Stability and dynamics of G-actin: back-door water diffusion and behavior of a subdomain 3/4 loop.

Molecular dynamics simulations have been performed on solvated G-actin bound to ADP and ATP, starting with the crystal structure of the actin-DNase 1 complex, including a Ca2+ or Mg2+ ion at the high-affinity divalent cation-binding site. Water molecules have been found to enter the nucleotide-binding site (phosphate vicinity) along two pathways, from the side where the nucleotide base is exposed to water, as well as from the opposite side. The water channels suggest a "back-door" mechanism for ATP hydrolysis in which the phosphate is released to a side opposite that of nucleotide binding and unbinding. The simulations also reveal a propensity of G-actin to alter its crystallographic structure toward the filamentous structure. Domain movement closes the nucleotide cleft, the movement being more pronounced for bound Mg2+. The conformational change is interpreted as a response of the system to missing water molecules in the crystal structure. The structures arising in the simulations, classified according to nucleotide cleft separation and radius of gyration of the protein, fall into two distinct clusters: a cluster of states that are similar to the G-actin crystal structure, and a cluster of states with small cleft separation and with the subdomain 3/4 loop 264-273 detached from the protein. The latter states resemble the putative filamentous structure of actin, in which the loop connects the two strands of the actin filament.     

Polymerization and structure of nucleotide-free actin filaments

Two factors have limited studies of the properties of nucleotide-free actin (NFA). First, actin lacking bound nucleotide denatures rapidly without stabilizing agents such as sucrose; and second, without denaturants such as urea, it is difficult to remove all of the bound nucleotide. We used apyrase, EDTA and Dowex-1 to prepare actin that is stable in sucrose and approximately 99 % free of bound nucleotide. In high concentrations of sucrose where NFA is stable, it polymerizes more favorably with a lag phase shorter than ATP-actin and a critical concentration close to zero. NFA filaments are stable, but depolymerize at low sucrose concentrations due to denaturation of subunits when they dissociate from filament ends. By electron microscopy of negatively stained specimens, NFA forms long filaments with a persistence length 1.5 times greater than ADP-actin filaments. Three-dimensional helical reconstructions of NFA and ADP-actin filaments at 2.5 nm resolution reveal similar intersubunit contacts along the two long-pitch helical strands but statistically significant less mass density between the two strands of NFA filaments. When compared with ADP-actin filaments, the major difference peak of NFA filaments is near, but does not coincide with, the vacated nucleotide binding site. The empty nucleotide binding site in these NFA filaments is not accessible to free nucleotide in the solution. The affinity of NFA filaments for rhodamine phalloidin is lower than that of native actin filaments, due to a lower association rate. This work confirms that bound nucleotide is not essential for actin polymerization, so the main functions of the nucleotide are to stabilize monomers, modulate the mechanical and dynamic properties of filaments through ATP hydrolysis and phosphate release, and to provide an internal timer for the age of the filament.     

Crystal structures of expressed non-polymerizable monomeric actin in the ADP and ATP states

Actin filament growth and disassembly, as well as affinity for actin-binding proteins, is mediated by the nucleotide-bound state of the component actin monomers. The structural differences between ATP-actin and ADP-actin, however, remain controversial. We expressed a cytoplasmic actin in Sf9 cells, which was rendered non-polymerizable by virtue of two point mutations in subdomain 4 (A204E/P243K). This homogeneous monomer, called AP-actin, was crystallized in the absence of toxins, binding proteins, or chemical modification, with ATP or ADP at the active site. The two surface mutations do not perturb the structure. Significant differences between the two states are confined to the active site region and sensor loop. The active site cleft remains closed in both states. Minor structural shifts propagate from the active site toward subdomain 2, but dissipate before reaching the DNase binding loop (D-loop), which remains disordered in both the ADP and ATP states. This result contrasts with previous structures of actin made monomeric by modification with tetramethylrhodamine, which show formation of an alpha-helix at the distal end of the D-loop in the ADP-bound but not the ATP-bound form (Otterbein, L. R., Graceffa, P., and Dominguez, R. (2001) Science 293, 708-711). Our reanalysis of the TMR-modified actin structures suggests that the nucleotide-dependent formation of the D-loop helix may result from signal propagation through crystal packing interactions. Whereas the observed nucleotide-dependent changes in the structure present significantly different surfaces on the exterior of the actin monomer, current models of the actin filament lack any actin-actin interactions that involve the region of these key structural changes.     

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.     

Conformational and dynamic differences between actin filaments polymerized from ATP- or ADP-actin monomers

Conformational and dynamic properties of actin filaments polymerized from ATP- or ADP-actin monomers were compared by using fluorescence spectroscopic methods. The fluorescence intensity of IAEDANS attached to the Cys(374) residue of actin was smaller in filaments from ADP-actin than in filaments from ATP-actin monomers, which reflected a nucleotide-induced conformational difference in subdomain 1 of the monomer. Radial coordinate calculations revealed that this conformational difference did not modify the distance of Cys(374) from the longitudinal filament axis. Temperature-dependent fluorescence resonance energy transfer measurements between donor and acceptor molecules on Cys(374) of neighboring actin protomers revealed that the inter-monomer flexibility of filaments assembled from ADP-actin monomers were substantially greater than the one of filaments from ATP-actin monomers. Flexibility was reduced by phalloidin in both types of 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.     

Conformational changes in actin induced by its interaction with gelsolin.

Actin cleaved by the protease from Escherichia coli A2 strain between Gly42 and Val43 (ECP-actin) is no longer polymerizable when it contains Ca2+ as a tightly bound cation, but polymerizes when Mg2+ is bound. We have investigated the interactions of gelsolin with this actin with regard to conformational changes in the actin molecule induced by the binding of gelsolin. ECP-(Ca)actin interacts with gelsolin in a manner similar to that in which it reacts with intact actin, and forms a stoichiometric 2:1 complex. Despite the nonpolymerizability of ECP-(Ca)actin, this complex can act as a nucleus for the polymerization of intact actin, thus indicating that upon interaction with gelsolin, ECP-(Ca)actin undergoes a conformational change that enables its interaction with another actin monomer. By gel filtration and fluorometry it was shown that the binding of at least one of the ECP-cleaved actins to gelsolin is considerably weaker than of intact actin, suggesting that conformational changes in subdomain 2 of actin monomer may directly or allosterically affect actin-gelsolin interactions. On the other hand, interaction with gelsolin changes the conformation of actin within the DNase I-binding loop, as indicated by inhibition of limited proteolysis of actin by ECP and subtilisin. Cross-linking experiments with gelsolin-nucleated actin filaments using N,N-phenylene-bismaleimide (which cross-links adjacent actin monomers between Cys374 and Lys191) reveal that gelsolin causes a significant increase in the yield of the 115-kDa cross-linking product, confirming the evidence that gelsolin stabilizes or changes the conformation of the C-terminal region of the actin molecule, and these changes are propagated from the capped end along the filament. These results allow us to conclude that nucleation of actin polymerization by gelsolin is promoted by conformational changes within subdomain 2 and at the C-terminus of the actin monomer.     

Insights into the influence of nucleotides on actin family proteins from seven structures of Arp2/3 complex

ATP is required for nucleation of actin filament branches by Arp2/3 complex, but the influence of ATP binding and hydrolysis are poorly understood. We determined crystal structures of bovine Arp2/3 complex cocrystallized with various bound adenine nucleotides and cations. Nucleotide binding favors closure of the nucleotide-binding cleft of Arp3, but no large-scale conformational changes in the complex. Thus, ATP binding does not directly activate Arp2/3 complex but is part of a network of interactions that contribute to nucleation. We compared nucleotide-induced conformational changes of residues lining the cleft in Arp3 and actin structures to construct a movie depicting the proposed ATPase cycle for the actin family. Chemical crosslinking stabilized subdomain 1 of Arp2, revealing new electron density for 69 residues in this subdomain. Steric clashes with Arp3 appear to be responsible for intrinsic disorder of subdomains 1 and 2 of Arp2 in inactive Arp2/3 complex.     

Structural connectivity in actin: effect of C-terminal modifications on the properties of actin.

In this study, we use fluorescent probes and proteolytic digestions to demonstrate structural coupling between distant regions of actin. We show that modifications of Cys-374 in the C-terminus of actin slow the rate of nucleotide exchange in the nucleotide cleft. Conformational coupling between the C-terminus and the DNasal loop in subdomain II is observed in proteolytic digestion experiments in which a new C-terminal cleavage site is exposed upon DNasel binding. The functional consequences of C-terminal modification are evident from S-1 ATPase activity and the in vitro motility experiments with modified actins. Pyrene actin, labeled at Cys-374, activates S-1 ATPase activity only half as well as control actin. This reduction is attributed to a lower Vmax value because the affinity of pyrene actin to S-1 is not significantly altered. The in vitro sliding velocity of pyrene actin is also decreased. However, IAEDANS labeling of actin (also at Cys-374) enhances the Vmax of acto-S-1 ATPase activity and the in vitro sliding velocity by approximately 25%. These results are discussed in terms of conformational coupling between distant regions in actin and the functional implications of the interactions of actin-binding proteins with the C-terminus of actin.     

The control of actin nucleotide exchange by thymosin beta 4 and profilin. A potential regulatory mechanism for actin polymerization in cells.

We present evidence for a new mechanism by which two major actin monomer binding proteins, thymosin beta 4 and profilin, may control the rate and the extent of actin polymerization in cells. Both proteins bind actin monomers transiently with a stoichiometry of 1:1. When bound to actin, thymosin beta 4 strongly inhibits the exchange of the nucleotide bound to actin by blocking its dissociation, while profilin catalytically promotes nucleotide exchange. Because both proteins exchange rapidly between actin molecules, low concentrations of profilin can overcome the inhibitory effects of high concentrations of thymosin beta 4 on the nucleotide exchange. These reactions may allow variations in profilin concentration (which may be regulated by membrane polyphosphoinositide metabolism) to control the ratio of ATP-actin to ADP-actin. Because ATP-actin subunits polymerize more readily than ADP-actin subunits, this ratio may play a key regulatory role in the assembly of cellular actin structures, particularly under circumstances of rapid filament turnover.     

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.     

Thymosin-beta(4) changes the conformation and dynamics of actin monomers

Thymosin-beta(4) (Tbeta(4)) binds actin monomers stoichiometrically and maintains the bulk of the actin monomer pool in metazoan cells. Tbeta(4) binding quenches the fluorescence of N-iodoacetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine (AEDANS) conjugated to Cys(374) of actin monomers. The K(d) of the actin-Tbeta(4) complex depends on the cation and nucleotide bound to actin but is not affected by the AEDANS probe. The different stabilities are determined primarily by the rates of dissociation. At 25 degrees C, the free energy of Tbeta(4) binding MgATP-actin is primarily enthalpic in origin but entropic for CaATP-actin. Binding is coupled to the dissociation of bound water molecules, which is greater for CaATP-actin than MgATP-actin monomers. Proteolysis of MgATP-actin, but not CaATP-actin, at Gly(46) on subdomain 2 is >12 times faster when Tbeta(4) is bound. The C terminus of Tbeta(4) contacts actin near this cleavage site, at His(40). By tritium exchange, Tbeta(4) slows the exchange rate of approximately eight rapidly exchanging amide protons on actin. We conclude that Tbeta(4) changes the conformation and structural dynamics ("breathing") of actin monomers. The conformational change may reflect the unique ability of Tbeta(4) to sequester actin monomers and inhibit nucleotide exchange.     

Divalent cation-, nucleotide-, and polymerization-dependent changes in the conformation of subdomain 2 of actin.

Conformational changes in subdomain 2 of actin were investigated using fluorescence probes dansyl cadaverine (DC) or dansyl ethylenediamine (DED) covalently attached to Gln41. Examination of changes in the fluorescence emission spectra as a function of time during Ca2+/Mg2+ and ATP/ADP exchange at the high-affinity site for divalent cation-nucleotide complex in G-actin confirmed a profound influence of the type of nucleotide but failed to detect a significant cation-dependent difference in the environment of Gln41. No significant difference between Ca- and Mg-actin was also seen in the magnitude of the fluorescence changes resulting from the polymerization of these two actin forms. Evidence is presented that earlier reported cation-dependent differences in the conformation of the loop 38-52 may be related to time-dependent changes in the conformation of subdomain 2 in DED- or DC-labeled G-actin, accelerated by substitution of Mg2+ for Ca2+ in CaATP-G-actin and, in particular, by conversion of MgATP- into MgADP-G-actin. These spontaneous changes are associated with a denaturation-driven release of the bound nucleotide that is promoted by two effects of DED or DC labeling: lowered affinity of actin for nucleotide and acceleration of ATP hydrolysis on MgATP-G-actin that converts it into a less stable MgADP form. Evidence is presented that the changes in the environment of Gln41 accompanying actin polymerization result in part from the release of Pi after the hydrolysis of ATP on the polymer. A similarity of this change to that accompanying replacement of the bound ATP with ADP in G-actin is discussed.     

Two conserved lysines at the 50/20-kDa junction of myosin are necessary for triggering actin activation

Actin stimulates myosin's activity by inducing structural alterations that correlate with the transition from a weakly to a strongly bound state, during which time inorganic phosphate (P(i)) is released from myosin's active site. The surface loop at the 50/20-kDa junction of myosin (loop 2) is part of the actin interface. Here we demonstrate that elimination of two highly conserved lysines at the C-terminal end of loop 2 specifically blocks the ability of heavy meromyosin to undergo a weak to strong binding transition with actin in the presence of ATP. Removal of these lysines has no effect on strong binding in the absence of nucleotide, on the rate of ADP binding or release, or on the basal ATPase activity. We further show that the 16 amino acids of loop 2 preceding the lysine-rich region are not essential for actin activation, although they do modulate myosin's affinity for actin in the presence of ATP. We conclude that interaction of the conserved lysines with acidic residues in subdomain 1 of actin either triggers a structural change or stabilizes a conformation that is necessary for actin-activated release of P(i) and completion of the ATPase cycle.     

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.     

The regulation of subtilisin-cleaved actin by tropomyosin/troponin

Vertebrate striated muscle contraction is regulated in a Ca(2+)-dependent fashion by tropomyosin (Tm) and troponin (Tn). This regulation involves shifts in the position of Tm and Tn on actin filaments and may include conformational changes in actin that are then communicated to myosin subfragment 1 (S1). To determine whether subdomain 2 of actin plays a role in this regulation, the DNase-I loop 38-52 of this subdomain was cleaved by subtilisin between residues Met(47) and Gly(48). Despite impaired unregulated function, the potentiation and regulation of cleaved actin movement in the in vitro motility assay was not significantly different from that of uncleaved actin. Stopped-flow measurements of ADP release from regulated and unregulated cleaved acto-S1 showed a marked increase in ADP release from acto-S1 in the presence of the regulatory complex. The enhancement of the actin affinity for S1 in the presence of regulatory proteins was greater for uncleaved than for cleaved F-actin. Finally, both cleaved and uncleaved actins protect myosin loop 1 from papain cleavage equally well. Our results suggest that the potentiation of actin function in the in vitro motility assay by regulatory proteins stems from changes in cross-bridge cycle kinetics. In addition, the unimpaired calcium-sensitive regulation of cleaved actin indicates that subdomain 2 conformation does not play an essential role in the regulation process.     

Crystal structure of polymerization-competent actin

All actin crystal structures reported to date represent actin complexed or chemically modified with molecules that prevent its polymerization. Actin cleaved with ECP32 protease at a single site between Gly42 and Val43 is virtually non-polymerizable in the Ca-ATP bound form but remains polymerization-competent in the Mg-bound form. Here, a crystal structure of the true uncomplexed ECP32-cleaved actin (ECP-actin) solved to 1.9 A resolution is reported. In contrast to the much more open conformation of the ECP-actin's nucleotide binding cleft in solution, the crystal structure of uncomplexed ECP-actin contains actin in a typical closed conformation similar to the complexed actin structures. This unambiguously demonstrates that the overall structure of monomeric actin is not significantly affected by a multitude of actin-binding proteins and toxins. The invariance of actin crystal structures suggests that the salt and precipitants necessary for crystallization stabilize actin in only one of its possible conformations. The asymmetric unit cell contains a new type of antiparallel actin dimer that may correspond to the "lower dimer" implicated in F-actin nucleation and branching. In addition, symmetry-related actin-actin contacts form a head to tail dimer that is strikingly similar to the longitudinal dimer predicted by the Holmes F-actin model, including a rotation of the monomers relative to each other not observed previously in actin crystal structures.     

Evidence for the direct interaction between tightly bound divalent metal ion and ATP on actin. Binding of the lambda isomers of beta gamma-bidentate CrATP to actin

Competition between Ca2+ and Mg2+ for binding to a single high affinity site on actin has been confirmed. Occupancy of this site only by either Ca2+ or Mg2+ affects the conformation of actin and its ability to form nuclei and hydrolyze ATP. G-actin binds the beta gamma-bidentate CrATP, a substitution inert analog of metal-ATP complexes, and shows a high specificity for the lambda isomers. Binding of CrATP to ADP-actin is accompanied by the dissociation of tightly bound ADP and Ca2+. CrATP-actin shows a high tendency to form nuclei, like MgATP-actin. Polymerization of CrATP-actin is accompanied by cleavage of the gamma-phosphate, but subsequent Pi release cannot occur because the product of the reaction is the stable CrADP-Pi complex. All these results support the view that the divalent metal ion tightly bound to actin interacts with the beta- and gamma-phosphates of ATP in the nucleotide site.     

Crystal structures of monomeric actin bound to cytochalasin D

The fungal toxin cytochalasin D (CD) interferes with the normal dynamics of the actin cytoskeleton by binding to the barbed end of actin filaments. Despite its widespread use as a tool for studying actin-mediated processes, the exact location and nature of its binding to actin have not been previously determined. Here we describe two crystal structures of an expressed monomeric actin in complex with CD: one obtained by soaking preformed actin crystals with CD, and the other obtained by cocrystallization. The binding site for CD, in the hydrophobic cleft between actin subdomains 1 and 3, is the same in the two structures. Polar and hydrophobic contacts play equally important roles in CD binding, and six hydrogen bonds stabilize the actin-CD complex. Many unrelated actin-binding proteins and marine toxins target this cleft and the hydrophobic pocket at the front end of the cleft (viewing actin with subdomain 2 in the upper right corner). CD differs in that it binds to the back half of the cleft. The ability of CD to induce actin dimer formation and actin-catalyzed ATP hydrolysis may be related to its unique binding site and the necessity to fit its bulky macrocycle into this cleft. Contacts with residues lining this cleft appear to be crucial to capping and/or severing. The cocrystallized actin-CD structure also revealed changes in actin conformation. An ∼ 6° rotation of the smaller actin domain (subdomains 1 and 2) with respect to the larger domain (subdomains 3 and 4) results in small changes in crystal packing that allow the D-loop to adopt an extended loop structure instead of being disordered, as it is in most crystal structures of actin. We speculate that these changes represent a potential conformation that the actin monomer can adopt on the pathway to polymerization or in the filament.     

Nucleotide dependent differences between the alpha-skeletal and alpha-cardiac actin isoforms

The thermodynamic properties of the actin filaments prepared from cardiomyocytes were investigated with differential scanning calorimetry. This method could distinguish between the α-cardiac and α-skeletal components of the actin filaments polymerised from ADP-actin monomers by their different melting temperatures (T_m). Similar separation was not possible with filaments polymerised from ATP-actin monomers. Further analyses revealed that the activation energy (E_act) was greater for filaments of α-skeletal actin than for α-cardiac actin monomers when the filaments were polymerised from ADP-actin monomers. These results showed that the α-cardiac actin filaments were thermodynamically less stable than the filaments of α-skeletal actin and their difference was nucleotide dependent. Based on these results and considering previous observations it was concluded that the existence of two actin isoforms and their nucleotide dependent conformational differences are part of the tuning regulatory mechanism by which the cardiac muscle cells can maintain their biological function under pathological conditions.