Nucleotide-mediated conformational changes of monomeric actin and Arp3 studied by molecular dynamics simulations

Members of the actin family of proteins exhibit different biochemical properties when ATP, ADP-P_i, ADP, or no nucleotide is bound. We used molecular dynamics simulations to study the effect of nucleotides on the behavior of actin and actin-related protein 3 (Arp3). In all of the actin simulations, the nucleotide cleft stayed closed, as in most crystal structures. ADP was much more mobile within the cleft than ATP, despite the fact that both nucleotides adopt identical conformations in actin crystal structures. The nucleotide cleft of Arp3 opened in most simulations with ATP, ADP, and no bound nucleotide. Deletion of a C-terminal region of Arp3 that extends beyond the conserved actin sequence reduced the tendency of the Arp3 cleft to open. When the Arp3 cleft opened, we observed multiple instances of partial release of the nucleotide. Cleft opening in Arp3 also allowed us to observe correlated movements of the phosphate clamp, cleft mouth, and barbed-end groove, providing a way for changes in the nucleotide state to be relayed to other parts of Arp3. The DNase binding loop of actin was highly flexible regardless of the nucleotide state. The conformation of Ser14/Thr14 in the P1 loop was sensitive to the presence of the γ-phosphate, but other changes observed in crystal structures were not correlated with the nucleotide state on nanosecond timescales. The divalent cation occupied three positions in the nucleotide cleft, one of which was not previously observed in actin or Arp2/3 complex structures. In sum, these simulations show that subtle differences in structures of actin family proteins have profound effects on their nucleotide-driven behavior.     

Structure and Dynamics of the Actin Filament

We used all-atom molecular dynamics simulations to investigate the structure and properties of the actin filament, starting with either the recent Oda model or the older Holmes model. Simulations of monomeric and polymerized actin show that polymerization changes the nucleotide-binding cleft, bringing together the Q137 side chain and bound ATP in a way that may enhance the ATP hydrolysis rate in the filament. Simulations with different bound nucleotides and conformations of the DNase I binding loop show that the persistence length of the filament depends only on loop conformation. Computational modeling reveals how bound phalloidin stiffens actin filaments and inhibits the release of γ-phosphate from ADP-P_i actin.     

Dimer opening of the nucleotide binding domains of ABC transporters after ATP hydrolysis

ABC transporters constitute one of the most abundant membrane transporter families. The most common feature shared in the family is the highly conserved nucleotide binding domains (NBDs) that drive the transport process through binding and hydrolysis of ATP. Molecular dynamics simulations are used to investigate the effect of ATP hydrolysis in the NBDs. Starting with the ATP-bound, closed dimer of MalK, four simulation systems with all possible combinations of ATP or ADP-P_i bound to the two nucleotide binding sites are constructed and simulated with equilibrium molecular dynamics for ∼70 ns each. The results suggest that the closed form of the NBD dimer can only be maintained with two bound ATP molecules; in other words, hydrolysis of one ATP can lead to the opening of the dimer interface of the NBD dimer. Furthermore, we observed that the opening is an immediate effect of hydrolysis of ATP into ADP and P_i rather than the dissociation of hydrolysis products. In addition, the opening is mechanistically triggered by the dissociation of the LSGGQ motif from the bound nucleotide. A metastable ADP-P_i bound conformational state is consistently observed before the dimer opening in all the simulation systems.     

Functional Characterization of Human Myosin-18A and Its Interaction with F-actin and GOLPH3

Molecular motors of the myosin superfamily share a generic motor domain region. They commonly bind actin in an ATP-sensitive manner, exhibit actin-activated ATPase activity, and generate force and movement in this interaction. Class-18 myosins form heavy chain dimers and contain protein interaction domains located at their unique N-terminal extension. Here, we characterized human myosin-18A molecular function in the interaction with nucleotides, F-actin, and its putative binding partner, the Golgi-associated phosphoprotein GOLPH3. We show that myosin-18A comprises two actin binding sites. One is located in the KE-rich region at the start of the N-terminal extension and appears to mediate ATP-independent binding to F-actin. The second actin-binding site resides in the generic motor domain and is regulated by nucleotide binding in the absence of intrinsic ATP hydrolysis competence. This core motor domain displays its highest actin affinity in the ADP state. Electron micrographs of myosin-18A motor domain-decorated F-actin filaments show a periodic binding pattern independent of the nucleotide state. We show that the PDZ module mediates direct binding of myosin-18A to GOLPH3, and this interaction in turn modulates the actin binding properties of the N-terminal extension. Thus, myosin-18A can act as an actin cross-linker with multiple regulatory modulators that targets interacting proteins or complexes to the actin-based cytoskeleton.     

The ATPase cycle mechanism of the DEAD-box rRNA helicase, DbpA

DEAD-box proteins are ATPase enzymes that destabilize and unwind duplex RNA. Quantitative knowledge of the ATPase cycle parameters is critical for developing models of helicase activity. However, limited information regarding the rate and equilibrium constants defining the ATPase cycle of RNA helicases is available, including the distribution of populated biochemical intermediates, the catalytic step(s) that limits the enzymatic reaction cycle, and how ATP utilization and RNA interactions are linked. We present a quantitative kinetic and equilibrium characterization of the ribosomal RNA (rRNA)-activated ATPase cycle mechanism of DbpA, a DEAD-box rRNA helicase implicated in ribosome biogenesis. rRNA activates the ATPase activity of DbpA by promoting a conformational change after ATP binding that is associated with hydrolysis. Chemical cleavage of bound ATP is reversible and occurs via a γ-phosphate attack mechanism. ADP-P_i and RNA binding display strong thermodynamic coupling, which causes DbpA-ADP-P_i to bind rRNA with > 10-fold higher affinity than with bound ATP, ADP or in the absence of nucleotide. The rRNA-activated steady-state ATPase cycle of DbpA is limited both by ATP hydrolysis and by P_i release, which occur with comparable rates. Consequently, the predominantly populated biochemical states during steady-state cycling are the ATP- and ADP-P_i-bound intermediates. Thermodynamic linkage analysis of the ATPase cycle transitions favors a model in which rRNA duplex destabilization is linked to strong rRNA and nucleotide binding. The presented analysis of the DbpA ATPase cycle reaction mechanism provides a rigorous kinetic and thermodynamic foundation for developing testable hypotheses regarding the functions and molecular mechanisms of DEAD-box helicases.     

Nucleotide effects on the structure and dynamics of actin

Adenosine 5'-triphosphate or ATP is the primary energy source within the cell, releasing its energy via hydrolysis into adenosine 5'-diphosphate or ADP. Actin is an important ATPase involved in many aspects of cellular function, and the binding and hydrolysis of ATP regulates its polymerization into actin filaments as well as its interaction with a host of actin-associated proteins. Here we study the dynamics of monomeric actin in ATP, ADP-Pi, and ADP states via molecular dynamics simulations. As observed in some crystal structures we see that the DNase-I loop is an alpha-helix in the ADP state but forms an unstructured coil domain in the ADP-Pi and ATP states. We also find that this secondary structure change is reversible, and by mimicking nucleotide exchange we can observe the transition between the helical and coil states. Apart from the DNase-I loop, we also see several key structural differences in the nucleotide binding cleft as well as in the hydrophobic cleft between subdomains 1 and 3 where WH2-containing proteins have been shown to interact. These differences provide a structural basis for understanding the observed differences between the various nucleotide states of actin and provide some insight into how ATP regulates the interaction of actin with itself and other proteins.     

Mechanism of Mss116 ATPase reveals functional diversity of DEAD-Box proteins

Mss116 is a Saccharomyces cerevisiae mitochondrial DEAD-box RNA helicase protein that is essential for efficient in vivo splicing of all group I and group II introns and for activation of mRNA translation. Catalysis of intron splicing by Mss116 is coupled to its ATPase activity. Knowledge of the kinetic pathway(s) and biochemical intermediates populated during RNA-stimulated Mss116 ATPase is fundamental for defining how Mss116 ATP utilization is linked to in vivo function. We therefore measured the rate and equilibrium constants underlying Mss116 ATP utilization and nucleotide-linked RNA binding. RNA accelerates the Mss116 steady-state ATPase ∼ 7-fold by promoting rate-limiting ATP hydrolysis such that inorganic phosphate (P_i) release becomes (partially) rate-limiting. RNA binding displays strong thermodynamic coupling to the chemical states of the Mss116-bound nucleotide such that Mss116 with bound ADP-P_i binds RNA more strongly than Mss116 with bound ADP or in the absence of nucleotide. The predominant biochemical intermediate populated during in vivo steady-state cycling is the strong RNA-binding Mss116-ADP-P_i state. Strong RNA binding allows Mss116 to fulfill its biological role in the stabilization of group II intron folding intermediates. ATPase cycling allows for transient population of the weak RNA-binding ADP state of Mss116 and linked dissociation from RNA, which is required for the final stages of intron folding. In cases where Mss116 functions as a helicase, the data collectively favor a model in which ATP hydrolysis promotes a weak-to-strong RNA binding transition that disrupts stable RNA duplexes. The subsequent strong-to-weak RNA binding transition associated with P_i release dissociates Mss116-RNA complexes, regenerating free Mss116.     

Switch II mutants reveal coupling between the nucleotide- and actin-binding regions in myosin V

Conserved active-site elements in myosins and other P-loop NTPases play critical roles in nucleotide binding and hydrolysis; however, the mechanisms of allosteric communication among these mechanoenzymes remain unresolved. In this work we introduced the E442A mutation, which abrogates a salt-bridge between switch I and switch II, and the G440A mutation, which abolishes a main-chain hydrogen bond associated with the interaction of switch II with the γ phosphate of ATP, into myosin V. We used fluorescence resonance energy transfer between mant-labeled nucleotides or IAEDANS-labeled actin and FlAsH-labeled myosin V to examine the conformation of the nucleotide- and actin-binding regions, respectively. We demonstrate that in the absence of actin, both the G440A and E442A mutants bind ATP with similar affinity and result in only minor alterations in the conformation of the nucleotide-binding pocket (NBP). In the presence of ADP and actin, both switch II mutants disrupt the formation of a closed NBP actomyosin.ADP state. The G440A mutant also prevents ATP-induced opening of the actin-binding cleft. Our results indicate that the switch II region is critical for stabilizing the closed NBP conformation in the presence of actin, and is essential for communication between the active site and actin-binding region.     

Interaction of F-actin-AMPPNP with myosin subfragment-1 and troponin-tropomyosin: influence of an extra phosphate at the nucleotide binding site in F-actin on its function

An unsplitable analogue of ATP (adenylyl imidodiphosphate; AMPPNP) was incorporated into F-actin [Cooke, R. (1975) Biochemistry 14, 3250-3256]. The resulting polymers (F-actin-AMPPNP) activated the ATPase activity of myosin subfragment-1 (S1) as efficiently as normal F-actin; neither the maximum velocity at infinite actin concentration (Vmax) nor the affinity of actin to S1 in the presence of ATP (1/KATPase) changed, which indicates that the terminal phosphate of the bound nucleotide at the cleft region between the two domains of the actin molecule [Kabsch, W., Mannherz, H.G., & Suck, D. (1985) EMBO J. 4, 2113-2118] is not directly involved in a myosin binding site. However, the interaction of F-actin with troponin-tropomyosin was strongly modulated by the replacement of ADP with AMPPNP. The troponin-tropomyosin complex strongly enhanced the activation of S1-ATPase activity by F-actin-AMPPNP in the presence of Ca2+, although it has no effect on the activation by normal F-actin-ADP. KATPase was enhanced about threefold by troponin-tropomyosin in the presence of Ca2+, while Vmax was not markedly changed. F-actin-AMPPNP is highly potentiated by troponin-tropomyosin even with low S1 to actin ratios and at high ATP conditions. In the absence of Ca2+, the activation by F-actin-AMPPNP was inhibited normally by troponin-tropomyosin. The results suggest that the terminal beta-phosphate of the bound nucleotide in F-actin is located in a region which is important for regulation of the interaction with myosin.     

Evidence that F-actin can hydrolyze ATP independent of monomer-polymer end interactions

The rate of ATP hydrolysis in solutions of F-actin at steady state in 50 mM KC1, 0.1 mM CaC12 was inhibited by AMP and ADP. The inhibition was competitive with ATP (Km of about 600 microM) with Ki values of 9 microM for AMP and 44 microM for ADP. ATP hydrolysis was inhibited greater than 95% by 1 mM AMP. AMP had no effect on the time course of actin polymerization, ATP hydrolysis during polymerization, or the critical actin concentration. Simultaneous measurements of G-actin/F-actin subunit exchange and nucleotide exchange showed that nucleotide exchange occurred much more rapidly than subunit exchange; during the experiment over 50% of the F-actin-bound nucleotide was replaced when less than 1% of the F-actin subunits had exchanged. When AMP was present it was incorporated into the polymer, preventing incorporation of ADP from ATP in solution. F-actin with bound Mg2+ was much less sensitive to AMP than F-actin with bound Ca2+. These data provide evidence for an ATP hydrolysis cycle associated with direct exchange of F-actin-bound ADP for ATP free in solution independent of monomer-polymer end interactions. This exchange and hydrolysis of nucleotide may be enhanced when Ca2+ is bound to the F-actin protomers.     

Modulation of the Chaperone DnaK Allosterism by the Nucleotide Exchange Factor GrpE

Hsp70 chaperones comprise two domains, the nucleotide-binding domain (Hsp70_NBD), responsible for structural and functional changes in the chaperone, and the substrate-binding domain (Hsp70_SBD), involved in substrate interaction. Substrate binding and release in Hsp70 is controlled by the nucleotide state of DnaK_NBD, with ATP inducing the open, substrate-receptive DnaK_SBD conformation, whereas ADP forces its closure. DnaK cycles between the two conformations through interaction with two cofactors, the Hsp40 co-chaperones (DnaJ in Escherichia coli) induce the ADP state, and the nucleotide exchange factors (GrpE in E. coli) induce the ATP state. X-ray crystallography showed that the GrpE dimer is a nucleotide exchange factor that works by interaction of one of its monomers with DnaK_NBD. DnaK_SBD location in this complex is debated; there is evidence that it interacts with the GrpE N-terminal disordered region, far from DnaK_NBD. Although we confirmed this interaction using biochemical and biophysical techniques, our EM-based three-dimensional reconstruction of the DnaK-GrpE complex located DnaK_SBD near DnaK_NBD. This apparent discrepancy between the functional and structural results is explained by our finding that the tail region of the GrpE dimer in the DnaK-GrpE complex bends and its tip contacts DnaK_SBD, whereas the DnaK_NBD-DnaK_SBD linker contacts the GrpE helical region. We suggest that these interactions define a more complex role for GrpE in the control of DnaK function.     

The effect of toxins on inorganic phosphate release during actin polymerization

During the polymerization of actin, hydrolysis of bound ATP occurs in two consecutive steps: chemical cleavage of the high-energy nucleotide and slow release of the γ-phosphate. In this study the effect of phalloidin and jasplakinolide on the kinetics of P _i release was monitored during the formation of actin filaments. An enzyme-linked assay based spectrophotometric technique was used to follow the liberation of inorganic phosphate. It was verified that jasplakinolide reduced the P _i release in the same way as phalloidin. It was not possible to demonstrate long-range allosteric effects of the toxins by release of P _i from F-actin. The products of ATP hydrolysis were released by denaturation of the actin filaments. HPLC analysis of the samples revealed that the ATP in the toxin-bound region was completely hydrolysed into ADP and P _i . The effect of both toxins can be sufficiently explained by local and mechanical blockade of P _i dissociation.     

Water in actin polymerization.

We have addressed the question whether water is part of the G- to F-actin polymerization reaction. Under osmotic stress, the critical concentration for G-Ca-ATP actin was reduced for six different osmolytes. These results are interpreted as showing that reducing water activity favored the polymerized state. The magnitude of the effect correlated, then saturated, with increasing MW of the osmolyte and suggested that up to 10-12 fewer water molecules were associated with actin when it polymerized. By contrast, osmotic effects were insignificant for Mg-ATP actin. The nucleotide binding site of the Mg conformation is more closed than the Ca and more closely resembles the closed actin conformation in the polymerized state. These results suggest that the water may come from the cleft of the nucleotide binding site.     

Effects of Nucleotide and End-Dependent Actin Conformations on Polymerization

The regulation of actin is key for controlled cellular function. Filaments are regulated by actin-binding proteins, but the nucleotide state of actin is also an important factor. From extended molecular dynamics simulations, we find that both nucleotide states of the actin monomer have significantly less twist than their crystal structures and that the ATP monomer is flatter than the ADP form. We also find that the filament’s pointed end is flatter than the remainder of the filament and has a conformation distinct from G-actin, meaning that incoming monomers would need to undergo isomerization that would weaken the affinity and slow polymerization. Conversely, the barbed end of the filament takes on a conformation nearly identical to the ATP monomer, enhancing ATP G-actin’s ability to polymerize as compared with ADP G-actin. The thermodynamic penalty imposed by differences in isomerization for the ATP and ADP growth at the barbed end exactly matches experimental results.     

F-Actin Structure Destabilization and DNase I Binding Loop Fluctuations: Mutational Cross-Linking and Electron Microscopy Analysis of Loop States and Effects on F-Actin

The conformational dynamics of filamentous actin (F-actin) is essential for the regulation and functions of cellular actin networks. The main contribution to F-actin dynamics and its multiple conformational states arises from the mobility and flexibility of the DNase I binding loop (D-loop; residues 40-50) on subdomain 2. Therefore, we explored the structural constraints on D-loop plasticity at the F-actin interprotomer space by probing its dynamic interactions with the hydrophobic loop (H-loop), the C-terminus, and the W-loop via mutational disulfide cross-linking. To this end, residues of the D-loop were mutated to cysteines on yeast actin with a C374A background. These mutants showed no major changes in their polymerization and nucleotide exchange properties compared to wild-type actin. Copper-catalyzed disulfide cross-linking was investigated in equimolar copolymers of cysteine mutants from the D-loop with either wild-type (C374) actin or mutant S265C/C374A (on the H-loop) or mutant F169C/C374A (on the W-loop). Remarkably, all tested residues of the D-loop could be cross-linked to residues 374, 265, and 169 by disulfide bonds, demonstrating the plasticity of the interprotomer region. However, each cross-link resulted in different effects on the filament structure, as detected by electron microscopy and light-scattering measurements. Disulfide cross-linking in the longitudinal orientation produced mostly no visible changes in filament morphology, whereas the cross-linking of D-loop residues > 45 to the H-loop, in the lateral direction, resulted in filament disruption and the presence of amorphous aggregates on electron microscopy images. A similar aggregation was also observed upon cross-linking the residues of the D-loop (> 41) to residue 169. The effects of disulfide cross-links on F-actin stability were only partially accounted for by the simulations of current F-actin models. Thus, our results present evidence for the high level of conformational plasticity in the interprotomer space and document the link between D-loop interactions and F-actin stability.     

The critical concentration of actin in the presence of ATP increases with the number concentration of filaments and approaches the critical concentration of actin.ADP

F-actin at steady state in the presence of ATP partially depolymerized to a new steady state upon mechanical fragmentation. The increase in critical concentration with the number concentration of filaments has been quantitatively studied. The data can be explained by a model in which the preferred pathway for actin association-dissociation reactions at steady state in the presence of ATP involves binding of G-actin . ATP to filaments, ATP hydrolysis, and dissociation of G-actin . ADP which is then slowly converted to G-actin . ATP. As a consequence of the slow exchange of nucleotide on G-actin, the respective amounts of G-actin . ATP and G-actin . ADP coexisting with F-actin at steady state depend on the filament number concentration. G-actin coexisting with F-actin at zero number concentration of filaments would then consist of G-actin . ATP only, while the critical concentration obtained at infinite number of filaments would be that for G-actin . ADP. Values of 0.35 and 8 microM, respectively, were found for these two extreme critical concentrations for skeletal muscle actin at 20 degrees C, pH 7.8, 0.1 mM CaCl2, 1 mM MgCl2, and 0.2 mM ATP. The same value of 8 microM was directly measured for the critical concentration of G-actin . ADP polymerized in the presence of ADP and absence of ATP, and it was unaffected by fragmentation. These results have important implications for experiments in which critical concentrations are compared under conditions that change the filament number concentrations.     

Allostery in Hsp70 Chaperones Is Transduced by Subdomain Rotations

Hsp70s (heat shock protein 70 kDa) are central to protein folding, refolding, and trafficking in organisms ranging from archaea to Homo sapiens under both normal and stressed cellular conditions. Hsp70s are comprised of a nucleotide-binding domain (NBD) and a substrate-binding domain (SBD). The nucleotide binding site in the NBD and the substrate binding site in the SBD are allosterically linked: ADP binding promotes substrate binding, while ATP binding promotes substrate release. Hsp70s have been linked to inhibition of apoptosis (i.e., cancer) and diseases associated with protein misfolding such as Alzheimer's, Parkinson's, and Huntington's.It has long been a goal to characterize the nature of allosteric coupling in these proteins. However, earlier studies of the isolated NBD could not show any difference in overall conformation between the ATP state and the ADP state. Hence the question: How is the state of the nucleotide communicated between NBD and SBD?Here we report a solution NMR study of the 44-kDa NBD of Hsp70 from Thermus thermophilus in the ADP and AMPPNP states. Using the solution NMR methods of residual dipolar coupling analysis, we determine that significant rotations occur for different subdomains of the NBD upon exchange of nucleotide. These rotations modulate access to the nucleotide binding cleft in the absence of a nucleotide exchange factor. Moreover, the rotations cause a change in the accessibility of a hydrophobic surface cleft remote from the nucleotide binding site, which previously has been identified as essential to allosteric communication between NBD and SBD. We propose that it is this change in the NBD surface cleft that constitutes the allosteric signal that can be recognized by the SBD.     

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.     

Noncooperative stabilization effect of phalloidin on ADP.BeFx- and ADP.AlF4-actin filaments

Actin plays important roles in eukaryotic cell motility. During actin polymerization, the actin-bound ATP is hydrolyzed to ADP and P i. We carried out differential scanning calorimetry experiments to characterize the cooperativity of the stabilizing effect of phalloidin on actin filaments in their ADP.P i state. The ADP.P i state was mimicked by using ADP.BeF x or ADP.AlF 4. The results showed that the binding of the nucleotide analogues or phalloidin stabilized the actin filaments to a similar extent when added separately. Phalloidin binding to ADP.BeF x- or ADP.AlF 4-actin filaments further stabilized them, indicating that the mechanism by which phalloidin and the nucleotide analogues affect the filament structure was different. The results also showed that the stabilization effect of phalloidin binding to ADP.BeF x or ADP.AlF 4-bound actin filaments was not cooperative. Since the effect of phalloidin binding was cooperative in the absence of these nucleotide analogues, these results suggest that the binding of ADP.BeF x or ADP.AlF 4 to the actin modified the protomer-protomer interactions along the actin filaments.     

ATPase activity and conformational changes in the regulation of actin.

The eukaryotic microfilament system is regulated in part through the nucleotide- and cation-dependent conformation of the actin molecule. In this review, recent literature on the crystal and solution structures of actin and other actin-superfamily proteins is summarized. Furthermore, the structure of the nucleotide binding cleft is discussed in terms of the mechanism of ATP hydrolysis and P(i) release. Two distinct domain movements are suggested to participate in the regulation of actin. (1) High-affinity binding of Mg(2+) to actin induces a rearrangement of side chains in the nucleotide binding site leading to an increased ATPase activity and polymerizability, as well as a rotation of subdomain 2 which is mediated by the hydroxyl of serine-14. (2) Hydrolysis of ATP and subsequent release of inorganic phosphate lead to a butterfly-like opening of the actin molecule brought about by a shearing in the interdomain helix 135-150. These domain rearrangements modulate the interaction of actin with a variety of different proteins, and conversely, protein binding to actin can restrict these conformational changes, with ultimate effects on the assembly state of the microfilament system.