Motion of actin filaments in the presence of myosin heads and ATP.

We measured, by fluorescence correlation spectroscopy, the motion of actin filaments in solution during hydrolysis of ATP by acto-heavy meromyosin (acto-HMM). The method relies on the fact that the intensity of fluorescence fluctuates as fluorescently labeled actin filaments enter and leave a small sample volume. The rapidity of these number fluctuations is characterized by the autocorrelation function, which decays to 0 in time that is related to the average velocity of translation of filaments. The time of decay of the autocorrelation function of bare actin filaments in solution was 10.59 +/- 0.85 s. Strongly bound (rigor) heads slowed down the diffusion. Direct observation of filaments under an optical microscope showed that addition of HMM did not change the average length or flexibility of actin filaments, suggesting that the decrease in diffusion was not due to a HMM-induced change in the shape of filaments. Rather, slowing down of translational motion was caused by an increase in the volume of the diffusing complex. Surprisingly, the addition of ATP to acto-HMM accelerated the motion of actin filaments. The acceleration was the greatest at the low molar ratios of HMM:actin. Direct observation of filaments under an optical microscope showed that in the presence of ATP the average length of filaments did not change and that the filaments became stiffer, suggesting that acceleration of diffusion was not due to an ATP-induced increase in flexibility of filaments. These results show that some of the energy of splitting of ATP is impaired to actin filaments and suggest that 0.06 +/- 0.02 of HMM interferes with the diffusion of actin filaments during hydrolysis of ATP.     

Time-resolved electron microscopic analysis of the behavior of myosin heads on actin filaments after photolysis of caged ATP

The interaction between myosin subfragment 1 (S1) and actin filaments after the photolysis of P3-1-(2-nitrophenyl)ethyl ester of ATP (caged ATP) was analyzed with a newly developed freezing system using liquid helium. Actin and S1 (100 microM each) formed a ropelike double-helix characteristic of rigor in the presence of 5 mM caged ATP at room temperature. At 15 ms after photolysis, the ropelike double helix was partially disintegrated. The number of S1 attached to actin filaments gradually decreased up to 35 ms after photolysis, and no more changes were detected from 35 to 200 ms. After depletion of ATP, the ropelike double helix was reformed. Taking recent analyses of actomyosin kinetics into consideration, we concluded that most S1 observed on actin filaments at 35-200 ms are so called "weakly bound S1" (S1.ATP or S1.ADP.Pi) and that the weakly bound S1 under a rapid association- dissociation equilibrium with actin filaments can be captured by electron microscopy by means of our newly developed freezing system. This enabled us to directly compare the conformation of weakly and strongly bound S1. Within the resolution of deep-etch replica technique, there were no significant conformational differences between weakly and strongly bound S1, and neither types of S1 showed any positive cooperativity in their binding to actin filaments. Close comparison revealed that the weakly and strongly bound S1 have different angles of attachment to actin filaments. As compared to strongly bound S1, weakly bound S1 showed a significantly broader distribution of attachment angles. These results are discussed with special reference to the molecular mechanism of acto-myosin interaction in the presence of ATP.     

Structural changes induced in Ca2+-regulated myosin filaments by Ca2+ and ATP

We have used electron microscopy and proteolytic susceptibility to study the structural basis of myosin-linked regulation in synthetic filaments of scallop striated muscle myosin. Using papain as a probe of the structure of the head-rod junction, we find that this region of myosin is approximately five times more susceptible to proteolytic attack under activating (ATP/high Ca2+) or rigor (no ATP) conditions than under relaxing conditions (ATP/low Ca2+). A similar result was obtained with native myosin filaments in a crude homogenate of scallop muscle. Proteolytic susceptibility under conditions in which ADP or adenosine 5'-(beta, gamma-imidotriphosphate) (AMPPNP) replaced ATP was similar to that in the absence of nucleotide. Synthetic myosin filaments negatively stained under relaxing conditions showed a compact structure, in which the myosin cross-bridges were close to the filament backbone and well ordered, with a clear 14.5-nm axial repeat. Under activating or rigor conditions, the cross-bridges became clumped and disordered and frequently projected further from the filament backbone, as has been found with native filaments; when ADP or AMPPNP replaced ATP, the cross-bridges were also disordered. We conclude (a) that Ca2+ and ATP affect the affinity of the myosin cross-bridges for the filament backbone or for each other; (b) that the changes observed in the myosin filaments reflect a property of the myosin molecules alone, and are unlikely to be an artifact of negative staining; and (c) that the ordered structure occurs only in the relaxed state, requiring both the presence of hydrolyzed ATP on the myosin heads and the absence of Ca2+.     

Dynamic light scattering study of the effect of Mg2+ and ATP on synthetic myosin filaments.

The dynamic light scattering (DLS) method provides us with information about the apparent diffusion coefficient, Dapp, as well as the static scattering intensity, Is, of particles in solution. For long but thin rods with length L and diameter d, the dependence on L and d of Dapp is quite different from that of Is. By means of DLS we studied synthetic myosin filaments of rabbit skeletal muscle in solution at pH 8.3 and 10 degrees C. It appeared that Mg2+ ions induced thickening and lengthening of the filaments, whereas ATP (and ADP) induced thinning and shortening (depolymerization) of the filaments. When ATP was added to the filament preparation in the presence of Mg2+ ions, it was clearly observed that thinning of the filament (or splitting into subfilaments) occurred before shortening (or depolymerization).     

ATP induces microsecond rotational motions of myosin heads crosslinked to actin.

We have used saturation transfer electron paramagnetic resonance (ST-EPR) to study the effect of ATP on the rotational dynamics of spin-labeled myosin heads crosslinked to actin (XLAS1). We have previously shown that ATP induces microsecond rotational motions in activated myofibrils or muscle fibers, but the possibility remained that the motion occurred only in the detached phase of the cross-bridge cycle. The addition of ATP to the crosslinked preparation has been shown to be a model system for active cross-bridges, presumably providing an opportunity to measure the motion in the attached state, without interference from unattached heads. In the absence of ATP, XLAS1 had very little microsecond rotational mobility, yielding a spectrum identical to that observed for uncrosslinked acto-S1. This suggests that all of the labeled S1 forms normal rigor complexes when crosslinked to actin. The addition of 5 mM ATP greatly increased the microsecond rotational mobility of XLAS1, and the effects were reversed upon depletion of ATP. The most plausible explanation for these results is that myosin heads undergo microsecond rotational motion while attached actively to actin during steady state ATPase activity. These results have important implications for the interpretation of spectroscopic data obtained during muscle contraction.     

Activation of smooth muscle myosin Mg2+-ATPase by native thin filaments and actin/tropomyosin

Application of the myosin competition test (Lehman, W., and Szent-Gy?rgyi, A. G. (1975) J. Gen. Physiol. 66, 1-30) to chicken gizzard actomyosin indicated that this smooth muscle contains a thin filament-linked regulatory mechanism. Chicken gizzard thin filaments, isolated as described previously (Marston, S. B., and Lehman, W. (1985) Biochem. J. 231, 517-522), consisted almost exclusively of actin, tropomyosin, caldesmon, and an unidentified 32-kilodalton polypeptide in molar ratios of 1:1/6:1/26:1/17, respectively. When reconstituted with phosphorylated gizzard myosin, these thin filaments conferred Ca2+ sensitivity (67.8 +/- 2.1%; n = 5) on the myosin Mg2+-ATPase. On the other hand, no Ca2+ sensitivity of the myosin Mg2+-ATPase was observed when purified gizzard actin or actin plus tropomyosin was reconstituted with phosphorylated gizzard myosin. Native thin filaments were rendered essentially free of caldesmon and the 32-kilodalton polypeptide by extraction with 25 mM MgCl2. When reconstituted with phosphorylated gizzard myosin, caldesmon-free thin filaments and native thin filaments exhibited approximately the same Ca2+ sensitivity (45.1 and 42.7%, respectively). The observed Ca2+ sensitivity appears, therefore, not to be due to caldesmon. Only trace amounts of two Ca2+-binding proteins could be detected in native thin filaments. These were identified as calmodulin (present at a molar ratio to actin of 1:733) and the 20-kilodalton light chain of myosin (present at a molar ratio to actin of 1:270). The Ca2+ sensitivity observed in an in vitro system reconstituted from gizzard thin filaments and either skeletal myosin or phosphorylated gizzard myosin is due, therefore, to calmodulin and/or an unidentified minor protein component of the thin filaments which may be an actin-binding protein involved in regulating actin filament structure in a Ca2+-dependent manner.     

Ca2+-induced fragmentation of actin filaments in pollen tubes

Summary To control the intracellular free Ca²⁺ concentration from the cell exterior, pollen tubes ofLilium longiflorum were treated with a Ca²⁺ ionophore, A23187. Cytoplasmic streaming was inhibited when the free Ca²⁺ concentration of the external medium ([Ca²⁺]) was raised to 5×10^–6 M or higher. At [Ca²⁺] below 1×10^–6 M, the rhodamine-phalloidin stained actin filaments appeared straight and thin. However, at [Ca²⁺] which inhibited cytoplasmic streaming, the actin filaments appeared fragmented. In pollen tubes, Ca²⁺ regulation of cytoplasmic streaming may be linked not only to myosin (Shimmen 1987) but also to actin.Abbreviations ATP adenosine-5-triphosphoric acid - [Ca²⁺] concentration of free Ca²⁺ - EGTA ethyleneglycol-bis-(-aminoethylether)N,N,N,N-tetraacetic acid - HEPES N-2-hydroxyethylpiperazine-N-2-ethanesulfonic acid - PIPES piperazine-N,N-bis(2-ethanesulfonic acid) - Rh-ph rhodamine-conjugated phalloidin     

t-Butylhydroperoxide-induced Ca2+ efflux from liver mitochondria in the presence of physiological concentrations of Mg2+ and ATP

Isolated rat liver mitochondria, energized either by succinate oxidation or by ATP hydrolysis, present a transient increase in the rate of Ca2+ efflux concomitant to NAD(P)H oxidation by hydroperoxides when suspended in a medium containing 3 mM ATP, 4 mM Mg2+ and acetate as permeant anion. This is paralleled by an increase in the steady-state concentration of extramitochondrial Ca2+, a small decrease in delta psi and an increase in the rate of respiration and mitochondrial swelling. With the exception of mitochondrial swelling all other events were found to be reversible. If Ca2+ cycling was prevented by ruthenium red, the changes in delta psi, the rate of respiration and the extent of mitochondrial swelling were significantly diminished. In addition, there was no significant decrease in the content of mitochondrial pyridine nucleotides. Mitochondrial coupling was preserved after a cycle of Ca2+ release and re-uptake under these experimental conditions. It is concluded that hydroperoxide-induced Ca2+ efflux from intact mitochondria is related to the redox state of pyridine nucleotides.     

ATP synthesis by Ca2+ + Mg2+-ATPase in detergent solution at constant Ca2+ levels.

ATP has been synthesized by the purified Ca2+ + Mg2+-dependent ATPase from sarcoplasmic reticulum (SR) solubilized in nonionic detergent dodecyloctaoxyethylenglycol-monoether in a solution containing inorganic phosphate and glycerol by changing pH upon addition of ADP. The Ca2+ concentration is kept constant during the experiment. Optimum synthesis is found at CaCl2 = 0.6 mM and the delta pH = 2.9 +/- 0.2. The enzyme has been digested by trypsin for 1 and 20 min, and it is found that synthesis of ATP is correlated with the Ca2+-uptake into SR. The data indicate that the enzyme alone is responsible for active transport of Ca2+ in SR. The driving force for the ATP synthesis of the process may be due to various ion-protein interactions. H+ cannot substitute for Ca2+ in the synthesis of ATP but acts probably through a modification of the Ca2+ binding sites. The data give support that the integrity of the enzyme molecule between its hydrolytic site and the Ca2+-binding sites is essential for the overall Ca2+ transport.     

Differences in G-actin containing bound ATP or ADP: the Mg2+-induced conformational change requires ATP

The role of adenosine 5'-triphosphate (ATP) in the Mg2+-induced conformational change of rabbit skeletal muscle G-actin has been investigated by comparing actin containing bound ADP with actin containing bound ATP. As previously described [Frieden, C. (1982) J. Biol. Chem. 257, 2882-2886], N-acetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine-labeled G-actin containing ATP undergoes a time-dependent Mg2+-induced fluorescence change that reflects a conformational change in the actin. Addition of Mg2+ to labeled G-actin containing ADP gives no fluorescence change, suggesting that the conformational change does not occur. The fluorescence change can be restored on the addition of ATP. Examination of the time courses of these experiments suggests that ATP must replace ADP prior to the Mg2+-induced change. The Mg2+-induced polymerization of actin containing ADP is extraordinarily slow compared to that of actin containing ATP. The lack of the Mg2+-induced conformational change, which is an essential step in the Mg2+-induced polymerization, is probably the cause for the very slow polymerization of actin containing ADP. On the other hand, at 20 degrees C, at pH 8, and in 2 mM Mg2+, the elongation rate from the slow growing end of an actin filament, measured by using the protein brevin to block growth at the fast growing end, is only 4 times slower for actin containing ADP than for actin containing ATP.     

Ca2+ control of actin gelation. Interaction of gelsolin with actin filaments and regulation of actin gelation

We elucidated the mechanism by which gelsolin, a Ca2+-dependent regulatory protein from lung macrophages, controls the network structure of actin filaments. In the presence of micromolar Ca2+, gelsolin bound Ca2+. The Ca2+-gelsolin complex reduced the apparent viscosity and flow birefringence of F-actin and the lengths of actin filaments viewed in the electron microscope. However, concentrations of gelsolin causing these alterations did not effect proportionate changes in the turbidity of actin filament solutions or in the quantity of nonsedimentable actin as determined by a radioassay. From these findings, we conclude that gelsolin shortens actin filaments without net depolymerization. Such an effect on the distribution of actin filament lengths led to the prediction that low concentrations of gelsolin would increase the critical concentration of actin-binding protein required for incipient gelation of actin filaments in the presence of Ca2+, providing an efficient mechanism for controlling actin network structure. We verified the prediction experimentally, and we estimated that the Ca2+-gelsolin complex effectively breaks the bond between actin monomers in filaments with a stoichiometry of 1:1. The effect of Ca2+-gelsolin complex on actin solation was rapid, independent of temperature between 0 degrees and 37 degrees C, and reversed by reducing the free Ca2+ concentration.     

10 nm RecA protein filaments formed in the presence of Mg2+ and ATP gamma S may contain RNA

Summary Filaments formed by the polymerization of RecA protein along DNA in the presence of Mg²⁺ and adenosine 5-0-(3-thiotriphosphate) (ATPS) are seen by electron microscopy to have a 10 nm diameter with a 9 nm helical repeat. When certain preparations of apparently pure RecA protein are incubated with Mg²⁺ and ATPS in the absence of nucleic acid for extended times, very long filaments with the same 10 nm diameter and 9 nm axial repeat are seen. We show here that these long 10 nm filaments can contain RNA which is present as a contaminant of the RecA protein and poly(A) which is synthesized during the incubations by an activity that is apparently polynucleotide phosphorylase. RecA protein purified by a procedure developed in this laboratory did not contain RNA and did not form these very long 10 nm filaments. However, when exogenous RNA was added to this protein, 10 nm filament formation was observed.     

Kinetic effects of Ca2+ and Mg2+ on ATP hydrolysis by the purified ATP diphosphohydrolase

ATP diphosphohydrolase (EC 3.6.1.5) catalyzes the hydrolysis of diphospho- and triphosphonucleosides and is sensitive to divalent cations. In this paper, we investigated the dependence of ATP hydrolysis on the concentration of free Mg2+ and Ca2+ and the cation ATP complexes. The enzyme was isolated from porcine zymogen granule membranes, solubilized in Triton X-100, and purified on a 5'-AMP-Sepharose 4B affinity column resulting in a 1500-fold purification. Free unprotonated ATP4- was hydrolyzed in the presence of ethylene glycol bis(beta-aminoethyl ether)-N,N,N',N'-tetraacetic acid. When hydrolysis rate was measured at different concentrations of the cation-ATP complex at constant free cation concentrations, normal hyperbolic curves were obtained. In CaCl2, both Kapp and Vapp increased as free Ca2+ increased from 25 to 1000 microM. In MgCl2, Kapp increased and Vapp decreased as free Mg2+ increased from 25 to 500 microM. From the rapid equilibrium rate equation, Ks and Vmax values of the substrates were calculated. We found that free ATP4-, Ca-ATP2-, and Mg-ATP2- are substrates and free cations do not bind the enzyme.     

Millisecond time-resolved changes occurring in Ca2+-regulated myosin filaments upon relaxation

Contraction of many muscles is activated in part by the binding of Ca²⁺ to, or phosphorylation of, the myosin heads on the surface of the thick filaments. In relaxed muscle, the myosin heads are helically ordered and undergo minimal interaction with actin. On Ca²⁺ binding or phosphorylation, the head array becomes disordered, reflecting breakage of the head-head and other interactions that underlie the ordered structure. Loosening of the heads from the filament surface enables them to interact with actin filaments, bringing about contraction. On relaxation, the heads return to their ordered positions on the filament backbone. In scallop striated adductor muscle, the disordering that takes place on Ca²⁺ binding occurs on the millisecond time scale, suggesting that it is a key element of muscle activation. Here we have studied the reverse process. Using time-resolved negative staining electron microscopy, we show that the rate of reordering on removal of Ca²⁺ also occurs on the same physiological time scale. Direct observation of images together with analysis of their Fourier transforms shows that activated heads regain their axial ordering within 20 ms and become ordered in their final helical positions within 50 ms. This rapid reordering suggests that reformation of the ordered structure, and the head-head and other interactions that underlie it, is a critical element of the relaxation process.     

The polyelectrolyte behavior of actin filaments: a 25Mg NMR study.

Under physiological conditions, filamentous actin (F-actin) is a polyanionic protein filament. Key features of the behavior of F-actin are shared with other well-characterized polyelectrolytes, in particular, duplex DNA. For example, the bundle formation of F-actin by polyvalent cations, including divalent metal ions such as Mg2+, has been proposed to be a natural consequence of the polyelectrolyte nature of actin filaments [Tang and Janmey (1996) J. Biol. Chem. 271, 8556-8563]. This recently proposed model also suggests that weak interactions between F-actin and Mg2+ ions reflect a nonspecific trapping of counterions in the electric field surrounding F-actin due to its polyelectrolyte nature. To test this hypothesis, we have performed 25Mg NMR measurements in F-actin solutions. Based on the NMR data, we estimate that the rotational correlation times of Mg2+ are independent of the overall rotational dynamics of the actin filaments. Moreover, competitive binding experiments demonstrate a facile displacement of F-actin-bound Mg2+ by Co(NH3)63+. At higher Co(NH3)63+ concentrations, a fraction of the magnesium ions are trapped as actin filaments aggregate. ATP also competes effectively with actin filaments for binding to Mg2+. These results support the hypothesis that magnesium ions bind loosely and nonspecifically to actin filaments, and thus show a behavior typical of counterions in polyelectrolyte solutions. The observed features mimic to some extent the well-documented behavior of counterions in DNA solutions.     

Interaction of cytochalasin D with actin filaments in the presence of ADP and ATP

Cytochalasin D strongly inhibits the faster components in the reactions of actin filament depolymerization and elongation in the presence of 10 mM Tris-Cl-, pH 7.8, 0.2 mM dithiothreitol, 1 mM MgCl2, 0.1 mM CaCl2, and 0.2 mM ATP or ADP. Assuming an exclusive and total capping of the barbed end by the drug, the kinetic parameters derived at saturation by cytochalasin D refer to the pointed end and are 10-15-fold lower than at the barbed end. In ATP, the critical concentration increases with cytochalasin D up to 12-fold its value when both ends are free; as a result of the lowering of the free energy of nucleation by cytochalasin D, short oligomers of F-actin exist just above and below the critical concentration. Cytochalasin D interacts strongly with the barbed ends independently of the ADP-G-actin concentration (K = 0.5 nM-1). In contrast, the affinity of cytochalasin D decreases cooperatively with increasing ATP-G-actin concentration. These data are equally well accounted for by two different models: either cytochalasin D binds very poorly to ATP-capped filament ends whose proportion increases with actin concentration, or cytochalasin D binds equally well to ATP-ends and ADP-ends and also binds to actin dimers in ATP but not in ADP. A linear actin concentration dependence of the rate of growth was found at the pointed end, consistent with the virtual absence of an ATP cap at that end.     

Distribution of profilin in fibroblasts correlates with the presence of highly dynamic actin filaments.

We have used polyclonal and monoclonal antibodies raised against calf thymus profilin to localize the corresponding protein in translocating, spreading, and stationary rat fibroblasts. Immunofluorescence of whole cells and immunogold labeling on ventral membranes of lysis-squirted cells showed that profilin was markedly enriched in the highly dynamic lamellipodia or pseudopodial lobes. Within these regions, a significant fraction was colocalized with dynamic actin filaments organized in actin ribs, cortical filaments, or stress fiber-like bundles, and little profilin was found in membrane areas appearing free of actin. In contrast, stress fibers of stationary cells as well as actin arcs and ring-like bundles of spreading and migrating cells showed very little label. These results are discussed in context with the proposed role of profilin in regional membrane dynamics typical for fibroblasts and are compared to previous data (Hartwig et al.: J. Cell Biol. 109:1571-1579, 1989) on profilin distribution in platelets and granulocytes.     

Inhibition by Mg2+ of the interaction of Ca2+ with spin-labeled g2 bound to myosin.

According to the measurement of ESR spectrum, Ca2+ induced conformational change of spin-labeled g2 bound to myosin in the presence of 1 mM Mg2+. The half-maximal changes were observed at pCa 6.8 and at pCa 3.7. Spin-labeled phosphorylated g2 bound to myosin showed one transition at pCa 4.5, which shifted to pCa 6.5 after the dephosphorylation with E. coli alkaliphosphatase.     

Ca2+ and calmodulin regulate the binding of filamin A to actin filaments

Filamin A (FLNa) cross-links actin filaments (F-actin) into three-dimensional gels in cells, attaches F-actin to membrane proteins, and is a scaffold that collects numerous and diverse proteins. We report that Ca(2+)-calmodulin binds the actin-binding domain (ABD) of FLNa and dissociates FLNa from F-actin, thereby dissolving FLNa.F-actin gels. The FLNa ABD has two calponin homology domains (CH1 and CH2) separated by a linker. Recombinant CH1 but neither FLNa nor its ABD binds Ca(2+)-calmodulin in the absence of F-actin. Extending recombinant CH1 to include the negatively charged region linker domain makes it, like full-length FLNa, unable to bind Ca(2+)-calmodulin. Ca(2+)-calmodulin does, however, dissociate the FLNa ABD from F-actin provided that the CH2 domain is present. These findings identify the first evidence for direct regulation of FLNa, implicating a mechanism whereby Ca(2+)-calmodulin selectively targets the FLNa.F-actin complex.