal muscle tropomyosins have the ability to increase the strength of the interaction between actin monomers within the filament. This also suggests that the binding sites of gelsolin along the filaments are not localized in the groove of the F-actin helix.     

Small-angle diffuse x-ray scattering on fine muscle filaments

Theoretical small-angle diffuse scattering curves from muscle thin filament models have been calculated. The curves reveal a maximum at 115' scattering angle. It has been shown that the maximum is due to the pitch of F-actin helix. Theoretical curves are in good agreement with the earlier obtained curves of small-angle diffuse scattering from F-actin dilute solutions.     

Effect of ethanol on tropomyosin in solution and in reconstituted thin filaments

The effects of ethanol at concentrations below 10% on the conformation of tropomyosin, its end-to-end polymerization, its binding to F-actin, and its effects on actomyosin ATPase activity were studied. Ethanol stabilized the tropomyosin conformation by shifting the helix thermal unfolding profile to higher temperatures, and increased the end-to-end polymerization of tropomyosin. Ethanol-induced changes in the excimer fluorescence of pyrene-tropomyosin indicated that its conformation was stabilized by ethanol both free and bound to F-actin. Effects of tropomyosin and tropomyosin-troponin on actomyosin ATPase activity were measured under conditions for which tropomyosin binding to F-actin increases the activity. Under conditions for which the binding of tropomyosin to F-actin is optimum, in the presence of tropomyosin, the actomyosin ATPase activity decreased as the ethanol concentration increased, further indicating that ethanol induces a structural change in the tropomyosin-F-actin complex. Under conditions for which the binding of tropomyosin to F-actin is weak (low salt or high temperature), addition of ethanol increased the ATPase activity due to increased binding of tropomyosin to F-actin. Thus, ethanol appears to modify actomyosin ATPase activity by increasing the binding of tropomyosin to F-actin and affecting the structure of tropomyosin in the tropomyosin-F-actin filament.     

A three-dimensional FRET analysis to construct an atomic model of the actin-tropomyosin complex on a reconstituted thin filament

Fluorescence resonance energy transfer (FRET) was used to construct an atomic model of the actin–tropomyosin (Tm) complex on a reconstituted thin filament. We generated five single-cysteine mutants in the 146–174 region of rabbit skeletal muscle α-Tm. An energy donor probe was attached to a single-cysteine Tm residue, while an energy acceptor probe was located in actin Gln41, actin Cys374, or the actin nucleotide binding site. From these donor–acceptor pairs, FRET efficiencies were determined with and without Ca²⁺. Using the atomic coordinates for F-actin and Tm, we searched all possible arrangements for Tm segment 146–174 on F-actin to calculate the FRET efficiency for each donor–acceptor pair in each arrangement. By minimizing the squared sum of deviations for the calculated FRET efficiencies from the observed FRET efficiencies, we determined the location of the Tm segment on the F-actin filament. Furthermore, we generated a set of five single-cysteine mutants in each of the four Tm regions 41–69, 83–111, 216–244, and 252–279. Using the same procedures, we determined each segment's location on the F-actin filament. In the best-fit model, Tm runs along actin residues 217–236, which were reported to compose the Tm binding site. Electrostatic, hydrogen-bonding, and hydrophobic interactions are involved in actin and Tm binding. The C-terminal region of Tm was observed to contact actin more closely than did the N-terminal region. Tm contacts more residues on actin without Ca²⁺ than with it. Ca²⁺-induced changes on the actin–Tm contact surface strongly affect the F-actin structure, which is important for muscle regulation.     

Titin-actin interaction in mouse myocardium: passive tension modulation and its regulation by calcium/S100A1

Passive tension in striated muscles derives primarily from the extension of the giant protein titin. However, several studies have suggested that, in cardiac muscle, interactions between titin and actin might also contribute to passive tension. We expressed recombinant fragments representing the subdomains of the extensible region of cardiac N2B titin (tandem-Ig segments, the N2B splice element, and the PEVK domain), and assayed them for binding to F-actin. The PEVK fragment bound F-actin, but no binding was detected for the other fragments. Comparison with a skeletal muscle PEVK fragment revealed that only the cardiac PEVK binds actin at physiological ionic strengths. The significance of PEVK-actin interaction was investigated using in vitro motility and single-myocyte mechanics. As F-actin slid relative to titin in the motility assay, a dynamic interaction between the PEVK domain and F-actin retarded filament sliding. Myocyte results suggest that a similar interaction makes a significant contribution to the passive tension. We also investigated the effect of calcium on PEVK-actin interaction. Although calcium alone had no effect, S100A1, a soluble calcium-binding protein found at high concentrations in the myocardium, inhibited PEVK-actin interaction in a calcium-dependent manner. Gel overlay analysis revealed that S100A1 bound the PEVK region in vitro in a calcium-dependent manner, and S100A1 binding was observed at several sites along titin's extensible region in situ, including the PEVK domain. In vitro motility results indicate that S100A1-PEVK interaction reduces the force that arises as F-actin slides relative to the PEVK domain, and we speculate that S100A1 may provide a mechanism to free the thin filament from titin and reduce titin-based tension before active contraction.     

Position and orientation of phalloidin in F-actin determined by X-ray fiber diffraction analysis

Knowledge of the phalloidin binding position in F-actin and the relevant understanding of the mechanism of F-actin stabilization would help to define the structural characteristics of the F-actin filament. To determine the position of bound phalloidin experimentally, x-ray fiber diffraction data were obtained from well-oriented sols of F-actin and the phalloidin-F-actin complex. The differences in the layer-line intensity distributions, which were clearly observed even at low resolution (8 A), produced well-resolved peaks corresponding to interphalloidin vectors in the cylindrically averaged difference-Patterson map, from which the radial binding position was determined to be approximately 10 A from the filament axis. Then, the azimuthal and axial positions were determined by single isomorphous replacement phasing and a cross-Patterson map in radial projection to be approximately 84 degrees and 0.5 A relative to the actin mass center. The refined position was close to the position found by prior researchers. The position of rhodamine attached to phalloidin in the rhodamine-phalloidin-F-actin complex was also determined, in which the conjugated Leu(OH)(7) residue was found to face the outside of the filament. The position and orientation of the bound phalloidin so determined explain the increase in the interactions between long-pitch strands of F-actin and would also account for the inhibition of phosphate release, which might also contribute to the F-actin stabilization. The method of analysis developed in this study is applicable for the determination of binding positions of other drugs, such as jasplakinolide and dolastatin 11.     

Proton nuclear magnetic resonance and electron paramagnetic resonance studies on skeletal muscle actin indicate that the metal and nucleotide binding sites are separate

The distance separating the high-affinity binding sites of actin for a divalent metal ion and nucleotide was evaluated by using high-resolution proton NMR and EPR spectroscopy. Replacement of the Ca2+ or Mg2+ bound to the high-affinity divalent cation site of G-actin by trivalent lanthanide ions such as La3+, EU3+, or Gd3+ results in an increase in the mobility of the bound ATP as observed in the NMR spectra of G-actin monomers. Little difference was observed between the spectra obtained in the presence of the diamagnetic La3+ control and the paramagnetic ions Eu3+ and Gd3+ which respectively shift and broaden the proton resonances of amino acids in the vicinity of the binding site. Analysis of the NMR spectra indicates that the metal and nucleotide binding sites are separated by a distance of at least 16 A. In the past, the metal and ATP have been widely assumed to bind as a complex. Further verification that the two sites on actin are physically separated was obtained by using an ATP analogue with a nitroxide spin-label bound at the 6' position of the purine ring. An estimate of the distance was made between the site containing the ATP analogue and the paramagnetic ion, Mn2+, bound to the cation binding site. These EPR experiments were not affected by the state of polymerization of the actin. The data obtained by using this technique support the conclusion stated above, namely, that the cation and nucleotide sites on either G- or F-actin are well separated.     

Two distinct regions of calponin share common binding sites on actin resulting in different modes of calponin–actin interaction

Calponins are a small family of proteins that alter the interaction between actin and myosin II and mediate signal transduction. These proteins bind F-actin in a complex manner that depends on a variety of parameters such as stoichiometry and ionic strength. Calponin binds G-actin and F-actin, bundling the latter primarily through two distinct and adjacent binding sites (ABS1 and ABS2). Calponin binds other proteins that bind F-actin and considerable disagreements exist as to how calponin is located on the filament, especially in the presence of other proteins. A study (Galkin, V.E., Orlova, A., Fattoum, A., Walsh, M.P. and Egelman, E.H. (2006) J. Mol. Biol. 359, 478–485.), using EM single-particle reconstruction has shown that there may be four modes of interaction, but how these occur is not yet known. We report that two distinct regions of calponin are capable of binding some of the same sites on actin (such as 18–28 and 360–372 in subdomain 1). This accounts for the finding that calponin binds the filament with different apparent geometries. We suggest that the four modes of filament binding account for differences in stoichiometry and that these, in turn, arise from differential binding of the two calponin regions to actin. It is likely that the modes of binding are reciprocally influenced by other actin-binding proteins since members of the α-actinin group also adopt different actin-binding positions and bind actin principally through a domain that is similar to calponin's ABS1.     

Each actin subunit has three nebulin binding sites: implications for steric blocking

Nebulin is a giant protein that spans most of the muscle thin filament. Mutations in nebulin result in myopathies and dystrophies. Nebulin contains approximately 200 copies of approximately 35 residue modules, each believed to contain an actin binding site, organized into seven-module superrepeats. The strong correlation between the number of nebulin modules and the length of skeletal muscle thin filaments in different species suggests that nebulin determines thin filament length. Little information exists about the interactions between intact nebulin and F-actin. More insight has come from working with fragments of nebulin, containing from one to hundreds of actin binding modules. However, the observed stoichiometry of binding between these fragments and actin has ranged from 0.4 to 13 modules per actin subunit. We have used electron microscopy and a novel method of helical image analysis to characterize complexes of F-actin with a nebulin fragment. The fragment binds as an extended structure spanning three actin subunits and binding to different sites on each actin. Muscle regulation involves tropomyosin movement on the surface of actin, with binding in three states. Our results suggest the intriguing possibility that intact nebulin may also be able to occupy three different sites on F-actin.     

Mapping the functional surface of domain 2 in the gelsolin superfamily

The crystal structure of the F-actin binding domain 2 of severin, the gelsolin homologue from Dictyostelium discoideum, has been determined by multiple isomorphous replacement and refined to 1.75 A resolution. The structure reveals an alpha-helix-beta-sheet sandwich similar to the domains of gelsolin and villin, and contains two cation-binding sites, as observed in other domain 1 and domain 2 homologues. Comparison of the structures of several gelsolin family domains has identified residues that may mediate F-actin binding in gelsolin domain 2 homologues. To assess the involvement of these residues in F-actin binding, three mutants of human gelsolin domain 2 were assayed for F-actin binding activity and thermodynamic stability. Two of the mutants, RRV168AAA and RLK210AAA, demonstrated a lowered affinity for F-actin, indicating a role for those residues in filament binding. Using both structural and biochemical data, we have constructed a model of the gelsolin domain 1-domain 2-F-actin complex. This model highlights a number of interactions that may serve as positive and negative determinants of filament end- and side-binding.     

Inorganic phosphate regulates the binding of cofilin to actin filaments

Inorganic phosphate (Pi) and cofilin/actin depolymerizing factor proteins have opposite effects on actin filament structure and dynamics. Pi stabilizes the subdomain 2 in F-actin and decreases the critical concentration for actin polymerization. Conversely, cofilin enhances disorder in subdomain 2, increases the critical concentration, and accelerates actin treadmilling. Here, we report that Pi inhibits the rate, but not the extent of cofilin binding to actin filaments. This inhibition is also significant at physiological concentrations of Pi, and more pronounced at low pH. Cofilin prevents conformational changes in F-actin induced by Pi, even at high Pi concentrations, probably because allosteric changes in the nucleotide cleft decrease the affinity of Pi to F-actin. Cofilin induced allosteric changes in the nucleotide cleft of F-actin are also indicated by an increase in fluorescence emission and a decrease in the accessibility of etheno-ADP to collisional quenchers. These changes transform the nucleotide cleft of F-actin to G-actin-like. Pi regulation of cofilin binding and the cofilin regulation of Pi binding to F-actin can be important aspects of actin based cell motility.