Myosin subfragment 1 inhibits dissociation of nucleotide and calcium from G-actin

Role of actin DNase-I-binding loop in myosin subfragment 1-induced polymerization of G-actin: implications for the mechanism of polymerization

Proteolytic cleavage of actin between Gly(42) and Val(43) within its DNase-I-binding loop (D-loop) abolishes the ability of Ca-G-actin to spontaneously polymerize in the presence of KCl. Here we show that such modified actin is assembled into filaments, albeit at a lower rate than unmodified actin, by myosin subfragment 1 (S1) carrying the A1 essential light chain but not by S1(A2). S1 titration of pyrene-G-actin showed a diminished affinity of cleaved actin for S1, but this could be compensated for by using S1 in excess. The most significant effect of the cleavage, revealed by measuring the fluorescence of pyrene-actin and light-scattering intensities as a function of actin concentration at saturating concentrations of S1, is strong inhibition of association of G-actin-S1 complexes into oligomers. Measurements of the fluorescence of dansyl cadaverine attached to Gln(41) indicate substantial inhibition of the initial association of G-actin-S1 into longitudinal dimers. The data provide experimental evidence for the critical role of D-loop conformation in both longitudinal and lateral, cross-strand actin-actin contact formation in the nucleation reaction. Electron microscopic analysis of the changes in filament-length distribution during polymerization of actin by S1(A1) and S1(A2) suggests that the mechanism of S1-induced polymerization is not substantially different from the nucleation-elongation scheme of spontaneous actin polymerization.

Differences in the ionic interaction of actin with the motor domains of nonmuscle and muscle myosin II

Changes in the actin-myosin interface are thought to play an important role in microfilament-linked cellular movements. In this study, we compared the actin binding properties of the motor domain of Dictyostelium discoideum (M765) and rabbit skeletal muscle myosin subfragment-1 (S1). The Dictyostelium motor domain resembles S1(A2) (S1 carrying the A2 light chain) in its interaction with G-actin. Similar to S1(A2), none of the Dictyostelium motor domain constructs induced G-actin polymerization. The affinity of monomeric actin (G-actin) was 20-fold lower for M765 than for S1(A2) but increasing the number of positive charges in the loop 2 region of the D. discoideum motor domain (residues 613-623) resulted in equivalent affinities of G-actin for M765 and for S1. Proteolytic cleavage and cross-linking approaches were used to show that M765, like S1, interacts via the loop 2 region with filamentous actin (F-actin). For both types of myosin, F-actin prevents trypsin cleavage in the loop 2 region and F-actin segment 1-28 can be cross-linked to loop 2 residues by a carbodiimide-induced reaction. In contrast with the S1, loop residues 559-565 of D. discoideum myosin was not cross-linked to F-actin, probably due to the lower number of positive charges. These results confirm the importance of the loop 2 region of myosin for the interaction with both G-actin and F-actin, regardless of the source of myosin. The differences observed in the way in which M765 and S1 interact with actin may be linked to more general differences in the structure of the actomyosin interface of muscle and nonmuscle myosins.

Effect of nucleotides and actin on the orientation of the light chain-binding domain in myosin subfragment 1

The X-ray structure of myosin head (S1) reveals the presence of a long alpha-helical structure that supports both the essential and the regulatory light chains. It has been proposed that small structural changes in the catalytic domain of S1 are amplified by swinging the long alpha-helix (the "lever arm") to produce approximately 11 nm steps. To probe the spatial position of the putative lever in various S1 states, we have measured, by fluorescence resonance energy transfer (FRET), the effect of nucleotides and actin on the distances between Cys-177 of the essential light chain A1 (which is attached to the alpha-helix) and three loci in the catalytic domain. Cys-177 (donor) was labeled with 1,5-IAEDANS. The trinitrophenylated ADP analog (TNP-ADP, acceptor) was used to measure the distance to the active site. Lys-553 at the actin-binding site, labeled with a fluorescein derivative, and Lys-83 modified with trinitrobenzenesulfonic acid served as two other acceptors. FRET measurements were performed for S1 alone, for its complexes with MgADP and MgATP, for the analogs of the transition state of the ATPase reaction, S1.ADP.BeFx, S1.ADP.AlF4, and S1.ADP.VO4, and for acto-S1 in the absence and in the presence of ADP. When the transition state and acto-S1 complexes were formed, the change in the Cys-177 --> Lys-83 distance was <1.1 A, for the distance Cys-177 --> Lys-553, the change was +/-2.5 A. These distance changes correspond to rotations by <10 degrees and approximately 25 degrees, respectively. For the Cys-177 --> TNP-ADP the interprobe separation decreased by approximately 6 A in the presence of BeFx and AlF4- but only 1.9 A in the presence of vanadate; we do not interpret the 6 A change as resulting from the lever rotation. Using the coordinates of the acto-S1 complex, we have computed the expected changes in these distances resulting from rotation of the lever. These changes were much greater than the ones observed. The above results are inconsistent with models of force generation by S1 in which the head assumes two distinct conformations characterized by large differences in the angle between the motor and the light chain-binding domain. Several alternative mechanisms are proposed.

Kinetics of myosin subfragment-1-induced condensation of G-actin into oligomers, precursors in the assembly of F-actin-S1. Role of the tightly bound metal ion and ATP hydrolysis

In a low ionic strength buffer and in the absence of free ATP, the interaction of G-actin (G) with myosin subfragment-1 (S1) leads to the formation of arrowhead-decorated F-actin-S1 filaments, through a series of elementary steps. The initial formation of GS and G2S complexes is followed by their condensation into short oligomers. The kinetics of formation of G-actin-S1 oligomers have been monitored in a stopped-flow apparatus using a combination of light scattering and fluorescence of NBD-labeled actin. Oligomers appear more stable and are formed at a faster rate from MgATP-G-actin than from CaATP-G-actin. The actin-bound ATP is hydrolyzed when oligomers are formed from MgATP-G-actin, not when they are formed from CaATP-G-actin. The formation of oligomers is energetically favored in the presence of cytochalasin D. All data are consistent with the view that the actin-actin interactions which take place upon condensation of GS and G2S into oligomers are very similar to lateral actin-actin interactions along the short pitch helix of actin filaments, which are involved in actin nucleation. These interactions trigger ATP hydrolysis on actin.

Actin and the actomyosin interface: a review

This review deals with the structure of the actin monomer, its assembly into filaments and the loci on F-actin involved in binding myosin. Two distinctly different arrangements of monomers have been suggested for actin filaments. One model proposed by Holmes et al. is well developed. It places the so-called 'large' domain close to the filament axis and the so-called 'small' domain out near the surface of the filament. A second, less-well developed, model proposed by Schutt et al. locates the 'small' domain close to the filament axis and they rotate the monomer so that 'bottom' of the 'large' domain is at the highest radius. We analyze the available evidence for the models of F-actin derived from X-ray diffraction, reconstructions from electron micrographs, fluorescence resonance energy transfer spectroscopy, chemical cross-linking, antibody probes, limited proteolysis, site-directed and natural mutations, nuclear magnetic resonance spectroscopy and other techniques. The result is an actin-centered view of the loci on actin which are probably involved in its interaction with the myosin 'head'. From these multiple contacts we speculate on the sequence of steps between the initial weak-binding state of S-1 to the actin filament through to the stable strong-binding state seen in the absence of free Mg-ATP, i.e., the rigor state.

Sequence 18-29 on actin: antibody and spectroscopic probing of conformational changes

Experimental evidence for the involvement of the 18-29 site within actin subdomain-1 in the actomyosin weak binding interface includes the inhibition of actomyosin ATPase activity by specific peptide antibodies [Adams, S., & Reisler, E. (1993) Biochemistry 32, 5051-5056] and by the Dictyostelium actin mutant D24H/D25H [Johara, M., et al. (1993) Proc. Natl. Acad. Sci. U.S.A. 90, 2127-2131]. In this work, the effect of the 18-29 peptide antibodies on the polymerization and conformation of actin has been characterized. Binding of antibody to the 18-29 site strongly inhibited the MgCl2-induced polymerization of G-actin, had a much weaker impact on the CaCl2 polymerization of actin, and showed very little effect on the NaCl polymerization of G-actin. These observations were linked to the binding of the 18-29 antibody to the different forms of actin. In sedimentation assays, the (18-29) IgG bound more strongly to Mg-F- and Mg-G-actins than to Ca-F- and Ca-G-actins, respectively. The binding of IgG to F-actin decreased sharply with an increase in ionic strength. Antibody binding to the 18-29 site induced conformational changes within the nucleotide cleft, both slowing the rate of nucleotide exchange and increasing the fluorescence intensity of actin-bound epsilon ATP. The increased fluorescence of a dansyl probe attached to Gln-41 and a pyrene probe attached to Cys-374 demonstrated that antibody binding also caused local perturbations in the DNase I loop of subdomain-2 and at the C-terminus of actin. These results are discussed in terms of actin plasticity and its implications for actomyosin interactions.

Interaction and polymerization of the G-actin-myosin head complex: effect of DNase I

The properties of polymerization and interaction of the G-actin-myosin S1 complexes (formed with either the S1(A1) or the S1(A2) isoform) have been studied by light-scattering and fluorescence measurements in the absence and in the presence of DNase I. In the absence of DNase I, the G-actin-S1(A1) and G-actin-S1(A2) complexes were found to be characterized by different limiting concentrations (l.c.), defined as the complex concentrations above which the polymerization occurs spontaneously within 20 h at 20 degrees C in a "no salt" buffer (l.c. = 0.42 and 8.8 microM for G-actin-S1(A1) and G-actin-S1(A2), respectively). The occurrence of a limiting concentration for either complex together with the kinetic properties of the polymerization led us to conclude that the G-actin-S1 polymerization occurs via a nucleation-elongation process. Fluorescence titrations and proteolysis experiments revealed that G-actin interacts with S1 with a 1:1 stoichiometry (independently of the presence of ATP) with dissociation constants, in the absence of nucleotide, of 20 and 50 nM for the G-actin-S1(A1) and G-actin-S1(A2) complexes, respectively. In the presence of at least a 1.5-fold excess of DNase I, the polymerization of the G-actin-S1 complexes was blocked even at high protein concentration or in the presence of salts. In addition, the affinity of either S1 isoform to actin was reduced 4-5-fold by DNase I, while the stoichiometry of the G-actin-S1 complexes was not changed. However, since the dissociation constants remain in the submicromolar range, we could demonstrate the existence of ternary DNase I-G-actin-S1 complexes stable under polymerizing conditions. Finally, the study of the effect of nucleotides and of various salts on the G-actin-S1 interaction further showed significant differences between the G-actin-S1 and F-actin-S1 interactions.