Light chain-dependent myosin structural dynamics in solution investigated by transient electrical birefringence.

The technique of transient electrical birefringence was used to compare some of the electric and structural dynamic properties of myosin subfragment 1 (S1(elc, rlc)), which has both the essential and regulatory light chains bound, to S1(elc), which has only an essential light chain. The rates of rotational Brownian motion indicate that S1(elc, rlc) is larger, as expected. The permanent electric dipole moment of S1(elc, rlc) is also larger, indicating that the regulatory light chain portion of S1(elc, rlc) has a dipole moment and that it is aligned head-to-tail with the dipole moment of the S1(elc) portion. The permanent electric dipoles decrease with increasing ionic strength, apparently because of ion binding to surface charges. Both S1(elc, rlc) and S1(elc) have intrinsic segmental flexibility, as detected by the ability to selectively align segments with a brief weak electric field. However, unlike S1(elc), which can be structurally distorted by the action of a brief strong electric field, S1(elc, rlc) is stiffer and cannot be distorted by fields as high as 7800 V/cm applied to its approximately 8000 D permanent electric dipole moment. The S1 . MgADP . Pi analog S1 . MgADP . Vi is smaller than S1 . MgADP, for both S1(elc, rlc) and S1(elc). Interestingly, the smaller, stiffer S1(elc, rlc) . MgADP . Vi complex retains intrinsic segmental flexibility. These results are discussed within a framework of current hypotheses of force-producing mechanisms that involve S1 segmental motion and/or the loss of cross-bridge flexibility during force production.     

Conformational flexibility of the Cys 697-Cys 707 segment of myosin subfragment-1. Distance distributions by frequency-domain fluorometry

The separation between Cys 697 (SH1) and Cys 707 (SH2) of the heavy chain of myosin subfragment-1 was previously measured by fluorescence resonance energy transfer with a donor linked to SH1 and an acceptor to SH2. In the present study the distribution of the distances between the two thiols was recovered from frequency-domain fluorometry. In the native state and in the presence of ligands such as MgADP, pyrophosphate, orthovanadate (Vi) and actin, we found wide distributions of the separations between SH1 and SH2 (11-16 A) comparable to that found in the random-coil state (20 A). These results suggest that the SH1-SH2 segment has a high degree of conformational flexibility even in native S1. The flexibility is not much affected by the physiological state of S1. However, the ligands MgADP, Vi and MgADP + Vi decrease significantly the mean SH1-SH2 distance from 27 to 17 A with the effect of MgADP+ Vi being the most pronounced. The anisotropy decay of donor-labeled S1 is biphasic with two rotational correlation times. The long component is decreased by these ligands from 289 to 93 ns, suggesting a more compact symmetric structure of S1 in the presence of the ligands. The complex S1(MgADP)Vi has been shown to be a stable analogue of S1(MgADP)Pi, an unstable intermediate that is generated in the actomyosin ATPase cycle during muscle contraction. Since the power stroke of muscle is accompanied by release of Pi from S1(MgADP)Pi, the present results are consistent with a model in which force generation can be accompanied by transition of S1 from a highly symmetric or compact structure to a more extended structure.     

The ADP release step of the smooth muscle cross-bridge cycle is not directly associated with force generation.

When smooth muscle myosin subfragment 1 (S1) is bound to actin filaments in vitro, the light chain domain tilts upon release of MgADP, producing a approximately 3.5-nm axial motion of the head-rod junction (Whittaker et al., 1995. Nature. 378:748-751). If this motion contributes significantly to the power stroke, rigor tension of smooth muscle should decrease substantially in response to cross-bridge binding of MgADP. To test this prediction, we monitored mechanical properties of permeabilized strips of chicken gizzard muscle in rigor and in the presence of MgADP. For comparison, we also tested psoas and soleus muscle fibers. Any residual bound ADP was minimized by incubation in Mg2+-free rigor solution containing 15 mM EDTA. The addition of 2 mM MgADP, while keeping ionic strength and free Mg2+ concentration constant, resulted in a slight increase in rigor tension in both gizzard and soleus muscles, but a decrease in psoas muscle. In-phase stiffness monitored during small (<0.1%) 500-Hz sinusoidal length oscillations decreased in all three muscle types when MgADP was added. The changes in force and stiffness with the addition of MgADP were similar at ionic strengths from 50 to 200 mM and were reversible. The results with gizzard muscle were similar after thiophosphorylation of the regulatory light chain of myosin. These results suggest that the axial motion of smooth muscle S1 bound to actin, upon dissociation of MgADP, is not associated with force generation. The difference between the present mechanical data and previous structural studies of smooth S1 may be explained if geometrical constraints of the intact contractile filament array alter the motions of the myosin heads.     

UV-induced vanadate-dependent modification and cleavage of skeletal myosin subfragment 1 heavy chain. 1. Evidence for active site modification

Ultraviolet irradiation above 300 nm of the stable MgADP-orthovanadate (Vi)-myosin subfragment 1 (S1) complex resulted in covalent modification of the S1 and in the rapid release of trapped MgADP and Vi. This photomodified S1 had Ca2+ATPase activity 4-5-fold higher than that of the non-irradiated control S1, while the K+EDTA-ATPase activity was below 10% of controls. There was a linear correlation between the activation of the Ca2+ATPase and the release of both ADP and Vi with irradiation time. Analysis of the total number of thiols and the ability of photomodified S1 to retrap MgADP by cross-linking SH1 and SH2 with various bifunctional thiol reagents indicated that the photomodification did not involve these reactive thiols. Irradiation of the S1-MgADP-Vi complex caused a large increase in absorbance of the enzyme at 270 nm which was correlated with the release of Vi from the active site, suggesting an aromatic amino acid(s) was (were) involved. However, analysis by three different methods showed no loss of tryptophan. All the irradiation-dependent phenomena could be prevented by replacing Mg2+ with either Co2+, Mn2+, or Ni2+. Unlike previous irradiation studies of Vi-dynein complexes [Lee-Eiford, A., Ow, R. A., & Gibbons, I. R. (1986) J. Biol. Chem. 261, 2337-2342], no peptide bonds were cleaved in photomodified S1. Photomodified S1 was able to retrap MgADP-Vi at levels similar to unmodified S1. Upon irradiation of the photomodified S1-MgADP-Vi complex, MgADP and Vi were again released from the active site, resulting in heavy chain cleavage to form NH2-terminal 21-kDa and COOH-terminal 74-kDa peptides. All evidence indicates that this new photomodification and subsequent chain cleavage occur specifically at the active site.     

Nucleotide- and temperature-induced changes in myosin subfragment-1 structure.

The effects of nucleotide binding and temperature on the internal structural dynamics of myosin subfragment 1 (S1) were monitored by intrinsic tryptophan phosphorescence lifetime and fluorescence anisotropy measurements. Changes in the global conformation of S1 were monitored by measuring its rate of rotational diffusion using transient electric birefringence techniques. At 5 degrees C, the binding of MgADP, MgADP,P and MgADP,V (vanadate) progressively reduce the rotational freedom of S1 tryptophans, producing what appear to be increasingly more rigidified S1-nucleotide structures. The changes in the luminescence properties of the tryptophans suggest that at least one is located at the interface of two S1 subdomains. Increasing the temperature from 0 to 25 degrees C increases the apparent internal mobility of S1 tryptophans in all cases and, in addition, a reversible temperature-dependent transition centered near 15 degrees C was observed for S1, S1-MgADP and S1-MgADP,P, but not for S1-MgADP,V. The rotational diffusion constants of S1 and S1-MgADP were measured at temperatures between 0 and 25 degrees C. After adjusting for the temperature and viscosity of the solvent, the data indicate that the thermally induced transition at 15 degrees C comprises local conformational changes, but no global conformational change. Structural features of S1-MgADP,P, which may relate to its role in force generation while bound to actin, are presented.     

MgATP-induced conformational change of the catalytic subunit of cAMP-dependent protein kinase

Conformational changes of the cAMP-dependent protein kinase (PKA) catalytic (C) subunit are critical for the catalysis of gamma-phosphate transfer from adenosine 5'-triphosphate (ATP) to target proteins. Time-resolved fluorescence anisotropy (TRFA) was used to investigate the respective roles of Mg(2+), ATP, MgATP, and the inhibitor peptide (IP20) in the conformational changes of a 5,6-carboxyfluorescein succinimidyl ester (CF) labeled C subunit ((CF)C). TRFA decays were fit to a biexponential equation incorporating the fast and slow rotational correlation times phi(F) and phi(S). The (CF)C apoenzyme exhibited the rotational correlation times phi(F)=1.8+/-0.3 ns and phi(S)=20.1+/-0.6 ns which were reduced to phi(F)=1.1+/-0.2 ns and phi(S)=13.3+/-0.9 ns in the presence of MgATP. The reduction in rotational correlation times indicated that the (CF)C subunit adopted a more compact shape upon formation of a (CF)C.MgATP binary complex. Neither Mg(2+) (1-3 mM) nor ATP (0.4 mM) alone induced changes in the (CF)C subunit conformation equivalent to those induced by MgATP. The effect of MgATP was removed in the presence of ethylenediaminetetraacetic acid (EDTA). The addition of IP20 and MgATP to form the (CF)C x MgATP x IP20 ternary complex produced rotational correlation times similar to those of the (CF)C x MgATP binary complex. However, IP20 alone did not elicit an equivalent reduction in rotational correlation times. The results indicate that binding of MgATP to the C subunit may induce conformation changes in the C subunit necessary for the proper stereochemical alignment of substrates in the subsequent phosphorylation.     

Characterization of the ethenoadenosine diphosphate binding site of myosin subfragment 1. Energetics of the equilibrium between two states of nucleotide.S1 and vanadate-induced global conformation changes detected by energy transfer

The fluorescence decay of 1,N6-ethenoadenosine diphosphate (epsilon ADP) bound to myosin subfragment 1 (S1) was studied as a function of temperature. The decay was biexponential, and the two lifetimes were quenched relative to the single lifetime of free epsilon ADP. The temperature dependence of the fractional intensities of the decay components showed two states of the S1.epsilon ADP complex. At pH 7.5 in 30 mM TES, 60 mM KCl, and 3 mM MgCl2, the equilibrium constant for the conversion of the low-temperature state (S1L.epsilon ADP) to the high-temperature state (S1H.epsilon ADP) was 40 at physiological temperatures, and delta H degrees = 13 kcal.mol-1 and delta S degrees = 49 cal.deg-1.mol-1. At 10 degrees C the equilibrium constant of S1 for epsilon ADP was 5, indicating that S1H.epsilon ADP was the dominant state, and that for the vanadate complex epsilon ADP.Vi was 0.7, suggesting that in S1.epsilon ADP.Vi the dominant state of the S1-nucleotide complex was converted from S1H.epsilon ADP to S1L.epsilon ADP. The single rotational correlation time of bound epsilon ADP at 10 degrees C decreased from 107 ns in S1.epsilon ADP to 74 ns in S1+.epsilon ADP.Vi. Conversion of the binary complex to the ternary vanadate complex resulted in a 3-A decrease in the energy transfer distance between bound epsilon ADP and N-[4-(dimethylamino)-3,5-dinitrophenyl]maleimide attached to SH1 and a decrease of the average distance between bound epsilon ADP and bound Co2+ from 12.6 to 8.3 A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Rotational dynamics of actin-bound intermediates in the myosin ATPase cycle.

We have used saturation-transfer electron paramagnetic resonance (ST-EPR) to detect the microsecond rotational motions of spin-labeled myosin subfragment one (MSL-S1) bound to actin in the presence of the ATP analogues AMPPNP (5'-adenylylimido diphosphate) and ATP gamma S [adenosine 5'-O-(3-thiotriphosphate)], which are believed to trap myosin in strongly and weakly bound intermediate states of the actomyosin ATPase cycle, respectively. Sedimentation binding measurements were used to determine the fraction of myosin heads bound to actin under ST-EPR conditions and the fraction of heads containing bound nucleotide. ST-EPR spectra were then corrected to obtain the spectrum corresponding to the ternary complex (actin.MSL-S1.nucleotide). The ST-EPR spectrum of MSL-S1.AMPPNP bound to actin is identical to that obtained in the absence of nucleotide (rigor complex), indicating no rotational motion of MSL-S1 relative to actin on the microsecond time scale. However, MSL-S1-ATP gamma S bound to actin is rotationally mobile, with an effective rotational correlation time (tau r) of 17 +/- 2 microseconds. This motion is similar to that observed previously for actin-bound MSL-S1 during the steady-state hydrolysis of ATP [Berger et al. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 8753-8757]. We conclude that, in solution, the weakly bound actin-attached states of the myosin ATPase cycle undergo microsecond rotational motions, while the strongly bound intermediates do not, and that these motions are likely to be involved in the molecular mechanism of muscle contraction.     

Differential mobility of skeletal and cardiac tropomyosin on the surface of F-actin.

Polarized phosphorescence from the triplet probe erythrosin-5-iodoacetamide attached to sulfhydryls in rabbit skeletal and cardiac muscle tropomyosin (Tm) was used to measure the microsecond rotational dynamics of these tropomyosins in a complex with F-actin. The steady-state phosphorescence anisotropy of skeletal tropomyosin on F-actin was 0.025 +/- 0.005 at 20 degrees C; the comparable anisotropy for cardiac tropomyosin was 0.010 +/- 0. 003. Measurements of the anisotropy as a function of temperature and solution viscosity (modulated by addition of glycerol) indicated that both skeletal and cardiac tropomyosin undergo complex rotational motions on the surface of F-actin. Models assuming either long axis rotation of a rigid rod or torsional twisting of a flexible rod adequately fit these data; both analyses indicated that cardiac Tm is more mobile than skeletal Tm and that the increased mobility on the surface of F-actin reflected either the rotational motion of a smaller physical unit or the torsional twisting of a less rigid molecule. The binding of myosin heads (S1) to the Tm-F-actin complexes increased the anisotropy to 0.049 +/- 0.004 for skeletal and 0.054 +/- 0.007 for cardiac tropomyosin. The titration of the skeletal tropomyosin-F-actin complex by S1 showed a break at an S1/actin ratio of 0.14; this complex had an anisotropy of 0.040 +/- 0.007, suggesting that one bound head effectively restricted the motion of each skeletal tropomyosin. A similar titration with cardiac tropomyosin reached a plateau at an S1/actin ratio of 0.4, suggesting that 2-3 myosin heads are required to immobilize cardiac Tm. Surface mobility is predicted by structural models of the interaction of tropomyosin with the actin filament while the decrease in tropomyosin mobility upon S1 binding is consistent with current theories for the proposed role of myosin binding in the mechanism of tropomyosin-based regulation of muscle contraction.     

Myosin subfragment 1 has tertiary structural domains

Transient electrical birefringence measurements were made on skeletal muscle myosin subfragment 1 (S1) at 3.7 degrees C in 10 mM tris(hydroxymethyl)aminomethane-acetate and 0.10 mM MgCl2, pH 7.0. The specific birefringence for 4.5 microM S1 was determined from steady-state measurements to be (8.1 +/- 0.3) X 10(-7) (cm/statvolt)2. For electric fields in the range of 2.47-24.7 statvolts/cm, the alignment was due to a large permanent dipole moment for S1, estimated to be 8500 +/- 2000 D. The duration and the strength of the transient electric field was varied, and the temporal response of the decay of the birefringence signal was analyzed. The rate of rotational motion after the field was removed increased with increasing field strength for short (0.35-microseconds) pulses and decreased with increasing pulse lengths for all field strengths. The rate of decay from a steady-state birefringence signal was independent of field strength. A model of S1 structure is proposed, which is consistent with these data and most other data on S1 structure. In this model, S1 is composed of two tertiary structural domains that are connected by a flexible linkage with a substantial restoring force. The electric dipole moments on the two domains are arranged head to tail. The segmental movement of the domains is restricted to certain directions. The average conformation of the molecule is elongated, but it can be made more compact by the torque exerted by an electric field. The structural changes depend on the strength and duration of the pulse.(ABSTRACT TRUNCATED AT 250 WORDS)     

The effects of ligands on the conformation of phosphoglycerate kinase: fluorescence anisotropy decay and theoretical interpretation

Horse muscle phosphoglycerate kinase (PGK) is a monomer folded into two widely distant domains. In the glycolytic pathway, this enzyme catalyzes the first reaction that produces ATP. It was suggested, by analogy with yeast hexokinase, that a hinge-bending motion may be induced by the binding of specific substrates to the protein. To analyze such a motion, or any structural changes induced by ligand binding, fluorescence anisotropy decay of tryptophan residues in free and liganded PGK was studied. At 293 K, for the free protein and the binary complex with 3-phosphoglycerate, a single correlation time of 26 ns was observed, corresponding to the rotation of the overall protein, whereas upon addition of MgADP, this correlation time decreased to 10 ns. Such a decrease cannot be merely due to a change of the protein's shape and volume. To explain this, it was suggested that the fluorescence anisotropy decay of the PGK-MgADP complex corresponded to the rotation of the only buried tryptophan (Trp 335). The rotational paths of this tryptophan, in the presence and absence of the nucleotide, were established by potential energy minimization calculations. The results indicated that MgADP induces a displacement of helix alpha-13 that decreases the rotational energy barrier of Trp 335 from 16 kcal/mol in the free protein to 8 kcal/mol in the complex.     

Saturation transfer electron spin resonance study on the rotational diffusion of calcium- and magnesium-dependent adenosine triphosphatase in sarcoplasmic reticulum membranes.

The technique of saturation transfer electron spin resonance has been applied to study the rotational diffusion of spin-labeled Ca2+, Mg2+-dependent ATPase molecules in the membranes of sarcoplasmic reticulum vesicles. Comparison of the present data with those for spin-labeled hemoglobin undergoing isotropic rotation leads to a value of 2 X 10(-4) s for the apparent rotational correlation time at 20 degrees C for the membrane-bound protein. Consideration of the anisotropy of the Brownian rotation of the membrane-bound ATPase suggests that the true correlation time for the expected axial rotation may be somewhat smaller than the apparent value. An Arrhenius plot of the rotational motion shows a break, which is interpreted as indicating the occurrence of a conformational change of the ATPase molecule at about 15 degrees C.     

The vanadium- and molybdenum-containing nitrogenases of Azotobacter chroococcum. Comparison of mid-point potentials and kinetics of reduction by sodium dithionite of the iron proteins with bound magnesium adenosine 5''-diphosphate.

The mid-point potentials of the Fe protein components (Ac2 and Ac2* respectively) of the Mo nitrogenase and V nitrogenase from Azotobacter chroococcum were determined in the presence of MgADP to be -450 mV (NHE) [Ac2(MgADP)2-Ac2*ox.(MgADP)2 couple] and -463 mV (NHE) [Ac2* (MgADP)2-Ac2*ox.(ADP)2 couple] at 23 degrees C at pH 7.2. These values are consistent with a flavodoxin characterized by Deistung & Thorneley [(1986) Biochem. J. 239, 69-75] with Em = -522 mV (NHE) being an effective electron donor to both the Mo nitrogenase and the V nitrogenase in vivo. Ac2*ox.(MgADP)2 and Ac2*ox.(MgADP)2 were reduced by SO2.- (formed by the predissociation of dithionite ion, S2O4(2-)) at similar rates, k = 4.7 X 10(6) +/- 0.5 X 10(6) M-1.s-1 and 3.2 X 10(6) +/- 0.2 X 10(6) M-1.s-1 respectively, indicating structural homology at the electron-transfer site associated with the [4Fe-4S] centre in these proteins.     

Unusual conformational changes in 6-hydroxymethyl-7,8-dihydropterin pyrophosphokinase as revealed by X-ray crystallography and NMR

The crystal structure of Escherichia coli 6-hydroxymethyl-7,8-dihydropterin pyrophosphokinase (HPPK) in complex with MgADP has been determined at 1.5-A resolution with a crystallographic R factor of 0.191. The solution structure of HPPK in complex with Mg(2+) and beta,gamma-methyleneadenosine 5'-triphosphate (MgAMPPCP) has been determined using a simulated annealing protocol with 3,523 experimental NMR restraints. The root mean square deviation of the ensemble of 20 refined conformers that represent the solution structure from the mean coordinate set derived from them is 0.74 +/- 0.26 A for all backbone atoms and 0.49 +/- 0.22 A when residues Pro(14), Pro(44)-Gln(50), and Arg(84)-Pro(91) are excluded. Binding of MgADP causes significant changes in the conformation and dynamical property of three loops of HPPK that are involved in catalysis. A dramatic, unusual conformational change is that loop 3 moves away from the active center significantly with some residues moving by >17 A. The binding of MgADP also stabilizes loop 1 and loop 3 but makes loop 2 more mobile. Very similar conformational and dynamical changes are observed in the NMR solution structure of HPPK.MgAMPPCP. The conformational and dynamical changes may play important roles in both substrate binding and product release in the catalytic cycle.     

Adenine nucleotides regulate the functional transition in mitochondrial H+-ATPase and the kinetic behaviour of its ATP-synthetase form

The kinetics of the SMP-catalyzed Pi-ATP exchange and oxidative phosphorylation was studied at variable [MgATP] + + [MgADP] and [MgATP]/[MgADP]. The existence on F1 of a center with a low affinity was demonstrated (KM = 0.4-2.7 mM). Saturation of this center with the Mg2+-complex of one of the nucleotides is obligatory for H+-ATPase to exhibit its ATP synthetase activity. It was found that with a decrease of [MgATP]/[MgADP] the lag periods, tau, of the reactions and KM(Pi) also show a decrease. Besides, in the Pi-ATP exchange reactions delta microH+ (steady-state) diminishes and SMP coupling is enhanced (the Vhydr/Vsynth ratio is decreased). Preincubation of SMP with MgADP eliminates the lags but does not affect the course of the steady-state reaction. It is concluded that F1 when bound to MgATP or MgADP changes to a "more" or "less coupled" conformational state, thus determining the rate of conversion to the ATP-synthetase functional state (ko = tau-1), the threshold potential of this conversion and the kinetic behaviour of ATP-synthetase (KM for Pi).     

Photosensitized cleavage of dynein heavy chains. Cleavage at the "V1 site" by irradiation at 365 nm in the presence of ATP and vanadate

Irradiation of soluble dynein 1 from sea urchin sperm flagella at 365 nm in the presence of MgATP and 0.05-50 microM vanadate (Vi) cleaves the alpha and beta heavy chains (Mr 428,000) at their V1 sites to give peptides of Mr 228,000 and 200,000, without the nonspecific side effects produced by irradiation at 254 nm as described earlier (Lee-Eiford, A., Ow, R. A., and Gibbons, I. R. (1986) J. Biol. Chem. 261, 2337-2342). The decrease in intact heavy chain material is biphasic; in 10 microM Vi, approximately 80% occurs with a half-time of 7 min and the remainder with a half-time of about 90 min, and the yield of cleavage peptides is better than 90%. Loss of dynein ATPase activity appears to be a direct result of the cleavage process and is not significantly affected by the presence of up to 0.1 M cysteamine (CA, 60-23-1) or 2-aminoethyl carbamimidothioic acid dihydrobromide (CA, 56-10-0) as free radical trapping agents. The concentration of Vi required for 50% maximal initial cleavage rate is 4.5 microM, while that for 50% ATPase inhibition is 0.8 microM, both in a 0.6 M NaCl medium. In the presence of 20 microM Vi, CTP and UTP support cleavage at about half the rate of ATP, whereas GTP and ITP support cleavage only if the Vi concentration is raised to about 200 microM. Substitution of any of the transition metal cations Cr2+, Mn2+, Fe2+, or Co2+ for the usual Mg2+ suppresses the photocleavage, presumably by quenching the excited chromophore prior to scission of the heavy chain. The photocleaved dynein 1 binds to dynein-depleted flagella similarly to intact dynein 1, but upon reactivation of the flagella with 1 mM ATP their motility is partially inhibited, rather than being augmented as with intact dynein. These results indicate that Vi acts as a photosensitizing catalyst and suggest that the cleavage proceeds through excitation of Vi bound to dynein at the hydrolytic ATP binding site on each heavy chain, probably in a dynein X MgADP X Vi complex. The exquisite specificity of Vi-sensitized photocleavage will aid the peptide mapping of dynein heavy chains and may be of broader use in studies of protein structure.     

Effect of Nucleotides on the Orientation and Mobility of Myosin Subfragment-1 in Ghost Muscle Fiber

Using polarization fluorimetry, the orientation and mobility of 1,5-IAEDANS specifically bound to Cys707 of myosin subfragment-1 (S1) were studied in ghost muscle tropomyosin-containing fibers in the absence and in the presence of MgADP, MgAMP-PNP, MgATPgammaS, or MgATP. Modeling of various intermediate states was accompanied by discrete changes in actomyosin orientation and mobility of fluorescent dye dipoles. This suggests multistep changes in the structural state of the myosin head during the ATPase cycle. Maximal differences in the probe orientation by 4 degrees and its mobility by 30% were found between actomyosin states in the presence of MgADP and MgATP. It is suggested that interaction of S1 with F-actin induces nucleotide-dependent rotation of the whole motor domain of the myosin head or only the dye-binding site and also change in the head mobility.     

Differential scanning calorimetric study of myosin subfragment 1 with tryptic cleavage at the N-terminal region of the heavy chain.

The thermal unfolding of myosin subfragment 1 (S1) cleaved by trypsin was studied by differential scanning calorimetry. In the absence of nucleotides, trypsin splits the S1 heavy chain into three fragments (25, 50, and 20 kDa). This cleavage has no appreciable influence on the thermal unfolding of S1 examined in the presence of ADP, in the ternary complexes of S1 with ADP and phosphate analogs, such as orthovanadate (Vi) or beryllium fluoride (BeFx), and in the presence of F-actin. In the presence of ATP and in the complexes S1.ADP.Vi or S1.ADP.BeFx, trypsin produces two additional cleavages in the S1 heavy chain: a faster cleavage in the N-terminal region between Arg23 and Ile24, and a slower cleavage at the 50 kDa fragment. It has been shown that the N-terminal cleavage strongly decreases the thermal stability of S1 by shifting the maximum of its thermal transition by about 7 degrees C to a lower temperature, from 50 degrees C to 42.4 degrees C, whereas the cleavage at both these sites causes dramatic destabilization of the S1 molecule leading to total loss of its thermal transition. Our results show that S1 with ATP-induced N-terminal cleavage is able, like uncleaved S1, to undergo global structural changes in forming the stable ternary complexes with ADP and Pi analogs (Vi, BeFx). These changes are reflected in a pronounced increase of S1 thermal stability. However, S1 cleaved by trypsin in the N-terminal region is unable, unlike S1, to undergo structural changes induced by interaction with F-actin that are expressed in a 4-5 degrees C shift of the S1 thermal transition to higher temperature. Thus, the cleavage between Arg23 and Ile24 does not significantly affect nucleotide-induced structural changes in the S1, but it prevents structural changes that occur when S1 is bound to F-actin. The results suggest that the N-terminal region of the S1 heavy chain plays an important role in structural stabilization of the entire motor domain of the myosin head, and a long-distance communication pathway may exist between this region and the actin-binding sites.     

Linear dichroism of acrylodan-labeled tropomyosin and myosin subfragment 1 bound to actin in myofibrils.

Muscle contraction can be activated by the binding of myosin heads to the thin filament, which appears to result in thin filament structural changes. In vitro studies of reconstituted muscle thin filaments have shown changes in tropomyosin-actin geometry associated with the binding of myosin subfragment 1 to actin. Further information about these structural changes was obtained with fluorescence-detected linear dichroism of tropomyosin, which was labeled at Cys 190 with acrylodan and incorporated into oriented ghost myofibrils. The fluorescence from three sarcomeres of the fibril was collected with the high numerical aperture objective of a microscope and the dichroic ratio, R (0/90 degrees), for excitation parallel/perpendicular to the fibril, was obtained, which gave the average probe dipole polar angle, Theta. For both acrylodan-labeled tropomyosin bound to actin in fibrils and in Mg2+ paracrystals, Theta congruent to 52 degrees +/- 1.0 degrees, allowing for a small degree of orientational disorder. Binding of myosin subfragment 1 to actin in fibrils did not change Theta; i.e., the orientation of the rigidly bound probe on tropomyosin did not change relative to the actin axis. These data indicate that myosin subfragment 1 binding to actin does not appreciably perturb the structure of tropomyosin near the probe and suggest that the geometry changes are such as to maintain the parallel orientation of the tropomyosin and actin axes, a finding consistent with models of muscle regulation. Data are also presented for effects of MgADP on the orientation of labeled myosin subfragment 1 bound to actin in myofibrils.     

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)