Fluorescent staining of microfilaments with heavy meromyosin labeled with N-(7-dimethylamino-4-methylcoumarinyl) maleimide

For fluorescent staining of microfilaments in cells, heavy meromyosin (HMM) or subfragment-1 (S-1) was labeled with a novel thiol-directed fluorescent dye, N-(7-dimethylamino-4-methylcoumarinyl) maleimide (DACM), instead of the usual dyes, such as fluorescein-isothiocyanate (FITC). DACM-labeled HMM or S-1 gave characteristic fluorescence patterns to a variety of cell types similar to those reported with the use of FITC-labeled HMM or S-1 or with immunofluorescence techniques using anti-actin antibody. The fluorescence of DACM was fairly photoresistant as compared with FITC, so that HMM or S-1 required only 1 mol of the dye per myosin head. Consequently, F-actin need not be used to preserve the actin binding activity of the myosin fragments when labeling with the dye.     

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.     

Substructure of the myosin molecule: IV. Interactions of myosin and its subfragments with adenosine triphosphate and F-actin

The enzymic activity of several single-headed subfragments of myosin (HMM S-1 and single-headed HMM) has been compared to the double-headed derivative of myosin (HMM) both in the presence and absence of aetin. Under the assay conditions of our experiments, we find that HMM hydrolyses ATP at approximately twice the rate of any single-headed species. These results suggest a relatively independent functional role for each of the two heads of the myosin molecule.An attempt has been made to determine the stoichiometry of association between subfragments and actin, either in the absence of nucleotide or during the hydrolysis of ATP. It was originally thought that a comparison of the maximum turnover rate of HMM at infinite concentrations of actin with the maximum rate at infinite concentrations of enzyme (but with a fixed amount of actin) would yield the combining ratio of actin to HMM. However, the considerable variation of ATP turnover rates with the conditions of the experiment has made it impossible to reach any firm conclusions regarding stoichiometry. A more direct approach to the question of stoichiometry is possible in the absence of ATP. By reacting varying amounts of F-actin with a given concentration of subfragment and centrifuging the resulting complex, it is possible to determine the unbound concentration of subfragment in the supernatant. These data provide sufficient information to construct a Scatchard plot and show that twice as many moles of actin are bound by HMM as by HMM S-1. Furthermore, the association constant of actin for HMM is several orders of magnitude higher than that for the single-headed species.In connection with the question of why myosin has two “heads”, we have examined the ability of single-headed molecules to undergo the phenomenon of “superprecipitation”. We find that single-headed myosin (the preparation of which was discussed in the preceding paper) is able to superprecipitate in much the same manner as native myosin.We conclude from these studies that each head of the myosin molecule is able to function in a relatively independent fashion. These studies do not, of course, exclude the possibility of more subtle interactions between the heads of myosin which our techniques are not able to detect.     

Heavy meromyosin binds actin with negative cooperativity.

The association of fluorescently labeled heavy meromyosin (HMM) and F-actin was measured by time-resolved fluorescence depolarization. The effects of varying the protein concentrations, temperature, KCl concentration, and pH were determined. Measurements of HMM mobility supported a model of no interaction between the two heads in the absence of actin. Measurements of actin binding, when compared with results for myosin subfragment I, indicated that the two heads of HMM do not bind independently in the rigor complex. This could result from actin-transmitted negative cooperativity or from steric inhibition due to the structure of HMM. For HMM and actin in 0.15 7 kcl at 25 degrees C: Ka = 3.9 X 10(7) M-1, deltaHco' = 36 +/- 2 J M-1, deltaSco' = 0.26 +/- 0.02 kJ M-1 K-1; the slope of ln Ka vs. [KCl]1/2 = -3.88 and the pH of maximum association was 6.9.     

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”.     

Conformational change in actin filament induced by the interaction with heavy meromyosin: effects of pH, tropomyosin and deoxy-ATP.

Conformational changes in pure and tropomyosin-containing F-actin during interaction with heavy meromyosin in the absence and presence of deoxy-ATP, were studied by measurements of the changes in fluorescence intensity of e-ADP² incorporated into the F-actin instead of ADP. The actin filaments were found to be stabilized by tropomyosin and were more stable at pH 7 than at pH 8. The rigor binding of HMM to F-actin caused an increase in the fluorescence intensity. The increase with F-actin containing TM was higher than that with pure F-actin at each HMM concentration. A linear relation between the fluoresence change and moles of HMM per actin was found regardless of the presence of TM, with a maximum value of 0.5 moles of HMM per actin. In the presence of deoxy-ATP, (which is a substrate for acto-HMM but cannot bind to actin) no changes in fluorescence intensity of e-ADP bound to pure F-actin were observed. In the case of F-actin containing TM, the fluorescence intensity increased with increasing HMM concentration, although the light scattering intensity of the acto-HMM solutions indicated that almost all the HMM was dissociated from the F-actin. This suggests that the conformational change in F-actin-TM induced by the interaction with HMM in the presence of deoxy-ATP has a long lifetime which continues for some time even after the detachment of the HMM.     

Interaction of two heads of myosin with F-actin: binding of H-meromyosin with F-actin in the absence of nucleotide

The bindings of S-1 and the two heads of HMM with pyrene-labeled F-actin were studied using the change in light-scattering intensity or that in the fluorescence intensity of the pyrenyl group. At low ionic strength (50 mM KCl), both S-1 and HMM became bound tightly with F-actin (Kd less than 0.1 microM) and both heads of HMM became bound to F-actin. The affinities of S-1 and HMM for F-actin decreased with increasing KCl concentration. In 1 M KCl, the Kd values of S-1 and HMM for F-actin were 11 and 0.58 microM, respectively. Thus, HMM was bound to F-actin 19 times more tightly than S-1. We compared the extent of binding of HMM to F-actin measured by a centrifugation method with that measured by the fluorescence change of pyrenyl-group, and found that even in 1 M KCl, HMM became bound to F-actin with a two-headed attachment. We measured the kinetics of binding and dissociation of acto-S-1 and acto-HMM from the time course of the change in light-scattering intensity after mixing S-1 or HMM with F-actin at 1 M KCl and that after mixing 1 M KCl with acto-S-1 or acto-HMM formed at low ionic strength.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of F-actin upon the binding of ADP to myosin and its fragments.

The effect of F-actin upon the binding of ADP to rabbit skeletal muscle myosin, heavy meromyosin, and subfragment 1 was studied by equilibrium dialysis, ultracentrifuge transport, and light scattering techniques. Both myosin and H-meromyosin (HMM) bind a maximum of approximately 1.6 mol of ADP/mol of protein, while S-1 binds approximately 0.9 mol of ADP/mol of protein. The affinity for ADP of all three preparations was similar at a given ionic strength (approximately 10(6) M-1 at 0.05 M KCl) and decreased with increasing ionic strength. Under conditions similar to those used for the measurement of ADP binding, the binding sites of myosin, HMM, and subfragment 1 (S-1) are saturated with actin at molar ratios of 2, 2, and 1 mol of actin monomer/mol of protein, respectively, as determined by light scattering, ultracentrifuge transport, and in the case of myosin by ATPase measurements. F-actin was found to inhibit ADP binding, but even at an actin concentration at least twice that required for saturation of myosin, HMM, or S-1, significant ADP binding remained. This ADP binding was inhibited by 10(-4) M pyrophosphate. The observations are consistent with the formation of an actomyosin-ADP complex in which actin and ADP are bound to myosin at distinct but interacting sites.     

Orientation of the agarose gel matrix in pulsed electric fields.

The technique of transient electric birefringence was used to investigate the effect of pulsed electric fields on the orientation of the agarose gel matrix. Orientation of the gel was observed at all electric field strengths. Very slow, time-dependent effects were observed when pulses of 10-100 V/cm were applied to 1% gels for 0.5-2 seconds, indicating that domains of the matrix were being oriented by the electric field. The sign of the birefringence reversed when the direction of the applied electric field was reversed, indicating that the domains tend to orient in the perpendicular direction after field reversal. Theories of gel electrophoresis will need to incorporate the orientation of the matrix in order to provide a complete explanation of electrophoresis in agarose gels.     

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

Fluorescently labeled myosin heads (S1) were added to muscle fibers and myofibrils at various concentrations. The orientation of the absorption dipole of the dye with respect to the axis of F-actin was calculated from polarization of fluorescence which was measured by a novel method from video images of muscle. In this method light emitted from muscle was split by a birefringent crystal into two nonoverlapping images: the first image was created with light polarized in the direction parallel to muscle axis, and the second image was created with light polarized in the direction perpendicular to muscle axis. Images were recorded by high-sensitivity video camera and polarization was calculated from the relative intensity of both images. The method allows measurement of the fluorescence polarization from single myofibril irrigated with low concentrations of S1 labeled with dye. Orientation was also measured by fluorescence-detected linear dichroism. The orientation was different when muscle was irrigated with high concentration of S1 (molar ratio S1:actin in the I bands equal to 1) then when it was irrigated with low concentration of S1 (molar ratio S1:actin in the I bands equal to 0.32). The results support our earlier proposal that S1 could form two different rigor complexes with F-actin depending on the molar ratio of S1:actin.     

The dissociation constant of the actin-heavy meromyosin subfragment-1 complex.

We measured the binding of [14C]iodoacetamide labeled heavy meromyosin subfragment-1 (S-1) to F-actin by sedimenting the actin-S-1 complex and assaying the radioactivity remaining in the supernatant. The apparent dissociation constants (Kd) at 25 degrees, pH 7.0, were 0.01 to 0.04 muM at 0.027 and 0.08 ionic strengths and 0.07 to 0.14 muM at 0.14 ionic strength. Kd was not altered when the troponin-tropomyosin complex was bound on the actin, nor was it affected by free calcium concentration in the range 10(-4) to 10(-9) M. Measurements of the displacement of labeled S-1 from actin by native S-1 showed labeling had not altered Kd. In control experiments we found that at the low actin concentrations used (0.001-0.5 muM) not all of the actin sedimented and, furthermore, the data suggested that some of the S-1 in the supernatant was bound to supernatant actin. Our estimation of Kd, based on the assumption that all the supernatant S-1 was free, therefore resulted in an apparent Kd greater than the true Kd. We minimized the effect of the supernatant actin artefact by using only the data for high ratios of S-1 to actin, where no less than 75% of the actin sedimented; we estimate that the true Kd values could not be less than half the apparent Kd values.     

Conformational changes of actin induced by strong or weak myosin subfragment-1 binding

Movements of different areas of polypeptide chains within F-actin monomers induced by S1 or pPDM-S1 binding were studied by polarized fluorimetry. Thin filaments of ghost muscle were reconstructed by adding G-actin labeled with fluorescent probes attached alternatively to different sites of actin molecule. These sites were: Cys-374 labeled with 1,5-IAEDANS, TMRIA or 5-IAF; Lys-373 labeled with NBD-Cl; Lys-113 labeled with Alexa-488; Lys-61 labeled with FITC; Gln-41 labeled with DED and Cys-10 labeled with 1,5-IAEDANS, 5-IAF or fluorescein-maleimid. In addition, we used TRITC-, FITC-falloidin and e-ADP that were located, respectively, in filament groove and interdomain cleft. The data were analysed by model-dependent and model-independent methods (see appendixes). The orientation and mobility of fluorescent probes were significantly changed when actin and myosin interacted, depending on fluorophore location and binding site of actomyosin. Strong binding of S with actin leads to 1) a decrease in the orientation of oscillators of derivatives of falloidin (TRITC-falloidin, FITC-falloidin) and actin-bound nucleotide (e-ADP); 2) an increase in the orientation of dye oscillators located in the "front' surface of the small domain (where actin is viewed in the standard orientation with subdomains 1/2 and 3/4 oriented to the right and to the left, respectively); 3) a decrease in the angles of dye oscillators located on the "back" surface of subdomain-1. In contrast, a weak binding of S1 to actin induces the opposite effects in orientation of these probes. These data suggest that during the ATP hydrolysis cycle myosin heads induce a change in actin monomer (a tilt and twisting of its small domain). Presumably, these alterations in F-actin conformation play an important role in muscle contraction.     

Effects of tryptic digestion on myosin subfragment 1 and its actin-activated adenosinetriphosphatase

Myosin subfragment 1 (S-1) was fluorescently labeled at its rapidly reacting thiol ("SH1"). Short exposure to trypsin cuts the S-1 heavy chain into three still-associated fragments (20K, 50K, and 27K) [Balint, M., Wolf, L., Tarcsafalvi, A., Gergely, J., & Sreter, F.A. (1978) Arch. Biochem. Biophys. 190, 793-799] which bind F-actin to the same extent as does the uncut labeled S-1, as indicated by time-resolved fluorescence anisotropy decay (at 4 degrees C, pH 7, in 0.15 M KC1 and 5 mM MgC12, +/- 1 mM ADP). These results are thus in agreement with turbidity measurements on similar systems as reported by Mornet et al. [Mornet, D., Pantel, P., Audemard, E., & Kassab, R. (1979) Biochem. Biophys. Res. Commun. 89, 925-932]. The excited-state lifetime of the fluorescent label on cut S-1 is indistinguishable from that on normal S-1 (+/- ADP, +/- F-actin). F-Actin activation of MgATPase of cut S-1 is lower than that for normal S-1 at moderate concentrations of F-actin, as reported by Mornet et al. (1979). But as the F-actin concentration is increased, the MgATPase activities for cut S-1 approach those for uncut S-1. In terms of an eight-species steady-state kinetics scheme involving actin binding to free S-1, S-1 . ATP, S-1. ADP X P, and S-1 . ADP, actin affinity for the species S-1 . ADP X P was found to be 13.4 times greater for uncut S-1 than for cut S-1 [at 24 degrees C, pH 7.0, in 3 mM KC1, 1 mM ATP, 1 mM MgCl2, and 20 mM N-[tris(hydroxymethyl)methyl]-2-aminoethanesulfonic acid].     

A synthetic peptide of the N-terminus of actin interacts with myosin

Research reported from numerous laboratories suggested that the N-terminal region of actin contained one of the binding sites between actin and myosin. A synthetic peptide corresponding to residues 1-28 of skeletal actin was prepared by solid-phase peptide methodology. The formation of a complex between this peptide and myosin subfragment 1 (S1) was demonstrated by high-performance size-exclusion chromatography (pH 6.8). The actin peptide precipitated S1 at higher pH (7.4-8.2) but remained soluble when bound to heavy meromyosin (HMM) or S1 in the presence of F-actin. The actin peptide 1-28 bound to S1 and HMM and activated the ATPase activity in a manner similar to that of F-actin. These results demonstrate that the N-terminal region of actin, residues 1-28, contains a biologically important binding site for myosin.     

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.     

Electrophoresis of DNA in oriented agarose gels

Oriented agarose gels were prepared by applying an electric field to molten agarose while it was solidifying. Immediately afterwards, DNA samples were applied to the gel and electrophoresed in a constant unidirectional electric field. Regardless of whether the orienting field was applied parallel or perpendicular to the eventual direction of electrophoresis, the mobilities of linear and supercoiled DNA molecules were either faster (80% of the time) or slower (20% of the time) than observed in control, unoriented gels run simultaneously. The difference in mobility in the oriented gel (whether faster or slower) usually increased with increasing DNA molecular weight and increasing voltage applied to orient the agarose matrix. In perpendicularly oriented gels linear DNA fragments traveled in lanes skewed toward the side of the gel; supercoiled DNA molecules traveled in straight lanes. If the orienting voltage was applied parallel to the direction of electrophoresis, both linear and supercoiled DNA molecules migrated in straight lanes. These effects were observed in gels cast from different types of agarose, using various agarose concentrations and two different running buffers, and were observed both with and without ethidium bromide incorporated in the gel. Similar results were observed if the agarose was allowed to solidify first, and the orienting electric field was then applied to the gel for several hours before the DNA samples were added and electrophoresed. The results suggest that the agarose matrix can be oriented by electric fields applied to the gel before and probably during electrophoresis, and that orientation of the matrix affects the mobility and direction of migration of DNA molecules. The skewed lanes observed in the perpendicularly oriented gels suggest that pores or channels can be created in the matrix by application of an electric field. The oriented matrix becomes randomized with time, because DNA fragments in oriented and unoriented gels migrated in straight lanes with identical velocities 24 hours later.     

Skeletal muscle myosin subfragment-1 induces bundle formation by actin filaments

As is well known, the light scattering intensity of F-actin solutions increases immediately upon formation of the rigor complex with subfragment-1 (S-1). We have found that after the initial rise in scattering, there is a further gradual increase in scattering (we call it "super-opalescence"). Fluorescence and electron microscopic observations of acto-S-1 solutions showed that super-opalescence results from formation of actin filament bundles once S-1 binds to F-actin. The actin bundles possessed transverse stripes with a periodicity of about 350 A, which suggested that in the bundles actin filaments are arranged in parallel register. The rate of the initial process of bundle formation (i.e. side-by-side dimerization) could be approximately estimated by measuring the initial rate of super-opalescence (V0). V0 had a maximum (V0m) at a molar ratio of S-1 to actin of 1;6-1;7, regardless of the actin concentration, pH (6-8.5), Mg2+ concentration (up to 5 mM), or ionic strength (up to 0.3 M KC1). Lower pH, higher Mg2+ concentration, and higher ionic strength increased V0m; V0 was proportional to the square of the actin concentration, regardless of the solution conditions.     

A novel actin label: a fluorescent probe at glutamine-41 and its consequences

By peptide isolation and analysis, it has been shown that the dansyl fluorophore of dansylcadaverine [N-(5-aminopentyl)-5-(dimethylamino)naphthalene-1-sulfonamide] transfers to Gln-41 of actin from rabbit skeletal muscle when the reaction is catalyzed by guinea pig liver transglutaminase. As a function of time, the degree of labeling asymptotically approaches 1 mol of dansyl/l mol of actin. About 80-85% of the attached dansyl fluorophore was found at Gln-41. Such labeled G-actin polymerizes to the same extent as control actin, but the polymerization rate is greater and the critical concentration is less than for control actin. Complete polymerization is accompanied by a 1.5-2.0-fold increase in the emission intensity of the attached fluorophore. Labeled F-actin thus obtained activates myosin subfragment 1 (S-1) Mg2+-ATPase activity with the same Kapp, and to the same Vmax, as control actin; moreover, when such labeled F-actin is cross-linked to S-1 by 1-ethyl-3-[3-(dimethylamino)propyl]carbodiimide, the resulting superactivation of Mg2+-ATPase is the same as that attained with control actin. The attributes of this label thus make it an ideal reporter of events in the N-terminal 10-kilodalton region of actin, and a new topological point for proximity mapping.     

Inhibition of sliding movement of F-actin by crosslinking emphasizes the role of actin structure in the mechanism of motility

The effects of crosslinking of monomeric and polymeric actin with 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide (EDC), disuccinimidyl suberate (DSS) and glutaraldehyde on the interaction with heavy meromyosin (HMM) in solution and on the sliding movement on glass-attached HMM were examined. The Vmax values of actin-activated HMM ATPase decreased in the following order: intact actin = EDC F-actin greater than DSS actin greater than glutaraldehyde F-actin = glutaraldehyde G-actin greater than EDC G-actin. The affinity of actin for HMM in the presence of ATP decreased in the following order: DSS actin greater than glutaraldehyde F-actin = glutaraldehyde G-actin greater than intact actin greater than EDC F-actin greater than EDC G-actin. However, sliding movement was inhibited only in the case of glutaraldehyde-crosslinked F and G-actin and EDC-crosslinked G-actin. Interestingly, after copolymerization of "non-motile" glutaraldehyde or EDC-crosslinked monomers with "motile" monomers of intact actin sliding of the copolymers was observed and its rate was independent of the type of crosslinked monomer, i.e. of the manner of their interaction with HMM. These data strongly indicate that inhibition of the sliding of actin by crosslinking cannot be explained entirely by changes in the Vmax value or affinity for myosin heads. We conclude that movement is generated by interaction of myosin with segments of F-actin containing a number of intact monomers, and the mechanism of inhibition involves an effect of the crosslinkers on the structure of F-actin itself.