Rotational dynamics of spin-labeled F-actin in the sub-millisecond time range.

The rotational motions of F-actin filaments and myosin heads attached to them have been measured by saturation transfer electron paramagnetic resonance spectroscopy using spin-labels rigidly bound to actin, or to the myosin head region in intact myosin molecules, heavy meromyosin, and subfragment-1. The spin-label attached to F-actin undergoes rotational motion having an effective correlation time of the order of 10^?4 seconds. This cannot be interpreted as rotation of the entire F-actin filament or local rotation of the spin-label, but must represent an internal rotational mode of F-actin, possibly a bending or flexing motion, or a rotation of an actin monomer or a segment of it. The rate of this rotational motion is reduced approximately fourfold by myosin, HMM or S-1; HMM and S-1 are equally effective, on a molar basis, in slowing this rotation and both produce their maximal effect at a ratio of about one molecule of HMM or S-1 per ten actin monomers. With chymotryptic S-1, the effect is partially reversed at higher concentrations. With S-1 prepared with papain in the presence of Mg²⁺, the reversal is smaller, while with HMM or myosin there is no reversal at higher concentrations. Tropomyosin slightly decreases the actin rotational mobility, and the addition of HMM to the actin-tropomyosin complex produces a further slowing. The rotational correlation time for acto-HMM is the same whether the spin-label is on actin or HMM, indicating that the rotation of the head region of HMM when bound to F-actin is controlled by a mode of rotation within the F-actin filaments.     

Modulation of the actin-activated adenosinetriphosphatase activity of myosin by tropomyosin from vascular and gizzard smooth muscles

Tropomyosins from bovine aorta and pulmonary artery exhibit identical electrophoretic patterns in sodium dodecyl sulfate but differ from tropomyosins of either chicken gizzard or rabbit skeletal muscle. Each of the four tropomyosins binds readily to skeletal muscle F-actin as indicated by their sedimentation with actin and by their ability to maximally stimulate or inhibit actin-activated ATPase activity at a molar ratio of one tropomyosin per seven actin monomers. Smooth and skeletal muscle tropomyosins differ in their effects on activity of skeletal myosin or heavy meromyosin (HMM); the former can enhance activity under conditions in which the latter inhibits. Gizzard and arterial tropomyosins are usually equally effective in stimulating ATPase activity of skeletal acto-HMM, but at high concentrations of Mg2+ gizzard tropomyosin is more effective, a result that cannot be attributed to differences in the binding of the two tropomyosins to F-actin. The effects of tropomyosin also depend on the type of myosin; tropomyosin enhances activity of gizzard myosin under conditions in which it inhibits that of skeletal myosin. Increasing the pH or the Mg2+ concentration can reverse the effect of tropomyosin on actin-stimulated ATPase activity of skeletal HMM from activation to inhibition, but this reversal is not found with gizzard myosin. Activity in the absence of tropomyosin is independent of pH, and the loss of activation with increasing pH is not accompanied by loss of binding of tropomyosin to actin.     

The effect of caldesmon on dynamic properties of F-actin alone and bound to heavy meromyosin and/or tropomyosin

The effect of caldesmon on the rotational dynamics of actin filaments alone or conjugated with heavy meromyosin and/or tropomyosin has been measured by the electron paramagnetic resonance (EPR) technique using a maleimide spin label rigidly bound to Cys374 of actin. The rotation of actin protomers in filaments and the angular distribution of spin probes on actin were determined by conventional EPR spectroscopy, while torsional motions within actin filaments were detected by saturation transfer EPR measurements. Binding of caldesmon to F-actin resulted in the reduction of torsional mobility of actin filaments. The maximum effect was produced at a ratio of about one molecule of caldesmon/seven actin protomers. Smooth muscle tropomyosin enhanced the effect of caldesmon, i.e. caused further slowing down of internal motions within actin filaments. Caldesmon increased the degree of order of spin labels on F-actin in macroscopically oriented pellets in the presence of tropomyosin but not in its absence. Computer analysis of the spectra revealed that caldesmon alone slightly changed the orientation of spin probes relative to the long axis of the filament. In the presence of tropomyosin this effect of caldesmon was potentiated and then approximately every twentieth protomer along the actin filament was affected. Caldesmon weakened the effect of heavy meromyosin both on the polarity of environment of the spin label attached to F-actin and on the degree of order of labels on actin in macroscopically oriented pellets. Whereas the former effect of caldesmon was independent of tropomyosin, the latter one was observed only in the absence of tropomyosin.     

Intermonomer cross-linking of F-actin alters the dynamics of its interaction with H-meromyosin in the weak-binding state

Previous cross-linking studies [Kim E, Bobkova E, Hegyi G, Muhlrad A & Reisler E (2002) Biochemistry 41, 86-93] have shown that site-specific cross-linking among F-actin monomers inhibits the motion and force generation of actomyosin. However, it does not change the steady-state ATPase parameters of actomyosin. These apparently contradictory findings have been attributed to the uncoupling of force generation from other processes of actomyosin interaction as a consequence of reduced flexibility at the interface between actin subdomains-1 and -2. In this study, we use EPR spectroscopy to investigate the effects of cross-linking constituent monomers upon the molecular dynamics of the F-actin complex. We show that cross-linking reduces the rotational mobility of an attached probe. It is consistent with the filaments becoming more rigid. Addition of heavy meromyosin (HMM) to the cross-linked filaments further restricts the rotational mobility of the probe. The effect of HMM on the actin filaments is highly cooperative: even a 1 : 10 molar ratio of HMM to actin strongly restricts the dynamics of the filaments. More interesting results are obtained when nucleotides are also added. In the presence of HMM and ADP, similar strongly reduced mobility of the probe was found than in a rigor state. In the presence of adenosine 5'[betagamma-imido] triphosphate (AMPPNP), a nonhydrolyzable analogue of ATP, weak binding of HMM to either cross-linked or native F-actin increases probe mobility. By contrast, weak binding by the HMM/ADP/AlF4 complex has different effects upon the two systems. This protein-nucleotide complex increases probe mobility in native actin filaments, as does HMM + AMPPNP. However, its addition to cross-linked filaments leaves probe mobility as constrained as in the rigor state. These findings suggest that the dynamic change upon weak binding by HMM/ADP/AlF4 which is inhibited by cross-linking is essential to the proper mechanical behaviour of the filaments during movement.     

Regulatory and catalytic domain dynamics of smooth muscle myosin filaments

Domain dynamics of the chicken gizzard smooth muscle myosin catalytic domain (heavy chain Cys-717) and regulatory domain (regulatory light chain Cys-108) were determined in the absence of nucleotides using saturation-transfer electron paramagnetic resonance. In unphosphorylated synthetic filaments, the effective rotational correlation times, tau(r), were 24 +/- 6 micros and 441 +/- 79 micros for the catalytic and regulatory domains, respectively. The corresponding amplitudes of motion were 42 +/- 4 degrees and 24 +/- 9 degrees as determined from steady-state phosphorescence anisotropy. These results suggest that the two domains have independent mobility due to a hinge between the two domains. Although a similar hinge was observed for skeletal myosin (Adhikari and Fajer (1997) Proc. Natl. Acad. Sci. U.S.A. 94, 9643-9647. Brown et al. (2001) Biochemistry 40, 8283-8291), the latter displayed higher regulatory domain mobility, tau(r)= 40 +/- 3 micros, suggesting a smooth muscle specific mechanism of constraining regulatory domain dynamics. In the myosin monomers the correlation times for both domains were the same (approximately 4 micros) for both smooth and skeletal myosin, suggesting that the motional difference between the two isoforms in the filaments was not due to intrinsic variation of hinge stiffness. Heavy chain/regulatory light chain chimeras of smooth and skeletal myosin pinpointed the origin of the restriction to the heavy chain and established correlation between the regulatory domain dynamics with the ability of myosin to switch off but not to switch on the ATPase and the actin sliding velocity. Phosphorylation of smooth muscle myosin filaments caused a small increase in the amplitude of motion of the regulatory domain (from 24 +/- 4 degrees to 36 +/- 7 degrees ) but did not significantly affect the rotational correlation time of the regulatory domain (441 to 408 micros) or the catalytic domain (24 to 17 micros). These data are not consistent with a stable interaction between the two catalytic domains in unphosphorylated smooth muscle myosin filaments in the absence of nucleotides.     

Identification of amino acid substitutions differentiating actin isoforms in their interaction with myosin

Various aspects of actin--myosin interaction were studied with actin preparations from two types of smooth muscle: bovine aorta and chicken gizzard, and from two types of sarcomeric muscle: bovine cardiac and rabbit skeletal. All four preparations activated the Mg2+-ATPase activity of skeletal muscle myosin to the same Vmax, but the Kapp for the smooth muscle preparations was higher. At low KCl, pH 8.0 and millimolar substrate concentrations the Kapp values differed by a factor of 2.5. This differential behaviour of the four actin preparations correlates with amino acid substitutions at positions 17 and 89 of actin polypeptide chain, differentiating the smooth-muscle-specific gamma and alpha isomers from cardiac and skeletal-muscle-specific alpha isomers. This correlation provides evidence for involvement of the NH2-terminal portion of the actin polypeptide chain in the interaction with myosin. The differences in the activation of myosin ATPase by various actins were sensitive to changes in the substrate and KCl concentration and pH of the assay medium. Addition of myosin subfragment-1 or heavy meromyosin in the absence of nucleotide produced similar changes in the fluorescence of a fluorescent reagent N-(1-pyrenyl)-iodoacetamide, attached at Cys-374, or 1,N6-ethenoadenosine 5'-diphosphate substituted for the bound ADP in actin protomers in gizzard and skeletal muscle F-actin. The results are consistent with an influence of the amino acid substitutions on ionic interactions leading to complex formation between actin and myosin intermediates in the ATPase cycle but not on the associated states.     

Intermolecular dynamics and function in actin filaments

Structural models of F-actin suggest that three segments in actin, the DNase I binding loop (residues 38-52), the hydrophobic plug (residues 262-274) and the C-terminus, contribute to the formation of an intermolecular interface between three monomers in F-actin. To test these predictions and also to assess the dynamic properties of intermolecular contacts in F-actin, Cys-374 pyrene-labeled skeletal alpha-actin and pyrene-labeled yeast actin mutants, with Gln-41 or Ser-265 replaced with cysteine, were used in fluorescence experiments. Large differences in Cys-374 pyrene fluorescence among copolymers of subtilisin-cleaved (between Met-47 and Gly-48) and uncleaved alpha-actin showed both intra- and intermolecular interactions between the C-terminus and loop 38-52 in F-actin. Excimer band formation due to intermolecular stacking of pyrene probes attached to Cys-41 and Cys-265, and Cys-41 and Cys-374, in mutant yeast F-actin confirmed the proximity of these residues on the paired sites (to within 18 A) in accordance with the models of F-actin structure. The dynamic properties of the intermolecular interface in F-actin formed by loop 38-52, plug 262-274 and the C-terminus may account for the observed cross-linking of these sites with reagents < 18 A. The functional importance of actin filament dynamics was demonstrated by the inhibition of the in vitro motility in the Gln-41-Cys-374 cross-linked actin filaments.     

Influence of the bound nucleotide on the molecular dynamics of actin

Rotational dynamics of actin spin-labelled with maleimide probes at the reactive thiol Cys-374 were studied. Replacement of the bound nucleotide by Br8ATP in G-actin and Br8ADP in F-actin causes significant increase of the rotational correlation time of the spin probe, indicating reduced motion in both G and F-actin. The orientation dependence of the electron paramagnetic resonance spectra in oriented F-actin filaments revealed an altered molecular order of the probe when the nucleotide was a Br-substituted one. The bound nucleotide affects the myosin S1 ATPase activation by actin; both Vmax and K(actin) decreased significantly when the bound nucleotide of actin was Br8ADP.     

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.     

Comparison of the effects of smooth and skeletal muscle actins on smooth muscle actomyosin Mg2+-ATPase

Actin has been purified from smooth muscle (chicken gizzard) by two different procedures and its activation of smooth muscle myosin Mg2+-ATPase activity compared with that achieved with rabbit skeletal muscle actin. The procedure of Pardee and Spudich (Methods Enzymol. (1982) 85, 164-181) for the purification of rabbit skeletal muscle actin is readily applicable to the isolation of chicken gizzard actin, enabling large quantities to be purified in two days. Smooth muscle actin could be successfully stored as F-actin at -80 degrees C and survived freezing and thawing at least twice. Smooth muscle actin activated myosin Mg2+-ATPase to a higher level than its skeletal muscle counterpart (77.9 nmol Pi/min/mg myosin vs 48.1 nmol Pi/min/mg myosin).     

Tropomyosin from smooth and skeletal muscles initiates various conformational changes in skeletal F-actin

Changes in F-actin conformation in myosin-free single ghost fibers of rabbit skeletal muscle induced by the binding of skeletal and gizzard tropomyosin to F-actin were studied by measuring intrinsic tryptophan-polarized fluorescence of F-actin. It was found that skeletal and gizzard tropomyosin binding to F-actin initiate different conformational changes in actin filaments. Skeletal tropomyosin inhibits, while gizzard tropomyosin activates the Mg2+-ATPase activity of skeletal actomyosin. It is supposed that in muscle fibers tropomyosin modulates the ATPase activity of actomyosin via conformational changes in F-actin.     

Drebrin-induced Stabilization of Actin Filaments

Drebrin is a mammalian neuronal protein that binds to and organizes filamentous actin (F-actin) in dendritic spines, the receptive regions of most excitatory synapses that play a crucial role in higher brain functions. Here, the structural effects of drebrin on F-actin were examined in solution. Depolymerization and differential scanning calorimetry assays show that F-actin is stabilized by the binding of drebrin. Drebrin inhibits depolymerization mainly at the barbed end of F-actin. Full-length drebrin and its C-terminal truncated constructs were used to clarify the domain requirements for these effects. The actin binding domain of drebrin decreases the intrastrand disulfide cross-linking of Cys-41 (in the DNase I binding loop) to Cys-374 (C-terminal) but increases the interstrand disulfide cross-linking of Cys-265 (hydrophobic loop) to Cys-374 in the yeast mutants Q41C and S265C, respectively. We also demonstrate, using solution biochemistry methods and EM, the rescue of filament formation by drebrin in different cases of longitudinal interprotomer contact perturbation: the T203C/C374S yeast actin mutant and grimelysin-cleaved skeletal actin (between Gly-42 and Val-43). Additionally, we show that drebrin rescues the polymerization of V266G/L267G, a hydrophobic loop yeast actin mutant with an impaired lateral interface formation between the two filament strands. Overall, our data suggest that drebrin stabilizes actin filaments through its effect on their interstrand and intrastrand contacts.     

Orientation of the myosin light chain region by single molecule total internal reflection fluorescence polarization microscopy

To study the orientation and dynamics of myosin, we measured fluorescence polarization of single molecules and ensembles of myosin decorating actin filaments. Engineered chicken gizzard regulatory light chain (RLC), labeled with bisiodoacetamidorhodamine at cysteine residues 100 and 108 or 104 and 115, was exchanged for endogenous RLC in rabbit skeletal muscle HMM or S1. AEDANS-labeled actin, fully decorated with labeled myosin fragment or a ratio of approximately 1:1000 labeled:unlabeled myosin fragment, was adhered to a quartz slide. Eight polarized fluorescence intensities were combined with the actin orientation from the AEDANS fluorescence to determine the axial angle (relative to actin), the azimuthal angle (around actin), and RLC mobility on the <10 ms timescale. Order parameters of the orientation distributions from heavily labeled filaments agree well with comparable measurements in muscle fibers, verifying the technique. Experiments with HMM provide sufficient angular resolution to detect two orientations corresponding to the two heads in rigor. Experiments with S1 show a single orientation intermediate to the two seen for HMM. The angles measured for HMM are consistent with heads bound on adjacent actin monomers of a filament, under strain, similar to predictions based on ensemble measurements made on muscle fibers with electron microscopy and spectroscopic experiments.     

Molecular properties and functions in vitro of chicken smooth-muscle alpha-actinin in comparison with those of striated-muscle alpha-actinins

alpha-Actinin purified from chicken gizzard smooth muscle was characterized in comparison with alpha-actinins from chicken striated muscles, or fast-skeletal muscle, slow-skeletal muscle, and cardiac muscle. The gizzard alpha-actinin molecule consisted of two apparently identical subunits with a molecular weight of 100,000 on SDS-polyacrylamide gel electrophoresis, as do striated-muscle alpha-actinins. Its isoelectric points in the presence of urea were similar to the striated-muscle counterparts. Despite these similarities, distinctive amino acid sequences between smooth-muscle alpha-actinin and striated-muscle alpha-actinins were revealed by peptide mapping using limited proteolysis in SDS. Gizzard alpha-actinin was immunologically distinguished from striated-muscle alpha-actinins. Gizzard alpha-actinin formed bundles of gizzard F-actin as well as of skeletal-muscle F-actin, but could not form any cross-bridges between adjacent actin filaments under conditions where skeletal-muscle alpha-actinin could. Temperature-dependent competition between gizzard alpha-actinin and tropomyosin on binding to gizzard thin filaments was demonstrated by electron microscopic observations. Gizzard alpha-actinin promoted Mg2+-ATPase activity of reconstituted skeletal actomyosin, gizzard acto-skeletal myosin, and gizzard actomyosin. This promoting effect was depressed by the addition of gizzard tropomyosin. These findings imply that, despite structural differences between gizzard and striated-muscle alpha-actinin molecules, they function similarly in vitro, and that gizzard alpha-actinin can interact not only with smooth-muscle actin (gamma- and beta-actin) but also with skeletal-muscle actin (alpha-actin).     

Carbodiimide-catalyzed cross-linking sites in the heads of gizzard heavy meromyosin attached to F-actin

In the rigor complex between rabbit skeletal muscle F-actin and chicken gizzard heavy meromyosin (HMM), the direct contact between two HMM heads was demonstrated by using a zero-length cross-linker 1-ethyl-3-[3-(dimethylamino)propyl]maleimide (EDC) [Onishi, H., Maita, T., Matsuda, G., & Fujiwara, K. (1989) Biochemistry (preceding paper in this issue)]. Here, the 60K peptide which was a product of the EDC cross-linking between two 24K heavy chain (tryptic) fragments of HMM was further fragmented with cyanogen bromide, and the location of the cross-linking sites on the amino acid sequence of the HMM heavy chain was investigated. The result showed that one site resided within the 77-residue peptide region (residues 1-77) on one head of HMM, whereas the other site belonged to the 40-residue peptide region (residues 164-203) on the other head. This finding suggests that the two HMM heads are in contact with each other at different sites. Ultracentrifugal fractionation revealed that the head-to-head cross-linked gizzard HMM could be reversibly released from F-actin in the presence of Mg-ATP. The yield of the head-to-head cross-linking was not significantly changed with the acto-HMM complex between actin/HMM head molar ratios of 1 and 4, and it was very slightly decreased even at a molar ratio of 8, where HMM molecules were attached sparsely to actin filaments.(ABSTRACT TRUNCATED AT 250 WORDS)     

Actin dynamics studied by solid-state NMR spectroscopy

Solid-state nuclear magnetic resonance spectroscopy was used to study the motion of ²H and ¹⁹F probes attached to the skeletal muscle actin residues Cys-10, Lys-61 and Cys-374. The probe resonances were observed in dried and hydrated G-actin, F-actin and F-actin-myosin subfragment-1 complexes. Restricted motion was exhibited by ¹⁹F probes attached to Cys-10 and Cys-374 on actin. The dynamics of probes attached to dry cysteine powder or F-actin were very similar and the binding of myosin had little effect indicating that the local probe environment imposes the major influence on motion in the solid state. Correlation times determined for the solid state probes indicated that they were undergoing some rapid internal motion in both G-actin and F-actin such as domain twisting. The probe size influenced the motion in G-actin and appeared to sense monomer rotation but not in F-actin where segmental mobility and intramonomer co-ordination appeared to dominate.     

Evidence for the association between two myosin heads in rigor acto-smooth muscle heavy meromyosin

The rigor complexes that formed between rabbit skeletal muscle F-actin and chicken gizzard heavy meromyosin (HMM), in which the heavy chains had been cleaved with trypsin into 24K, 50K, and 68K fragments, were examined by using the zero-length chemical cross-linker 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide (EDC). Two cross-linked products of approximate Mr 115K and 60K were generated. These products were not obtained by EDC treatment of HMM in the absence of F-actin. The HMM fragments that participated in cross-linking were identified by fluorescent labeling and amino acid composition studies. The 115K peptide was determined to be a covalently cross-linked complex that formed between actin and the COOH-terminal 68K fragment of the HMM heavy chain. Our results are in agreement with a previous study which proposed that the site of cross-linking between HMM and F-actin resides within the COOH-terminal 22K fragment of the myosin subfragment 1 heavy chain [Marianne-Pépin, T., Mornet, D., Bertrand, R., Labbé, J.-P., & Kassab, R. (1985) Biochemistry 24, 3024-3029]. The 60K peptide, however, was not a product of cross-linking between HMM and F-actin. On the basis of its amino acid composition, we concluded that this 60K peptide was a cross-linked dimer of the NH2-terminal 24K fragments of the HMM heavy chain. The cross-linking of acto-gizzard HMM significantly increased the Mg-ATPase activity of gizzard HMM without any observable phosphorylation of the regulatory (20K) light chains.(ABSTRACT TRUNCATED AT 250 WORDS)     

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

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

Fluorescence depolarization of actin filaments in reconstructed myofibers: the effect of S1 or pPDM-S1 on movements of distinct areas of actin

Fluorescence polarization measurements were used to study changes in the orientation and order of different sites on actin monomers within muscle thin filaments during weak or strong binding states with myosin subfragment-1. Ghost muscle fibers were supplemented with actin monomers specifically labeled with different fluorescent probes at Cys-10, Gln-41, Lys-61, Lys-373, Cys-374, and the nucleotide binding site. We also used fluorescent phalloidin as a probe near the filament axis. Changes in the orientation of the fluorophores depend not only on the state of acto-myosin binding but also on the location of the fluorescent probes. We observed changes in polarization (i.e., orientation) for those fluorophores attached at the sites directly involved in myosin binding (and located at high radii from the filament axis) that were contrary to the fluorophores located at the sites close to the axis of thin filament. These altered probe orientations suggest that myosin binding alters the conformation of F-actin. Strong binding by myosin heads produces changes in probe orientation that are opposite to those observed during weak binding.     

The rigor configuration of smooth muscle heavy meromyosin trapped by a zero-length cross-linker

When chicken gizzard heavy meromyosin (HMM) in its rigor complex with actin was reacted with the zero-length cross-linker 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide (EDC), HMM cross-linked with actin but also the two heads of the HMM molecule cross-linked to each other [Onishi, H., Maita, T., Matsuda, G., & Fujiwara, K. (1989) Biochemistry 28, 1898-1904, 1905-1912]. By ultracentrifugal fractionation of the EDC-treated acto-HMM in the presence of Mg-ATP, we obtained a preparation enriched for gizzard HMM with cross-linked heads. When HMM molecules in this preparation were rotary-shadowed and observed in an electron microscope, many head pairs were in contact with each other. The amount of HMM with cross-linked heads determined by electron microscopy was equal to that of the cross-linked NH2-terminal 24K tryptic fragments of HMM heavy chains determined by NaDodSO4 gel electrophoresis, indicating that this cross-linking is primarily responsible for the contact observed between two HMM heads. Most pairs of the contacted heads originated in the same HMM molecule, although a few pairs belonged to different HMM molecules. Cross-linking between the two heads of the same HMM molecule appeared to occur within the distal, more globular half of each head. However, the cross-linking sites were located at different positions within the globular portion. The actin-activated Mg-ATPase activity of the HMM sample treated with EDC in the presence of actin increased in a biphasic manner, depending on the concentration of F-actin, with two apparent association constants: 2.9 x 10(4) M-1 and one much less than 1 x 10(4) M-1. Since the apparent association constant obtained with the HMM control was similar to the latter value, the association constant for HMM molecules with cross-linked heads was identified to be the former value. The binding of HMM to actin was thus strengthened at least by a factor of 3 by the cross-linking between two HMM heads. These results suggest that HMM heads are trapped by treatment with EDC in the rigor complex configuration and that this configuration is retained even after the HMM has been released from actin. The EDC reactivity of rabbit skeletal muscle HMM, however, was different from that of chicken gizzard HMM. The treatment of acto-HMM complexes with EDC did not generate cross-linking between two skeletal muscle HMM heads.