Actin filament dynamics in the actomyosin VI complex is regulated allosterically by calcium-calmodulin light chain

The contractile and enzymatic activities of myosin VI are regulated by calcium binding to associated calmodulin (CaM) light chains. We have used transient phosphorescence anisotropy to monitor the microsecond rotational dynamics of erythrosin-iodoacetamide-labeled actin with strongly bound myosin VI (MVI) and to evaluate the effect of MVI-bound CaM light chain on actin filament dynamics. MVI binding lowers the amplitude but accelerates actin filament microsecond dynamics in a Ca²⁺- and CaM-dependent manner, as indicated from an increase in the final anisotropy and a decrease in the correlation time of transient phosphorescence anisotropy decays. MVI with bound apo-CaM or Ca²⁺-CaM weakly affects actin filament microsecond dynamics, relative to other myosins (e.g., muscle myosin II and myosin Va). CaM dissociation from bound MVI damps filament rotational dynamics (i.e., increases the torsional rigidity), such that the perturbation is comparable to that induced by other characterized myosins. Analysis of individual actin filament shape fluctuations imaged by fluorescence microscopy reveals a correlated effect on filament bending mechanics. These data support a model in which Ca²⁺-dependent CaM binding to the IQ domain of MVI is linked to an allosteric reorganization of the actin binding site(s), which alters the structural dynamics and the mechanical rigidity of actin filaments. Such modulation of filament dynamics may contribute to the Ca²⁺- and CaM-dependent regulation of myosin VI motility and ATP utilization.     

Rotational dynamics of spin-labeled F-actin in the sub-millisecond time range.

The rotational motions of F-actin filaments and myosin heads attached to them have been measured by saturation transfer electron paramagnetic resonance spectroscopy using spin-labels rigidly bound to actin, or to the myosin head region in intact myosin molecules, heavy meromyosin, and subfragment-1. The spin-label attached to F-actin undergoes rotational motion having an effective correlation time of the order of 10^?4 seconds. This cannot be interpreted as rotation of the entire F-actin filament or local rotation of the spin-label, but must represent an internal rotational mode of F-actin, possibly a bending or flexing motion, or a rotation of an actin monomer or a segment of it. The rate of this rotational motion is reduced approximately fourfold by myosin, HMM or S-1; HMM and S-1 are equally effective, on a molar basis, in slowing this rotation and both produce their maximal effect at a ratio of about one molecule of HMM or S-1 per ten actin monomers. With chymotryptic S-1, the effect is partially reversed at higher concentrations. With S-1 prepared with papain in the presence of Mg²⁺, the reversal is smaller, while with HMM or myosin there is no reversal at higher concentrations. Tropomyosin slightly decreases the actin rotational mobility, and the addition of HMM to the actin-tropomyosin complex produces a further slowing. The rotational correlation time for acto-HMM is the same whether the spin-label is on actin or HMM, indicating that the rotation of the head region of HMM when bound to F-actin is controlled by a mode of rotation within the F-actin filaments.     

Polarized fluorescence from epsilon-ADP incorporated into F-actin in a myosin-free single fiber: conformation of F-actin and changes induced in it by heavy meromyosin.

Fluorescent ADP analog, ε-ADP (1:N⁶-ethenoadenosine 5′-diphosphate), was incorporated into F-actin in a myosin-free ghost single fiber and polarized fluorescence measurements were performed under a microspectrophotometer to investigate the conformation of F-actin and the changes induced in it by heavy meromyosin and subfragment-1. Four components of polarized fluorescence were obtained by exciting the fiber with light polarized parallel and perpendicular to the long axis of the fiber and measuring the intensity of emission polarized parallel and perpendicular. From these data it was shown that F-actin in the fiber was not rigid but flexible, with a value for the elastic modulus for bending of 5.3 × 10^?17 dyn cm². The angles of absorption dipole and emission dipole of bound ε-ADP with the long axis of F-actin were both about 75 °.The binding of heavy meromyosin decreased the elastic modulus of F-actin by 30% and the angles of absorption and emission dipoles by 2.5 ° and 1.5 °, respectively. The molar ratios of bound heavy meromyosin and subfragment-1 to actin in the ghost fiber at saturation were 0.3 and 0.6, respectively, being smaller than those in solution.     

Cooperativity in F-actin filaments on binding of myosin subfragments, demonstrated by fluorescence of 1, N6- ethenoadenosine diphosphate.

The fluorescence lifetime of 1,N⁶-ethenoadenosine diphosphate (?-ADP) is 33 ns when bound to F-actin at 4 °C. When heavy meromyosin or myosin subfragment-1 binds to the F-actin filament, the lifetime of ?-ADP drops, reaching 29 ns when every actin monomer is bound to a myosin head. The change in lifetime is a consequence of cooperative conformational changes among the actin monomers. The results of these experiments support the contention that there are differences in the ways in which the two heads of the myosin molecule interact with the actin filament.     

Tropomyosin dynamics in cardiac thin filaments: a multisite forster resonance energy transfer and anisotropy study

Cryoelectron microscopy studies have identified distinct locations of tropomyosin (Tm) within the Ca²⁺-free, Ca²⁺-saturated, and myosin-S1-saturated states of the thin filament. On the other hand, steady-state Förster resonance energy transfer (FRET) studies using functional, reconstituted thin filaments under physiological conditions of temperature and solvent have failed to detect any movement of Tm upon Ca²⁺ binding. In this investigation, an optimized system for FRET and anisotropy analyses of cardiac tropomyosin (cTm) dynamics was developed that employed a single tethered donor probe within a Tm dimer. Multisite FRET and fluorescence anisotropy analyses showed that S1 binding to Ca²⁺ thin filaments triggered a uniform displacement of cTm toward F-actin but that Ca²⁺ binding alone did not change FRET efficiency, most likely due to thermally driven fluctuations of cTm on the thin filament that decreased the effective separation of the donor probe between the blocked and closed states. Although Ca²⁺ binding to the thin filament did not significantly change FRET efficiency, such a change was demonstrated when the thin filament was partially saturated with S1. FRET was also used to show that stoichiometric binding of S1 to Ca²⁺-activated thin filaments decreased the amplitude of Tm fluctuations and revealed a strong correlation between the cooperative binding of S1 to the closed state and the movement of cTm.     

Ca2+ regulation of gelsolin activity: binding and severing of F-actin.

Regulation of the F-actin severing activity of gelsolin by Ca2+ has been investigated under physiologic ionic conditions. Tryptophan fluorescence intensity measurements indicate that gelsolin contains at least two Ca2+ binding sites with affinities of 2.5 x 10(7) M-1 and 1.5 x 10(5) M-1. At F-actin and gelsolin concentrations in the range of those found intracellularly, gelsolin is able to bind F-actin with half-maximum binding at 0.14 microM free Ca2+ concentration. Steady-state measurements of gelsolin-induced actin depolymerization suggest that half-maximum depolymerization occurs at approximately 0.4 microM free Ca2+ concentration. Dynamic light scattering measurements of the translational diffusion coefficient for actin filaments and nucleated polymerization assays for number concentration of actin filaments both indicate that severing of F-actin occurs slowly at micromolar free Ca2+ concentrations. The data suggest that binding of Ca2+ to the gelsolin-F-actin complex is the rate-limiting step for F-actin severing by gelsolin; this Ca2+ binding event is a committed step that results in a Ca2+ ion bound at a high-affinity, EGTA-resistant site. The very high affinity of gelsolin for the barbed end of an actin filament drives the binding reaction equilibrium toward completion under conditions where the reaction rate is slow.     

Time-resolved fluorescence depolarization measurements of F-actin binding to myosin subfragments-1 bearing different alkali light chains.

Experiments were designed to test for functional differences which might shed light on the differences in actin-activated ATPase activities recently reported for myosin subfragments-1 bearing different light chains. By using the method of A. G. Weeds and R. S. Taylor (1975, Nature (London)257, 54), two types of subfragment-1 (S-1) from myosin of rabbit fast skeletal muscle were prepared: (S-1)·A1 and (S-1)·A2 bearing, respectively, the alkali-1 and alkali-2 light chains. (In agreement with the findings of these investigators, actin enhanced the ATPase activity of (S-1)·A1 more than that of (S-1)·A2 at lower actin concentrations.) Through use of time-resolved fluorescence depolarization techniques, the affinity constants for the binding of the two types of S-1 to F-actin in the absence of ATP were found to be very similar: 3.4 ± 0.3 × 10⁶m^?1 (N = 10) for (S-1)·A1 and 3.9 ± 0.2 × 10⁶m^?1 (N = 7) for (S-1)·A2 of one preparation, and 6.4 ± 0.2 × 10⁶m^?1 (N = 6) for (S-1)·A1 and 7.7 ± 0.5 × 10⁶m^?1 (N = 12) for (S-1)·A2 of another preparation (pH 7.0, 25 °C, 0.28 m KCl, 1.5 mm MgCl₂, 0.5 mm ethylene glycol bis (β-aminoethyl ether) N,N′-tetracetic acid, 10 mm imidazole, and 0.1 mmN-tris (hydroxymethyl) methyl-2-aminoethane sulfonate). The affinity constants for the two species of S-1 and actin also have a similar dependence on ionic strength and are not affected by addition of 0.6 mm CaCl₂ to the above solution. The CaATPase (or the CaITPase) activities of the two species of S-1 show the same pH dependence.     

Effect of Ca2+ Ions on the Viscometric Behavior of F-actin

Changes in the viscosity of the F-actin solutions which occur on addition of Ca²⁺ ions were investigated. The viscosity of F-actin decreased on addition of Ca²⁺ ions. The amount of Ca²⁺ ions needed to decrease the viscosity changed with pH of the solution, namely, 20~30 mm at pH 7, 15~20 mm at pH 6 and 5~10mm at pH 5.5. Other divalent cations had the same action on F-actin, but monovalent cations did not affect the F-actin viscosity even at the concentration as high as 1 m. Intrinsic viscosity of F-actin with and without Ca²⁺ions was 250 ±40 (ml/g) and 670 ±80 (ml/g), respectively. The cause of this viscosity change was discussed from the results of electron microscopic observation and light scattering measurements.     

The N-terminal domains of myosin binding protein C can bind polymorphically to F-actin

The regulation of vertebrate striated muscle contraction involves a number of different molecules, including the thin-filament accessory proteins tropomyosin and troponin that provide Ca²⁺-dependent regulation by controlling access to myosin binding sites on actin. Cardiac myosin binding protein C (cMyBP-C) appears to modulate this Ca²⁺-dependent regulation and has attracted increasing interest due to links with inherited cardiac diseases. A number of single amino acid mutations linked to clinical diseases occur in the N-terminal region of cMyBP-C, including domains C0 and C1, which previously have been shown to bind to F-actin. This N-terminal region also has been shown to both inhibit and activate actomyosin interactions in vitro. Using electron microscopy and three-dimensional reconstruction, we show that C0 and C1 can each bind to the same two distinctly different positions on F-actin. One position aligns well with the previously reported binding site that clashes with the binding of myosin to actin, but would force tropomyosin into an “on” position that exposes myosin binding sites along the filament. The second position identified here would not interfere with either myosin binding or tropomyosin positioning. It thus appears that the ability to bind to at least two distinctly different positions on F-actin, as observed for tropomyosin, may be more common than previously considered for other actin binding proteins. These observations help to explain many of the seemingly contradictory results obtained with cMyBP-C and show how cMyBP-C can provide an additional layer of regulation to actin-myosin interactions. They also suggest a redundancy of C0 and C1 that may explain the absence of C0 in skeletal muscle.     

Stability differences of muscle F-actin in formamide in the presence of Mg2+ and Ca2+

Muscle G-actin was polymerized by addition of 2 mM Mg²⁺ or 2 mM Ca²⁺. Subsequent addition of formamide reduced the specific viscosity of the polymer solution. However, kinetic analysis of this reduction in the presence or absence of 0.1 M KCl revealed differences between F-actin formed in the presence of Mg²⁺ and F-actin formed in the presence of Ca²⁺. In the presence of Mg²⁺ the viscosity dropped instantaneously, reaching within minutes a steady-state level that was constant for many hours. In contrast, in the presence of Ca²⁺ the high-shear viscosity continued to decrease slowly after an initial drop, and it could take hours until a quasi-equilibrium was obtained. The time was dependent on both formamide and protein concentration. Addition of formamide increased the critical actin concentration in the presence of Ca²⁺, but not in the presence of Mg²⁺. This is taken as evidence that in the presence of Ca²⁺, but not in the presence of Mg²⁺, formamide causes partial depolymerization of F-actin.     

Properties of the complexes formed by 1-anilinonaphthalene-8-sulfonate with phosphorylase kinase and calmodulin

Phosphorylase kinase contains four approximately equivalent binding sites for 1-anilinonaphthalene-8-sulfonate (1,8-ANS). Measurements of the time decay of fluorescence anisotropy have failed to give any indication of internal degrees of rotational freedom involving a significant portion of the tertiary structure. In the presence of 1 mM Ca²⁺, calmodulin binds one molecule of 1,8-ANS. No binding occurs in the absence of Ca²⁺. The binding is strongly temperature-dependent, a decrease in binding occurring with increasing temperature. Determinations of the time decay of fluorescence anisotropy indicate the presence of internal rotations, which become more important with increasing temperature. Complex formation between phosphorylase kinase and calmodulin reduces the binding of 1,8-ANS.     

Pathways that control cortical F-actin dynamics during secretion

Chromaffin cells possess a mesh of filamentous actin underneath the plasma membrane which acts as a barrier to the chromaffin vesicles access to exocytotic sites. Disassembly of cortical F-actin in response to stimulation allows the movement of vesicles from the reserve pool to the release-ready vesicle pool and, therefore, to exocytotic sites. The dynamics of cortical F-actin is controlled by two mechanisms: a) stimulation-induced Ca²⁺ entry and scinderin activation and b) protein kinase C (PKC) activation and MARCKS phosphorylation as demonstrated here by experiments with recombinant proteins, antisense olygodeoxynucleotides and vector mediated transient expressions. Under physiological conditions (i.e., cholinergic receptor stimulation followed by Ca²⁺ entry), mechanism (a) is the most important for the control of cortical F-actin network whereas when Ca²⁺ is released from intracellular stores (i.e., histamine stimulation) cortical F-actin is regulated mainly by mechanism b.     

Thermodynamics and molecular dynamics simulations of calcium binding to the regulatory site of human cardiac troponin C: evidence for communication with the structural calcium binding sites

Human cardiac troponin C (HcTnC), a member of the EF hand family of proteins, is a calcium sensor responsible for initiating contraction of the myocardium. Ca²⁺ binding to the regulatory domain induces a slight change in HcTnC conformation which modifies subsequent interactions in the troponin–tropomyosin–actin complex. Herein, we report a calorimetric study of Ca²⁺ binding to HcTnC. Isotherms obtained at 25 °C (10 mM 2-morpholinoethanesulfonic acid, 50 mM KCl, pH 7.0) provided thermodynamic parameters for Ca²⁺ binding to both the high-affinity and the low-affinity domain of HcTnC. Ca²⁺ binding to the N-domain was shown to be endothermic in 2-morpholinoethanesulfonic acid buffer and allowed us to extract the thermodynamics of Ca²⁺ binding to the regulatory domain. This pattern stems from changes that occur at the Ca²⁺ site rather than structural changes of the protein. Molecular dynamics simulations performed on apo and calcium-bound HcTnC_1–89 support this claim. The values of the Gibbs free energy for Ca²⁺ binding to the N-domain in the full-length protein and to the isolated domain (HcTnC_1–89) are similar; however, differences in the entropic and enthalpic contributions to the free energy provide supporting evidence for the cooperativity of the C-domain and the N-domain. Thermograms obtained at two additional temperatures (10 and 37 °C) revealed interesting trends in the enthalpies and entropies of binding for both thermodynamic events. This allowed the determination of the change in heat capacity (?C _p ) from a plot of ?H verses temperature and may provide evidence for positive cooperativity of Ca²⁺ binding to the C-domain.     

Fluorescence dynamics studies of troponin C

The time decay of fluorescence anisotropy for a dansylaziridine (DANZ) conjugate with Met-25, which lies within the N-terminal lobe of troponin C (TnC), shows at 10 and 25°C a longer correlation time characteristic of the entire molecule and a shorter correlation time arising from a more localized motion of the probe. In the absence of Ca²⁺, the amplitude of the shorter correlation time increases, suggesting an increased mobility of the probe. At 40°C, in both the absence and presence of Ca²⁺, a significant increase in probe mobility occurs. A 2,6-toluidinyl naphthalene sulfonate (2,6-TNS) complex with Ca²⁺-liganded TnC shows only the longer correlation time at 12 and 25°C. An N-(iodoacetylaminoethyl-5-naphthylamine-1-sulfonate) conjugate with Cys-98 shows both a long and a short correlation time; the amplitude of the shorter correlation time is greater than for the DANZ conjugate. At 9, 25, and 40°C in the presence of Ca²⁺, and at 9°C in its absence, the magnitude of the long correlation time is consistent with motion of the entire molecule; at higher temperatures in the absence of Ca²⁺ it is substantially smaller, suggesting the presence of internal rotation. For Ca²⁺-liganded TnC at temperatures of 25°C or lower, the results with all three labels are interpretable in terms of the crystallographic structure of TnC.     

Timemresolved fluorescence of S-100a protein: effect of Ca, Mg and unilamellar vesicles of egg phosphatidylcholine

Phase-modulation fluorescence lifetime measurements were used to study the single Trp residue of the Ca²⁺-binding protein S-100a both in the absence and in the presence of Ca²⁺ and/or Mg²⁺. Trp fluorescence decay for the protein was satisfactorily described by Lorentzian lifetime distributions centered around two components (approximately 4 ns and 0.5 ns). Lifetime values were unchanged by 2 mM Ca²⁺, but the fractional intensity associated with longer lifetime increased up to 75%. In the presence of Mg²⁺, the Ca²⁺ induced increase of the fractional intensity associated with longer lifetime was only 57%. For the protein in buffer, about the 85% of the recovered anisotropy was associated to a rotational correlation time of 6.7 ns. After the addition of Ca²⁺, this value was increased to 16.08 ns. In the presence of Mg²⁺, Ca⁺² increased the rotational correlation time to 33.75 ns. Similar studies were performed with S-100a interacting with egg phosphatidylcholine vesicles (SUV). Our data suggest that the conformation of the protein may be influenced by structural features of the lipidic membrane. Moreover, data obtained in the presence of Mg²⁺ indicate some interaction between lipids and S-100, likely mediated by this ion.     

Molecular cloning and functional expression of chromaffin cell scinderin indicates that it belongs to the family of Ca2+-dependent F-actin severing proteins

Scienderin is a Ca⁺-dependent actin filament severing protein present in chromaffin cells, platelets and a variety of secretory cells. It has been suggested that scinderin is involved in chromaffin cell F-actin dynamics and that this actin network controls the delivery of secretory vesicles to plasma membrane exocytotic sites. Moreover, scinderin redistribution and activity may be regulated by pH and Ca²⁺ in resting and stimulated cells. Here we describe the molecular cloning, the nucleotide sequence and the expression of bovine chromaffin cell scinderin cDNA. The fusion protein obtained cross-reacts with native scinderin antibodies and binds phosphatidylserine (PS), phosphatidylinositol 4,5-bisphosphate (PIP₂) and actin in a Ca⁺-dependent manner. Antibodies raised against the fusion protein produced the same cellular staining patterns for scinderin as anti-native scinderin. Nucleotide and amino acid sequence analysis indicate that scinderin has six domains each containing three internal sequence motifs, two actin and two PIP₂ binding sites and has 63 and 53% homology with gelsolin and villin. These data indicate that scinderin is a novel member of the family of Ca²⁺-dependent F-actin severing proteins which includes gelsolin and villin.Abbreviations PIP₂ phosphatidylinositol 4,5 bisphosphate - PKC protein kinase C - Sc scinderin - PS phosphatidyl serine - F-Sc scinderin fusion protein - PCR polymerase chain reaction     

Compressibility and specific volume of actin decrease upon G to F transformation

We measured the densities as well as the sound velocities in solutions of G-actin, F-actin and the reconstituted thin filament. Using the data obtained, we determined their partial specific volumes and partial specific adiabatic compressibilities. The objectives were to investigate the volume change of actin upon polymerization and to detect the conformational change associated with the Ca²⁺-binding to the reconstituted thin filament. The partial specific volume and the partial specific adiabatic compressibility of G-actin were 0.749 cm³/g and 9.3 · 10⁻¹² cm²/dyne, respectively. The results suggest that G-actin is a rather soft protein compared with other globular proteins. The partial specific volumes of F-actin were in a range of 0.63–0.66 cm³/g depending on the solvent conditions. The partial specific adiabatic compressibilities of F-actin were negative (−(7–13) · 10⁻¹² cm³/dyne). These data indicate that the amount of hydration may increase by several times upon polymerization assuming that the size of the cavity remains constant. We detected little difference between the partial specific adiabatic compressibility of the reconstituted thin filament in a Ca²⁺-bound state and that in a Ca²⁺-unbound state. This suggests that the Ca²⁺ binding affected not the subunit itself but the inter-subunit junction.     

Fluorimetric studies of actin labeled with dansyl aziridine.

F-actin has been specifically labeled with a fluorescent probe, dansyl aziridine, at cysteine-373 of the protein. The fluorescence property of the conjugated probe serves as a spectroscopic indicator of several processes in which actin participates. The sulfhydryl modification does not impair the G-F transformation of actin, nor does it affect the complex formation of actin and myosin or the dissociation of the complex by ATP as judged by viscosity measurements. However, both labeled actin and actin modified by N-ethylmaleimide, which also reacts at cysteine-373, stimulate the Mg²⁺-ATPase of myosin only about 75% as well as unmodified actin. The probe attached to actin exhibits a 65-nm blue shift of its emission maximum from 560 to 495 nm and a sixfold fluorescence enhancement indicating that it is located in a hydrophobic environment. The excitation spectrum of labeled actin indicates that a tryptophan and a tyrosine residue are close to the probe and transfer excitation energy to the dansyl fluorophore. Upon depolymerization of F-actin, the fluorescence intensity of labeled actin increases about 20%. The fluorescence of labeled actin is also enhanced by the addition of EDTA, ATP, and pyrophosphate, but Mg²⁺ antagonizes this effect reversibly. However, in the presence of 10 mm orthophosphate buffer (pH 7.4) these effects disappear. When labeled F-actin binds with myosin subfragment-1 (SF-1) or heavy meromyosin (HMM), the fluorescence of the actin adduct is enhanced. The fluorescence properties of labeled acto-SF-1 and acto-HMM become insensitive to EDTA and polyphosphates even in the absence of orthophosphate. These results suggest that the two-stranded helical structure of the F-actin filament is stabilized by the presence of phosphate and/or the binding of the myosin “head”.     

Binding of 1,N6-ethanoadenosine triphosphate to actin

G-actin is known to bind one molecule of ATP. Its polymerization to F-actin is accompanied by the splitting off of the terminal phosphate of the bound nucleotide. We have found that the fluorescent 1,N⁶-ethanoadenosine triphosphate (?ATP) can substitute for ATP in G-actin and that G-actin containing bound ?ATP possesses essentially full polymerizability. The binding of this ATP analog has been studied by following the inactivation of the ?ATP·G-actin complex. The binding constant (4?5.7 × 10⁶ M^?1) obtained in the absence of EDTA is about 50% of that for ATP, while the binding constant obtained in the presence of EDTA (0.9?3.0 × 10⁵ M^?1) is comparable to those for ATP and ADP. These findings suggest that ?ATP can be used as a structural probe for actin. The fluorescence lifetime of ?ATP bound to G·actin is 36 nsec. The rotational relaxation time of ?ATP·G-actin is near 60 nsec. at 20°C.     

The mechanochemical basis of amoeboid movement: II. Cytoplasmic filament stability at low divalent cation concentrations

The role played by Ca²⁺ in the stability of cytoplasmic actin and myosin filaments was investigated ultrastructurally with negatively stained isolated cytoplasm from Chaos carolinensis. Cytoplasm was incubated in solutions containing 5, 10, 15 and 25 mM EGTA for periods of time varying from 2 to 20 min. As either the EGTA concentration or duration of incubation was increased, the extent of myosin and actin filament depolymerization increased. The actin filaments depolymerized except where they were stabilized by interaction with myosin. With longer incubation times or higher EGTA concentrations complete depolymerization of the actin filaments could be accomplished. Myosin aggregates also disassembled and became shorter, while monomeric myosin labelled adjacent thin filaments to form arrowhead complexes resembling myosin enriched actomyosin [1]. These actomyosin complexes were relatively stable at low Ca²⁺ concentrations. In addition, the complexes showed a characteristic 35 nm periodicity and were dissociable in the presence of Mg²⁺-ATP. The actin containing filaments were more labile at low Ca²⁺ concentrations than the myosin aggregates. These results suggest that in cells capable of regulating their Ca²⁺ concentrations efficiently, filament polymerization-depolymerization could play a role in the control of cytoplasmic streaming.