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

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

Isolation and characterization of covalently cross-linked actin dimer

Covalently cross-linked actin dimer was isolated from rabbit skeletal muscle F-actin reacted with phenylenebismaleimide (Knight, P., and Offer, G. (1978) Biochem. J. 175, 1023-1032). The UV spectrum of the purified cross-linked actin dimer, in a nonpolymerizing buffer, was very similar to that of native F-actin and not to the spectrum of G-actin. Cross-linked actin dimer polymerized to filaments that were indistinguishable in the electron microscope from F-actin made from native G-actin and that were similar to native F-actin in their ability to activate the Mg2+-ATPase of myosin subfragment-1. The critical concentrations of polymerization of cross-linked actin dimer in 0.5 mM and 2.0 mM MgCl2, 2 to 4 microM, and 1 to 2 microM, respectively, were similar to the values for native G-actin. Cross-linked actin dimer contained 2 mol of bound nucleotide/mol of dimer. One bound nucleotide exchanged with ATP in solution with a t 1/2 of 55 min and with ADP with a t 1/2 of 5 h. The second bound nucleotide exchanged much more slowly. The more rapidly exchangeable site contained 10 to 15% bound ADP.Pi and 85 to 90% bound ATP while the second site contained much less, if any, bound ADP.Pi. Cross-linked actin dimer had an ATPase activity in 0.5 mM MgCl2 that was 7 times greater than the ATPase activity of native G-actin and that was also stimulated by cytochalasin D. These data are discussed in relation to the possible role of ATP in actin polymerization and function with the speculation that the cross-linked actin dimer may serve simultaneously as a useful model for each of the two different ends of native F-actin.     

Evidence for an ATP cap at the ends of actin filaments and its regulation of the F-actin steady state

The correlation between the time courses of actin polymerization under continuous sonication and the associated ATP hydrolysis has been studied. ATP hydrolysis was not mechanistically coupled to polymerization, i.e. not necessary for polymerization, but occurred on F-actin in a subsequent monomolecular reaction. Under sonication, polymerization was complete in 10 s while hydrolysis of ATP on the polymer required 200 s. A value of 0.023 s-1 was found for the first order rate constant of ATP hydrolysis on the polymer at 25 degrees C, pH 7.8, in the presence of 0.2 mM ATP, 0.1 mM CaCl2, and 1 mM MgCl2, independent of the F-actin concentration. The conversion of ATP X F-actin to ADP X F-actin was accompanied by an increase in fluorescence of a pyrenyl probe covalently attached to actin, consistent with a 2-fold greater fluorescence for ADP X F-actin than for ATP X F-actin, with a rate constant of 0.022 s-1. In contrast, the fluorescence of F-actin labeled with 7-chloro-4-nitrobenzeno-2-oxa-1,3-diazole did not change significantly when ATP or ADP was bound. The direct consequence of the uncoupling between polymerization and ATP hydrolysis is the formation of an ATP cap at the ends of the filaments, which maintains the stability of the polymer, while most of the filament contains bound ADP. The heterogeneity of the filament with respect to ATP and ADP results in a nonlinear relationship between the rate of elongation and the concentration of G-actin with a discontinuity at the critical concentration, where the rate of growth is zero. In this respect, F-actin in ATP behaves similarly to microtubules in GTP.     

Inhibition of sliding movement of F-actin by crosslinking emphasizes the role of actin structure in the mechanism of motility

The effects of crosslinking of monomeric and polymeric actin with 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide (EDC), disuccinimidyl suberate (DSS) and glutaraldehyde on the interaction with heavy meromyosin (HMM) in solution and on the sliding movement on glass-attached HMM were examined. The Vmax values of actin-activated HMM ATPase decreased in the following order: intact actin = EDC F-actin greater than DSS actin greater than glutaraldehyde F-actin = glutaraldehyde G-actin greater than EDC G-actin. The affinity of actin for HMM in the presence of ATP decreased in the following order: DSS actin greater than glutaraldehyde F-actin = glutaraldehyde G-actin greater than intact actin greater than EDC F-actin greater than EDC G-actin. However, sliding movement was inhibited only in the case of glutaraldehyde-crosslinked F and G-actin and EDC-crosslinked G-actin. Interestingly, after copolymerization of "non-motile" glutaraldehyde or EDC-crosslinked monomers with "motile" monomers of intact actin sliding of the copolymers was observed and its rate was independent of the type of crosslinked monomer, i.e. of the manner of their interaction with HMM. These data strongly indicate that inhibition of the sliding of actin by crosslinking cannot be explained entirely by changes in the Vmax value or affinity for myosin heads. We conclude that movement is generated by interaction of myosin with segments of F-actin containing a number of intact monomers, and the mechanism of inhibition involves an effect of the crosslinkers on the structure of F-actin itself.     

Rapid exchange of actin-bound nucleotide in perfused rat heart

In the rat heart the actin-bound nucleotide contained both ATP and ADP. The ratio of bound ATP to bound ADP depended on the functional state of the heart; it was higher in hearts stopped reversibly in diastole (low Ca(2+), high Mg(2+), or high K(+)), than in stimulated (inotropic agents or pacing) hearts. Immunoblotting and gel electrophoresis showed the existence of G-actin (30% of total actin) in the cytoplasm of the heart. Pure actin was isolated from rat hearts: in G-actin the bound nucleotide readily exchanged with ATP or ADP, and in F-actin the bound nucleotide did not exchange with ATP or ADP. The free and bound nucleotides were separated in the intact heart by extraction with 75% methanol at -15 degrees C. In rat hearts perfused with (32)P-labeled orthophosphate the actin-bound nucleotide rapidly exchanged with the cytoplasmic ATP. The full exchange of the bound ATP was immediate, whereas the full exchange of the bound ADP was slower. The full exchange of the bound ATP was independent of the heartbeat frequency, whereas the full exchange of the bound ADP was frequency dependent. The data suggest that the transformation of actin monomer-ATP to actin polymer-ADP is a part of the normal contraction-relaxation cycle of the rat heart.     

The dissociation of 1-N6-ethenoadenosine diphosphate from regulated actomyosin subfragment 1

The effective rate of dissociation of 1-N6-ethenoadenosine diphosphate (epsilon ADP) from the regulated actin X subfragment 1 X epsilon ADP complex of rabbit skeletal muscle is approximately 10-15 times smaller in the absence of calcium ion compared to the presence of calcium ion. The decrease in fluorescence emission with dissociation of the bound epsilon ADP fitted two exponential terms. The evidence is consistent with a kinetic scheme in which two first-order transitions precede the dissociation step: (Formula: see text) where D is epsilon ADP, A is regulated actin, M is subfragment 1, the asterisks refer to the degree of fluorescence enhancement, and AM(D) is a collision complex in equilibrium with free epsilon ADP. Both rate constants k-2 and k-1 were reduced approximately 15-fold in the absence of calcium ion. The rate constants for the dissociation of epsilon ATP, epsilon ADP X Pi, formed in the enzyme cycle, and epsilon ADP are all reduced in the absence of calcium ion; consequently, the primary effect in calcium regulation of the actin-subfragment 1 ATPase is on the rate constant of a transition (or transitions) between actomyosin-nucleoside phosphate complexes.     

Influence of the bound nucleotide on the molecular dynamics of actin

Rotational dynamics of actin spin-labelled with maleimide probes at the reactive thiol Cys-374 were studied. Replacement of the bound nucleotide by Br8ATP in G-actin and Br8ADP in F-actin causes significant increase of the rotational correlation time of the spin probe, indicating reduced motion in both G and F-actin. The orientation dependence of the electron paramagnetic resonance spectra in oriented F-actin filaments revealed an altered molecular order of the probe when the nucleotide was a Br-substituted one. The bound nucleotide affects the myosin S1 ATPase activation by actin; both Vmax and K(actin) decreased significantly when the bound nucleotide of actin was Br8ADP.     

Kinetic analysis of the polymerization process of actin.

The polymerization process of actin was examined by measuring the amount of flow birefringence and by analyzing release of labeled inorganic phosphate from the bound [gamma-32P]ATP upon polymerization of G-actin to F-actin. Comparison of the above experimental results with the electron microscopic data of Kawamura and Maruyama (J. Biochem., 67, 437-457, 1970) suggested that growth and redistribution steps occurred simultaneously during polymerization. Attempt was made to simulate the polymerization process of actin by calculating the kinetic equations numerically. The results of simulation suggested that it was necessary to take into consideration the association and dissociation between F-actin particles as well as the association and dissociation between F-actin and G-actin.     

Effect of F-actin upon the binding of ADP to myosin and its fragments.

The effect of F-actin upon the binding of ADP to rabbit skeletal muscle myosin, heavy meromyosin, and subfragment 1 was studied by equilibrium dialysis, ultracentrifuge transport, and light scattering techniques. Both myosin and H-meromyosin (HMM) bind a maximum of approximately 1.6 mol of ADP/mol of protein, while S-1 binds approximately 0.9 mol of ADP/mol of protein. The affinity for ADP of all three preparations was similar at a given ionic strength (approximately 10(6) M-1 at 0.05 M KCl) and decreased with increasing ionic strength. Under conditions similar to those used for the measurement of ADP binding, the binding sites of myosin, HMM, and subfragment 1 (S-1) are saturated with actin at molar ratios of 2, 2, and 1 mol of actin monomer/mol of protein, respectively, as determined by light scattering, ultracentrifuge transport, and in the case of myosin by ATPase measurements. F-actin was found to inhibit ADP binding, but even at an actin concentration at least twice that required for saturation of myosin, HMM, or S-1, significant ADP binding remained. This ADP binding was inhibited by 10(-4) M pyrophosphate. The observations are consistent with the formation of an actomyosin-ADP complex in which actin and ADP are bound to myosin at distinct but interacting sites.     

The bound nucleotide of actin

The extent of actin polymerization has been studied for samples in which the bound nucleotide of the actin was ATP, ADP, or an analog of ATP that was not split (AMPPNP). The equilibrium constants for the addition of a monomer to a polymer end were determined from the concentration of monomer coexisting with the polymer. An analysis of these results concludes that the bound ATP on G-actin provides little energy to promote the polymerization of the actin. AMPPNP was incorporated into F-actin and the interaction of F-actin · AMPPNP with myosin was studied. F-actin · AMPPNP activated the ATPase of myosin to the same extent as did F-actin · ADP. However, the rate of superprecipitation was slower in the case of F-actin · AMPPNP than in the control.     

Nucleotide exchange between cytosolic ATP and F-actin-bound ADP may be a major energy-utilizing process in unstimulated platelets

About 40% of the cytosolic ADP of human platelets is tightly bound to protein and the complex is precipitated from the cells by 43% ethanol. We show here that this ADP is bound to F-actin by three criteria (a) copurification with F-actin, (b) specific extraction with water and (c) by specific interaction with DNase I. Platelets contain 0.3 mumol/10(11) cells of this F-actin--ADP complex compared to the total actin content of 0.8 mumol/10(11) cells, which is consistent with the view that actin is maintained in different pools (F-actin--ADP, profilactin, G-actin). In intact platelets the F-actin-bound ADP turns over rapidly and we have determined a turnover rate at 37 degrees C of 0.1 +/- 0.025 s-1 by using a double-labelling procedure. This rapid turnover indicates that F-actin in intact platelets is in a very dynamic state, which may be necessary for rapid responses to stimuli. If it is assumed that the source of the ADP bound to F-actin is cytosolic ATP, the turnover of F-actin ADP measured represents an ATP-consuming process that would account for up to 50% of total ATP consumption in resting platelets.     

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

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

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.     

Microcalorimetric measurement of the enthalpy of binding of rabbit skeletal myosin subfragment 1 and heavy meromyosin to F-actin

The heat of binding of rabbit skeletal myosin subfragment 1 (myosin-S1) and heavy meromyosin (HMM) to F-actin has been measured by batch calorimetry. Proton release measurements in unbuffered solutions indicate that less than 0.1 mol of protons is absorbed or released per mol of myosin head bound to actin. Hence, the measured heats are approximately equal to the enthalpy of myosin-S1 and HMM binding to actin. The enthalpy of binding of myosin-S1 to actin was +22 +/- 3 and +27 +/- 5 kJ/mol of myosin-S1 in two series of experiments at 12 degrees C and +26 +/- 5 kJ/mol of myosin-S1 at 0 degrees C, indicating that delta Cp for this reaction in the range of 0-12 degrees C is small (-80 J/mol/K). The enthalpy of binding of HMM to actin at 12 degrees C was found to be +26 +/- 1 kJ/mol of myosin head. The enthalpies determined here and the equilibrium constants obtained from the literature for measurements at 20 degrees C under identical solvent conditions were used to estimate the entropy of the association of myosin S1 and HMM with F-actin: +235 J/mol/K for myosin-S1 and +190 J/mol of myosin head/K for HMM. Thermodynamic parameters of the interaction of myosin-S1 with actin and ADP or AMP-PNP can be evaluated using the enthalpy of association of myosin-S1 with actin determined here, together with literature values for the equilibrium constants and enthalpies of binding of these nucleotides to myosin-S1. The calculated enthalpies of binding of ADP or AMP-PNP to actomyosin-S1 are small and negative.     

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.     

Aggregation of platelets by muscle actin. A multivalent interaction model of platelet aggregation by ADP

Filamentous muscle actin (F-actin) aggregated blood platelets while G-actin was ineffective. This aggregation could be blocked by ATP suggesting a possible role of actin-bound ADP in this process. Actin-bound ADP caused platelet aggregation at concentrations significantly lower than equivalent concentrations of free ADP. Thus, actin potentiates the aggregating action of ADP. An actin antibody or DNase I inhibited this aggregation showing the requirement of actin in this process. Like other physiological agents, Ca⁺⁺ was necessary for platelet aggregation by actin. Platelets fixed in formaldehyde were not aggregated by actin showing the need for viable platelets. Since F-actin contains 1 mole of bound ADP/mole protein, it is postulated that actin potentiates ADP-induced aggregation by providing multiple interaction sites for platelets.     

Reactions of 1-N6-ethenoadenosine nucleotides with myosin subfragment 1 and acto-subfragment 1 of skeletal and smooth muscle

The fluorescent nucleotides epsilon ADP and epsilon ATP were used to study the binding and hydrolysis mechanisms of subfragment 1 (S-1) and acto-subfragment 1 from striated and smooth muscle. The quenching of the enhanced fluorescence emission of bound nucleotide by acrylamide analyzed either by the Stern-Volmer method or by fluorescence lifetime measurements showed the presence of two bound nucleotide states for 1-N6-ethenoadenosine triphosphate (epsilon ATP), 1-N6-ethenoadenosine diphosphate (epsilon ADP), and epsilon ADP-vanadate complexes with S-1. The equilibrium constant relating the two bound nucleotide states was close to unity. Transient kinetic studies showed two first-order transitions with rate constants of approximately 500 and 100 s-1 for both epsilon ATP and epsilon ADP and striated muscle S-1 and 300 and 30 s-1, respectively, for smooth muscle S-1. The hydrolysis of [gamma-32P] epsilon ATP yielded a transient phase of small amplitude (less than 0.2 mol/site) with a rate constant of 5-10 s-1. Consequently, the hydrolysis of the substrate is a step in the mechanism which is distinct from the two conformational changes induced by the binding of epsilon ATP. An essentially symmetric reaction mechanism is proposed in which two structural changes accompany substrate binding and the reversal of these steps occurs in product release. epsilon ATP dissociates acto-S-1 as effectively as ATP. For smooth muscle acto-S-1, dissociation proceeds in two steps, each accompanied by enhancement of fluorescence emission. A symmetric reaction scheme is proposed for the acto-S-1 epsilon ATPase cycle. The very similar kinetic properties of the reactions of epsilon ATP and ATP with S-1 and acto-S-1 suggest that two ATP intermediate states also occur in the ATPase reaction mechanism.     

Structural aspects of skeletal muscle F-actin as studied by tryptic digestion: evidence for a second nucleotide interacting site

Trypsin was used as a probe of F-actin conformation. F-actin is known to be refractory to proteolysis [Jacobson, G.R. and Rosenbusch, J.P. (1976) Proc. Natl. Acad. Sci. U.S. 73, 2742-2746]. However, here it was found that F-actin could also be digested by trypsin to a 33-kDa fragment (like G-actin) when free MgADP is present in the medium. The amounts of degradation of F-actin depended on the ADP concentration; saturation occurred at about 0.5 mM. Elimination of divalent cations from the medium completely suppressed the effect of ADP on the digestion of F-actin. Other nucleotides were also examined. The effect decreased in the order ADP greater than ATP much greater than IDP greater than GDP = UDP. Adenine, adenosine, AMP, and PPi had no effect at all. epsilon-ADP had the effect, and its fluorescence was changed on the addition of F-actin. The intrinsic tryptophan fluorescence spectrum of F-actin was ADP-dependent. These results suggest the presence of a second nucleotide interacting site on actin and that ADP interaction at this site induces conformational changes in monomeric actin molecule in F-actin filaments.     

Actin deoxyroboncuclease I interaction. Depolymerization and nucleotide exchange

Deoxyribonuclease I (DNase I) forms a 1:1 complex with globular actin (G-actin) and also will depolymerize filamentous actin (F-actin) to form a 1:1 complex. The effect of DNase I on the exchange of the actin nucleotide has been investigated. When DNase I is added to G-actin, the rate of nucleotide exchange is decreased from 1.16 +/- 0.25 X 10(-4) s-1 to 0.28 +/- 0.09 X 10(-4) s-1 (0 degrees C). The presence of ATP or ADP in the actin has little effect on the rate of exchange of the nucleotide for ATP. This suggests that the weaker affinity of ADP than ATP for actin is due to a slower association rate of ADP. The rate of the nucleotide exchange in the actinDNase I complex is increased by the addition of NaCl or MgCl2. When DNase I is added to F-actin, the rate of nucleotide exchange (6.2 +/- 1.6 X 10(-4) x-1, 0 degrees C) is similar to the rate of depolymerization as measured by loss of viscosity. The actinDNase I complex formed by depolymerization of F-actin exchanges nucleotide at a 4-fold faster rate than the G-actinDNase I complex in the same ionic conditions. This and other experiments suggest that DNase I binds first to F-actin before dissociating the monomer from the filament. These results are discussed in terms of possible mechanisms of action depolymerization.     

Hyper-mobility of water around actin filaments revealed using pulse-field gradient spin-echo 1H NMR and fluorescence spectroscopy

This paper reports that water molecules around F-actin, a polymerized form of actin, are more mobile than those around G-actin or in bulk water. A measurement using pulse-field gradient spin-echo (1)H NMR showed that the self-diffusion coefficient of water in aqueous F-actin solution increased with actin concentration by ～5%, whereas that in G-actin solution was close to that of pure water. This indicates that an F-actin/water interaction is responsible for the high self-diffusion of water. The local viscosity around actin was also investigated by fluorescence measurements of Cy3, a fluorescent dye, conjugated to Cys 374 of actin. The steady-state fluorescence anisotropy of Cy3 attached to F-actin was 0.270, which was lower than that for G-actin, 0.334. Taking into account the fluorescence lifetimes of the Cy3 bound to actin, their rotational correlation times were estimated to be 3.8 and 9.1ns for F- and G-actin, respectively. This indicates that Cy3 bound to F-actin rotates more freely than that bound to G-actin, and therefore the local water viscosity is lower around F-actin than around G-actin.