Polarization of fluorescently labeled myosin subfragment-1 fully or partially decorating muscle fibers and myofibrils

Interaction of myosin with F-actin: time-dependent changes at the interface are not slow

The kinetics of formation of the actin-myosin complex have been reinvestigated on the minute and second time scales in sedimentation and chemical cross-linking experiments. With the sedimentation method, we found that the binding of the skeletal muscle myosin motor domain (S1) to actin filament always saturates at one S1 bound to one actin monomer (or two S1 per actin dimer), whether S1 was added slowly (17 min between additions) or rapidly (10 s between additions) to an excess of F-actin. The carbodiimide (1-ethyl-3-(3-dimethylaminopropyl) carbodiimide, EDC)-induced cross-linking of the actin-S1 complex was performed on the subsecond time scale by a new approach that combines a two-step cross-linking protocol with the rapid flow-quench technique. The results showed that the time courses of S1 cross-linking to either of the two actin monomers are identical: they are not dependent on the actin/S1 ratio in the 0.3-20-s time range. The overall data rule out a mechanism by which myosin rolls from one to the other actin monomer on the second or minute time scales. Rather, they suggest that more subtle changes occur at the actomyosin interface during the ATP cycle.

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.

Conformational changes of contractile proteins and their role in muscle contraction

The review summarizes the results of studies on conformational changes in contractile proteins that occur during muscle contraction. Polarized fluorescence of tryptophan residues in actin and of fluorescent probes bound specifically to different sites on actin, myosin, or tropomyosin in muscle fibers was measured. The results show that the transition of actomyosin complex from the weak to the strong-binding state is accompanied by a change in the orientation of F-actin subunits with the C and N termini moving opposite to a large part of the subunit. Myosin light chains and some areas in the 20-kDa domain of myosin head move in the same direction as the C- and N-terminal regions of actin. It is established that troponin, caldesmon, calponin, and myosin systems of regulation of muscle contraction modify intramolecular actomyosin rearrangements in a Ca(2+)-dependent manner. The role of intramolecular movements of contractile proteins in muscle contraction is discussed.

Structural implications of fluorescence quenching in the Shaker K+ channel

When attached to specific sites near the S4 segment of the nonconducting (W434F) Shaker potassium channel, the fluorescent probe tetramethylrhodamine maleimide undergoes voltage-dependent changes in intensity that correlate with the movement of the voltage sensor (Mannuzzu, L.M., M.M. Moronne, and E.Y. Isacoff. 1996. Science. 271:213-216; Cha, A., and F. Bezanilla. 1997. Neuron. 19:1127-1140). The characteristics of this voltage-dependent fluorescence quenching are different in a conducting version of the channel with a different pore substitution (T449Y). Blocking the pore of the T449Y construct with either tetraethylammonium or agitoxin removes a fluorescence component that correlates with the voltage dependence but not the kinetics of ionic activation. This pore-mediated modulation of the fluorescence quenching near the S4 segment suggests that the fluorophore is affected by the state of the external pore. In addition, this modulation may reflect conformational changes associated with channel opening that are prevented by tetraethylammonium or agitoxin. Studies of pH titration, collisional quenchers, and anisotropy indicate that fluorophores attached to residues near the S4 segment are constrained by a nearby region of protein. The mechanism of fluorescence quenching near the S4 segment does not involve either reorientation of the fluorophore or a voltage-dependent excitation shift and is different from the quenching mechanism observed at a site near the S2 segment. Taken together, these results suggest that the extracellular portion of the S4 segment resides in an aqueous protein vestibule and is influenced by the state of the external pore.

Temporally and spectrally resolved imaging microscopy of lanthanide chelates

The combination of temporal and spectral resolution in fluorescence microscopy based on long-lived luminescent labels offers a dramatic increase in contrast and probe selectivity due to the suppression of scattered light and short-lived autofluorescence. We describe various configurations of a fluorescence microscope integrating spectral and microsecond temporal resolution with conventional digital imaging based on CCD cameras. The high-power, broad spectral distribution and microsecond time resolution provided by microsecond xenon flashlamps offers increased luminosity with recently developed fluorophores with lifetimes in the submicrosecond to microsecond range. On the detection side, a gated microchannel plate intensifier provides the required time resolution and amplification of the signal. Spectral resolution is achieved with a dual grating stigmatic spectrograph and has been applied to the analysis of luminescent markers of cytochemical specimens in situ and of very small volume elements in microchambers. The additional introduction of polarization optics enables the determination of emission polarization; this parameter reflects molecular orientation and rotational mobility and, consequently, the nature of the microenvironment. The dual spectral and temporal resolution modes of acquisition complemented by a posteriori image analysis gated on the spatial, spectral, and temporal dimensions lead to a very flexible and versatile tool. We have used a newly developed lanthanide chelate, Eu-DTPA-cs124, to demonstrate these capabilities. Such compounds are good labels for time-resolved imaging microscopy and for the estimation of molecular proximity in the microscope by fluorescence (luminescence) resonance energy transfer and of molecular rotation via fluorescence depolarization. We describe the spectral distribution, polarization states, and excited-state lifetimes of the lanthanide chelate crystals imaged in the microscope.

Interaction of the heavy and light chains of cardiac myosin subfragment-1 with F-actin

The interaction of the heavy chain (HC) and the light chain (cdLC1) of cardiac S1 (cdS1) with F-actin was studied by cross-linking, Western blotting, and fluorescence polarization methods. Incorporation of cdLC1 in cross-linked products was examined by Western blots using the primary antibody against 71-74 residues of cdLC1. Cross-linking with zero-length, water-soluble reagent yielded three products with apparent molecular masses of 150, 160, and 210 kD. Like in the case of cross-linking of skeletal S1 with actin, these complexes included only HC of S1 and actin. The composition of the products were as follows: 150 kD, one HC of S1 cross-linked through a primary site (on the C-terminal of the 20-kD fragment) to the N-terminus of actin; 160 kD, one HC of S1 cross-linked through a secondary site (on the 50 kD fragment) to the N-terminus of actin; and 210 kD, one HC of S1 cross-linked through primary and secondary sites to two actins. Four additional products with apparent molecular masses of 66, 120, 185, and 235 kD contained cdLC1 and were identified as cdLC1 + actin, cdLC1 + HCS1, cdLC1 + actin + HCS1, and cdLC1 + two actins + HCS1, respectively. The same products were observed when cross-linking was performed in cardiac myofibrils incubated with cdS1. The production of cross-linked complexes of the heavy and light chain with actin decreased with an increase in the molar ratio of cdS1:actin. To test whether the orientation of myosin heads depended on a degree of occupation of thin filaments, myofibrils were irrigated with varying concentrations of cdS1. Fluorescence polarization measurements of cdS1 bound to individual I-bands revealed that the orientation depended on the concentration.

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.

A myosin head can interact with two chemically modified G-actin monomers at ATP-modulated multiple sites

It has been reported that chemically modified [with m-maleimidobenzoic acid N-hydroxysuccinimide ester (MBS)] actin maintains its monomeric form and retains the ability to bind (and make chemical cross-links) to myosin head [Bettache, N., Bertrand, R., & Kassab, R. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 6028-6032; Arata, T. (1991) J. Biochem. (Tokyo) 109, 335-340]. Here, the interaction between MBS-G-actin and myosin subfragment 1 (S1) has been further studied by proteolytic susceptibility and chemical cross-linking. Two moles of MBS-actin monomers bound to 1 mol of myosin heads or S1 with different affinities. The first binding of MBS-G-actin to S1 strongly protected a 27-kDa/50-kDa junction of S1 heavy chain from trypsin digestion and also weakly protected a 50-kDa/20-kDa junction. The second binding protected a 50-kDa/20-kDa junction more strongly. ATP weakened these bindings more than 10-fold. MBS-G-actin was cross-linked to S1 by 1-ethyl-3-[3-(dimethylamino)propyl]-carbodiimide, producing the 175-185-kDa doublet bands similar to those of F-actin and S1. The first binding produced a complex migrating at 175 kDa on gels [Hozumi, T. (1992) Biochemistry 31, 10071-10073] and the second binding further produced an 185-kDa complex, suggesting that two binding sites correspond to two spatially separated cross-linking sites. MBS-G-actin was also cross-linked by MBS to S1 when the first actin binds, producing only 180-kDa complex. In the presence of ATP or ADP, an 140-kDa complex was produced together with the 180-kDa complex, suggesting shifting of the binding site.

Kinetics of association of myosin subfragment-1 to unlabeled and pyrenyl-labeled actin

The kinetics of reaction of myosin subfragment-1 (S1) with F-actin have been monitored by the changes in light scattering and in pyrenyl-actin fluorescence at 20 degrees C, pH 7.5, and physiological ionic strength. The association rate constant of S1 to F-actin decreases about 10-fold as the molar ratio of bound S1 increases from 0 to 1. This decrease in k+ is most likely due to the steric hindrance of available binding sites by initially bound S1. The apparent rate constant for association of S1 to bare filaments is 9 microM-1 s-1, a value 1 order of magnitude higher than the one previously estimated from experiments in which S1 was in excess over F-actin. The anticooperative binding kinetics of S1 to F-actin are consistent with the negative cooperativity displayed in the equilibrium binding curves of S1 to pyrenyl-F-actin. Fluorescence titration curves of partially labeled pyrenyl-F-actin by S1 are sigmoidal, consistent with a 4-fold higher affinity of S1 for unlabeled than for labeled action. This conclusion is strengthened by kinetic data of S1 binding to partially labeled F-actin, which exhibit a biphasic behavior due to the slower dissociation of S1 from unlabeled than from labeled actin.

Binding of S1(A1) and S1(A2) to F-actin

The binding curve of myosin subfragment-1 (S1) to F-actin is not a simple hyperbola: at high concentrations of S1 the binding curve can be transformed into a linear plot ("normal" binding), but at small concentrations of S1 the binding complications deform the binding curve and produce nonlinear transforms ("anomalous" binding) [Andreev, O. A., & Borejdo, J. (1992) J. Muscle Res. Cell Motil. 13, 523-533]. This anomalous behavior may result either from the heterogeneity of S1 in regard to light chain isoforms or from the cooperativity between S1's. To distinguish between these possibilities we measured the affinity and the orientation of S1(A1) and S1(A2) with respect to F-actin. Affinity was measured in vitro by ultracentrifugation in the presence of F-actin, and orientation was measured in vivo by a combination of polarization of fluorescence and linear dichroism. We found that both the affinity and the orientation depended on the relative concentration of S1 isomer and actin: when S1 was in excess or was equimolar with actin (filament saturated with S1), each isomer bound F-actin with an affinity of 2 x 10(6) M-1 and was oriented approximately perpendicularly to the muscle axis. When actin was in excess (filament unsaturated with S1), each isomer bound F-actin with an affinity of 1.2 x 10(7) M-1 and was oriented more parallel to the muscle axis. S1(A1) and S1(A2) labeled on the light chain had different polarizations when bound to unsaturated filaments but had the same polarizations when bound to saturated filaments. These results excluded heterogeneity as a reason for anomalous binding and suggested that binding occurred with negative cooperativity. We think that the negative cooperativity occurs when saturation of actin filaments with heads leads to the lack of vacant adjacent sites on a filament and a consequent prevention of S1 binding to two actin protomers.

Fluorescence polarization study of the rigor complexes formed at different degrees of saturation of actin filaments with myosin subfragment-1

A serine residue located in the active site of myosin head (S1) was labelled by 9-anthroylnitrile, an amino group located in the central domain of S1 was labelled by 7-diethylamino-3-(4'-isothio-cyanato-phenyl)-4-methylcoumari n, a cysteine residue located near the C-terminus of S1 was labelled by 5-[2-((iodoacetyl)-amino)ethyl]-amino-naphthalene-1-sulfonic acid (1,5-IAEDANS) and a cysteine residue located near the C-terminus of the alkali light chain 1 was labelled with iodoacetamido-tetramethyl-rhodamine. Polarization of fluorescence of S1 was measured in solution (where it indicated the mobility of actin-bound S1) and in myofibrils (where it indicated orientation of probes) to check whether the anisotropy of S1 labelled at different positions depended on the molar ratio S1:actin. In solution, when increasing amounts of actin were added to a fixed amount of labelled S1 (i.e. when myosin heads were initially in excess over actin), anisotropy saturated at 1 mol of S1 per 1 mol of actin. When increasing amounts of S1 were added to a fixed amount of F-actin (i.e. when actin was initially in excess over S1), the anisotropy saturated at 1 mol of S1 per 2 mols of actin. In myofibrils, orientation of S1 was different when S1 was added at nanomolar concentration (intrinsic actin was in excess over extrinsic S1) then when it was added at micromolar concentration (excess of S1 over actin). The fact that the anisotropy of S1 labelled at different positions depended on the molar ratio excluded the possibility that changes were confined to one part of the cross-bridge and supports our earlier proposal that the two rigor complexes which S1 can form with F-actin differ globally in conformation.

A single myosin head can be cross-linked to the N termini of two adjacent actin monomers

Myosin subfragment-1 (S1) can be cross-linked to two actin monomers by 1-ethyl-3-[3-(dimethylamino)-propyl]-carbodiimide only when F-actin is in excess over S1. Electron micrographs of the covalent actin2-S1 complex showed that S1 was cross-linked to two adjacent monomers of the same actin filament. Cross-linking experiments with pre-proteolyzed S1 derivatives in combination with a proteolytic dissection of the intact covalent actin2-S1 adduct (m = 265 kDa), revealed that two N-terminal segments of actin (residues 1-28) were covalently attached to a single S1 molecule. One was cross-linked to either the 20-kDa or the 50-kDa heavy chain fragments of S1, and the other only to the 50-kDa region. The doubly cross-linked product was formed under physiological ionic strength with S1 or with reconstituted myosin filaments, regardless of the presence of ADP or the regulatory proteins, tropomyosin and troponin. Finally, we found that this cross-linking could also take place within myofibrils in the rigor state. These results demonstrate that under nonsaturating conditions, the actin-S1 interface encompasses a much larger region than that recently proposed for the nonphysiological, fully saturated actin filaments.

Orientation of actin filaments during motion in in vitro motility assay

Rhodamine-phalloidin was added to F-actin, and the orientation of transition dipoles of the dye was measured in single actin filaments by polarization of fluorescence. Rhodamine-phalloidin was well immobilized on the surface of actin, indicating that changes in orientation of the dye reported changes in orientation of actin monomers. In stationary filaments the dipoles were inclined at 49.3 degrees with respect to the filament axis. The disorganization of dipoles in stationary filaments was insignificant. When the filaments were made to translate, the average orientation of the dye did not change, but disorganization slightly increased. Disorganization increased significantly when filaments were free in solution. We concluded that, within the accuracy of our measurements (approximately 18%), actin monomers did not undergo major reorientations during motion, but that binding of myosin heads deformed the structure of filaments.

Structure of the 265-kilodalton complex formed upon EDC cross-linking of subfragment 1 to F-actin

The conventional model of force generation in muscle requires the presence of at least two different contact areas between the myosin head (S1) and the actin filament. It has been found that S1 has two sites available for carbodiimide cross-linking, but it is generally believed that the myosin head can be cross-linked to only one actin through either site. We provide here, for the first time, evidence that one S1 can be cross-linked to two separate actin molecules. The covalent complex of one S1 with two actins was found to have an apparent molecular mass of 265 kDa. The formation of the 265-kDa acto-S1 complex was strongly dependent on the ratio of S1 to actin. Limited tryptic digestion converted the 265-kDa product into the 240-kDa complex by releasing a 27-kDa N-terminal S1 fragment. Limited subtilisin digestion of the 265-kDa covalent acto-S1 complex yielded 29-, 93-, and 66-kDa peptides which corresponded to the 29-kDa N-terminal domain of S1, actin-44-kDa (central domain of S1) and actin-22-kDa (C-terminal domain of S1) complexes, respectively. These peptides could be generated only if a single S1 has been cross-linked to two separate actins. The 265-kDa acto-S1 complex (S1:actin ratio = 0.5) had 60% of the ATPase activity of the 175-185-kDa acto-S1 complex (S1:actin ratio = 1).(ABSTRACT TRUNCATED AT 250 WORDS)