Combining EPR with Fluorescence Spectroscopy to Monitor Conformational Changes at the Myosin Nucleotide Pocket

We used spin-labeled nucleotide analogs and fluorescence spectroscopy to monitor conformational changes at the nucleotide-binding site of wild-type Dictyostelium discoideum (WT) myosin and a construct containing a single tryptophan at position F239 near the switch 1 loop. Electron paramagnetic resonance (EPR) spectroscopy and tryptophan fluorescence have been used previously to investigate changes at the myosin nucleotide site. A limitation of fluorescence spectroscopy is that it must be done on mutated myosins containing only a single tryptophan. A limitation of EPR spectroscopy is that one infers protein conformational changes from alterations in the mobility of an attached probe. These limitations have led to controversies regarding conclusions reached by the two approaches. For the first time, the data presented here allow direct correlations to be made between the results from the two spectroscopic approaches on the same proteins and extend our previous EPR studies to a nonmuscle myosin. EPR probe mobility indicates that the conformation of the nucleotide pocket of the WT⋅SLADP (spin-labeled ADP) complex is similar to that of skeletal myosin. The pocket is closed in the absence of actin for both diphosphate and triphosphate nucleotide states. In the actin⋅myosin⋅diphosphate state, the pocket is in equilibrium between closed and open conformations, with the open conformation slightly more favorable than that seen for fast skeletal actomyosin. The EPR spectra for the mutant show similar conformations to skeletal myosin, with one exception: in the absence of actin, the nucleotide pocket of the mutant displays an open component that was approximately 4-5 kJ/mol more favorable than in skeletal or WT myosin. These observations resolve the controversies between the two techniques. The data from both techniques confirm that binding of myosin to actin alters the conformation of the myosin nucleotide pocket with similar but not identical energetics in both muscle and nonmuscle myosins.     

EPR spectra and molecular dynamics agree that the nucleotide pocket of myosin V is closed and that it opens on binding actin

We have used EPR spectroscopy and computational modeling of nucleotide-analog spin probes to investigate conformational changes at the nucleotide site of myosin V. We find that, in the absence of actin, the mobility of a spin-labeled diphosphate analog [spin-labeled ADP (SLADP)] bound at the active site is strongly hindered, suggesting a closed nucleotide pocket. The mobility of the analog increases when the MV·SLADP complex (MV = myosin V) binds to actin, implying an opening of the active site in the A·MV·SLADP complex (A = actin). The probe mobilities are similar to those seen with myosin II, despite the fact that myosin V has dramatically altered kinetics. Molecular dynamics (MD) simulation was used to understand the EPR spectra in terms of the X-ray database. The X-ray structure of MV·ADP·BeFx shows a closed nucleotide site and has been proposed to be the detached state. The MV·ADP structure shows an open nucleotide site and has been proposed to be the A·MV·ADP state at the end of the working powerstroke. MD simulation of SLADP docked in the closed conformation gave a probe mobility comparable to that seen in the EPR spectrum of the MV·SLADP complex. The simulation of the open conformation gave a probe mobility that was 35-40° greater than that observed experimentally for the A·MV·SLADP state. Thus, EPR, X-ray diffraction, and computational analysis support the closed conformation as a myosin V state that is detached from actin. The MD results indicate that the MV·ADP crystal structure, which may correspond to the strained actin-bound post-powerstroke conformation resulting from head-head interaction in the dimeric processive motor, is superopened.     

A hydrophobicity on skeletal muscle actin molecule modulated by nucleotide binding at a second site

A hydrophobic region was detected on skeletal muscle actin molecule by change of fluorescence of a hydrophobic probe, 8-anilino-1-naphthalene-sulfonate (ANS). In previous papers (Hozumi, T. (1988) Biochem. Int. 17, 171-178; Hozumi, T. (1988) J. Biochem. (Tokyo) 104, 285-288) evidences for a second nucleotide binding site on a actin molecule were reported and it was shown that nucleotide interaction at the site induces conformational changes in actin molecule. The character of non-polar region of actin molecule was altered by the binding of nucleotide at a new site of actin molecule, the fluorescence of the ANS-actin being greatly decreased, and its emission maximum undergoing a red-shift. These results show that nucleotide binding at a second site on actin changes its conformation, and the conformational change induces changes in the native surface hydrophobicity on actin molecule.     

Switch I closure simultaneously promotes strong binding to actin and ADP in smooth muscle myosin

The motor protein myosin uses energy derived from ATP hydrolysis to produce force and motion. Important conserved components (P-loop, switch I, and switch II) help propagate small conformational changes at the active site into large scale conformational changes in distal regions of the protein. Structural and biochemical studies have indicated that switch I may be directly responsible for the reciprocal opening and closing of the actin and nucleotide-binding pockets during the ATPase cycle, thereby aiding in the coordination of these important substrate-binding sites. Smooth muscle myosin has displayed the ability to simultaneously bind tightly to both actin and ADP, although it is unclear how both substrate-binding clefts could be closed if they are rigidly coupled to switch I. Here we use single tryptophan mutants of smooth muscle myosin to determine how conformational changes in switch I are correlated with structural changes in the nucleotide and actin-binding clefts in the presence of actin and ADP. Our results suggest that a closed switch I conformation in the strongly bound actomyosin-ADP complex is responsible for maintaining tight nucleotide binding despite an open nucleotide-binding pocket. This unique state is likely to be crucial for prolonged tension maintenance in smooth muscle.     

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.     

The accessibility of etheno-nucleotides to collisional quenchers and the nucleotide cleft in G- and F-actin.

Recent publication of the atomic structure of G-actin (Kabsch, W., Mannherz, H. G., Suck, D., Pai, E. F., & Holmes, K. C., 1990, Nature 347, 37-44) raises questions about how the conformation of actin changes upon its polymerization. In this work, the effects of various quenchers of etheno-nucleotides bound to G- and F-actin were examined in order to assess polymerization-related changes in the nucleotide phosphate site. The Mg(2+)-induced polymerization of actin quenched the fluorescence of the etheno-nucleotides by approximately 20% simultaneously with the increase in light scattering by actin. A conformational change at the nucleotide binding site was also indicated by greater accessibility of F-actin than G-actin to positively, negatively, and neutrally charged collisional quenchers. The difference in accessibility between G- and F-actin was greatest for I-, indicating that the environment of the etheno group is more positively charged in the polymerized form of actin. Based on calculations of the change in electric potential of the environment of the etheno group, specific polymerization-related movements of charged residues in the atomic structure of G-actin are suggested. The binding of S-1 to epsilon-ATP-G-actin increased the accessibility of the etheno group to I- even over that in Mg(2+)-polymerized actin. The quenching of the etheno group by nitromethane was, however, unaffected by the binding of S-1 to actin. Thus, the binding of S-1 induces conformational changes in the cleft region of actin that are different from those caused by Mg2+ polymerization of actin.(ABSTRACT TRUNCATED AT 250 WORDS)     

Solution properties of tetramethylrhodamine-modified G-actin

In the recently solved structure of TMR-modified ADP-G-actin, the nucleotide cleft is in a closed state conformation, and the D-loop contains an alpha-helix (L. R. Otterbein, P. Graceffa, and R. Dominguez, 2001, Science, 293:708-711). Subsequently, questions were raised regarding the possible role of the TMR label on Cys(374) in determining these aspects of G-actin structure. We show here that the susceptibility of D-loop on G-actin to subtilisin cleavage, and ATP/ADP-dependent changes in this cleavage, are not affected by TMR-labeling of actin. The TMR modification inhibits nucleotide exchange, but has no effect on DNase I binding and the fast phase of tryptic digestion of actin. These results show an absence of allosteric effects of TMR on subdomain 2, while confirming ATP/ADP-dependent changes in D-loop structure. In conjunction with similar results obtained on actin-gelsolin segment 1 complex, this works reveals the limitations of solution methods in probing the putative open and closed nucleotide cleft states of G-actin.     

Dynamics of the nucleotide pocket of myosin measured by spin-labeled nucleotides

We have used electron paramagnetic probes attached to the ribose of ATP (SL-ATP) to monitor conformational changes in the nucleotide pocket of myosin. Spectra for analogs bound to myosin in the absence of actin showed a high degree of immobilization, indicating a closed nucleotide pocket. In the Actin.Myosin.SL-AMPPNP, Actin.Myosin.SL-ADP.BeF(3), and Actin.Myosin.SL-ADP.AlF(4) complexes, which mimic weakly binding states near the beginning of the power stroke, the nucleotide pocket remained closed. The spectra of the strongly bound Actin.Myosin.SL-ADP complex consisted of two components, one similar to the closed pocket and one with increased probe mobility, indicating a more open pocket, The temperature dependence of the spectra showed that the two conformations of the nucleotide pocket were in equilibrium, with the open conformation more favorable at higher temperatures. These results, which show that opening of the pocket occurs only in the strongly bound states, appear reasonable, as this would tend to keep ADP bound until the end of the power stroke. This conclusion also suggests that force is initially generated by a myosin with a closed nucleotide pocket.     

Kinetic and spectroscopic evidence for three actomyosin:ADP states in smooth muscle

Smooth muscle myosin II undergoes an additional movement of the regulatory domain with ADP release that is not seen with fast skeletal muscle myosin II. In this study, we have examined the interactions of smooth muscle myosin subfragment 1 with ADP to see if this additional movement corresponds to an identifiable state change. These studies indicate that for this myosin:ADP, both the catalytic site and the actin-binding site can each assume one of two conformations. Relatively loose coupling between these two binding sites leads to three discrete actin-associated ADP states. Following an initial, weakly bound state, binding of myosin:ADP to actin shifts the equilibrium toward a mixture of two states that each bind actin strongly but differ in the conformation of their catalytic sites. By contrast, fast myosins, including Dictyostelium myosin II, have reciprocal coupling between the actin- and ADP-binding sites, so that either actin or nucleotide, but not both, can be tightly bound. This uncoupling, which generates a second strongly bound actomyosin ADP state in smooth muscle, would prolong the fraction of the ATPase cycle time that this actomyosin spends in a force-generating conformation and may be central to explaining the physiologic differences between this and other myosins.     

The open nucleotide pocket of the profilin/actin x-ray structure is unstable and closes in the absence of profilin

The open nucleotide pocket conformation of actin in the profilin:actinCaATP x-ray structure has been hypothesized to be a crucial intermediate for nucleotide exchange in the actin depolymerization/polymerization cycle. The requirement for ancillary modification of actin for crystallization leads to ambiguities in this interpretation, however. We have used molecular dynamics simulations to model the thermodynamic properties of the actin x-ray structure, outside the crystal lattice, in an aqueous environment with profilin removed. Our simulations show that the open-nucleotide-pocket, profilin-free structure is actually unstable, and closes. The coordination of actin to the nucleotide in the molecular-dynamics-derived closed structure is virtually identical to that in the closed profilin:actinSrATP x-ray structure. Thus, there is currently no thermodynamically stable structure representing the open-nucleotide-pocket state of actin.     

Molecular Dynamics Simulation Studies of dTTP Binding and Catalysis Mediated by YhdE Dimerization

YhdE is a Maf-like (multicopy associated filamentation) protein that primarily acts as dTTPase to hydrolyze dTTP into dTMP and two phosphate molecules in cell metabolism pathway. Two crystal structures of YhdE have been previously determined, representing the open and closed active site conformations, respectively. Based on the structures, we have carried out molecular dynamics simulations and free energy calculations to investigate dTTP binding to and hydrolysis by YhdE. Our results suggest that YhdE closed state is structurally more compact than its open state at room temperature. YhdE open state is a favorable conformation for dTTP binding and closed state is a structurally favorable conformation for catalytic reaction. This observation is supported by the structure of YhdE homolog in complex with a nucleotide analog. Free energy calculations reveal that YhdE dimerization occurs preferentially in dTTP binding and is favorable for successive cooperative reaction. The key residues R11, R12 and K80, are found to contribute to the substrate stabilization. Further, YhdE dimerization and binding of dTTP induce the cooperative effect through a direct allosteric communication network in YhdE from the dTTP binding sites in the catalytic center to the intermolecular β-strand in YhdE dimer.     

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.     

A Nucleotide State-sensing Region on Actin

The nucleotide state of actin (ATP, ADP-P_i, or ADP) is known to impact its interactions with other actin molecules upon polymerization as well as with multiple actin binding proteins both in the monomeric and filamentous states of actin. Recently, molecular dynamics simulations predicted that a sequence located at the interface of subdomains 1 and 3 (W-loop; residues 165–172) changes from an unstructured loop to a β-turn conformation upon ATP hydrolysis (Zheng, X., Diraviyam, K., and Sept, D. (2007) Biophys. J. 93, 1277–1283). This region participates directly in the binding to other subunits in F-actin as well as to cofilin, profilin, and WH2 domain proteins and, therefore, could contribute to the nucleotide sensitivity of these interactions. The present study demonstrates a reciprocal communication between the W-loop region and the nucleotide binding cleft on actin. Point mutagenesis of residues 167, 169, and 170 and their site-specific labeling significantly affect the nucleotide release from the cleft region, whereas the ATP/ADP switch alters the fluorescence of probes located in the W-loop. In the ADP-P_i state, the W-loop adopts a conformation similar to that in the ATP state but different from the ADP state. Binding of latrunculin A to the nucleotide cleft favors the ATP-like conformation of the W-loop, whereas ADP-ribosylation of Arg-177 forces the W-loop into a conformation distinct from those in the ADP and ATP-states. Overall, our experimental data suggest that the W-loop of actin is a nucleotide sensor, which may contribute to the nucleotide state-dependent changes in F-actin and nucleotide state-modulated interactions of both G- and F-actin with actin-binding proteins.     

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.     

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.     

Substrate-induced fit of the ATP binding site of cytidine monophosphate kinase from Escherichia coli: time-resolved fluorescence of 3'-anthraniloyl-2'-deoxy-ADP and molecular modeling

The conformation and dynamics of the ATP binding site of cytidine monophosphate kinase from Escherichia coli (CMPK(coli)), which catalyzes specifically the phosphate exchange between ATP and CMP, was studied using the fluorescence properties of 3'-anthraniloyl-2'-deoxy-ADP, a specific ligand of the enzyme. The spectroscopic properties of the bound fluorescent nucleotide change strongly with respect to those in aqueous solution. These changes (red shift of the absorption and excitation spectra, large increase of the excited state lifetime) are compared to those observed in different solvents. These data, as well as acrylamide quenching experiments, suggest that the anthraniloyl moiety is protected from the aqueous solvent upon binding to the ATP binding site, irrespective of the presence of CMP or CDP. The protein-bound ADP analogue exhibits a restricted fast subnanosecond rotational motion, completely blocked by CMP binding. The energy-minimized models of CMPK(coli) complexed with 3'-anthraniloyl-2'-deoxy-ADP using the crystal structures of the ligand-free protein and of its complex with CDP (PDB codes and, respectively) were compared to the crystal structure of UMP/CMP kinase from Dictyostelium discoideum complexed with substrates (PDB code ). The key residues for ATP/ADP binding to CMPK(coli) were identified as R157 and I209, their side chains sandwiching the adenine ring. Moreover, the residues involved in the fixation of the phosphate groups are conserved in both proteins. In the model, the accessibility of the fluorescent ring to the solvent should be substantial if the LID conformation remained unchanged, by contrast to the fluorescence data. These results provide the first experimental arguments about an ATP-mediated induced-fit of the LID in CMPK(coli) modulated by CMP, leading to a closed conformation of the active site, protected from water.     

Detection of conformational changes in actin by proteolytic digestion: Evidence for a new monomeric species

When KCl is added to a solution of G-actin to induce full polymerization, a decrease in the rate at which actin undergoes enzymatic proteolysis occurs. This decrease cannot be accounted for by factors affecting the enzymes employed, but rather appears to be due to a change in the conformation of G-actin. Partially polymerized actin solutions also show a reduction in digestibility which is dependent on the F-actin content, suggesting that F-actin is essentially indigestible. Moreover, low rates of digestion were also observed at sub-critical actin concentrations, where actin in the presence of 0.1 m-KCl does not polymerize. This indicates that a confomational change occurs in G-actin before the polymerization step.At sub-critical concentrations in 0.1 m-KCl, actin is in a truly monomeric state as judged by its viscosity characteristics, its inability to enhance the rate of polymerization of G-actin and its possession of ATP as the actin-bound nucleotide. These data support the existence of a new species of actin, called F-ATP-actin monomer, which has the same physical properties and the same bound nucleotide as G-actin, but digestion characteristics like F-actin. Since F-ATP-actin monomers have the same low susceptibility to proteolysis as F-ADP-actin polymers, and because both G-ATP-actin and G-ADP-actin have similar high rates of digestion, the observed change in the conformation of actin cannot be due to the phosphorylated state of the actin-bound nucleotide. Instead, the conformational change appears to be caused by the addition of KCl to G-actin.The newly-detected monomeric species is considered to be an intermediate in the polymerization process where F-ATP-actin monomers form a population of polymerizable molecules which must reach a critical concentration before nucleation and F-actin polymer formation begin.     

Photoaffinity labeling of the nucleotide binding site of actin

Rabbit skeletal muscle actin was photoaffinity-labeled by the nucleotide analogue 8-azidoadenosine 5'-triphosphate. In both G-actin and F-actin about 25% covalent incorporation was achieved. The labeled actins were digested with cyanogen bromide, and the labeled peptides were isolated and sequenced. In F-actin the label was bound primarily to Lys-336, while in G-actin the label was bound to Lys-336 or to Trp-356. The results indicate that the nucleotide binding site is near the phalloidin binding site of actin [Vanderkerckhove, J., Deboben, A., Nassal, M., & Wieland, T. (1985) EMBO J. 4, 2815-2818]. The binding of the azido group to Trp-356 in G-actin but not in F-actin may indicate that a change in the conformation of actin occurs in this region.     

Effects of various amino acid replacements on the conformational stability of G-actin

Circular dichroic spectra of native, EDTA-treated and heat-denatured G-actin from chicken gizzard smooth muscle are virtually the same as those of rabbit skeletal muscle actin. The rates of changes produced by EDTA or heat in the secondary structure are, however, higher in the case of gizzard actin. Similar differences were found in the rates of inactivation as measured by loss of polymerizability during incubation with EDTA or Dowex 50. The results are explicable in terms of local differences in the conformation at specific site(s) important for maintaining the native state of actin monomer. Involvement of the ATP binding site was shown by measuring the equilibrium constant for the binding of ATP to the two actins. Difference in the conformation of some additional site(s) is indicated by a higher rate constant of inactivation of nucleotide-free actin observed for gizzard actin. No significant difference was found in the equilibrium constant for the binding of Ca2+ at the single high-affinity site in gizzard and skeletal muscle actin. Comparison of inactivation kinetics of actin from chicken gizzard, rabbit skeletal, bovine aorta, and bovine cardiac muscle suggests that the amino acid replacements Val-17----Cys-17 and/or Thr-89----Ser-89 have a destabilizing effect on the native conformation of G-actin. The results indicate that deletion of the acidic residue at position 1 of the amino acid sequence has no effect on the conformation of the ATP binding site and the high-affinity site for divalent cation as well.     

The crystal structure of the actin binding domain from alpha-actinin in its closed conformation: structural insight into phospholipid regulation of alpha-actinin

Alpha-actinin is the major F-actin crosslinking protein in both muscle and non-muscle cells. We report the crystal structure of the actin binding domain of human muscle alpha-actinin-3, which is formed by two consecutive calponin homology domains arranged in a "closed" conformation. Structural studies and available biochemical data on actin binding domains suggest that two calponin homology domains come in a closed conformation in the native apo-form, and that conformational changes involving the relative orientation of the two calponin homology domains are required for efficient binding to actin filaments. The actin binding activity of muscle isoforms is supposed to be regulated by phosphatidylinositol 4,5-bisphosphate (PtdIns(4,5)P2), which binds to the second calponin homology domain. On the basis of structural analysis we propose a distinct binding site for PtdIns(4,5)P2, where the fatty acid moiety would be oriented in a direction that allows it to interact with the linker sequence between the actin binding domain and the first spectrin-like repeat, regulating thereby the binding of the C-terminal calmodulin-like domain to this linker.