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)     

Energetics of the actomyosin bond in the filament array of muscle fibers.

The interaction between actin and myosin in the filament array of glycerinated muscle fibers has been monitored using paramagnetic probes and mechanical measurements. Both fiber stiffness and the spectra of probes bound to a reactive sulfydral on the myosin head were measured as the actomyosin bond was weakened by addition of magnesium pyrophosphate (MgPPi) and glycerol. In the absence of MgPPi, all myosin heads are attached to actin with oriented probes. When fibers were incubated in buffers containing MgPPi, a fraction of the probes became disordered, and this effect was greater in the presence of glycerol. To determine whether the heads with disordered probes were detached from actin, spin-labeled myosin subfragment-1 (MSL-S1) was diffused into unlabeled fibers, and the fractions bound to actin and free in the medium were correlated with the oriented and disordered spectral components. These experiments showed that the label was oriented when MSL-S1 was attached to actin in a ternary complex with the ligand and that all heads with disordered probes were detached from actin. Thus the fraction of oriented labels could be used to determine the fraction of heads attached to actin in a fiber in the presence of ligand. The fraction of myosin heads attached to actin decreased with increasing [MgPPi], and in the absence of glycerol approximately 50% of the myosin heads were dissociated at 3.3 mM ligand with little change in fiber stiffness. In the presence of 37% glycerol plus ligand, up to 80% of the heads could be detached with a 50% decrease in fiber stiffness. The data indicate that there are two populations of myosin heads in the fiber. All the data could be fit with a model in which one population of myosin heads (comprising approximately 50% of the total) sees an apparent actin concentration of 0.1 mM and can be released from actin with little change in fiber stiffness. A second population of myosin heads (approximately 50%) sees a higher actin concentration (5 mM) and is only released in the presence of both glycerol and ligand.     

A spin label that binds to myosin heads in muscle fibers with its principal axis parallel to the fiber axis.

We have used an indane-dione spin label (2-[-oxyl-2,2,5,5-tetramethyl-3-pyrrolin-3-yl)methenyl]in dane-1,3-dione), designated InVSL, to study the orientation of myosin heads in bundles of chemically skinned rabbit psoas muscle fibers, with electron paramagnetic resonance (EPR) spectroscopy. After reversible preblocking with 5,5'-dithiobis(2-nitro-benzoic acid) (DTNB), we were able to attach most of the spin label covalently and rigidly to either Cys 707 (SH1) or Cys 697 (SH2) on myosin heads. EPR spectra of labeled fibers contained substantial contributions from both oriented and disordered populations of spin labels. Similar spectra were obtained from fibers decorated with InVSL-labeled myosin heads (subfragment 1), indicating that virtually all the spin labels in labeled fibers are on the myosin head. We specifically labeled SH2 with InVSL after reversible preblocking of the SH1 sites with 1-fluoro-2,4-dinitrobenzene (FDNB), resulting in a spectrum that indicated only disordered spin labels. Therefore, the oriented and disordered populations correspond to labels on SH1 and SH2, respectively. The spectrum of SH2-bound labels was subtracted to produce a spectrum corresponding to SH1-bound labels, which was used for further analysis. For this corrected spectrum, the angle between the fiber axis and the principal axis of the spin label was fitted well by a Gaussian distribution centered at theta o = 11 +/- 1 degree, with a full width at half-maximum of delta theta = 15 +/- 2 degrees. The unique orientation of InVSL, with its principal axis almost parallel to the fiber axis, makes it complementary to spin labels previously studied in this system. This label can provide unambiguous information about axial rotations of myosin heads, since any axial rotation of the head must be reflected in the same axial rotation of the principal axis of the probe, thus changing the hyperfine splitting. Therefore, InVSL-labeled fibers have ideal properties needed for further exploration myosin head orientation and rotational motion in muscle.     

Fluorescence polarization transients from rhodamine isomers on the myosin regulatory light chain in skeletal muscle fibers.

Fluorescence polarization was used to examine orientation changes of two rhodamine probes bound to myosin heads in skeletal muscle fibers. Chicken gizzard myosin regulatory light chain (RLC) was labeled at Cys108 with either the 5- or the 6-isomer of iodoacetamidotetramethylrhodamine (IATR). Labeled RLC (termed Cys108-5 or Cys108-6) was exchanged for the endogenous RLC in single, skinned fibers from rabbit psoas muscle. Three independent fluorescence polarization ratios were used to determine the static angular distribution of the probe dipoles with respect to the fiber axis and the extent of probe motions on the nanosecond time scale of the fluorescence lifetime. We used step changes in fiber length to partially synchronize the transitions between biochemical, structural, and mechanical states of the myosin cross-bridges. Releases during active contraction tilted the Cys108-6 dipoles away from the fiber axis. This response saturated for releases beyond 3 nm/half-sarcomere (h.s.). Stretches in active contraction caused the dipoles to tilt toward the fiber axis, with no evidence of saturation for stretches up to 7 nm/h.s. These nonlinearities of the response to length changes are consistent with a partition of approximately 90% of the probes that did not tilt when length changes were applied and 10% of the probes that tilted. The responding fraction tilted approximately 30 degrees for a 7.5 nm/h.s. release and traversed the plane perpendicular to the fiber axis for larger releases. Stretches in rigor tilted Cys108-6 dipoles away from the fiber axis, which was the opposite of the response in active contraction. The transition from the rigor-type to the active-type response to stretch preceded the main force development when fibers were activated from rigor by photolysis of caged ATP in the presence of Ca2+. Polarization ratios for Cys108-6 in low ionic strength (20 mM) relaxing solution were compatible with a combination of the relaxed (200 mM ionic strength) and rigor intensities, but the response to length changes was of the active type. The nanosecond motions of the Cys108-6 dipole were restricted to a cone of approximately 20 degrees half-angle, and those of Cys108-5 dipole to a cone of approximately 25 degrees half-angle. These values changed little between relaxation, active contraction, and rigor. Cys108-5 showed very small-amplitude tilting toward the fiber axis for both stretches and releases in active contraction, but much larger amplitude tilting in rigor. The marked differences in these responses to length steps between the two probe isomers and between active contraction and rigor suggest that the RLC undergoes a large angle change (approximately 60 degrees) between these two states. This motion is likely to be a combination of tilting of the RLC relative to the fiber axis and twisting of the RLC about its own axis.     

Orientation of intermediate nucleotide states of indane dione spin-labeled myosin heads in muscle fibers.

We have used electron paramagnetic resonance to study the orientation of myosin heads in the presence of nucleotides and nucleotide analogs, to induce equilibrium states that mimic intermediates in the actomyosin ATPase cycle. We obtained electron paramagnetic resonance spectra of an indane dione spin label (InVSL) bound to Cys 707 (SH1) of the myosin head, in skinned rabbit psoas muscle fibers. This probe is rigidly immobilized on the catalytic domain of the head, and the principal axis of the probe is aligned nearly parallel to the fiber axis in rigor (no nucleotide), making it directly sensitive to axial rotation of the head. On ADP addition, all of the heads remained strongly bound to actin, but the spectral hyperfine splitting increased by 0.55 +/- 0.02 G, corresponding to a small but significant axial rotation of 7 degrees. Adenosine 5'-(adenylylim-idodiphosphate) (AMPPNP) or pyrophosphate reduced the actomyosin affinity and introduced a highly disordered population of heads similar to that observed in relaxation. For the remaining oriented population, pyrophosphate induced no significant change relative to rigor, but AMPPNP induced a slight but probably significant rotation (2.2 degrees +/- 1.6 degrees), in the direction opposite that induced by ADP. Adenosine 5'-O-(3-thiotriphosphate) (ATP gamma S) relaxed the muscle fiber, completely dissociated the heads from actin, and produced disorder similar to that in relaxation by ATP. ATP gamma S plus Ca induced a weak-binding state with most of the actin-bound heads disordered. Vanadate had negligible effect in the presence of ADP, but in isometric contraction vanadate substantially reduced both force and the fraction of oriented heads. These results are consistent with a model in which myosin heads are disordered early in the power stroke (weak-binding states) and rigidly oriented later in the power stroke (strong-binding states), whereas transitions among the strong-binding states induce only slight changes in the axial orientation of the catalytic domain.     

Fluorescence polarization of skeletal muscle fibers labeled with rhodamine isomers on the myosin heavy chain.

Fluorescence polarization was used to examine orientational changes of Rhodamine probes in single, skinned muscle fibers from rabbit psoas muscle following either photolysis of caged nucleotides or rapid length changes. Fibers were extensively and predominantly labeled at SH1 (Cys-707) of the myosin heavy chain with either the 5- or the 6-isomer of iodoacetamidotetramethylrhodamine. Results from spectroscopic experiments utilizing the two Rhodamine isomers were quite similar. Following photolysis of either caged ATP or caged ADP, probes promptly reoriented toward the muscle fiber axis. Changes in the fluorescence polarization signals with transients elicited by the photolysis of caged ATP in the presence of saturating Ca2+ greatly preceded active force generation. Photolysis of caged ADP caused only a small, rapid decrease in force but elicited changes in the fluorescence polarization signals with time course and amplitude similar to those following photolysis of caged ATP. Fluorescence polarization signals were virtually unchanged by rapid length steps in both rigor and active muscle fibers. These results indicate that structural changes monitored by Rhodamine probes at SH1 are not associated directly with the force-generating event of muscle contraction. However, the fluorescence polarization transients were slightly faster than the estimated rate of cross-bridge detachment following photolysis of caged ATP, suggesting that the observed structural changes at SH1 may be involved in the communication pathway between the nucleotide- and actin-binding sites of myosin.     

Steady-state fluorescence polarization studies of the orientation of myosin regulatory light chains in single skeletal muscle fibers using pure isomers of iodoacetamidotetramethylrhodamine.

The regulatory light chain (RLC) from chicken gizzard myosin was covalently modified on cysteine 108 with either the 5- or 6-isomer of iodoacetamidotetramethylrhodamine (IATR). Labeled RLCs were purified by fast protein liquid chromatography and characterized by reverse-phase high-performance liquid chromatography (HPLC), tryptic digestion, and electrospray mass spectrometry. Labeled RLCs were exchanged into the native myosin heads of single skinned fibers from rabbit psoas muscle, and the ATR dipole orientations were determined by fluorescence polarization. The 5- and 6-ATR dipoles had distinct orientations, and model orientational distributions suggest that they are more than 20 degrees apart in rigor. In the rigor-to-relaxed transition (sarcomere length 2.4 microm, 10 degrees C), the 5-ATR dipole became more perpendicular to the fiber axis, but the 6-ATR dipole became more parallel. This orientation change was absent at sarcomere length 4.0 microm, where overlap between myosin and actin filaments is abolished. When the temperature of relaxed fibers was raised to 30 degrees C, the 6-ATR dipoles became more parallel to the fiber axis and less ordered; when ionic strength was lowered from 160 mM to 20 mM (5 degrees C), the 6-ATR dipoles became more perpendicular to the fiber axis and more ordered. In active contraction (10 degrees C), the orientational distribution of the probe dipoles was similar but not identical to that in relaxation, and was not a linear combination of the orientational distributions in relaxation and rigor.     

Orientation of cross-bridges in skeletal muscle measured with a hydrophobic probe.

Cis-parinaric acid (PA) binds to a hydrophobic pocket formed between the heavy chain of myosin subfragment-1 (S1) and the 41-residue N-terminal of essential light chain 1 (A1). The binding is strong (Ka = 5.6 x 10(7) M-1) and rigid (polarization = 0.334). PA does not bind to myofibrils in which A1 has been extracted or replaced with alkali light chain 2 (A2). As in the case of S1 labeled with other probes, polarization of fluorescence of S1-PA added to myofibrils depended on fractional saturation of actin filament with S1, i.e., on whether the filaments were fully or partially saturated with myosin heads. Because fluorescence quantum yield of PA is enhanced manyfold upon binding, and because PA binds weakly to myofibrillar structures other then A1, the dye is a convenient probe of cross-bridge orientation in native muscle fibers. The polarization of a fiber irrigated with PA was equal to the polarization of S1-PA added to fibers at nonsaturating concentration. Cross-linking of S1 added to fibers at nonsaturating concentration showed that each S1 bound to two actin monomers of a thin filament. These results suggest that in rigor rabbit psoas muscle fiber each myosin cross-bridge binds to two actins.     

Cleavage of DNA-binding loops of actin by subtilisin prevent formation of a strong type of myosin binding with actin

In order to elucidate the role of DNA-binding loop of actin (amino acid residues 38-52) in mechanisms of muscle contraction, polarizational fluorimetry and ghost muscle fibers, containing thin filaments reconstructed by intact and subtilisin-cleaved G-actin were used. The thin filaments were modified by fluorescent probes rhodamin-phalloidin and 1,5-IAEDANS. Changes in orientation and mobility of the probes were considered as an indication of changes in actin conformation. The stage AM of ATP hydrolysis cycle was simulated. For this purpose, thin filaments were decorated by myosin subfragment-1 (S1) in the absence of nucleotide. It has been shown that S1 binding to actin is accompanied by changes in orientation and mobility of the fluorescent probes. For intact filaments, the changes of these parameters indicate the formation of a strong binding between S1 and actin. Cleavage of DNA-binding loop by subtilisin markedly inhibits this effect. The cleavage of actin by subtilisin has also been shown to diminish the changes in fiber birefringence, which takes place at the formation of F-actin-S1 complex in the muscle fiber. The spatial organization of the actin DNA-binding loop is suggested to play an important role in determining the character of myosin interaction with actin in the ATP hydrolysis cycle.     

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)     

Interaction of fluorescently labeled myosin subfragment 1 with nucleotides and actin

Isolated myosin heads (subfragment 1) were modified by covalent attachment of 5-(iodoacetamido)fluorescein or 5-(iodoacetamido)salicylic acid to the essential sulfhydryl group SH1. The extrinsic fluorescence of the modified proteins was sensitive to binding of nucleotides and F-actin. With the fluorescein derivative [subfragment 1 (S1) modified with 5-(iodoacetamido)fluorescein (IAF) at SH1 (S1-AF)], association with MgADP decreased the probe fluorescence by 30%, whereas binding to actin increased the emission by a factor of 2. In the ternary complex acto-S1-AF X MgADP, the effect of nucleotide on the intensity of the attached fluorescein canceled the effect of actin. The fluorescence state of this ternary complex was similar to that of S1-AF X MgADP. The emission of S1-AF was resolved into two components with lifetimes of 4.3 and 0.6 ns and relative contributions of 33% and 67%, respectively. Interaction of S1-AF with nucleotides and actin did not alter the lifetimes but significantly shifted their fractional contributions. Quenching studies showed that the short lifetime likely arose from the fluorescein moiety statically quenched by internal groups. Binding of MgADP to the salicylate derivative [S1 modified with 5-(iodoacetamido)salicylic acid at SH1 (S1-SAL)] induced a 25% enhancement of the probe fluorescence, whereas formation of acto-S1-SAL decreased the emission by 10% regardless of whether MgADP was bound to the protein. Both labeled S1 species bound MgADP with a similar affinity, comparable to that of unmodified S1 previously reported by other investigators.(ABSTRACT TRUNCATED AT 250 WORDS)     

Orientation of spin-labeled myosin heads in glycerinated muscle fibers.

We have used electron paramagnetic resonance (EPR) spectra to study spin labels selectively and rigidly attached to myosin heads in glycerinated rabbit psoas muscle fibers. Because the angle between the magnetic field and the principal axis of the probe determines the position of the EPR absorption line, spectra from labeled fibers oriented parallel to the magnetic field yielded directly the distribution of spin label orientations relative to the fiber axis. Two spin labels, having reactivities resembling iodoacetamide (IASL) and maleimide (MSL), were used. In rigor fibers with complete filament overlap, both labels displayed a narrow angular distribution, full width at half maximum approximately 15 degrees, centered at angles of 68 degrees (IASL) and 82 degrees (MSL). Myosin subfragments (heavy meromyosin and subfragment-1) were labeled and allowed to diffuse into fibers. The resulting spectra showed the same sharp angular distribution that was found for the labeled fibers. Thus is appears that virtually all myosin heads in a rigor fiber have the same orientation relative to the fiber axis, and this orientation is determined by the actomyosin bond. Experiments with stretched fibers indicated that the spin labels on the fraction of heads not interacting with actin filaments had a broad angular distribution. Addition of ATP to unstretched fibers under relaxing conditions produced orientational disorder, resulting in a spectrum almost indistinguishable from that of an isotropic distribution of probes. Addition of either an ATP analog (AMPPNP) or pyrophosphate produced partial disorder. That is a fraction of the probes remained sharply oriented as in rigor while a second fraction was in a disordered distribution similar to that of relaxed fibers.     

Interhead distances in myosin attached to F-actin estimated by fluorescence energy transfer spectroscopy.

Fluorescence resonance energy transfer (FRET) spectroscopy has been used to determine distances between probes attached to the most reactive sulfhydryl (SH1) group on individual myosin "heads." We measured intramolecular and intermolecular interhead distances as well as the distance between one head of heavy meromyosin (HMM) mixed with subfragment-1 (S1) heads attached to F-actin under rigor conditions. The SH1 cysteine was specifically labeled with either a donor (5-((((2-iodoacetyl)amino)ethyl)amino)naphthalene-1-sulfonic acid) or an acceptor probe (5-iodoacetamidofluorescein). In free solution, the distance between these probes was too large to allow significant FRET, but in the rigor complex with F-actin, intermolecular interhead distances between S1 molecules, HMM molecules, or S1 and HMM were determined to be 6.0-6.3 nm. The radial coordinate of the labels relative to F-actin was 5.0-6.4 nm. However, the intramolecular interhead distance in HMMs in which the two heads were labeled with D and A probes was estimated to be larger. The binding affinity of the second head of HMM(D/A) to F-actin may be reduced because of heterogeneous modification of the SH1 groups, such that the probability of single-head binding is increased.     

Differences in structural dynamics of muscle and yeast actin accompany differences in functional interactions with myosin.

We have used spectroscopic probes ErIA and IAEDANS attached to Cys374 to compare the structural dynamics of yeast actin filaments with that of muscle actin, to understand the structural basis of the less productive interaction of yeast actin with myosin. Time-resolved phosphorescence anisotropy (TPA) of ErIA and steady-state fluorescence of IAEDANS were measured. TPA indicated more rapid rotational motion and more restricted angular amplitude in yeast actin. The fluorescence spectrum was less intense and more red-shifted in yeast actin, suggesting more exposure of the probe to solvent. These results indicate that the two actins differ substantially in the conformational dynamics of the C-terminal region. Binding of myosin S1 induced significantly different spectroscopic changes in TPA and fluorescence of muscle and yeast actin. As a result, the spectroscopic differences between the two actins were decreased by the addition of S1. These results suggest that yeast actin is less effective at activating myosin because of larger changes required in the structure of actin upon strong myosin binding. These results provide insight into the relationship between actomyosin dynamics and function, and they provide a useful framework for structure-function analysis of mutant yeast actin.     

Orientation of spin-labeled light chain-2 exchanged onto myosin cross-bridges in glycerinated muscle fibers.

Electron paramagnetic resonance (EPR) spectroscopy has been used to study the angular distribution of a spin label attached to rabbit skeletal muscle myosin light chain 2. A cysteine reactive spin label, 3-(5-fluoro-2,4-dinitroanilino)-2,2,5,5- tetramethyl-1-pyrrolidinyloxy (FDNA-SL) was bound to purified LC2. The labeled LC2 was exchanged into glycerinated muscle fibers and into myosin and its subfragments. Analysis of the spectra of labeled fibers in rigor showed that the probe was oriented with respect to the fiber axis, but that it was also undergoing restricted rotations. The motion of the probe could be modeled assuming rapid rotational diffusion (rotational correlation time faster than 5 ns) within a "cone" whose full width was 70 degrees. Very different spectra of rigor fibers were obtained with the fiber oriented parallel and perpendicular to the magnetic field, showing that the centroid of each cone had the same orientation for all myosin heads, making an angle of approximately 74 degrees to the fiber axis. Binding of light chains or labeled myosin subfragment-1 to ion exchange heads immobilized the probes, showing that most of the motion of the probe arose from protein mobility and not from mobility of the probe relative to the protein. Relaxed labeled fibers produced EPR spectra with a highly disordered angular distribution, consistent with myosin heads being detached from the thin filament and undergoing large angular motions. Addition of pyrophosphate, ADP, or an ATP analogue (AMPPNP), in low ionic strength buffer where these ligands do not dissociate cross-bridges from actin, failed to perturb the rigor spectrum. Applying static strains as high as 0.16 N/mm2 to the labeled rigor fibers also failed to change the orientation of the spin label. Labeled light chain was exchanged into myosin subfragment-1 (S1) and the labeled S1 was diffused into fibers. EPR spectra of these fibers had a component similar to that seen in the spectra of fibers into which labeled LC2 had been exchanged directly. However, the fraction of disordered probes was greater than seen in fibers. In summary, the above data indicate that the region of the myosin head proximal to the thick filament is ordered in rigor, and disordered in relaxation.     

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).     

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.     

Effects of SH1 and SH2 modifications on myosin: similarities and differences.

The properties of myosin modified at the SH2 group (Cys-697) were studied and compared with the previously reported properties of myosin modified at the SH1 group (Cys-707). 4-[N-[(iodoacetoxy)ethyl]-N methylamino]-7-nitrobenz-2-oxa-1, 3-diazole (IANBD) was used for selective modification of the SH2 group on myosin. SH2-labeled heavy meromyosin (SH2-HMM), similar to SH1-labeled HMM (SH1-HMM), did not propel actin filaments in the in vitro motility assays. SH1- and SH2-HMM produced similar amounts of load in the mixtures with unmodified HMM; the sliding speed of actin filaments gradually decreased with an increase in the fraction of either one of the modified HMMs in the mixture. In analogy to SH1-labeled myosin subfragment 1 (SH1-S1), SH2-labeled S1 (SH2-S1) activated regulated actin in the in vitro motility assays. SH2 modification inhibited Mg-ATPase of S1 and its activation by actin. The weak binding of S1 to actin was unaffected whereas the strong binding was weakened by SH2 modification. Overall, our results demonstrate similar behavior of SH1- and SH2-modified myosin heads in the in vitro motility assays despite some differences in their enzymatic properties. The effects of these modifications are ascribed to the location of the SH1-SH2 helix relative to other functional centers of S1.     

Measurement of interprotein distances in the acto-subfragment 1 rigor complex

Using enzymatic labeling, we have conjugated the fluorescence probe dansylcadaverine (DNC) to Gln-41 of rabbit skeletal muscle actin with the intention of utilizing the dansyl chromophore as a donor in fluorescence resonance energy transfer (FRET) distance measurements. The fluorescence decay of DNC-actin was found to consist of two decay constants (8.23 and 21.2 ns) that were associated with two different but partially overlapping spectra of the dye. Three different chemical points on myosin subfragment 1 (S1) were labeled with suitable acceptors: reactive thiol 1 (SH1) and Cys-136 on LC3 were modified with tetramethylrhodamine 5- (and 6-) iodoacetamide (ITMR); Lys-83 (RLR) was derivatized with trinitrobenzenesulfonate. In the rigor complex of the two labeled proteins, fluorescence resonance energy transfer took place, the efficiency of which was 10.9, 9.28, and 3.73% for the transfer from Gln-41 to SH1, Cys-136 (LC3), and RLR, respectively. The limits of the F?rster critical distance for each pair were obtained from the analysis of the polarization spectra of the donor and of the acceptors. The kappa 2(2/3) distances from actin Gln-41 to the three points on S1 were 63, 66, and greater than 37 A for SH1, Cys-136 (LC3), and RLR, respectively.     

Caldesmon freezes the structure of actin filaments during the actomyosin ATPase cycle

Hybrid contractile apparatus was reconstituted in skeletal muscle ghost fibers by incorporation of skeletal muscle myosin subfragment 1 (S1), smooth muscle tropomyosin and caldesmon. The spatial orientation of FITC-phalloidin-labeled actin and IAEDANS-labeled S1 during sequential steps of the acto-S1 ATPase cycle was studied by measurement of polarized fluorescence in the absence or presence of nucleotides conditioning the binding affinity of both proteins. In the fibers devoid of caldesmon addition of nucleotides evoked unidirectional synchronous changes in the orientation of the fluorescent probes attached to F-actin or S1. The results support the suggestion on the multistep rotation of the cross-bridge (myosin head and actin monomers) during the ATPase cycle. The maximal cross-bridge rotation by 7 degrees relative to the fiber axis and the increase in its rigidity by 30% were observed at transition between A**.M**.ADP.Pi (weak binding) and A--.M--.ADP (strong binding) states. When caldesmon was present in the fibers (OFF-state of the thin filament) the unidirectional changes in the orientation of actin monomers and S1 were uncoupled. The tilting of the myosin head and of the actin monomer decreased by 29% and 90%, respectively. It is suggested that in the "closed" position caldesmon "freezes" the actin filament structure and induces the transition of the intermediate state of actomyosin towards the weak-binding states, thereby inhibiting the ATPase activity of the actomyosin.