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.     

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.     

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.     

Chemotactic peptide-induced changes in neutrophil actin conformation

The effect of the chemotatic peptide, N- formylmethionylleucylphenylalanine (FMLP), on actin conformation in human neutrophils (PMN) was studied by flow cytometry using fluorescent 7-nitrobenz-2-oxa-1,3-diazole (NBD)-phallacidin to quantitate cellular F-actin content. Uptake of NBD-phallacidin by fixed PMN was saturable and inhibited by fluid phase F-actin but not G-actin. Stimulation of PMN by greater than 1 nM FMLP resulted in a dose-dependent and reversible increase in F-actin in 70-95% of PMN by 30 s. The induced increase in F-actin was blocked by 30 microM cytochalasin B or by a t- BOC peptide that competitively inhibits FMLP binding. Under fluorescence microscopy, NBD-phallacidin stained, unstimulated PMN had faint homogeneous cytoplasmic fluorescence while cells exposed to FMLP for 30 s prior to NBD-phallacidin staining had accentuated subcortical fluorescence. In the continued presence of an initial stimulatory dose of FMLP, PMN could respond with increased F-actin content to the addition of an increased concentration of FMLP. Thus, FMLP binding to PMN induces a rapid transient conversion of unpolymerized actin to subcortical F-actin and repetitive stimulation of F-actin formation can be induced by increasing chemoattractant concentration. The directed movement of PMN in response to chemoattractant gradients may require similar rapid reversible changes in actin conformation.     

Diphasic transformations of F-actin. Effects of urea and MgCl2 on F-actin.

Asakura, Taniguchi and Oosawa [1]proposed that muscle actin polymer under sonic vibration is in a different state from that of the ordinary double stranded helical structure (F-actin), characterised by partially interrupted structures of F-actin, a state of "f-actin". In order to confirm different states for actin polymers [1, 2], physicochemical studies were made by measurements of viscosity, flow birefringence, electric birefringence, fluorescence, electron microscopy, quasielastic light scattering and ATP splitting. The following results were obtained. (1) F-actin polymers can undergo two processes of depolymerization upon treatment with urea and various salts as judged by measurements of flow birefringence and viscosity: one is a rapid process in a solution containing K+ or Ca2+ and urea; the other is a slow process following a brief rapid one in a solution containing Mg2+ and urea. (2) In the presence of Mg2+ and a suitable concentration of urea, F-actin (FMU-actin) appeared to exhibit different properties than ordinary F-actin; it had lower viscosity and lower flow birefringence and it had on the whole a more flexible polymer structure, also judging from experiments of quasielastic light scattering, electric birefringence. The different structure was confirmed directly be electron microscopic observation. The aromatic side chains of FMU-actin were also more mobile than those of F-actin judging from fluorescence measurements. The transformation between F-actin and FMU-actin was reversible. (3) The state of FMU-actin polymers was also characterized by ATP splitting; FMU-actin split about one mole of ATP into ADP and inorganic phosphate per mole of actin monomer at room temperature, where F-actin did not. A molar excess of Mg2+ with respect to actin monomer at room temperature, where F-actin did not. A molar excess of Mg2+ with respect to actin monomer is required for ATP splitting. F-actin in solutions containing K+ or Ca2+ and urea did not split ATP. FMU-actin activated on Mg-ATP-ase of myosin at nearly the same rate as that of F-actin. (4) We have postulated a flexible filament model (f-actin). The relationships between the structure of f-actin and its functional role for force generation during contraction are discussed.     

ADP-ribosylation of actins by arginine-specific ADP-ribosyltransferase purified from chicken heterophils.

We reported the purification and characterization of an arginine-specific ADP-ribosyltransferase and acceptor protein p33 in granules of chicken peripheral polymorphonuclear leukocytes (heterophils) [Mishima, K., Terashima, M., Obara, S., Yamada, K., Imai, K. & Shimoyama, M. (1991) J. Biochem. (Tokyo) 110, 388-394]. In the present study, we obtained evidence that chicken non-muscle beta/gamma-actin, skeletal muscle alpha-actin and smooth-muscle gamma-actin were ADP ribosylated by the heterophil ADP-ribosyltransferase. The stoichiometry of ADP-ribose incorporation into these actins was 1.2 mol, 1.0 mol and 2.0 mol ADP-ribose/mol of beta/gamma-actin, alpha-actin and gamma-actin, respectively. The optimal pH for the ADP ribosylation was at pH 8.5, with the respective actin. Km values for NAD were calculated to be 30 microM with beta/gamma-actin, 35 microM with alpha-actin and 20 microM with gamma-actin. The Km values for the actin isoforms were 15 microM for beta/gamma-actin, 2.5 microM for alpha-actin and 10 microM for gamma-actin. ADP ribosylation of actin inhibited its capacity to polymerize, as determined by the increase in fluorescence intensity with N-(1-pyrenyl)iodoacetamide-labelled actin. Filamentous actin (F-actin) polymerized with the respective actin isoform was also ADP ribosylated, although the extent of the modification of F-actin was lower than that of globular actin (G-actin). In situ ADP ribosylation of beta/gamma-actin was evidenced with chicken peripheral heterophils permeabilized with saponin. Thus, the endogenous ADP ribosylation of actin in the heterophils may be involved in the cellular processes such as phagocytosis, secretion and migration.     

Conformational change in actin filament induced by the interaction with heavy meromyosin: effects of pH, tropomyosin and deoxy-ATP.

Conformational changes in pure and tropomyosin-containing F-actin during interaction with heavy meromyosin in the absence and presence of deoxy-ATP, were studied by measurements of the changes in fluorescence intensity of e-ADP² incorporated into the F-actin instead of ADP. The actin filaments were found to be stabilized by tropomyosin and were more stable at pH 7 than at pH 8. The rigor binding of HMM to F-actin caused an increase in the fluorescence intensity. The increase with F-actin containing TM was higher than that with pure F-actin at each HMM concentration. A linear relation between the fluoresence change and moles of HMM per actin was found regardless of the presence of TM, with a maximum value of 0.5 moles of HMM per actin. In the presence of deoxy-ATP, (which is a substrate for acto-HMM but cannot bind to actin) no changes in fluorescence intensity of e-ADP bound to pure F-actin were observed. In the case of F-actin containing TM, the fluorescence intensity increased with increasing HMM concentration, although the light scattering intensity of the acto-HMM solutions indicated that almost all the HMM was dissociated from the F-actin. This suggests that the conformational change in F-actin-TM induced by the interaction with HMM in the presence of deoxy-ATP has a long lifetime which continues for some time even after the detachment of the HMM.     

Interactions of the actin and nucleotide binding sites on myosin subfragment 1.

The effects of selected nucleotides (N) on the binding of myosin subfragment 1 (S-1) and pure F-actin (A) were measured by time-resolved fluorescence depolarization for 0.15 M KCl, pH 7.0 at 4 degrees. The association constants K'A, KN, and K'N in the scheme (see article), were determined for the magnesium salts of ADP, adenyl-5'-yl imidodiphosphate AMP-P(NH)P, and PPi. The nucleotide binding site on S-1 was "mapped" with respect to its interaction on the actin binding site. The subsites were the beta- and gamma-phosphoryl groups of ATP bind had the largest effects. A quantitative measure of the interaction, the interaction free energy, was defined as -RT ln (KA/K'A). For ADP, K'A was 2.7 X 10(5) M-1 and the interaction free energy was -4.67 kJ M-1. For AMP-P(NH)P and PPi it was much larger. A ternary complex was shown to exist for ADP, S-1, and actin in the presence of Mg2+ and evidence from AMP-P(NH)P and PPi measurements indicated that ATP also likely forms a ternary complex. The mechanism of (S-1)-actin dissociation is discussed in light of these results.     

Fluorescence study of the high pressure-induced denaturation of skeletal muscle actin.

Ikkai & Ooi [Ikkai, T. & Ooi, T. (1966) Biochemistry 5, 1551-1560] made a thorough study of the effect of pressure on G- and F-actins. However, all of the measurements in their study were made after the release of pressure. In the present experiment in situ observations were attempted by using epsilon ATP to obtain further detailed kinetic and thermodynamic information about the behaviour of actin under pressure. The dissociation rate constants of nucleotides from actin molecules (the decay curve of the intensity of fluorescence of epsilon ATP-G-actin or epsilon ADP-F-actin) followed first-order kinetics. The volume changes for the denaturation of G-actin and F-actin were estimated to be -72 mL x mol(-1) and -67 mL x mol(-1) in the presence of ATP, respectively. Changes in the intensity of fluorescence of F-actin whilst under pressure suggested that epsilon ADP-F-actin was initially depolymerized to epsilon ADP-G-actin; subsequently there was quick exchange of the epsilon ADP for free epsilon ATP, and then polymerization occurred again with the liberation of phosphate from epsilon ATP bound to G-actin in the presence of excess ATP. In the higher pressure range (> 250 MPa), the partial collapse of the three-dimensional structure of actin, which had been depolymerized under pressure, proceeded immediately after release of the nucleotide, so that it lost the ability to exchange bound ADP with external free ATP and so was denatured irreversibly. An experiment monitoring epsilon ATP fluorescence also demonstrated that, in the absence of Mg(2+)-ATP, the dissociation of actin-heavy meromyosin (HMM) complex into actin and HMM did not occur under high pressure.     

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.     

Effects of tryptic digestion on myosin subfragment 1 and its actin-activated adenosinetriphosphatase

Myosin subfragment 1 (S-1) was fluorescently labeled at its rapidly reacting thiol ("SH1"). Short exposure to trypsin cuts the S-1 heavy chain into three still-associated fragments (20K, 50K, and 27K) [Balint, M., Wolf, L., Tarcsafalvi, A., Gergely, J., & Sreter, F.A. (1978) Arch. Biochem. Biophys. 190, 793-799] which bind F-actin to the same extent as does the uncut labeled S-1, as indicated by time-resolved fluorescence anisotropy decay (at 4 degrees C, pH 7, in 0.15 M KC1 and 5 mM MgC12, +/- 1 mM ADP). These results are thus in agreement with turbidity measurements on similar systems as reported by Mornet et al. [Mornet, D., Pantel, P., Audemard, E., & Kassab, R. (1979) Biochem. Biophys. Res. Commun. 89, 925-932]. The excited-state lifetime of the fluorescent label on cut S-1 is indistinguishable from that on normal S-1 (+/- ADP, +/- F-actin). F-Actin activation of MgATPase of cut S-1 is lower than that for normal S-1 at moderate concentrations of F-actin, as reported by Mornet et al. (1979). But as the F-actin concentration is increased, the MgATPase activities for cut S-1 approach those for uncut S-1. In terms of an eight-species steady-state kinetics scheme involving actin binding to free S-1, S-1 . ATP, S-1. ADP X P, and S-1 . ADP, actin affinity for the species S-1 . ADP X P was found to be 13.4 times greater for uncut S-1 than for cut S-1 [at 24 degrees C, pH 7.0, in 3 mM KC1, 1 mM ATP, 1 mM MgCl2, and 20 mM N-[tris(hydroxymethyl)methyl]-2-aminoethanesulfonic acid].     

Actin filaments undergo limited subunit exchange in physiological salt conditions

The exchange of actin filament subunits for unpolymerized actin or for subunits in other filaments has been quantitated by three experimental techniques: fluorescence energy transfer, incorporation of 35S-labeled actin monomers into unlabeled actin filaments, and exchange of [14C]ATP with filament-bound ADP. In the fluorescence energy transfer experiments, actin labeled with 5-(iodoacetamidoethyl)aminonaphthalene- 1-sulfonic acid (IAENS) served as the fluorescent energy donor, and actin labeled with either fluorescein-5-isothiocyanate (FITC) or fluorescein-5-maleimide (FM) served as the energy acceptor. Fluorescent- labeled actins from Dictyostelium amoebae and rabbit skeletal muscle were very similar to their unlabeled counterparts with respect to critical actin concentration for filament assembly, assembly rate, ATP hydrolysis upon assembly, and steady-state ATPase. As evidenced by two different types of fluorescence energy transfer experiments, less than 5% of the actin filament subunits exchanged under a variety of buffer conditions at actin concentrations greater than 0.5 mg/ml. At all actin concentrations limited exchange to a plateau level occurred with a half- time of about 20 min. Nearly identical results were obtained when exchange was quantitated by incorporation of 35S-labeled Dictyostelium actin monomers into unlabeled muscle actin or Dictyostelium actin filaments. Furthermore, the proportion of filament-bound ADP which exchanged with [14C]-ATP was nearly the same as actin subunit exchange measured by fluorescence energy transfer and 35S-labeled actin incorporation. These experiments demonstrate that under approximately physiologic ionic conditions only a small percentage of subunits in highly purified skeletal muscle or Dictyostelium F-actin participate in exchange.     

Myosin-induced changes in F-actin: fluorescence probing of subdomain 2 by dansyl ethylenediamine attached to Gln-41.

Actin labeled at Gln-41 with dansyl ethylenediamine (DED) via transglutaminase reaction was used for monitoring the interaction of myosin subfragment 1 (S1) with the His-40-Gly-42 site in the 38-52 loop on F-actin. Proteolytic digestions of F-actin with subtilisin and trypsin, and acto-S1 ATPase measurements on heat-treated F-actin revealed that the labeling of Gln-41 had a stabilizing effect on subdomain 2 and the actin filaments. DED on Gln-41 had no effect on the values of K(m) and Vmax of the acto-S1 ATPase and the sliding velocities of actin filaments in the in vitro motility assays. This suggests either that S1 does not bind to the 40-42 site on actin or that such binding is not functionally important. The binding of monoclonal antidansyl IgG to DED-F-actin did not affect acto-S1 binding in the absence of nucleotides, indicating that the 40-42 site does not contribute much to rigor acto-S1 binding. Myosin-induced changes in subdomain 2 on actin were manifested through an increase in the fluorescence of DED-F-actin, a decrease in the accessibility of the probe to collisional quenchers, and a partial displacement of antidansyl IgG from actin by S1. It is proposed that these changes in the 38-52 loop on actin originate from S1 binding to other myosin recognition sites on actin.     

The influence of adenosine triphosphate, adenosine diphosphate and cytochalasin B on nucleotide exchange of F-actin. Evidence that treadmilling is not involved

[14C]ATP-containing G-actin was polymerized to [14C]ADP-containing F-actin. The exchange of the filament-bound nucleotide with nucleotides of the medium was investigated by measuring the loss of radioactivity from the filaments under various conditions. Nucleotide exchange was faster in the presence of ATP than of ADP (this could be observed in the presence of Mg2+ as well as in the presence of Ca2+). Cytochalasin B had a small accelerating effect in the presence of ATP but had no effect in the presence of ADP. The kinetics of exchange remained unchanged when the filaments contained a 'cap' of actin with non-radioactive nucleotides, suggesting that nucleotide exchange was not a property of the filament ends.     

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.     

Dissociative mechanism of F-actin thermal denaturation

We have applied differential scanning calorimetry to investigate thermal unfolding of F-actin. It has been shown that the thermal stability of F-actin strongly depends on ADP concentration. The transition temperature, T(m), increases with increasing ADP concentration up to 1 mM. The T(m) value also depends on the concentration of F-actin: it increases by almost 3 degrees C as the F-actin concentration is increased from 0.5 to 2.0 mg/ml. Similar dependence of the T(m) value on protein concentration was demonstrated for F-actin stabilized by phalloidin, whereas it was much less pronounced in the presence of AlF4(-). However, T(m) was independent of protein concentration in the case of monomeric G-actin. The results suggest that at least two reversible stages precede irreversible thermal denaturation of F-actin; one of them is dissociation of ADP from actin subunits, and another is dissociation of subunits from the ends of actin filaments. The model explains why unfolding of F-actin depends on both ADP and protein concentration.     

Decavanadate binding to a high affinity site near the myosin catalytic centre inhibits F-actin-stimulated myosin ATPase activity

Decameric vanadate (V(10)) inhibits the actin-stimulated myosin ATPase activity, noncompetitively with actin or with ATP upon interaction with a high-affinity binding site (K(i) = 0.27 +/- 0.05 microM) in myosin subfragment-1 (S1). The binding of V(10) to S1 can be monitored from titration with V(10) of the fluorescence of S1 labeled at Cys-707 and Cys-697 with N-iodo-acetyl-N'-(5-sulfo-1-naphthyl)ethylenediamine (IAEDANS) or 5-(iodoacetamido) fluorescein, which showed the presence of only one V(10) binding site per monomer with a dissociation constant of 0.16-0.7 microM, indicating that S1 labeling with these dyes produced only a small distortion of the V(10) binding site. The large quenching of AEDANS-labeled S1 fluorescence produced by V(10) indicated that the V(10) binding site is close to Cys-697 and 707. Fluorescence studies demonstrated the following: (i) the binding of V(10) to S1 is not competitive either with actin or with ADP.V(1) or ADP.AlF(4); (ii) the affinity of V(10) for the complex S1/ADP.V(1) and S1/ADP.AlF(4) is 2- and 3-fold lower than for S1; and (iii) it is competitive with the S1 "back door" ligand P(1)P(5)-diadenosine pentaphosphate. A local conformational change in S1 upon binding of V(10) is supported by (i) a decrease of the efficiency of fluorescence energy transfer between eosin-labeled F-actin and fluorescein-labeled S1, and (ii) slower reassociation between S1 and F-actin after ATP hydrolysis. The results are consistent with binding of V(10) to the Walker A motif of ABC ATPases, which in S1 corresponds to conserved regions of the P-loop which form part of the phosphate tube.     

Phallotoxin and actin binding assay by fluorescence enhancement.

The fluorescence of five fluorophores conjugated to phallotoxins was found to be specifically enhanced upon binding to F-actin in a polymerizing buffer. Rhodamine phalloidin had the greatest fluorescence enhancement of ninefold. The fluorescence titration of rhodamine phalloidin by actin was shown to be consistent with stoichiometric binding. The fluorescence enhancement of rhodamine phalloidin at 5 microM is linearly related to F-actin concentrations up to 2 microM and therefore can be used as an easy means of F-actin quantitation. In a competition assay, other phallotoxins reduce the fluorescence enhancement that results from the binding of rhodamine phalloidin to polymerized actin. This reduction also permits a convenient measurement of the binding constants of any competing phallotoxins.     

Intermolecular coupling between loop 38-52 and the C-terminus in actin filaments.

The recently reported structural connectivity in F-actin between the DNase I binding loop on actin (residues 38-52) and the C-terminus region was investigated by fluorescence and proteolytic digestion methods. The binding of copper to Cys-374 on F- but not G-actin quenched the fluorescence of dansyl ethylenediamine (DED) attached to Gin-41 by more than 50%. The blocking of copper binding to DED-actin by N-ethylmaleimide labeling of Cys-374 on actin abolished the fluorescence quenching. The quenching of DED-actin fluorescence was restored in copolymers (1:9) of N-ethylmaleimide-DED-actin with unlabeled actin. The quenching of DED-actin fluorescence by copper was also abolished in copolymers (1:4) of DED-actin and N-ethylmaleimide-actin. These results show intermolecular coupling between loop 38-52 and the C-terminus in F-actin. Consistent with this, the rate of subtilisin cleavage of actin at loop 38-52 was increased by the bound copper by more than 10-fold in F-actin but not in G-actin. Neither acto-myosin subfragment-1 (S1) ATPase activity nor the tryptic digestion of G-actin and F-actin at the Lys-61 and Lys-69 sites were affected by the bound copper. These observations suggest that copper binding to Cys-374 does not induce extensive changes in actin structure and that the perturbation of loop 38-52 environment results from changes in the intermolecular contacts in F-actin.     

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.