The rate of MgADP binding to and dissociation from acto-S1

The rate of binding and dissociation of MgADP from its ternary complex with actin and S1 was measured by following the extent to which fixed concentrations of MgADP slow down MgATP-induced dissociation of acto-S1. The solution of the equations describing this process shows that at any MgADP concentration the apparent rate of acto-S1 dissociation should be proportional to a square root of the equilibrium constant for MgADP dissociation and to MgATP concentration. By measuring the apparent rate of acto-S1 dissociation as a function of MgATP concentration, the rate of MgADP binding and dissociation were determined as 5 X 10(6) M-1 X s-1 and 1400 s-1, respectively. These rates were unchanged by modification of SH1 thiol of S1 by a variety of fluorescence and spin-labels, but dissociation rate was drastically reduced when SH1 was labelled with 5-iodoacetamidofluorescein.     

Location of a contact site between actin and myosin in the three-dimensional structure of the acto-S1 complex

Using fluorescence resonance energy transfer (FRET), we measured distances from chromophores located at or near the actin-binding stretch of amino acids 633-642 of myosin subfragment 1 (S1), to five points in the acto-S1 complex. Specific labeling of this site was achieved by first attaching the desired chromophore to an "antipeptide" that by means of its charge complementarity specifically binds to this segment of S1 [Chaussepied & Morales (1988) Proc. Natl. Acad. Sci. U.S.A. 85, 7471] and then cross-linking the fluorescent peptide to the protein. According to this technique, antipeptides containing three different labels, viz., N-dansylaziridine, (iodoacetamido)fluorescein, and monobromobimane, were purified and covalently bound to S1. A second chromophoric group, required for FRET measurements, was selected in such a way as to provide a good spectral overlap with the corresponding peptide chromophore. Cys-707 (SH1) and Cys-697 (SH2) on S1 were modified by using iodoacetamido and maleimido derivatives of rhodamine, 1,N6-ethenoadenosine 5'-diphosphate was trapped at the S1 active site with orthovanadate, Cys-374 on actin was modified with either N-[4-[4-(dimethylamino)phenyl]azo]phenyl]maleimide or N-[(iodoacetyl)-amino]ethyl]-5-naphthylamine-1-sulfonate, and ADP bound to F-actin was exchanged with the fluorescent etheno analogue. By use of excited-state lifetime fluorometry, the following distances from the stretch 633-642 of S1 to other points on S1 or actin have been measured: Cys-707 (S1), 50.3 A; Cys-697 (S1), 49.4 A; active site of S1, greater than or equal to 44 A; nucleotide binding site (actin), 41.1 A; and Cys-374 (actin), approximately 53 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structure of the actin-myosin complex produced by crosslinking in the presence of ATP

The structure of the actin-myosin complex during ATP hydrolysis was studied by covalently crosslinking myosin subfragment 1 (S1) to F-actin in the presence of nucleotides (especially ATP) using 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide. The fluorescence energy transfer was measured between N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine and 6-(iodoacetamide)fluorescein bound to the SH1 thiol of S1 and the Cys374 thiol of actin. The covalent acto-S1, produced by crosslinking in the absence of nucleotide or in the presence of ADP, showed transfer efficiency of 0.50 to 0.52 and intersite distance of 4.5 to 4.7 nm, which were equal to those obtained with non-crosslinked acto-S1 in the absence of nucleotide. However, the covalent acto-S1, produced by crosslinking in the presence of either 5'-adenylyl imidodiphosphate (AMPPNP) at high ionic strength or ATP, showed a significant decrease in the efficiency to 0.26 to 0.34 and hence an increase in the distance to 5.2 to 5.5 nm. These results suggest that AM-ATP and/or AM-ADP-P (formed during ATP hydrolysis) and AM-AMPPNP have a very different conformation from AM and AM-ADP (in which A is actin and M is myosin).     

Two-state equilibria of myosin subfragment 1 and its complexes with ADP and actin

We previously reported that the nucleotide complex of myosin subfragment 1, S1.epsilon ADP, exists in two states on the basis of the temperature dependence of the fluorescence decay of bound 1,N6-ethenoadenosine diphosphate (epsilon ADP) [Aguirre, R., Lin. S.-H., Gonsoulin, F., Wang, C.-K., & Cheung, H.C. (1989) Biochemistry 28, 799-809]. We have extended the previous study of the equilibrium between the two states, S1L.ADP in equilibrium S1H.ADP, by using a fluorescently labeled myosin S1 (S1-AF). In S1 alkylated with IAF [5-(iodoacetamido)fluorescein], the decay of the label emission was biexponential both in the presence and absence of ADP and/or actin. In the presence of ADP, the two decay times were 4.30 (alpha 1 = 0.55) and 0.80 ns (alpha 2 = 0.45) at 12.4 degrees C, in a medium containing 60 mM KCl, 30 mM TES (pH 7.5), and 2 mM MgCl2. The steady-state fluorescence intensities of S1-AF, (S1-AF).ADP, acto.(S1-AF), and acto.(S1-AF).ADP were dependent on temperature over the range of 5-30 degrees C. By combining lifetime and steady-state intensity data, we obtained for the two-state transition (S1-AF)L.ADP in equilibrium (S1-AF)H.ADP the following parameters: delta H degrees = 16.1 kcal/mol (67.3 kJ/mol) and delta S degrees = 55.8 cal/(deg.mol) [233.5 J/(deg.mol)], in agreement with previous results obtained with epsilon ADP. The delta H degrees values for the two-state transition of S1-AF, acto.(S1-AF), and acto.(S1-AF).ADP are 13.0, 21.6, and 5.2 kcal/mol, respectively. The corresponding delta S degrees values are 46.9, 79.5, and 17.4 cal/(deg.mol).(ABSTRACT TRUNCATED AT 250 WORDS)     

The kinetics of a two-state transition of myosin subfragment 1. A temperature-jump relaxation study.

Temperature-jump measurements were carried out on myosin subfragment 1 (S1) labeled at Cys-707 with 5-(iodoacetamido)fluorescein (S1-AF). The relaxation was monitored by following the increase in the fluorescence intensity of the attached probe after a jump of 5.8 degrees C. A single relaxation process was observed over a range of final temperatures, and the relaxation time decreased from 16.69 ms at 15 degrees C to 3.91 ms at 27 degrees C. The relaxation results are interpreted in terms of a two-state transition: (S1-AF)L K+ in equilibrium with K- (S1-AF)H, and the observed single relaxation time (tau) equals l/(k(+) + k-). The individual first-order rate constants, k+ and k-, were calculated from tau and the equilibrium constant previously determined. The activation energy was 21.9 kcal/mol for the forward reaction and 9.3 kcal/mol for the reverse reaction, corresponding to an enthalpy value of 12.6 kcal/mol for the two-state transition. The results provide, for the first time, direct kinetic evidence of a two-state transition of S1 in the absence of bound nucleotide, and support a two-state model of unliganded myosin subfragment 1.     

Fluorescence resonance energy transfer within the complex formed by actin and myosin subfragment 1. Comparison between weakly and strongly attached states

Fluorescence resonance energy transfer measurements have been made between Cys-374 on actin and Cys-177 on the alkali light chain of myosin subfragment 1 (S1) using several pairs of donor-acceptor chromophores. The labeled light chain was exchanged into subfragment 1 and the resulting fluorescently labeled subfragment 1 isolated by ion-exchange chromatography on SP-Trisacryl. The efficiency of energy transfer was measured by steady-state fluorescence in a strong binding complex of acto-S1 and found to represent a spatial separation between the two probes of 5.6-6.3 nm. The same measurements were then made with weak binding acto-S1 complexes generated in two ways. First, actin was complexed with p-phenylenedimaleimide-S1, a stable analogue of S1-adenosine 5'-triphosphate (ATP), obtained by cross-linking the SH1 and SH2 heavy-chain thiols of subfragment 1 [Greene, L. E., Chalovich, J. M., & Eisenberg, E. (1986) Biochemistry 25, 704-709]. Large increases in transfer efficiency indicated that the two probes had moved closer together by some 3 nm. Second, weak binding complexes were formed between subfragment 1 and actin in the presence of the regulatory proteins troponin and tropomyosin, the absence of calcium, and the presence of ATP [Chalovich, J. M., & Eisenberg, E. (1982) J. Biol. Chem. 257, 2432-2437]. The measured efficiency of energy transfer again indicated that the distance between the two labeled sites had moved closer by about 3 nm. These data support the idea that there is a considerable difference in the structure of the acto-S1 complex between the weakly and strongly bound states.     

Specificity and orientation of (iodoacetamido)proxyl spin-labeled myosin subfragment 1 decorating muscle fibers: localization of protein-bound spin labels using SDS-PAGE

The nitroxide spin label (iodoacetamido)proxyl (IPSL) was specifically and rigidly attached to sulfhydryl 1 (SH1) on myosin subfragment 1 (S1). The specificity of this label for SH1 was demonstrated by using a technique where the spin label is localized on the electrophoresis-isolated proteolytic fragments of myosin using electron paramagnetic resonance (EPR). Studies of the rigidity of the probe on SH1 indicate that the IPSL is immobilized on the surface of S1 in the presence and absence of the nucleotides MgADP or MgATP. The EPR spectrum of muscle fibers decorated with IPSL-S1 shows that the IPSL-S1 rotates from its orientation in rigor upon binding MgADP. The angular displacement due to nucleotide binding is larger than that detected with the (maleimido)tempo spin label [Ajtai, K., French, A. R., & Burghardt, T. P. (1989) Biophys. J. 56, 535-541], demonstrating that the IPSL is oriented on the myosin cross-bridge in a manner that is favorable for detecting cross-bridge rotation during the rigor to MgADP state transition.     

Transient kinetics of the interaction of actin with myosin subfragment-1 in the absence of nucleotide.

The kinetics of the association of actin with myosin subfragment-1 (S1) has been studied by using S1 labeled at the sulfhydryl group SH1 with 5-(iodoacetamido)fluorescein (S1-AF). Upon rapid mixing in a stopped-flow apparatus, the fluorescence intensity of the fluorescein moiety increased by 50%, followed by a slower increase that was well resolved. This slow phase of the fluorescence change could not be fitted to either a monoexponential or a biexponential function, but it could be fitted to a sum of three exponential terms yielding three observed first-order rate constants (lambda i). The dissociation of acto.-(S1-AF) was studied by displacement of S1-AF from the complex with native S1. The dissociation kinetics was characterized by a single rate constant (approximately 0.012 s-1 at 20 degrees C), and this constant was independent of S1 concentration. Together with previous equilibrium data that were obtained under identified conditions for formation of acto-subfragment-1 (Lin, S.-H., and H. C. Cheung. 1991. Biochemistry. 30:4317-4323), a six-state two-pathway model is proposed as a minimum kinetic scheme for formation of rigor acto.S1. In this model, unbound subfragment-1 exists in two conformational states (S1' and S1) which are in equilibrium with each other, one corresponding to the previously established low-temperature state and the other to the high-temperature state. Each subfragment-1 state can interact with actin to form a collision complex, followed by two isomerizations to form two acto-subfragment-1 states (A.S1' and A.S1). Both isomerizations were visible in stopped-flow experiments. Two special cases of the model were considered: 1) a rapid pre-equilibration of the initial collision complex with actin and S1, and 2) trace accumulation of the collision complex. The first case required that the three combinations of the three observed rate constants be independent of actin concentration. The data were incompatible with this approximation. The other special case required that the sum of the lambda i vary linearly with actin concentration and the other two combinations of lambda i vary with actin concentration in a quadratic fashion. The present data were in agreement with the second case. At 20 degrees C and in 60 mM KCl, 2 mM MgCl2, 30 mM 2-([-hydroxy-1,1-bis(hydroxymethyl)ethyl]amino)ethanesulfonic acid, and pH 7.5, the biomolecular association rate constants for the interaction of actin with S1' and S1 were 8.58 x 10(5) and 1.11 x 10(6) M-1 s-1, respectively.     

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.     

Fluorescent modification and orientation of myosin sulfhydryl 2 in skeletal muscle fibers

We describe a protocol for the selective covalent labeling of the sulfhydryl 2 (SH2) on the myosin cross-bridge in glycerinated muscle fibers using the sulfhydryl-selective label 4-[N-[(iodoacetoxy)ethyl]-N-methylamino]-7-nitrobenz-2-oxa-1,3-diazole (IANBD). The protocol promotes the specificity of IANBD by using the ability to protect sulfhydryl 1 (SH1) from modification by binding the cross-bridge to the actin filament and using cross-bridge-bound MgADP to promote the accessibility of SH2. We determined the specificity of the probe using fluorescence gel scanning of fiber-extracted proteins to isolate the probe on myosin subfragment 1 (S1), limited proteolysis of the purified S1 to isolate the probe on the 20-kilodalton fragment of S1, and titration of the free SH1's on purified S1 using the radiolabeled SH1-specific reagent [14C]iodoacetamide or enzymatic activity measurements. We estimated the distribution of the IANBD on the fiber proteins to be approximately 77% on SH2, approximately 5% on SH1, and approximately 18% on troponin I. We characterized the angular distribution of the IANBD on cross-bridges in fibers when the fibers are in rigor, in relaxation, in the presence of MgADP, and in isometric contraction using wavelength-dependent fluorescence polarization [Ajtai, K., & Burghardt, T. P. (1987) Biochemistry 26, 4517-4523]. With wavelength-dependent fluorescence polarization we use the ability to rotate the transition dipole in the molecular frame using excitation wavelength variation to investigate the three angular degrees of freedom of the cross-bridge.(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformation and dynamics of the SH1-SH2 helix in scallop myosin

Atomic structures of scallop myosin subfragment 1(S1) with the bound MgADP, MgAMPPNP, and MgADP.BeF(x) provide crystallographic evidence for a destabilization of the helix containing reactive thiols SH1 (Cys703) and SH2 (Cys693). A destabilization of this helix was not observed in previous structures of S1 (from chicken skeletal, Dictyostelium discoideum, and smooth muscle myosins), including complexes for which solution experiments indicated such a destabilization. In this study, the factors that influence the SH1-SH2 helix in scallop S1 were examined using monofunctional and bifunctional thiol reagents. The rate of monofunctional labeling of scallop S1 was increased in the presence of MgADP and MgATPgammaS but was inhibited by MgADP.V(i) and actin. The resulting changes in ATPase activities of S1 were symptomatic of SH2 and not SH1 modification, which was confirmed by mass spectrometry analysis. With bifunctional reagents of various lengths, cross-linking did not occur on a short time scale in the absence of nucleotides. In the presence of MgADP, cross-linking was greatly enhanced for all of the reagents. These reactions, as well as the formation of a disulfide bond between SH1 and SH2, were much faster in scallop S1.ADP than in rabbit skeletal S1.ADP and were rate-limited by the initial attachment of the reagent to scallop S1. The cross-linking sites were mapped by mass spectrometry to SH1 and SH2. These results reveal isoform-specific differences in the conformation and dynamics of the SH1-SH2 helix, providing a possible explanation for destabilization of this helix in some scallop S1 but not in other S1 isoform structures.     

ATP-induced dissociation of rabbit skeletal actomyosin subfragment 1. Characterization of an isomerization of the ternary acto-S1-ATP complex

The adenosine 5'-O-(3-thiotriphosphate) (ATP gamma S) induced dissociation of actomyosin subfragment 1 (S1) has been investigated by monitoring the light scattering changes that occur on dissociation. We have shown that ATP gamma S dissociates acto-S1 by a mechanism similar to that of ATP but at a rate 10 times slower. The maximum rate of dissociation is limited by an isomerization of the ternary actin-S1-nucleotide complex, which has a rate of 500 s-1 for ATP gamma S and an estimated rate of 5000 s-1 for ATP (20 degrees C, 0.1 M KCl, pH 7.0). The activation energy for the isomerization is the same for ATP and ATP gamma S, and both show a break in the Arrhenius plot at 5 degrees C. The reaction between acto-S1 and ATP was also followed by the fluorescence of a pyrene group covalently attached to Cys-374. We show that the fluorescence of the pyrene group reports the isomerization step and not actin dissociation. The characterization of this isomerization is discussed in relation to force-generating models of the actomyosin cross-bridge cycle.     

Fluorescence energy transfer between subfragment-1 and actin points in the rigor complex of actosubfragment-1.

The fast-reacting thiol (SH1) of myosin subfragment-1 (S-1) was covalently and specifically labeled with (iodoacetamido)fluorescein (IAF), while Cys-373 of actin was also covalently and preferentially labeled with N-(iodoacetyl)-N'-(1-sulfo-5-naphthyl)ethylenediamine (1,5-IAEDANS). The method of fluorescence energy transfer was used to examine the spatial proximity between the two sites, i.e., SH1 and Cys-373, in the rigor complex of acto-S-1. Approximately 30% fluorescence energy transfer was observed from the 1,5-IAEDANS on actin as a donor to the IAF on S-1 as an acceptor in their rigor complex; under certain assumptions this corresponds to a distance of ca. 6.0 nm.     

40-kDa protein from thin filaments of the mussel Crenomytilus grayanus changes the conformation of F-actin during the ATPase cycle

Polarized fluorimetry was used to study in ghost muscle fibers the influence of a 40-kDa protein from the thin filaments of the mussel Crenomytilus grayanus on conformational changes of F-actin modified by the fluorescent probes 1,5-IAEDANS and FITC-phalloidin during myosin subfragment (S1) binding in the absence of nucleotides and in the presence of MgADP or MgATP. The fluorescence probes were rigidly bound with actin, which made the absorption and emission dipoles of the probes sensitive to changes in the orientation and mobility of both actin monomer and its subdomain-1 in thin filaments of the muscle fiber. On modeling different intermediate states of actomyosin, the orientation and mobility of oscillators of the dyes were changed discretely, which suggests multistep changes in the actin conformation during the cycle of ATP hydrolysis. The 40-kDa protein influenced the orientation and mobility of the fluorescent probes markedly, suppressing changes in their orientation and mobility in the absence of nucleotides and in the presence of MgADP, but enhancing these changes in the presence of MgATP. The calponin-like 40-kDa protein is supposed to prevent formation of the strong binding state of actomyosin in the absence of nucleotides and in the presence of MgADP but to activate formation of this state in the presence of MgATP.     

Time-dependent fluorescence depolarization and lifetime studies of myosin subfragment-one in the presence of nucleotide and actin

Time-dependent fluorescence depolarization and lifetime studies have been made on myosin subfragment 1 to obtain information about mobility changes and dye environment changes when different nucleotides are added. Data are reported for static and actively hydrolyzing systems containing G- and F-actin. Preliminary data indicate that myosin labeled with the fluorophore 1,5 IAEDANS¹-and treated with DTT preserves its actin-activated V_max. S1 prepared in this manner gives lifetime changes which are nearly identical for all systems studied. S1 labeling without DTT addition gives a pattern of lifetimes similar, though not identical to ESR work. Either type of labeling produces no observable change in the polarization decay, and we set an upper limit of 15% length change for the elongate S1. An unusually long fluorescence decay lifetime for the S1-Mg⁺⁺ ATP-G-actin system is found which may indicate a new acto-S1 state stabilized by G-actin. The method for obtaining the bound fraction of S1's in the presence of actin is presented and applied to the S1-F-actin-Mg⁺⁺ ATP system. Qualitative agreement is obtained with other methods.     

Electrostatic changes at the actomyosin-subfragment 1 interface during force-generating reactions.

The ionic strength dependence of the binding of rabbit skeletal muscle myosin subfragment 1, S1, to F-actin in the presence of saturating concentrations of MgATP or MgADP was analyzed in order to determine the association constants at zero ionic strength [K(0)] and the products of the net effective electric charges (magnitude of zMzA) at the binding interfaces. K(0) and magnitude of zM A were 1 x 10(6) M-1 and 17 esu2 for S1-MgADP,P, and 5 x 10(7) M-1 and 7 esu2 for S1-MgADP, respectively, for binding to F-actin at 25 degrees C. At ionic strengths near physiological, the increase in affinity is close to 10(4)-fold for this transition that may correspond to force generation in muscle fibers. The large, from 17 to 7 esu2, decrease in the electrostatic contribution to binding appears to be correlated with a much larger increase in nonelectrostatic interactions, unlike the simpler transition of actin-bound S1-MgADP to S1, which appears to be due entirely to electrostatic changes [Highsmith, S. (1990) Biochemistry 29, 10690-10694]. These results for acto-S1-MgADP,P to acto-S1-MgADP suggest that a substantial transformation of the actin binding site on S1 occurs even if there is a translocation to a new interface.     

Stereospecific reaction of muscle fiber proteins with the 5' or 6' isomer of (iodoacetamido)tetramethylrhodamine.

The labeling of muscle fiber proteins with iodoacetamido)tetramethylrhodamine (IATR) was reinvestigated with the purified 5' or 6' isomers of IATR. Both isomers modify the myosin heavy chain within the 20-kDa fragment of myosin subfragment 1 (S1) but with different rates, and only the 5'-IATR alters K(+)-EDTA- and Ca(2+)-activated ATPases. Absorption spectroscopic and ATPase studies of probe stoichiometry indicate that for 5'-IATR there are two probes per myosin sulfhydryl 1 (SH1). Quantitative fluorograms of the SDS-PAGE gels confirm that there are one covalent and one noncovalent probe per SH1 when S1 is labeled with 5'-IATR (5'-IATR-S1) and that there are one covalent and two noncovalent probes per S1 when S1 is labeled with 6'-IATR (6'-IATR-S1). The 5'- and 6'-IATR probes have similar fluorescent lifetimes when bound to S1, but quenching studies with potassium iodide show that 5'-IATR-S1 has a single class of strongly bound chromophores while 6'-IATR-S1 has two or more classes of chromophores. It is possible that 5'-IATR labels SH1 as a dimer. The polarization anisotropies of 5'- and 6'-IATR-S1 indicate that 5'-IATR is immobilized, while 6'-IATR is moving independently, on the surface of S1. The emission spectrum from 5'-IATR-S1 is unaffected by the addition of MgATP, while 6'-IATR-S1 shows a spectral shift and total intensity change. When labeling muscle fibers, 5'-IATR labels myosin SH1 and differentiates between the fiber physiological states by indicating cross-bridge rotation in quantitative agreement with previous results [Burghardt et al. (1983) Proc. Natl. Acad. Sci. U.S.A. 80, 7515]. 6'-IATR reacts preferentially with actin in muscle fibers and does not differentiate between fiber physiological states as expected for an actin probe. The stereospecificity of the rhodamine isomers for SH1 indicates features of the local protein structure. The experimental results are used with theoretical methods for determining molecular structure to suggest a qualitative scheme for the specific interaction of 5'-IATR with its binding pocket on the surface of S1.     

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.     

Osmotic pressure probe of actin-myosin hydration changes during ATP hydrolysis.

Osmotic stress in the 0.5-5 x 10(6) dyne/cm2 range was used to perturb the hydration of actin-myosin-ATP intermediates during steady-state hydrolysis. Polyethylene glycol (PEG) (1000 to 4000 Da), in the 1 to 10 wt% range, which does not cause protein precipitation, did not significantly affect the apparent KM or the Vmax for MgATP hydrolysis by myosin subfragment 1 (S1) alone, nor did it affect the value for the phosphate burst. Consistent with the kinetic data, osmotic stress did not affect nucleotide-induced changes in the fluorescence intensities of S1 tryptophans or of fluorescein attached to Cys-707. The accessibility of the fluorescent ATP analog, epsilon ADP, to acrylamide quenching was also unchanged. These data suggest that none of the steps in the ATP hydrolysis cycle involve substantial hydration changes, which might occur for the opening or closing of the ATP site or of other crevices in the S1 structure. In contrast, KM for the interaction of S1.MgADP.Pi with actin decreased tenfold in this range of osmotic pressure, suggesting that formation of actin.S1.MgADP.Pi involves net dehydration of the proteins. The dehydration volume increases as the size of the PEG is increased, as expected for a surface-excluded osmolyte. The measured dehydration volume for the formation of actin.S1.MgADP.Pi was used to estimate the surface area of the binding interface. This estimate was consistent with the area determined from the atomic structures of actin and myosin, indicating that osmotic stress is a reliable probe of actin.myosin.ATP interactions. The approach developed here should be useful for determining osmotic stress and excluded volume effects in situ, which are much larger than those of typical in vitro conditions.     

Differential behavior of two cysteine residues on the myosin head in muscle fibers

We have previously shown that the orientation of (iodoacetamido)tetramethylrhodamine labels on SH1 thiol of S-1 moieties changes when MgADP is added to the fibers in rigor [Borejdo, J., Assulin, O., Ando, T., & Putnam, S. (1982) J. Mol. Biol. 158, 391-414. Burghardt, T.P., Ando, T., & Borejdo, J. (1983) Proc. Natl. Acad. Sci. U.S.A. 80, 7515-7519]. Here we report the results of experiments in which the SH2 of S-1 was labeled with maleimidorhodamine. The specificity of modification of thiols was checked by measuring the stoichiometry of attached dye, by determining the extent of the decrease in EDTA (K+)- and Ca2+-ATPase activities, and by the localization of the dyes on peptides containing SH1 and/or SH2. Labeled S-1 was diffused into single glycerinated fibers of rabbit psoas muscle, and the orientation of chromophores was measured by fluorescence detected dichroism. The dye attached to SH1 was oriented at 65 degrees with respect to the fiber axis in rigor and at 51 degrees in the presence of MgADP, regardless of whether SH2 was modified or not. The dye on SH2 was oriented near 42 degrees both in the presence and in the absence of ADP, regardless of whether SH1 was modified or not. Our results show that rhodamine oriented differently when attached to SH2 compared with when attached to SH1 and that in the former placement it was not sensitive to MgADP. We think this indicates that the SH2-containing region has a mobility different from that of the SH1-containing region, i.e., that this is evidence for internal flexibility of S-1.