Mechanism of the active movement of actin: Is actin sliding directly or indirectly related to binding with myosin and activation of myosin ATPase?

In the present work we examined the effect of crosslinking of polymerized and monomeric actin with glutaraldehyde, EDC and DSS on: 1) binding of actin to HMM in solution; 2) activation of HMM ATPase; 3) sliding movement of actin on glass-attached myosin; 4) properties of actin itself, like polymerizability and exchangeability of tightly bound nucleotide. The obtained data show that inhibition of sliding cannot be explained only by changes in the extent of activation of HMM ATPase and binding of actin to HMM; this result emphasizes the role of structural properties of actin in the mechanism of movement generation.     

In vitro motility of skeletal muscle myosin and its proteolytic fragments

We have compared actin-activated myosin ATPase activity, myosin binding to actin, and the velocity of myosin-induced actin sliding in order to understand the mechanism of myosin motility. In our in vitro assay, F-actin slides at a constant velocity, regardless of length. The F-actin could slide over myosin heads at KCl concentrations below a critical value (60 mM with myosin and HMM, 100 mM with S-1), and the sliding velocities were quite similar below the critical KCl concentration. However, at KCl concentrations close to the critical value, the sliding F-actin is attached to only one or a few particular points on the surface, each of which perhaps consists of a single head of myosin. The KATPase values for actin-activated ATPase were approximately 300 microM for S-1 and approximately 200 microM with HMM below the critical KCl concentration, and approximately 5,000 microM above the critical KCl concentration. This increase in KATPase is due to a drastic reduction in the binding affinity of myosin heads to F-actin, as determined by a proteolytic digestion method and direct observation by fluorescence microscopy. We also show that the Vmax of actin-activated myosin ATPase activity decreases steadily with increasing KCl concentration, even though the velocity of F-actin sliding remains unchanged. This result provides evidence that the ATPase activity is not necessarily linked to motility. We discuss possible models that do not require a tight coupling between myosin ATPase and motility.     

Cooperativity in F-actin: chemical modifications of actin monomers affect the functional interactions of myosin with unmodified monomers in the same actin filament.

We have chemically modified a fraction of the monomers in actin filaments, and then measured the effects on the functional interaction of myosin with unmodified monomers within the same filament. Two modifications were used: (a) covalent attachment of various amounts of myosin subfragment-1 (S1) with the bifunctional reagent disuccinimidyl suberate and (b) copolymerization of unmodified actin monomers with monomers cross-linked internally with 1-ethyl-3-(dimethylaminopropyl)-carbodiimide. Each of these modifications abolished the interaction of the modified monomers with myosin, so the remaining interactions were exclusively with unmodified monomers. The two modifications had similar effects on the interaction of actin with myosin in solution: decreased affinity of myosin heads for unmodified actin monomers, without a change in the Vmax of actin-activated myosin ATPase activity. However, modification (b) produced much greater inhibition of actin sliding on a myosin-coated surface, as measured by an in vitro motility assay. These results provide insight into the functional consequences of cooperative interactions within the actin filament.     

Muscle actin cleaved by proteinase K: its polymerization and in vitro motility.

Skeletal muscle actin was lightly digested by proteinase K, which cleaved the peptide bond between Met-47 and Gly-48, producing a C-terminal 35 kDa fragment. Proteinase K-cleaved actin (proK-actin) did not polymerize into F-actin upon addition of salt. In the presence of phalloidin, however, it polymerized slowly into F-actin (proK-F-actin), indicating that the cleaved actin did not dissociate into the individual cleaved fragments but retained the global structure of actin. Electron microscopy showed that proK-F-actin had the typical double-stranded structure of a normal actin filament and formed the arrowhead structure when decorated with HMM. Heavy meromyosin ATPase was weakly activated by proK-F-actin: Vmax = 0.24 s-1, and Kapp = 2.8 microM, while Vmax = 7.6 s-1, and Kapp = 13 microM by F-actin. Correspondingly, in vitro this proK-F-actin slid very slowly on HMM attached to a glass surface at an average velocity of 0.47 microns/s, or 1/12 of that of intact F-actin. The fraction of sliding filaments was less than 50%. Assuming that the nonmotile filaments attached to HMM were not involved in ATPase activation, the sliding velocity correlated with the ATPase activity activated by proK-F-actin.     

Subtilisin cleavage of actin inhibits in vitro sliding movement of actin filaments over myosin

Subtilisin cleaved actin was shown to retain several properties of intact actin including the binding of heavy meromyosin (HMM), the dissociation from HMM by ATP, and the activation of HMM ATPase activity. Similar Vmax but different Km values were obtained for acto-HMM ATPase with the cleaved and intact actins. The ATPase activity of HMM stimulated by copolymers of intact and cleaved actin showed a linear dependence on the fraction of intact actin in the copolymer. The most important difference between the intact and cleaved actin was observed in an in vitro motility assay for actin sliding movement over an HMM coated surface. Only 30% of the cleaved actin filaments appeared mobile in this assay and moreover, the velocity of the mobile filaments was approximately 30% that of intact actin filaments. These results suggest that the motility of actin filaments can be uncoupled from the activation of myosin ATPase activity and is dependent on the structural integrity of actin and perhaps, dynamic changes in the actin molecule.     

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.     

Differences in the ionic interaction of actin with the motor domains of nonmuscle and muscle myosin II.

Changes in the actin-myosin interface are thought to play an important role in microfilament-linked cellular movements. In this study, we compared the actin binding properties of the motor domain of Dictyostelium discoideum (M765) and rabbit skeletal muscle myosin subfragment-1 (S1). The Dictyostelium motor domain resembles S1(A2) (S1 carrying the A2 light chain) in its interaction with G-actin. Similar to S1(A2), none of the Dictyostelium motor domain constructs induced G-actin polymerization. The affinity of monomeric actin (G-actin) was 20-fold lower for M765 than for S1(A2) but increasing the number of positive charges in the loop 2 region of the D. discoideum motor domain (residues 613-623) resulted in equivalent affinities of G-actin for M765 and for S1. Proteolytic cleavage and cross-linking approaches were used to show that M765, like S1, interacts via the loop 2 region with filamentous actin (F-actin). For both types of myosin, F-actin prevents trypsin cleavage in the loop 2 region and F-actin segment 1-28 can be cross-linked to loop 2 residues by a carbodiimide-induced reaction. In contrast with the S1, loop residues 559-565 of D. discoideum myosin was not cross-linked to F-actin, probably due to the lower number of positive charges. These results confirm the importance of the loop 2 region of myosin for the interaction with both G-actin and F-actin, regardless of the source of myosin. The differences observed in the way in which M765 and S1 interact with actin may be linked to more general differences in the structure of the actomyosin interface of muscle and nonmuscle myosins.     

Characterization of caldesmon binding to myosin

Caldesmon inhibits the binding of skeletal muscle subfragment-1 (S-1).ATP to actin but enhances the binding of smooth muscle heavy meromyosin (HMM).ATP to actin. This effect results from the direct binding of caldesmon to myosin in the order of affinity: smooth muscle HMM greater than skeletal muscle HMM greater than smooth muscle S-1 greater than skeletal muscle S-1 (Hemric, M. E., and Chalovich, J. M. (1988) J. Biol. Chem. 263, 1878-1885). We now show that the difference between skeletal muscle HMM and S-1 is due to the presence of the S-2 region in HMM and is unrelated to light chain composition or to two-headed versus single-headed binding. Differences between the binding of smooth and skeletal muscle myosin subfragments to actin do not result from the lack of light chain 2 in skeletal muscle S-1. In the presence of ATP, caldesmon binds to smooth muscle myosin filaments with a stoichiometry of 1:1 (K = 1 x 10(6) M-1). Similar results were obtained for the binding of caldesmon to smooth muscle rod as well as the binding of the purified myosin-binding fragment of caldesmon to smooth muscle myosin. The binding of caldesmon to intact myosin is ATP sensitive. The interaction of caldesmon with myosin is apparently specific and sensitive to the structure of both proteins.     

Effect of phosphorylation on the binding of smooth muscle heavy meromyosin X ADP to actin

Relaxation of both smooth and skeletal muscles appears to be caused primarily by inhibition of the step associated with Pi release in the actomyosin ATPase cycle, rather than by a block in the binding of the myosin X ATP and myosin X ADP X Pi complexes to actin. In skeletal muscle, troponin-tropomyosin not only causes marked inhibition of Pi release, but it also markedly inhibits the binding of myosin subfragment-1 X ADP to actin, raising the possibility that the two phenomena are coupled in some way. In the present study we determined whether phosphorylation of smooth muscle heavy meromyosin (HMM) also affects both the binding of HMM X ADP to actin and the Pi release step. This was done by having phosphorylated and unphosphorylated HMM X ADP compete for sites on F-actin. At mu = 30 mM, phosphorylation increased the affinity of the HMM molecule for actin about 12-fold and at mu = 170 mM, there was less than a 3-fold increase in the affinity of HMM. If phosphorylation affects the binding of each head of HMM to the same extent, then phosphorylation caused about a 4- and 2-fold increase in the affinity of each head of HMM for actin at mu = 30 and 170 mM, respectively. In contrast, at both ionic strengths, phosphorylation caused more than 100-fold actin activation of the ATPase activity of smooth muscle HMM. Therefore, the marked activation of Pi release in the acto X HMM ATPase cycle upon phosphorylation of HMM is not accompanied by a comparable increase in the affinity of HMM X ADP for actin. We have also found that phosphorylation increases by only 4-fold the rate of Pi release from HMM alone. These results suggest that in smooth muscle, phosphorylation accelerates the step associated with the release of Pi both in the forward and the reverse direction without correspondingly affecting the binding of myosin X ADP to actin.     

Germinal center-specific protein human germinal center associated lymphoma directly interacts with both myosin and actin and increases the binding of myosin to actin

Human germinal center associated lymphoma (HGAL) is a germinal center-specific gene whose expression correlates with a favorable prognosis in patients with diffuse large B-cell and classic Hodgkin lymphomas. HGAL is involved in negative regulation of lymphocyte motility. The movement of lymphocytes is directly driven by actin polymerization and actin-myosin interactions. We demonstrate that HGAL interacts directly and independently with both actin and myosin and delineate the HGAL and myosin domains responsible for the interaction. Furthermore, we show that HGAL increases the binding of myosin to F-actin and inhibits the ability of myosin to translocate actin by reducing the maximal velocity of myosin head/actin movement. No effects of HGAL on actomyosin ATPase activity and the rate of actin polymerization from G-actin to F-actin were observed. These findings reveal a new mechanism underlying the inhibitory effects of germinal center-specific HGAL protein on lymphocyte and lymphoma cell motility.     

Calcium-sensitive binding of heavy meromyosin to regulated actin requires light chain 2 and the head-tail junction

Sedimentation in a preparative ultracentrifuge was used to determine the affinity of heavy meromyosin, HMM, for regulated actin, F-actin plus troponin-tropomyosin, in the presence of MgATP at pH 7.0, 20 degrees C, and mu = 18 mM. HMM was prepared from vertebrate striated muscle myosin by a mild chymotryptic digestion. This HMM contained 85-90% intact 19 000-dalton light chains, LC2. In the presence of calcium, 90% of the HMM bound to regulated actin with an association constant of (2-4) X 10(4) M-1. In the absence of calcium, while one-third of the HMM bound with an affinity similar to that observed in the presence of calcium, the rest bound much more weakly. It was not possible to accurately determine the association constant for this weakly binding HMM, but a 20-fold reduction in affinity is consistent with the binding data. The binding of single-headed heavy meromyosin to regulated actin was similarly sensitive to the calcium concentration. Since removal of calcium inhibits the regulated actin-activated ATPase of HMM greater than 20-fold, troponin-tropomyosin must be capable of inhibiting both the binding of HMM to regulated actin and a step which occurs after binding but prior to product release. Removal of LC2 increased the fraction of HMM with calcium-insensitive binding, and adding LC2 back to this depleted HMM restored most of the calcium sensitivity. Chymotryptic cleavage of LC2 to a 17 000-dalton fragment destroyed the calcium-sensitive binding of HMM to regulated actin. Phosphorylation of LC2, however, had no detectable effect on this binding. Thus, the calcium-sensitive binding of HMM to regulated actin requires that both the head-tail junction and the N-terminal part of LC2 be intact. Binding studies with cross-linked regulated actins and kinetic measurements of the rates of change in turbidity demonstrate that this calcium sensitivity is due to calcium binding to troponin and not to LC2.     

Investigation of the actin-deoxyribonuclease I interaction using a pyrene-conjugated actin derivative

The interaction of deoxyribonuclease I with muscle actin was studied with the aid of a pyrenyl derivative of the actin [Kouyama, T., & Mihashi, K. (1981) Eur. J. Biochem. 114, 33-38] that increases its quantum yield by an order of magnitude on polymerization. It is shown that this derivative copolymerizes with unlabeled G-actin in a random manner and will also bind to deoxyribonuclease with inhibition of enzymic activity. The derivative affords a highly sensitive means of following nucleated polymerization. Preincubation of F-actin with deoxyribonuclease at a concentration of 5% or less of that of total subunits causes inhibition of polymerization of additional G-actin onto the filaments. In red cell membranes that contain stabilized short filaments of actin such that the concentration of filament ends is large relative to monomers, complete inhibition of nucleated polymerization of G-actin is achieved by preincubation with deoxyribonuclease. The results indicate that binding of DNase occurs at the "plus" ends of the actin filaments. Competition with cytochalasin E, which is known to have a high affinity for the plus or preferentially growing ends of F-actin, can be observed. Whereas the activity of deoxyribonuclease in the 1:1 complex with G-actin is inhibited, the enzyme attached to the ends of filaments appears to be fully active. This causes a reduction in the inhibition of enzymic activity with increasing F-actin concentration, presumably by reason of a change in the partition of the enzyme between monomers and filament ends. The degree of inhibition increases with time, however, as the actin depolymerizes. Implications for measurements of actin monomer concentrations by the deoxyribonuclease assay procedure are considered.     

Mechanism for the inhibition of acto-heavy meromyosin ATPase by the actin/calmodulin binding domain of caldesmon.

Caldesmon, an actin/calmodulin binding protein, inhibits acto-heavy meromyosin (HMM) ATPase, while it increases the binding of HMM to actin, presumably mediated through an interaction between the myosin subfragment 2 region of HMM and caldesmon, which is bound to actin. In order to study the mechanism for the inhibition of acto-HM ATPase, we utilized the chymotryptic fragment of caldesmon (38-kDa fragment), which possesses the actin/calmodulin binding region but lacks the myosin binding portion. The 38-kDa fragment inhibits the actin-activated HMM ATPase to the same extent as does the intact caldesmon molecule. In the absence of tropomyosin, the 38-kDa fragment decreased the KATPase and Kbinding without any effect on the Vmax. However, when the actin filament contained bound tropomyosin, the caldesmon fragment caused a 2-3-fold decrease in the Vmax, in addition to lowering the KATPase and the Kbinding. The 38-kDa fragment-induced inhibition is partially reversed by calmodulin at a 10:1 molar ratio to caldesmon fragment; the reversal was more remarkable in 100 mM ionic strength at 37 degrees C than in 20 or 50 mM at 25 degrees C. Results from these experiments demonstrate that the 38-kDa domain of caldesmon fragment of myosin head to actin; however, when the actin filament contains bound tropomyosin, caldesmon fragment affects not only the binding of HMM to/actin but also the catalytic step in the ATPase cycle. The interaction between the 38-kDa domain of caldesmon and tropomyosin-actin is likely to play a role in the regulation of actomyosin ATPase and contraction in smooth muscle.     

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.     

Effects of urea and guanidine hydrochloride on the sliding movement of actin filaments with ATP hydrolysis by myosin molecules

To evaluate the role of the hydration layer on the protein surface of actomyosin, we compared the effects of urea and guanidine-HCl on the sliding velocities and ATPase activities of the actin-heavy meromyosin (HMM) system. Both chemicals denature proteins, but only urea perturbs the hydration layer. Both the sliding velocity of actin filaments and actin-activated ATPase activity decreased with increasing urea concentrations. The sliding movement was completely inhibited at 1.0 M urea, while actin filaments were bound to HMM molecules fixed on the glass surface. Guanidine-HCl (0-0.05 M) drastically decreased both the sliding velocity and ATPase activation of acto-HMM complexes. Under this condition, actin filaments almost detached from HMM molecules. In contrast, the ATPase activity of HMM without actin filaments was almost independent of urea concentrations <1.0 M and guanidine-HCl concentrations <0.05 M. An increase in urea concentrations up to 2.0 M partly induced changes in the ternary structure of HMM molecules, while the actin filaments were stable in this concentration range. Hydration changes around such actomyosin complexes may alter both the stability of part of the myosin molecules, and the affinity for force transmission between actin filaments and myosin heads.     

Functional characterization of skeletal F-actin labeled on the NH2-terminal segment of residues 1-28

Rabbit skeletal alpha-actin was covalently labeled in the filamentous state by the fluorescent nucleophile, N-(5-sulfo-1-naphthyl)ethylenediamine (EDANS) in the presence of the carboxyl group activator 1-(3-dimethyl-aminopropyl)-3-ethylcarbodiimide (EDC). The coupling reaction was continued until the incorporation of nearly 1 mol EDANS/mol actin. After limited proteolytic digestion of the labeled protein and chromatographic identification of the EDANS-peptides, about 80% of the attached fluorophore was found on the actin segment of residues 1-28, most probably within the N-terminal acidic region of residues 1-7. A minor labeling site was located on the segment that consists of residues 40-113. No label was incorporated into the COOH-terminal moiety consisting of residues 113-375. The isolated EDANS-G-actin undergoes polymerization in the presence of salts but at a rate significantly greater than unlabeled actin. The EDANS-F-actin could be complexed to skeletal chymotryptic myosin subfragment 1 (S-1) and to tropomyosin. The complex formed between EDANS-F-actin and S-1 could not be further crosslinked by EDC but the two proteins were readily joined by glutaraldehyde as observed for native actin-S-1, suggesting that the EDANS-substituted carboxyl site is also involved in the EDC crosslinking of native actin to S-1. Moreover, the EDANS labeling of F-actin resulted in a 20-fold increase in the Km of the actin-activated Mg2+.ATPase of S-1. Thus, this labeling, while it did not much affect the rigor actin-S-1 interaction, changes the actin binding to the S-1-nucleotide complexes significantly. The selective introduction of a variety of spectral probes, like EDANS, or other classes of fluorophores, on the N-terminal region of actin, through the reported carbodiimide coupling reaction, would provide several different derivatives valuable for assessing the functional role of the negatively charged N-terminus of actin during its interaction with myosin and other actin-binding proteins.     

A kinetic model for the molecular basis of the contractile activity of Acanthamoeba myosins IA and IB

Acanthamoeba myosins IA and IB are single-headed, monomeric molecules consisting of one heavy chain and one light chain. Both have high actin-activated Mg2+-ATPase activity, when the heavy chain is phosphorylated, but neither seems to be able to form the bipolar filaments that are generally thought to be required for actomyosin-dependent contractility. In this paper, we show that, at fixed F-actin concentration, the actin-activated Mg2+-ATPase activities of myosins IA and IB increase about 5-fold in specific activity in a cooperative manner as the myosin concentration is increased. The myosin concentration range over which this cooperative change occurs depends on the actin concentration. More myosin I is required for the cooperative increase in activity at high concentrations of F-actin. The cooperative increase in specific activity at limiting actin concentrations is caused by a decrease in the KATPase for F-actin. The high and low KATPase states of the myosin have about the same Vmax at infinite actin concentration. Both myosins are completely bound to the F-actin long before the Vmax values are reached. Therefore, much of the actin activation must be the result of interactions between F-actin and actomyosin. These kinetic data can be explained by a model in which the cooperative shift of myosin I from the high KATPase to the low KATPase state results from the cross-linking of actin filaments by myosin I. Cross-linking might occur either through two actin-binding sites on a single molecule or by dimers or oligomers of myosin I induced to form by the interaction of myosin I monomers with the actin filaments. The ability of Acanthamoeba myosins IA and IB to cross-link actin filaments is demonstrated in the accompanying paper (Fujisaki, H., Albanesi, J.P., and Korn, E.D. (1985) J. Biol. Chem. 260, 11183-11189).     

Flexibility of myosin attachment to surfaces influences F-actin motion.

We have analyzed the dependence of actin filament sliding movement on the mode of myosin attachment to surfaces. Monoclonal antibodies (mAbs) that bind to three distinct sites were used to tether myosin to nitrocellulose-coated glass. One antibody reacts with an epitope on the regulatory light chain (LC2) located at the head-rod junction. The other two react with sites in the rod domain, one in the S2 region near the S2-LMM hinge, and the other at the C terminus of the myosin rod. This method of attachment provides a means of controlling the flexibility and density of myosin on the surface. Fast skeletal muscle myosin monomers were bound to the surfaces through the specific interaction with these mAbs, and the sliding movement of fluorescently labeled actin filaments was analyzed by video microscopy. Each of these antibodies produced stable myosin-coated surfaces that supported uniform motion of actin over the course of several hours. Attachment of myosin through the anti-S2 and anti-LMM mAbs yielded significantly higher velocities (10 microns/s at 30 degrees C) than attachment through anti-LC2 (4-5 microns/s at 30 degrees C). For each antibody, we observed a characteristic value of the myosin density for the onset of F-actin motion and a second critical density for velocity saturation. The specific mode of attachment influences the velocity of actin filaments and the characteristic surface density needed to support movement.     

Insight into the mechanism of fast movement of myosin from Chara corallina

Chara myosin, two-headed plant myosin belonging to class XI, slides F-actin at maximally 60 microm s(-1). To elucidate the mechanism of this fast sliding, we extensively investigated its mechanochemical properties. The maximum actin activated ATPase activity, Vmax, was 21.3 s(-1) head(-1) in a solution, but when myosin was immobilized on the surface, its activity was 57.6 s(-1) head(-1) at 2 mg ml(-1) of F-actin. The sliding velocity and the actin activated ATPase activity were greatly inhibited by ADP, suggesting that ADP dissociation was the rate limiting step. With the extensive assay of motility by varying the surface density, the duty ratio of Chara myosin was found to be 0.49-0.44 from velocity measurements and 0.34 from the landing rate analysis. At the surface density of 10 molecules microm(-2), Chara myosin exhibited pivot movement under physiological conditions. Based on the results obtained, we will discuss the sliding mechanism of Chara myosin according to the working stroke model in terms of its physiological aspects. aspects.     

An EPR study of the rotational dynamics of actins from striated and smooth muscle and their complexes with heavy meromyosin

The rotational motions of the actin from rabbit skeletal muscle and from chicken gizzard smooth muscle were measured by conventional and saturation transfer electron paramagnetic resonance (EPR) spectroscopy using maleimide spin-label rigidly bound at Cys-374. The conventional EPR spectra indicate a slight difference in the polarity of the environment of the label and in the rotational mobility of the monomeric gizzard actin compared to its skeletal muscle counterpart. These differences disappear upon polymerization. The EPR spectra of the two actins in their F form and in their complexes with heavy meromyosin (HMM) did not reveal any difference in the rotational dynamic properties that might be correlated with the known differences in the activation of myosin ATPase activity by smooth and skeletal muscle actin. Our results agree with earlier EPR studies on skeletal muscle actin in showing that polymerization stops the nanosecond rotational motion of actin monomers and that F-actin undergoes rotational motion having an effective correlation time of the order of 0.1 ms. However, our measurements show that complete elimination of the nanosecond motions requires prolonged incubation of F-actin, suggesting that the slow formation of interfilamental cross-links in concentrated F-actin solutions contributes to this process. We have also used the EPR spectroscopy to study the interaction between HMM and actin in the F and G form. Our results show that in the absence of salt one HMM molecule can cooperatively interact with eight monomers to produce a polymer which closely resembles F-actin in its rotational mobility but differs from the complex of F-actin with HMM. The results indicate that salt is necessary for further slowing down, in a cooperative manner, the sub-millisecond internal motion in actin polymer and for a non-cooperative change in the intramonomer conformation around Cys-374 on the binding of HMM.