Conformational changes of F-actin-ε-ADP in thin filaments in myosin-free muscle fibers induced by Ca2+

Polarized fluorescence from F-actin-ε-ADP in thin filaments reconstituted in a myosin-free single muscle fiber was measured at various concentrations of Ca²⁺. Four components of polarized fluorescence changed with increasing Ca²⁺ concentration at pCa values of around 7 to 6, concomitant with a change of the tension generated by the fiber irrigated with myosin in the presence of Mg-ATP. From analysis of observed values of the four components, it was found that the flexibility of the thin filament increased, or the elastic modulus for bending decreased from 5.7 × 10^?17 dyn cm² to 4.7 × 10^?17 dyn cm², when the pCa value decreased from 7 to 6. In the same range of pCa values, the angles of absorption and emission dipoles of ε-ADP changed, suggesting a small rotation of the base-plane of ε-ADP around an axis perpendicular to the F-actin axis.     

Cooperativity in F-actin filaments on binding of myosin subfragments, demonstrated by fluorescence of 1, N6- ethenoadenosine diphosphate.

The fluorescence lifetime of 1,N⁶-ethenoadenosine diphosphate (?-ADP) is 33 ns when bound to F-actin at 4 °C. When heavy meromyosin or myosin subfragment-1 binds to the F-actin filament, the lifetime of ?-ADP drops, reaching 29 ns when every actin monomer is bound to a myosin head. The change in lifetime is a consequence of cooperative conformational changes among the actin monomers. The results of these experiments support the contention that there are differences in the ways in which the two heads of the myosin molecule interact with the actin filament.     

Polarization of fluorescence from single skinned glycerinated rabbit psoas fibers in rigor and relaxation

Single skinned glycerinated muscle fibers were labelled with the fluorescent dye N-(iodoacetylamino)-1-naphthylamine-5-sulfonic acid (1,5-IAEDANS). The heavy chain of myosin (EC 3.6.1.3) was labelled predominantly when the reaction was carried out in relaxation at 0 °C. Mechanical properties of skinned fibers were little affected by labelling with the fluorophore. Rigor tension developed upon transferring native or labelled skinned fibers from relaxing to rigor solutions lacking Ca²⁺ was very small but could be enhanced by progressively increasing Ca²⁺ concentration; the rigor tension decreased with increasing sarcomere length.Polarization of fluorescence of skinned fibers reacted with 1,5-IAEDANS was measured along the line of excitation as well as at 90° to it. The mean values of parallel and perpendicular components of polarization of labelled fibers measured at 0° were close to the values obtained for native fibers irrigated with 1,5-IAEDANS-labelled heavy meromyosin, fiber “ghosts” irrigated with labelled heavy meromyosin, and oriented bundles of myofibrils reacted with the same fluorophore. Skinned fibers stretched above the rest length and then irrigated with 1,5-IAEDANS-labelled heavy meromyosin gave rise to polarized fluorescence close to the values theoretically predicted for an assembly of helically arranged fluorophores. Using 90° detection system a satisfactory fit to the theory could be obtained from single fibers labelled with 1,5-IAEDANS and measured in rigor. The angle between the fiber axis and the direction of the emission dipole of 1,5-IAEDANS attached to subfragment-1 was estimated to be near 40°.     

Influence of Mg2+ and Ca2+ bound to 1,5-IAEDANS-labeled phosphorylated and dephosphorylated heavy meromyosin complexed with F-actin on polarized fluorescence of the fluorophore

Dephosphorylated and phosphorylated heavy meromyosin, fluorescently labeled with 1,5-IAEDANS attached at the SH1 group, was introduced into myosin-free ghost fibres and the polarized fluorescence of the bound label was measured. The results depended on whether the divalent cation binding sites on heavy meromyosin were saturated with Mg2+ or Ca2+. The calculated angles of absorption and emission dipoles and the amount of random fluorophores were significantly changed, indicating that the random mobility and orientation of the fluorophores of phosphorylated and dephosphorylated heavy meromyosin heads complexed with F-actin in the ghost fibre depend on saturation of heavy meromyosin with Ca2+ or Mg2+. The presence of bound Ca2+ has an opposite effect on the polarized fluorescence of phosphorylated and dephosphorylated 1,5-IAEDANS-heavy meromyosin.     

Angles of nucleotides bound to cross-bridges in glycerinated muscle fiber at various concentrations of ϵ-ATP, ϵ-ADP and ϵ-AMPPNP detected by polarized fluorescence

The polarized fluorescence from nucleotides bound to myosin heads in glycerinated muscle fibers of rabbit psoas was measured as the number of myosin heads with bound nucleotides was varied by adding various concentrations of fluorescent ?-ATP, ?-ADP and ?-AMPPNP (1:N⁶-etheno-ATP, -ADP and -imido ATP). The angles of the absorption and emission dipoles of bound nucleotides to the fiber axis and their angular distribution were determined from the observed values of four components of the polarized fluorescence.The maximum amount of nucleotides bound to the myosin heads in the fiber, B_m, was 170 to 270 μm. The dissociation constant of nucleotides, $\text{K}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, increased in the order ?-ATP, ?-ADP, ?-AMPPNP, and was four to six times larger at a sarcomere length (SL) of 2.1 μm than at 3.7 μm.The polarized fluorescence from bound ?-ADP at SL = 2.1 μm was independent of the amount of bound ?-ADP when it was lower than one-half of B_m, indicating a single helical array of myosin heads having ?-ADP. The angles of the absorption dipole, φ_A, and the emission dipole, φ_E, to the fiber axis were 69 ° and 66 °, respectively. As the amount of bound ?-ADP exceeded one-half of B_m, the values of the polarized fluorescence showed that the extra ?-ADP bound to myosin heads with a lower affinity and had different angles to the fiber axis: φ_A and φ_E were 49 ° and 54 °, respectively. The half-maximum width of the angular distribution of these bound ?-ADP molecules, $\text{θ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, was about 20 °.During development of isometric tension in the presence of ?-ATP with Mg²⁺, the polarized fluorescence was independent of the amount of bound ?-ATP when it was lower than one-third of B_m or when the concentration of free ?-ATP was lower than 100 μm, indicating a single helical array of myosin heads undergoing the ATPase reaction. The angles of bound nucleotides, φ_A and φ_E, were 68 ° and 64 °, respectively. The half-maximum width of the angular distribution, $\text{θ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, was about 22 °. As the amount of bound nucleotides exceeded one-third of B_m, the polarized fluorescence showed deviation from the values expected for the single helical array.The angles φ_A and φ_E for bound ?-AMPPNP were about 58 ° and 62 °, respectively, but the angular distribution was broad; that is, $\text{θ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ was about 42 °. These angles were independent of the amount of bound ?-AMPPNP.In a stretched fiber with SL = 3.7 μm, the polarized fluorescence showed that the angles of ?-ADP, ?-ATP and ?-AMPPNP bound to myosin heads had almost random distributions; $\text{θ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ was 90 ° to 100 °, independent of the amount of bound nucleotides. Similar results were obtained with the relaxed fiber in the presence of ?-ATP.     

Phosphorylation of light chains of myosin from rabbit skeletal muscles affects the type of conformation changes of F-actin induced by heavy meromyosin

The changes in F-actin conformation in myosin-free single ghost fiber induced by the binding of heavy meromyosin (HMM) with dephosphorylated or phosphorylated light chains-2 (LC2) have been studied by measuring intrinsic tryptophan polarized fluorescence of F-actin. It has been found that at low concentrations of Ca2+ (pCa greater than or equal to 8), the binding of HMM with dephosphorylated LC2 to F-actin in ghost fibres increases, whereas the binding of HMM with phosphorylated LC2 decreases the anisotropy of polarized tryptophan fluorescence. The effect is reversed at high concentrations of Ca2+ (pCa = 5). It has been assumed that this effect of myosin light chains phosphorylation may be due to its influence on the type of myosin head binding to F-actin.     

Difference between subfragment-1 and heavy meromyosin in their interaction with F-actin

To elucidate the difference between subfragment-1 and heavy meromyosin in their interaction with F-actin, we used limited tryptic digestion and cross-linking with 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide. The binding of actin to subfragment-1 lowers the susceptibility of the 50K-20K junction of its heavy chain to tryptic digestion. At a molar ratio of one actin to one subfragment-1, all the sites were gradually cleaved by trypsin whereas the sites were completely protected in the presence of a 2-fold molar excess of actin over subfragment-1. In the case of heavy meromyosin, nearly half of the sites were protected completely by the presence of an equimolar amount of actin to its heads suggesting that the two heads of heavy meromyosin bound actin in a different manner. The rate of the cross-linking reaction between subfragment-1 heavy chain and actin with 1-ethyl-3-[3-(dimethylamino) propyl]carbodiimide also depended on the molar ratio of actin to subfragment-1. The rate was maximum at a molar ratio of about 5 actin to 1 subfragment-1. When heavy meromyosin was cross-linked to actin, the maximum rate was observed at a molar ratio of about 3 actin to 1 heavy meromyosin head, the level being about 60% that for subfragment-1 and actin. It was suggested that the presence of the subfragment-2 portion of heavy meromyosin caused these differences by restricting the motion of the two heads.     

Dark-field light microscopic study of the flexibility of F-actin complexes

The flexibility of F-actin complexed with saturating amounts of myosin subfragments has been measured by the use of a dark-field light microscope and a high-sensitivity television camera. When dilute solutions of F-actin complexes were observed in the microscope, single filaments in flexural thermal motion were visible to the eye. Images of the fluctuating filaments were recorded on videotapes using the high-sensitivity camera, and these records were used for the analysis of fluctuation to calculate flexibility in the framework of statistical mechanics of thermal fluctuation in semi-flexible rods. The analysis was carried out by two different methods. In method A, we selected many filaments (the entire length appeared near focus occasionally in the limited period of 10 to 100 seconds), measured the mean square end-to-end distance 〈R²〉 of each filament during the period and also its contour length L, and calculated a parameter λ representing flexibility by the equation given by Landau & Lifshitz (1958): $\text{〈R}{}^2\text{〉 =}\text{[2λL ? 1 +}\text{exp}\text{(?2λL)]}\text{2λ}{}^2$. Then, we obtained a value for λ = 0.040 ± 0.010 μm^?1 for the acto-heavy meromyosin filament at 24.0 °C ± 1.0 deg. C, and λ = 0.027 ± 0.005 μm^?1 for the acto-tropomyosin-heavy meromyosin filament at the same temperature.In method B, still photographs were taken of the video screen to collect a great number of filaments or parts of filaments which appeared just in focus over their length, and the contour length L of each filament and the angle θ(L) between the tangents at its two ends were measured, on the basis of the assumption that the whole length of each filament was in a plane perpendicular to the direction of view. The data were treated statistically and the results were approximated with 〈cosθ(L)〉 = exp(?λL), which holds for an ensemble of filaments with flexibility λ but in two-dimensional thermal motion (Landau & Lifshitz, 1958). The λ-values obtained by this method for acto-heavy meromyosin and acto-tropomyosin-heavy meromyosin filaments were both in good agreements with those obtained by method A, confirming the reliability of our measurement.F-actin complexed with a saturating amount of myosin subfragment-1 was examined by method B, and its flexibility was shown to be little different from that of acto-heavy meromyosin filaments.     

Effect of Ca2+ on conformation of actin in the F-actin--heavy meromyosin complex

The polarized fluorescence of intrinsic tryptophan residues and the birefringence of ghost muscle fibres of rabbit were measured during thin filaments binding to heavy meromyosin containing 5,5'-dithiobis [2-nitrobenzoic acid] light chains and to those devoid of them with a view of investigating conformational changes in F-actin. Ca2+ binding to heavy meromyosin containing 5,5'-dithiobis [2-nitrobenzoic acid] light chains was shown to affect the character of these changes during the formation of the F-actin - heavy meromyosin complex.     

Calcium modulates conformational changes in F-actin induced by smooth muscle heavy meromyosin

The effect of Ca²⁺ on conformational changes in rhodamine-phalloidin-labeled F-actin induced by binding of smooth muscle heavy meromyosin (HMM) with either phosphorylated or dephosphorylated regulatory light chains (LC₂₀) was studied by polarized fluorimetry. LC₂₀ phosphorylation caused alterations in the F-actin structure typical of the force-producing (strong-binding) state, while dephosphorylation of the chains led to alterations typical of the formation of non-force-producing (weak-binding) state of the actomyosin complex. The presence of Ca²⁺ enhanced the effect of LC₂₀ phosphorylation and weakened the effect of LC₂₀ dephosphorylation. These data suggest that Ca²⁺ modulates actin-myosin interaction in smooth muscle by promoting formation of the strong-binding state.     

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.     

Fluorescence and flow dichroism of F-actin-epsilon-ADP; the orientation of the admine plane relative to the long axis of F-actin.

The excitation polarization spectrum of epsilon-ADP bound to F-actin shows that two absorption dipoles at 260 nm and 340 nm are oriented in different directions relative to the emission dipole. On the other hand, the linear dichroism of F-actin-epsilon-ADP gives that the dichroic ratio of the bound epsilon-ADP is approximately constant (about-0.5) in the wavelength region form 250 to 350nm. Furthermore, the fluorescence polarization of epsilon-ADP bound to F-actin which is oriented in the field of flow shows that the emission dipole is nearly perpendicular to the long axis of F-actin. From these observations we conclude that the adenine plane of the bound nucleotide is almost perpendicular to the long axis of F-actin.     

Fluorescence polarization study on Ca2+-sensitivity of conformational changes in F-actin induced by the formation of F-actin-subfragment-1 complex

Ca2+-dependent conformational changes in F-actin during myosin subfragment-1 binding with thin filament (in the absence of troponin and tropomyosin) were found in myosin-free ghost fibres by polarized UV microscopy. The pattern of the conformational changes in F-actin changed cooperatively within the range of free Ca2+ concentrations from 10(-7) mol/l to 10(-6) mol/l. It should be suggested that in skeletal muscle of vertebrates there exists a myosin-linked modulation of contraction by Ca2+.     

Proteolytic cleavage of actin within the DNase-I-binding loop changes the conformation of F-actin and its sensitivity to myosin binding

Effects of subtilisin cleavage of actin between residues 47 and 48 on the conformation of F-actin and on its changes occurring upon binding of myosin subfragment-1 (S1) were investigated by measuring polarized fluorescence from rhodamine-phalloidin- or 1, 5-IAEDANS-labeled actin filaments reconstructed from intact or subtilisin-cleaved actin in myosin-free muscle fibers (ghost fibers). In separate experiments, polarized fluorescence from 1, 5-IAEDANS-labeled S1 bound to non-labeled actin filaments in ghost fibers was measured. The measurements revealed differences between the filaments of cleaved and intact actin in the orientation of rhodamine probe on the rhodamine-phalloidin-labeled filaments, orientation and mobility of the C-terminus of actin, filament flexibility, and orientation and mobility of the myosin heads bound to F-actin. The changes in the filament flexibility and orientation of the actin-bound fluorophores produced by S1 binding to actin in the absence of ATP were substantially diminished by subtilisin cleavage of actin. The results suggest that loop 38-52 plays an important role, not only in maintaining the F-actin structure, but also in the conformational transitions in actin accompanying the strong binding of the myosin heads that may be essential for the generation of force and movement during actin-myosin interaction.     

Fluorescence anisotropy of labeled F-actin: influence of divalent cations on the interaction between F-actin and myosin heads

The interaction between F-actin and soluble proteolytic fragments of myosin, heavy meromyosin and myosin subfragment 1 without ATP, has been studied by measuring the static anisotropy and the transient anisotropy decay of the fluorescent chromophore N-(iodoacetyl)-N'-(5-sulfo-1-naphthyl) ethylenediamine bound to F-actin. In the presence of Ca2+ ions, the mobility of the chromophore was strongly decreased by adding heavy meromyosin or myosin subfragment 1, and this conformation change of F-actin showed a strong cooperativity; that is, a very small amount of myosin heads induced the maximum anisotropy change. On the other hand, in the presence of Mg2+ ions, the addition of a small amount of myosin subfragment 1 or of heavy meromyosin increased the mobility of labeled F-actin that reached a maximum at a molar ratio of about 1/25 or 1/50, respectively. With further addition of myosin heads, the mobility of the labeled actin decreased. From these studies, one concludes that F-actin undergoes a conformation change by interacting with myosin heads, which depends on the nature of the divalent cations present in the solution.     

Lactate dehydrogenase-induced conformational changes of F-actin in myosin-free ghost single fibres

The changes in conformation of F-actin induced by the binding of the glycolytic enzyme lactate dehydrogenase were studied in myosin-free single ghost muscle fibres. The formation of the lactate dehydrogenase-F-actin complex was accompanied by changes in the parameters of intrinsic (tryptophan) and extrinsic (rhodaminyl-phalloin) polarized fluorescence of ghost muscle fibre F-actin. Lactate dehydrogenase stimulated actin-activated Mg2+-ATPase of myosin subfragment 1 by 30%. F-actin of ghost fibres depressed lactate dehydrogenase activity to 20% of the initial values. It is suggested that the energy-providing mechanism is coupled with that of muscle contraction through conformational changes in F-actin.     

Motion of myosin fragments during actin-activated ATPase: fluorescence correlation spectroscopy study.

The rates of the translational motion of myosin fragments, heavy meromyosin (HMM), and heavy meromyosin subfragment-1 (HMM S-1) were measured during actin-activated ATPase reaction by the method of fluorescence correlation spectroscopy. This technique monitors the random fluctuations in the concentration of fluorescent molecules in an open volume which result from the translational diffusion of the molecular species under observation. The statistical behavior of the fluctuations is represented in the form of the autocorrelation function, which is related to the translational diffusion coefficient of the fluorescent molecules. The translational motion of fluorescently labeled myosin fragments was progressively slowed down after additions of increasing amounts of actin in the presence of excess MgATP. When these results are interpreted according to a simple binding scheme, the extent of the retardation can be used to obtain the apparent association constant for binding of S-1 and HMM to actin in the presence of MgATP. In 0.1M KCl and at 23°C, the apparent association constants were determined as K_app^HMM = 2.2 × 10⁴M^?1 and K_app^S-1 = 8.8 × 10³ for HMM and S-1, respectively.     

Acrylamide fluorescence quenching studies on the actin-induced change in protein dynamics in the subfragment-1/subfragment-2 link region of cardiac myosin

In order to obtain information about the actin-induced conformational change around the subfragment-1/subfragment-2 link region of myosin, measurements of the fluorescence quenching by acrylamide were made on cardiac myosin and its heavy meromyosin, in which the reactive lysyl residue located in the link region was labeled with an extrinsic fluorophore, the N-methyl-2-anilino-6-naphthalenesulfonyl group. The results with the model compound indicated the involvement of a collisional quenching mechanism for the fluorophore. The quenching rate constant calculated from measured quenching constants using available lifetime data was extremely low for the labeled myosin (0.59 X 10(8) M-1 . S-1), suggesting that the fluorophore bound to myosin is surrounded by segments of proteins. This value was independent of the solvent viscosity, indicating that the quenching reaction is limited by fluctuations in the protein matrix, which produce the inward movement of acrylamide. Chymotryptic digestion of the labeled myosin, which yielded the light chain-2-deficient heavy meromyosin, made the bound fluorophore slightly exposed. Addition of F-actin resulted in about 40% reduction in the quenching rate constants for the labeled myosin and heavy meromyosin. The actin effect was reversed by adding ATP. These results suggest that the binding of actin to myosin makes the protein matrix around the subfragment-1/subfragment-2 link region less mobile.     

Electrophoresis and orientation of F-actin in agarose gels.

F-Actin was electrophoresed on agarose gels. In the presence of 2 mM MgCl2 and above pH 8.5 F-actin entered 1% agarose; when the electric field was 2.1 V/cm and the pH was 8.8, F-actin migrated through a gel as a single band at a rate of 2.5 mm/h. Labeling of actin with fluorophores did not affect its rate of migration, but an increase in ionic strength slowed it down. After the electrophoresis actin was able to bind phalloidin and heavy meromyosin (HMM) and it activated Mg2+-dependent ATPase activity of HMM. The mobility of F-actin increased with the rise in pH. Acto-S-1 complex was also able to migrate in agarose at basic pH, but at a lower rate than F-actin alone. The orientation of fluorescein labeled F-actin and of fluorescein labeled S-1 which formed rigor bonds with F-actin was measured during the electrophoresis by the fluorescence detected linear dichroism method. The former showed little orientation, probably because the dye was mobile on the surface of actin, but we were able to measure the orientation of the absorption dipole of the dye bound to S-1 which was attached to F-actin, and found that it assumed an orientation largely parallel to the direction of the electric field. These results show that actin can migrate in agarose gels in the F form and that it is oriented during the electrophoresis.     

Fluorimetric studies of actin labeled with dansyl aziridine.

F-actin has been specifically labeled with a fluorescent probe, dansyl aziridine, at cysteine-373 of the protein. The fluorescence property of the conjugated probe serves as a spectroscopic indicator of several processes in which actin participates. The sulfhydryl modification does not impair the G-F transformation of actin, nor does it affect the complex formation of actin and myosin or the dissociation of the complex by ATP as judged by viscosity measurements. However, both labeled actin and actin modified by N-ethylmaleimide, which also reacts at cysteine-373, stimulate the Mg²⁺-ATPase of myosin only about 75% as well as unmodified actin. The probe attached to actin exhibits a 65-nm blue shift of its emission maximum from 560 to 495 nm and a sixfold fluorescence enhancement indicating that it is located in a hydrophobic environment. The excitation spectrum of labeled actin indicates that a tryptophan and a tyrosine residue are close to the probe and transfer excitation energy to the dansyl fluorophore. Upon depolymerization of F-actin, the fluorescence intensity of labeled actin increases about 20%. The fluorescence of labeled actin is also enhanced by the addition of EDTA, ATP, and pyrophosphate, but Mg²⁺ antagonizes this effect reversibly. However, in the presence of 10 mm orthophosphate buffer (pH 7.4) these effects disappear. When labeled F-actin binds with myosin subfragment-1 (SF-1) or heavy meromyosin (HMM), the fluorescence of the actin adduct is enhanced. The fluorescence properties of labeled acto-SF-1 and acto-HMM become insensitive to EDTA and polyphosphates even in the absence of orthophosphate. These results suggest that the two-stranded helical structure of the F-actin filament is stabilized by the presence of phosphate and/or the binding of the myosin “head”.