Fluorescence energy transfer between nucleotide binding sites in an F-actin filament

Basic residues within the cardiac troponin T C terminus are required for full inhibition of muscle contraction and limit activation by calcium

Striated muscle is activated by myosin- and actin-linked processes, with the latter being regulated through changes in the position of tropomyosin relative to the actin surface. The C-terminal region of cardiac troponin T (TnT), a tropomyosin-associated protein, is required for full TnT inactivation at low Ca²⁺ and for limiting its activation at saturating Ca²⁺ Here, we investigated whether basic residues in this TnT region are involved in these activities, whether the TnT C terminus undergoes Ca²⁺-dependent conformational changes, and whether these residues affect cardiac muscle contraction. We generated a human cardiac TnT variant in which we replaced seven C-terminal Lys and Arg residues with Ala and added a Cys residue at either position 289 or 275 to affix a fluorescent probe. At pCa 3.7, actin filaments containing high-alanine TnT had an elevated ATPase rate like that obtained when the last TnT 14 residues were deleted. Acrylodan-tropomyosin fluorescence changes and S1-actin binding kinetics revealed that at pCa 8, the high-alanine TnT-containing filaments did not enter the first inactive state. FRET analyses indicated that the C-terminal TnT region approached Cys-190 of tropomyosin as actin filaments transitioned to the inactive B state; that transition was abolished with high-alanine TnT. High-alanine TnT-containing cardiac muscle preparations had increased Ca²⁺ sensitivity of both steady-state isometric force and sinusoidal stiffness as well as increased maximum steady-state isometric force and sinusoidal stiffness. We conclude that C-terminal basic residues in cardiac TnT are critical for the regulation of cardiac muscle contraction.

A three-dimensional FRET analysis to construct an atomic model of the actin-tropomyosin complex on a reconstituted thin filament

Fluorescence resonance energy transfer (FRET) was used to construct an atomic model of the actin-tropomyosin (Tm) complex on a reconstituted thin filament. We generated five single-cysteine mutants in the 146-174 region of rabbit skeletal muscle α-Tm. An energy donor probe was attached to a single-cysteine Tm residue, while an energy acceptor probe was located in actin Gln41, actin Cys374, or the actin nucleotide binding site. From these donor-acceptor pairs, FRET efficiencies were determined with and without Ca(2+). Using the atomic coordinates for F-actin and Tm, we searched all possible arrangements for Tm segment 146-174 on F-actin to calculate the FRET efficiency for each donor-acceptor pair in each arrangement. By minimizing the squared sum of deviations for the calculated FRET efficiencies from the observed FRET efficiencies, we determined the location of the Tm segment on the F-actin filament. Furthermore, we generated a set of five single-cysteine mutants in each of the four Tm regions 41-69, 83-111, 216-244, and 252-279. Using the same procedures, we determined each segment's location on the F-actin filament. In the best-fit model, Tm runs along actin residues 217-236, which were reported to compose the Tm binding site. Electrostatic, hydrogen-bonding, and hydrophobic interactions are involved in actin and Tm binding. The C-terminal region of Tm was observed to contact actin more closely than did the N-terminal region. Tm contacts more residues on actin without Ca(2+) than with it. Ca(2+)-induced changes on the actin-Tm contact surface strongly affect the F-actin structure, which is important for muscle regulation.

Fluorescence resonance energy transfer between residues on troponin and tropomyosin in the reconstituted thin filament: modeling the troponin-tropomyosin complex

Troponin (Tn), in association with tropomyosin (Tm), plays a central role in the calcium regulation of striated muscle contraction. Fluorescence resonance energy transfer (FRET) between probes attached to the Tn subunits (TnC, TnI, TnT) and to Tm was measured to study the spatial relationship between Tn and Tm on the thin filament. We generated single-cysteine mutants of rabbit skeletal muscle alpha-Tm, TnI and the beta-TnT 25-kDa fragment. The energy donor was attached to a single-cysteine residue at position 60, 73, 127, 159, 200 or 250 on TnT, at 98 on TnC and at 1, 9, 133 or 181 on TnI, while the energy acceptor was located at 13, 146, 160, 174, 190, 209, 230, 271 or 279 on Tm. FRET analysis showed a distinct Ca(2+)-induced conformational change of the Tm-Tn complex and revealed that TnT60 and TnT73 were closer to Tm13 than Tm279, indicating that the elongated N-terminal region of TnT extends beyond the beginning of the next Tm molecule on the actin filament. Using the atomic coordinates of the crystal structures of Tm and the Tn core domain, we searched for the disposition and orientation of these structures by minimizing the deviations of the calculated FRET efficiencies from the observed FRET efficiencies in order to construct atomic models of the Tn-Tm complex with and without bound Ca(2+). In the best-fit models, the Tn core domain is located on residues 160-200 of Tm, with the arrowhead-shaped I-T arm tilting toward the C-terminus of Tm. The angle between the Tm axis and the long axis of TnC is approximately 75 degrees and approximately 85 degrees with and without bound Ca(2+), respectively. The models indicate that the long axis of TnC is perpendicular to the thin filament without bound Ca(2+), and that TnC and the I-T arm tilt toward the filament axis and rotate around the Tm axis by approximately 20 degrees upon Ca(2+) binding.

The beta4-beta8 groove is an ATP-interactive site in the alpha crystallin core domain of the small heat shock protein, human alphaB crystallin

The site for ATP interactions in human alphaB crystallin, the archetype of small heat-shock proteins, was identified and characterized to resolve the controversial role of ATP in the function of small heat-shock proteins. Comparative sequence alignments identified the alphaB crystallin sequence, (82)KHFSPEELKVKVLGD(96) as a Walker-B ATP-binding motif that is found in several ATP-binding proteins, including five molecular chaperones. Fluorescence resonance energy transfer and mass spectrometry using a novel fluorescent ATP analog, 8-azido-ATP-[gamma]-1-naphthalenesulfonic acid-5(2-aminoethylamide) (azido-ATP-EDANS) and a cysteine mutant of human alphaB crystallin (S135C) conjugated with a fluorescent acceptor, eosin-5-maleimide (EMA) identified the beta4-beta8 groove as the ATP interactive site in alphaB crystallin. A 44% decrease in the emitted fluorescence of azido-ATP-EDANS at the absorption maximum of S135C-EMA and a corresponding 50% increase in the fluorescence emission of S135C-EMA indicated a close spatial relationship between azido-ATP-EDANS and the center of the beta8 strand ((131)LTITSSLS(138)). Liquid chromatography, electrospray ionization mass spectrometry identified two peptide fragments of the alphaB crystallin Walker-B motif photo-affinity-labeled with azido-ATP-EDANS confirming the beta4-beta8 groove as an ATP interactive site. The results presented here clearly establish the beta4-beta8 groove as the ATP interactive region in alphaB crystallin, and are in contrast to the existing paradigm that classifies small heat-shock proteins as ATP-independent chaperones.

Steady-state fluorescence quenching applications for studying protein structure and dynamics

Fluorescence quenching methods are useful to obtain information about the conformational and/or dynamic changes of proteins in complex macromolecular systems. In this review steady-state methods are described and the data interpretation is thoroughly discussed. As a special case of fluorescence quenching mechanism, fluorescence resonance energy transfer (FRET) phenomenon is also presented. Application of a FRET based method to characterize the temperature dependence of the flexibility of protein matrix is clearly demonstrated.

Conformational and dynamic differences between actin filaments polymerized from ATP- or ADP-actin monomers

Conformational and dynamic properties of actin filaments polymerized from ATP- or ADP-actin monomers were compared by using fluorescence spectroscopic methods. The fluorescence intensity of IAEDANS attached to the Cys(374) residue of actin was smaller in filaments from ADP-actin than in filaments from ATP-actin monomers, which reflected a nucleotide-induced conformational difference in subdomain 1 of the monomer. Radial coordinate calculations revealed that this conformational difference did not modify the distance of Cys(374) from the longitudinal filament axis. Temperature-dependent fluorescence resonance energy transfer measurements between donor and acceptor molecules on Cys(374) of neighboring actin protomers revealed that the inter-monomer flexibility of filaments assembled from ADP-actin monomers were substantially greater than the one of filaments from ATP-actin monomers. Flexibility was reduced by phalloidin in both types of filaments.

Conformational distributions and proximity relationships in the rigor complex of actin and myosin subfragment-1

Cyclic conformational changes in the myosin head are considered essential for muscle contraction. We hereby show that the extension of the fluorescence resonance energy transfer method described originally by Taylor et al. (Taylor, D. L., Reidler, J., Spudich, J. A., and Stryer, L. (1981) J. Cell Biol. 89, 362-367) allows determination of the position of a labeled point outside the actin filament in supramolecular complexes and also characterization of the conformational heterogeneity of an actin-binding protein while considering donor-acceptor distance distributions. Using this method we analyzed proximity relationships between two labeled points of S1 and the actin filament in the acto-S1 rigor complex. The donor (N-[[(iodoacetyl)amino]ethyl]-5-naphthylamine-1-sulfonate) was attached to either the catalytic domain (Cys-707) or the essential light chain (Cys-177) of S1, whereas the acceptor (5-(iodoacetamido)fluorescein) was attached to the actin filament (Cys-374). In contrast to the narrow positional distribution (assumed as being Gaussian) of Cys-707 (5 +/- 3 A), the positional distribution of Cys-177 was found to be broad (102 +/- 4 A). Such a broad positional distribution of the label on the essential light chain of S1 may be important in accommodating the helically arranged acto-myosin binding relative to the filament axis.

Effects of denervation and muscle inactivity on the organization of F-actin

To discriminate between the influences of a motoneuron and muscle activity on the conformation of actin filaments, the extrinsic polarized fluorescence [of rhodamine-phalloidin and N-(iodoacetylamine)-1-naphthylamine-5-sulfonic acid attached to F-actin] was measured in "ghost" fibers from intact rat soleus muscles and atrophying muscles after denervation, immobilization, or tenotomy. The results show that the conformation of F-actin changed in all the atrophying muscles, but differently. In the denervated muscle, the flexibility of the actin filaments decreased, whereas in the other experimental muscles it remained as in the intact muscle. In the denervated muscle, the mobility of the C-terminus of the actin polypeptide increased. Attachment of myosin subfragment-1 influenced the F-actin conformation differently in the denervated muscle than in the other muscles studied. These results suggest that changes in the conformation of the actin filament are induced by the lack of connection with the motoneuron rather than by muscle inactivity.

A conformational change in F-actin when myosin binds: fluorescence resonance energy transfer detects an increase in the radial coordinate of Cys-374

Interactions of myosin with actin filaments probably induce conformational changes in actin which are crucial for its function. Fluorescence resonance energy transfer spectroscopy can determine changes in distance (range 10-100 A) between two probes and therefore can sense conformational changes in proteins. We have investigated changes in the radial coordinates of fluorescent probes bound to Cys-374 of F-actin when either of the isozymes (S1A1 and S1A2) of myosin subfragment 1 (S-1) bind. Using 5-[[2-[(iodoacetyl)amino]ethyl]amino]naphthalene-1-sulfonic acid and N-(4-dimethylamino-3,5-dinitrophenyl)maleimide as donor and acceptor probes, respectively, we calculated a radius of 13-14 A. This distance increased by approximately 4.5 A upon addition of S-1. No differences were detected between the effects of S1A1 and S1A2. This increase is reversed by MgATP. The average position of the probes on Cys-374 is closer to the filament axis than expected from the current models of F-actin. S-1 increases the radial position of Cys-374 either by direct interaction or via an allosteric conformational change associated with its binding.

Actin and the actomyosin interface: a review

This review deals with the structure of the actin monomer, its assembly into filaments and the loci on F-actin involved in binding myosin. Two distinctly different arrangements of monomers have been suggested for actin filaments. One model proposed by Holmes et al. is well developed. It places the so-called 'large' domain close to the filament axis and the so-called 'small' domain out near the surface of the filament. A second, less-well developed, model proposed by Schutt et al. locates the 'small' domain close to the filament axis and they rotate the monomer so that 'bottom' of the 'large' domain is at the highest radius. We analyze the available evidence for the models of F-actin derived from X-ray diffraction, reconstructions from electron micrographs, fluorescence resonance energy transfer spectroscopy, chemical cross-linking, antibody probes, limited proteolysis, site-directed and natural mutations, nuclear magnetic resonance spectroscopy and other techniques. The result is an actin-centered view of the loci on actin which are probably involved in its interaction with the myosin 'head'. From these multiple contacts we speculate on the sequence of steps between the initial weak-binding state of S-1 to the actin filament through to the stable strong-binding state seen in the absence of free Mg-ATP, i.e., the rigor state.

Evidence for an F-actin like conformation in the actin:DNase I complex

We demonstrate that a ribose modified analogue of ATP, TNP-ATP, can exchange with a resident nucleotide in F-actin, but fails to bind to G-actin. TNP-ATP is also able to bind to actin in the actin:DNase I complex, suggesting that the nucleotide binding site in the actin:DNase I complex adopts a conformation similar to that found in F-actin. This result is consistent with the hypothesis that the two major domains of actin on either side of the cleft are able to "flex" or move relative to each other in G-actin, but that this flexing motion is limited as a consequence of either polymerisation or DNase I binding. F-actin, in which approximately 80% of the bound nucleotide is TNP-ADP, appears to be functionally similar to native ADP-F-actin. It can superprecipitate with myosin and, following regulation with troponin-tropomyosin, exhibits a Ca(2+)-sensitivity during superprecipitation. Sonication induced nucleotide exchange in regulated F-actin was not sensitive to the presence of Ca2+ which argues against a significant conformational change in the vicinity of the nucleotide binding site during Ca(2+)-sensitive thin filament regulation.

Effects of sulphydryl modification on skinned rat skeletal muscle fibres using 5,5'-dithiobis(2-nitrobenzoic acid)

1. The sulphydryl groups of skinned skeletal muscle fibres have been reacted with 5,5'-dithiobis(2-nitrobenzoic acid) (DTNB) in order to determine whether the effects of modifications to the contractile proteins are reflected in changes in the physiological properties of the contractile apparatus and Ca(2+)-regulatory system. 2. Results obtained from fast-twitch and slow-twitch rat fibres which were treated with DTNB (10 mM, pH 8.6, 5 degrees C) for various periods of time under relaxing conditions showed that a major effect of the modification was to reduce the level of maximally Ca(2+)-activated force and fibre stiffness. Force and fibre stiffness were found to decline in proportion. Treatment with DTNB under these conditions did not cause a rise in force or fibre stiffness in relaxed fibres of either type. 3. The effects induced by DTNB under relaxing conditions were substantially reversed by exposure to the reducing agent dithiothreitol (DTT) (10 mM, pH 7.1, 23 degrees C). Force abolished by 30-35 s treatment with DTNB recovered after subsequent DTT treatment to 67 +/- 3% (mean +/- S.E.M., n = 4) in fast-twitch fibres and to 91 +/- 2% (n = 7) in slow-twitch fibres. These results were significantly different (t test, P less than 0.001) indicating that the level of force recovery depended upon the fibre type. 4. DTNB was found to affect not only the maximal Ca(2+)-activated force, but also the force-pCa (pCa = -log10[Ca2+]) relationships of the fibres in a complex, fibre-type specific way. DTT treatment partially reversed these DTNB effects. 5. The skinned fibre preparations reacted differently with DTNB under rigor conditions than under relaxing conditions, indicating that rigor modifies the reactivity of the functional sulphydryl groups to the thiol-targeted agents. 6. When superprecipitation assays (an in vitro analogue of fibre contraction) were carried out with recombined myofibrillar proteins which had been previously reacted with DTNB it was found that modification of myosin, but not modification of thin filament proteins, led to changes in the superprecipitation reaction. 7. Both the skinned fibre results and the superprecipitation results indicate that the effects of DTNB upon the fibre characteristics are primarily due to modifications of the sulphydryl groups of myosin. Therefore, these results show that myosin is not only involved in determining the ability of the contractile apparatus to develop force but also in determining the Ca(2+)-regulatory characteristics of the muscle fibre.

Atomic model of the actin filament

The F-actin filament has been constructed from the atomic structure of the actin monomer to fit the observed X-ray fibre diagram from oriented gels of F-actin. A unique orientation of the monomer with respect to the actin helix has been found. The main interactions are along the two-start helix with a contribution from a loop extending across the filament axis provided by the molecule in the adjacent strand. There are also contacts along the left-handed genetic helix.

Distance between the substrate and regulatory reduced coenzyme binding sites of bovine liver glutamate dehydrogenase by resonance energy transfer

Bovine liver glutamate dehydrogenase is known to bind reduced coenzyme at two sites/subunit, one catalytic and one regulatory; ADP competes for the latter site. The enzyme is here shown to be catalytically active with the thionicotinamide analogue of NADPH [( S]NADPH). For native enzyme, ultrafiltration studies revealed that [S]NADPH reversibly occupies about two sites/enzyme subunit in the absence of other ligands; by the addition of ADP, [S]NADPH binding can be limited to one molecule/subunit. The enzyme is irreversibly inactivated by reaction with 4-(iodoacetamido)salicylic acid (ISA) at lysine126 within the 2-oxoglutarate binding site [Holbrook, J.J., Roberts, P.A. & Wallis, R.B. (1973) Biochem. J. 133, 165-171]. ISA-modified enzyme binds 1 molecule [S]NADPH/subunit in the absence of ADP, suggesting that reaction at the substrate site blocks binding at the catalytic, but not at the regulatory site. The fluorescence spectrum of ISA-modified enzyme overlaps the absorption spectrum of [S]NADPH allowing a distance measurement between these sites by resonance energy transfer. [S]NADPH quenches the emission of ISA-modified enzyme, yielding 3.2 nm as the average distance between sites. ADP competes for the [S]NADPH site but does not affect the fluorescence of ISA-modified enzyme, indicating that [S]NADPH quenching is attributable to energy transfer rather than to a conformational change. The 3.2 nm thus represents the distance between the 2-oxoglutarate and reduced coenzyme regulatory sites of glutamate dehydrogenase.

Spatial relationship between the nucleotide-binding site, Lys-61 and Cys-374 in actin and a conformational change induced by myosin subfragment-1 binding

The spatial relationship between Lys-61, the nucleotide binding site and Cys-374 was studied. Lys-61 was labelled with fluorescein-5-isothiocyanate as a resonance energy acceptor, the nucleotide-binding site was labelled with the fluorescent ATP analogues epsilon ATP or formycin-A 5'-triphosphate (FTP) and Cys-374 was labelled with 5-(2-[(iodoacetyl)amino]ethyl)aminonaphthalene-1-sulfonic acid (1,5-IAEDANS) as a resonance energy donor. The distances between the nucleotide binding site and Lys-61 or between Lys-61 and Cys-374 were calculated to be 3.5 +/- 0.3 nm and 4.60 +/- 0.03 nm, respectively. (The assumption has been made in calculating these distances that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime.) On the other hand, when doubly-labelled actin with 1,5-IAEDANS at Cys-374 and FITC at Lys-61 was polymerized in the presence of a twofold molar excess of phalloidin [Miki, M. (1987) Eur. J. Biochem. 164, 229-235], the fluorescence of 1,5-IAEDANS bound to actin was quenched significantly. This could be attributed to inter-monomer energy transfer. The inter-monomer distance between FITC attached to Lys-61 in a monomer and 1,5-IAEDANS attached to Cys-374 in its nearest-neighbour monomer in an F-actin filament was calculated to be 3.34 +/- 0.06 nm, assuming that the likely change in the intra-monomer distance does not change during polymerization by more than 0.4 nm. One possible spatial relationship between Lys-61, Cys-374 and the nucleotide binding site in an F-actin filament is proposed. The effect of myosin subfragment-1 (S1) binding on the energy transfer efficiency was studied. The fluorescence intensity of AEDANS-FITC-actin decreased by 30% upon interaction with S1. The fluorescence intensity of AEDANS-FITC-actin polymer in the presence of phalloidin increased by 21% upon interaction with S1. The addition of ATP led to the fluorescence intensity returning to the initial level. Assuming that the change of fluorescence intensity can be attributed to conformational change in the actin molecule induced by S1 binding, the intra-monomer distance was reduced by 0.4 nm and the inter-monomer distance was increased by 0.2 nm.

Interaction of phalloidin with chemically modified actin

Modification of Tyr-69 with tetranitromethane impairs the polymerizability of actin in accordance with the previous report [Lehrer, S. S. and Elzinga, M. (1972) Fed. Proc. 31, 502]. Phalloidin induces this chemically modified actin to form the same characteristic helical thread-like structure as normal F-actin. The filaments bind myosin heads and activate the myosin ATPase activity as effectively as normal F-actin. When a dansyl group is introduced at the same point [Chantler, P. D. and Gratzer, W. B. (1975) Eur. J. Biochem. 60, 67-72], phalloidin still induces the polymerization. The filaments bind myosin heads and activate the myosin ATPase activity. These results indicate that Tyr-69 is not directly involved in either an actin-actin binding site or the myosin binding site on actin. Moreover, the results suggest that phalloidin binds to actin monomer in the presence of salt and its binding induces a conformational change in actin which is essential for polymerization, or that actin monomer fluctuates between in unpolymerizable and polymerizable form while phalloidin binds to actin only in the polymerizable form and its binding locks the conformation which causes the irreversible polymerization of actin. Modification of Tyr-53 with 5-diazonium-(1H)tetrazole blocks actin polymerization [Bender, N., Fasold, H., Kenmoku, A., Middelhoff, G. and Volk, K. E. (1976) Eur. J. Biochem. 64, 215-218]. Phalloidin is unable to induce the polymerization of this modified actin nor does it bind to it. Phalloidin does not induce the polymerization of the trypsin-digested actin core. These results indicate that the site at which phalloidin binds is involved in polymerization and the probable conformational change involved in polymerization may be modulated through this site.

Fluorescence resonance energy transfer measurements of distances in actin and myosin. A critical evaluation

The contractile proteins actin and myosin are of considerable biological interest. They are essential for muscle contraction and in eukaryotic cells they play a crucial role in most contractile phenomena. Over the years since the first fluorescence resonance energy transfer (FRET) paper appeared, an extensive body of literature has accumulated on this technique using actin, myosin and the actomyosin complex. These papers are reviewed with several aims in mind: we assess the reliability and consistency of intra- and inter-molecular distances measured between the fluorescent probes attached to specific sites on these proteins; we determine whether the measurements can be assembled into an internally consistent model which can be fitted to the known dimensions of the actomyosin complex; several of the FRET distances are consistent with the available structural data from crystallographic and electron microscopic dimensions; the modelled FRET distances suggest that the assumed value of the orientation factor (k2 = 2/3) is reasonable; we conclude that the model has a predictive value, i.e. it suggests that a small number of the published dimensions may be incorrect and predicts the magnitude of a larger number of measurements which have not yet been reported; and finally (vi) we discuss the contribution of FRET determinations to the current debate on the molecular mechanism of contraction.

The recovery of the polymerizability of Lys-61-labelled actin by the addition of phalloidin. Fluorescence polarization and resonance-energy-transfer measurements

Modification of Lys-61 in actin with fluorescein-5-isothiocyanate (FITC) blocks actin polymerization [Burtnick, L. D. (1984) Biochim. Biophys. Acta 791, 57-62]. FITC-labelled actin recovered its ability to polymerize on addition of phalloidin. The polymers had the same characteristic helical thread-like structure as normal F-actin and the addition of myosin subfragment-1 to the polymers formed the characteristic arrowhead structure in electron microscopy. The polymers activated the ATPase activity of myosin subfragment-1 as efficiently as normal F-actin. These results indicate that Lys-61 is not directly involved in an actin-actin binding region nor in myosin binding site. From static fluorescence polarization measurements, the rotational relaxation time of FITC-labelled actin filaments was calculated to be 20 ns as the value reduced in water at 20 degrees C, while any rotational relaxation time of 1,5-IAEDANS bound to Cys-374 on F-actin in the presence of a twofold molar excess of phalloidin could not be detected by static polarization measurements under the same conditions. This indicates that the Lys-61 side chain is extremely mobile even in the filamentous structure. Fluorescence resonance energy transfer between the donor 1,5-IAEDANS bound to SH1 of myosin subfragment-1 and the acceptor fluorescein-5-isothiocyanate bound to Lys-61 of actin in the rigor complex was measured. The transfer efficiency was 0.39 +/- 0.05 which corresponds to the distance of 5.2 +/- 0.1 nm, assuming that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime and that the transfer occurs between a single donor and an acceptor.

Fluorescence resonance energy transfer between the nucleotide binding site and Cys-10 in G-actin and F-actin

Intramonomer fluorescence resonance energy transfer between the donor epsilon-ATP bound to the nucleotide site and the acceptor N-(4-dimethylamino-3,5-dinitrophenyl)maleimide (DDPM) or 4-dimethylaminophenyl-azophenyl-4'-maleimide bound to Cys-10 in G-actin was measured. The donor-acceptor distance was calculated to be about 40 A. The intermonomer energy transfer in F-actin occurring between epsilon-ADP and DABMI was also measured. The radial coordinate of Cys-10 was calculated to be 25 A based on the helical symmetry of F-actin and the recently calculated radial coordinate of the nucleotide binding site in F-actin i.e. 25 A (Miki, M., Hambly, B. and dos Remedios, C.G. (1986) Biochim. Biophys. Acta 871, 137-141). (The assumption has been made in calculating these distances that the energy donor and acceptor rotate rapidly relative to the fluorescence lifetime.) Corresponding distances separating the donor nucleotide in one monomer from acceptors on Cys-10 in the first and second nearest neighbours in F-actin are 39-40 A and 41-43 A.