The myosin filament: XI. Filament assembly

The critical parameters required for the assembly of myosin filaments with a length distribution comparable to that for native myosin filaments were examined. It was found that: Two steps are required in the dilution of a myosin solution from 0.6M KCl to 0.15M KCl. In Step I the KCl concentration is reduced from 0.6 to 0.3M KCl and in Step II from 0.3 to 0.15M KCl. The rate of change of KCl required for Step I is different than that required for Step II. Increasing the total time of dilution in either Step I or II alone leads to an increase in length and a broadening of the length distribution. In Step I assembly of myosin molecules into nonsedimentable units occurs. These may be the basic units from which the filaments are assembled in Step II. Rapid dilution in Step I alone has no effect on the length distribution obtained at 0.15M KCl, but rapid dilution in Step II alone leads to short filaments (about 0.6 micron). Increasing the time of dilution in Step II alone to 3 hrs or 6 hrs gives a bimodal distribution in lengths with one peak at about 0.8 micron and the other at about 2.2 microns. The length distribution obtained at 0.15M KCl is not critically dependent on information contained in the portion of the filament previously assembled in Step II, but is critically dependent on the rate of change of KCl concentration during the assembly of the rest of the filament.     

The aggregation characteristics of column-purified rabbit skeletal myosin in the presence and absence of C-protein at pH 7.0.

The aggregation properties of column-purified rabbit skeletal myosin at pH 7.0 were investigated as functions of ionic strength, protein concentration, and time. Filaments prepared by dialysis exhibited the same average length and population distribution at 0.10 and 0.15 M KCl at protein concentrations greater than 0.10 mg/ml; similar results were obtained at .0.20 M KCl, although average filament length was approximately 0.5 micrometer shorter. Once formed, these length distributions remained virtually unchanged over an 8-d period. At and below 0.10 mg/ml, average filament length decreased as a function of protein concentration; filaments prepared from an initial concentration of 0.02 mg/ml were half the length of those prepared at 0.2 mg/ml. Filaments prepared by dilution exhibited a sharp increase in average length as the time-course increased up to 40 s, then altered only slightly over a further period of 4 min. Addition of C-protein in a molar ratio of 1-3.3 myosin molecules affected most of these results. Average filament length was affected neither by ionic strength nor by initial protein concentration down to 0.04 mg/ml or over an 8-d period. Filaments formed by dilution in the presence of C-protein exhibited a constant average length and hypersharp length distribution over variable time courses up to 7 min. It is possible that C-protein acts to stabilize the antiparallel intermediate during filamentogenesis, and may also affect subunit addition to this nucleus.     

Thermal transitions of myosin and its helical fragments. II. Solvent-induced variations in conformational stability.

The melting behavior of myosin and myosin rod has been studied over the pH range 5.4-7.0, in 0.5 M KCl. Both proteins exhibit almost identical T-m values, which increase from about 37 to 43 degrees as the pH is elevated through the range of study, T-m follows a sigmoidal dependence upon pH, and the inflection point occurs near pH 6.5. The influence of salt concentration on T-m was studied, by the variation of KCl from 0.15 to 2.92 M. With an increasing KCl concentration, both proteins exhibit similar, sigmoidal declines in T-m from about 44 to 34 degrees. Under all conditions of pH and ionic strength studied, melting is accompanied by an absorption of H+ by the protein. The concentration of the protein, the age of the preparation, and the presence of divalent metal ions fail to exert a significant effect on the T-m values obtained by our methods. The effects of salt concentration and pH on the thermal stability of myosin and myosin rod are discussed in terms of the location of the melting process within the myosin molecule. Myosin is shown to possess several of the requisite features for energy transduction via a proton-coupling mechanism. These features provide a framework for investigating some aspects of the molecular basis of muscle contraction within the context of the sliding filament model.     

Binding of connectin to myosin filaments

Binding of native connectin (2,100 kDa fragment of alpha-connectin) to myosin filaments was investigated using a sedimentation technique and densitometric estimations of the separated proteins. In the presence of 60 mM KCl and 5 mM phosphate buffer, pH 7.0, as much as 1.5 mol of connectin was bound to 1 mol of myosin, suggesting that some 150 connectin filaments bound to a single myosin filament of approximately 0.5 micron in length. This value was much more than the ratio found in muscle (12:1). It appeared that C protein did not affect the binding of connectin to myosin filaments.     

Adenosine triphosphatase activity and "thick filament" formation of chicken gizzard myosin in low salt media.

The ATPase activity of chicken gizzard myosin was studied by varying the KCl concentration in the reaction medium. The following was thus found: (a) A sharp depression of the activity occurred when the KCl concentration was reduced to less than 0.3 M, showing the minimum activity around 0.15 M KCl. (b) The activity depression was removed by addition of urea or bay papain-digestion, but not by addition of p-chloromercuribenzoate. (c) In the KCl concentration where the activity depression occurred, the ATPase reaction proceeded in two distinct phases; the activity was relatively high in the early phase of the reaction and declined into the later phase where the steady state reaction took place. (d) In the KCl concentrations higher than that particular concentration or in the presence of urea, the ATPase reaction proceeded in one phase. (e) The temperature dependence of the ATPase activity in the early phase was of an ordinary magnitude being approximately equal to that of the ATPase activity in 0.6 M KCl. In contrast, the temperature dependence of the activity in the later phase was unusually small. Gizzard myosin in various concentrations of KCl was also examined by measuring the turbidity and the light-scattering intensity, and by observation under an electron microscope. The following was thus found: (a) In the KCl concentration where the activity depression occurred, there was a stagnation in the turbidity decrease as the KCl concentration was gradually increased and also the formation of "thick filaments," each of which was approximately 0.6-0.9 micron in length and 20-30 nm in diameter with no central "bare zone." (b) Addition of ATP induced dissociation of the thick filaments, and the dissociation occurred during the early phase of the ATPaseeaction. (c) Moreover, the temperature dependence of the ATP-induced dissociation rate was approximately equal to that of the ATPase activity in the early phase. On the basis of the findings mentioned above, it is concluded that the activity depression results from the ATP-induced dissociation of myosin filaments. Moreover, since high concentrations of KCl or urea also caused dissociation of myosin filaments and yet did not produce the activity depression, it was strongly suggested that gizzard myosin in the ATP-dissociated form must be different from that in the urea- or KCl-dissociated form, probably in the physical state of some myosin aggregates which were not detectable by the physical methods we used. As a side-observation, gizzard myosin filaments formed in the presence of ADP were found to be unusually long (longer than 2 micron), and they looked very similar to the particular filaments of skeletal myosin that were reported, by Moos, to be formed in the absence of the C protein.     

Expression in Escherichia coli of a functional Dictyostelium myosin tail fragment

The amino acid sequence of the myosin tail determines the specific manner in which myosin molecules are packed into the myosin filament, but the details of the molecular interactions are not known. Expression of genetically engineered myosin tail fragments would enable a study of the sequences important for myosin filament formation and its regulation. We report here the expression in Escherichia coli of a 1.5- kb fragment of the Dictyostelium myosin heavy chain gene coding for a 58-kD fragment of the myosin tail. The expressed protein (DdLMM-58) was purified to homogeneity from the soluble fraction of E. coli extracts. The expressed protein was found to be functional by the following criteria: (a) it appears in the electron microscope as a 74-nm-long rod, the predicted length for an alpha-helical coiled coil of 500 amino acids; (b) it assembles into filamentous structures that show the typical axial periodicity of 14 nm found in muscle myosin native filaments; (c) its assembly into filaments shows the same ionic strength dependence as Dictyostelium myosin; (d) it serves as a substrate for the Dictyostelium myosin heavy chain kinase which phosphorylates myosin in response to chemotactic signaling; (e) in its phosphorylated form it has the same phosphoamino acids and similar phosphopeptide maps to those of phosphorylated Dictyostelium myosin heavy chain; (f) it competes with myosin for the heavy chain kinase. Thus, all the information required for filament formation and phosphorylation is contained within this expressed protein.     

Structure transition in myosin association with the change of concentration: solubility equilibrium under specified KCl and pH condition

We observed, for the first time, the elementary process for the ordered self-assembly formation of myosin in solution. It was realized exclusively under the specific condition of 200 mM KCl, 5 mM phosphate buffer, pH 7.08, at 15-20 degrees C, which is called the transition-generating condition (TGC). Described more in detail: pure myosin extracted from rabbit skeletal muscle exhibited the structural transition in its association form only when the myosin concentration c was changed under TGC. The myosin solubility was saturated in both edges of the total myosin concentration c > 10.0 mg/mL (solubility region II) and c < or = 0.25 mg/mL (solubility region I). In the intermediate region, the association structure of myosin changed stepwise with decreasing c. The steps were classified into four regions: region I (c < or = 0.25 mg/mL), II (0.25 < or = c < or = 0.50 mg/mL), III (0.50 < or = c < or = 5.0 mg/mL), and IV (c > 5.0 mg/mL). In each region except II, the plot of the relative soluble myosin concentration c(aq)/c against c(-1) gave a straight line of different slopes, certifying that myosin constructs self-assemblies by the closed association mechanism and that the self-assembly takes dual structures in each region. In region II, a drastic transition occurred in the self-assembled dual structures. Here, a highly associated (insoluble) giant assembly would break into soluble assemblies composed of several myosin molecules. The solubility region I originates a driving force for this structural transition. The basic binding unit of the self-assembly would be a parallel myosin-dimer constructed by the intermolecular axial staggers of 14.3 and 43 nm, as is observed by X-ray diffraction for the thick filament assembly or light meromyosin paracrystals. Myosin could take a single rod-like chain form only in an extremely low concentration region of c < or = c(aq,0) (= 0.053 mg/mL). The association behavior revealed in the present study suggests strongly that the complementary charge cluster and its electrostatic interaction between parallel myosin rods play a crucial role for the ordered self-assembly formation and that the specific electrostatic atmosphere of the solution under TGC is essential to the association mechanism in skeletal muscle myosin, or the thick filament formation of the mammals.     

Effect of heavy chain phosphorylation on the polymerization and structure of Dictyostelium myosin filaments

In Dictyostelium amebas, myosin appears to be organized into filaments that relocalize during cell division and in response to stimulation by cAMP. To better understand the regulation of myosin assembly, we have studied the polymerization properties of purified Dictyostelium myosin. In 150 mM KCl, the myosin remained in the supernate following centrifugation at 100,000 g. Rotary shadowing showed that this soluble myosin was monomeric and that approximately 80% of the molecules had a single bend 98 nm from the head-tail junction. In very low concentrations of KCl (less than 10 mM) the Dictyostelium myosin was also soluble at 100,000 g. But rather than being monomeric, most of the molecules were associated into dimers or tetramers. At pH 7.5 in 50 mM KCl, dephosphorylated myosin polymerized into filaments whereas myosin phosphorylated to a level of 0.85 mol Pi/mol heavy chain failed to form filaments. The phosphorylated myosin could be induced to form filaments by lowering the pH or by increasing the magnesium concentration to 10 mM. The resulting filaments were bipolar, had blunt ends, and had a uniform length of approximately 0.43 micron. In contrast, filaments formed from fully dephosphorylated myosin were longer, had tapered ends, and aggregated to form very long, threadlike structures. The Dictyostelium myosin had a very low critical concentration for assembly of approximately 5 micrograms/ml, and this value did not appear to be affected by the level of heavy chain phosphorylation. The concentration of polymer at equilibrium, however, was significantly reduced, indicating that heavy chain phosphorylation inhibited the affinity of subunits for each other. Detailed assembly curves revealed that small changes in the concentration of KCl, magnesium, ATP, or H+ strongly influenced the degree of assembly. Thus, changes in both the intracellular milieu and the level of heavy chain phosphorylation may control the location and state of assembly of myosin in response to physiological stimuli.     

Cytoplasmic and plasma membrane adenosine triphosphatase of polymorphonuclear neutrophils: comparison of their enzymatic properties and attempt for a direct determination of myosin ATPase activity using polymorphonuclear neutrophil extract

Enzymatic properties of the ATPase of the plasma membrane and cytoplasmic myosin B from guinea-pig polymorphonuclear neutrophils were compared. In the plasma membrane, Mg2+- and Ca2+-activated ATPases showed the same dependence pattern on KCl concentration and pH, i.e., both ATPases increased with decreasing KCl concentration and with rising pH until pH 9.0. The maximum activation of Mg2+-ATPase was observed at 1 . 10(-3) M Mg2+. On the other hand, EDTA-activated ATPase activity was so low that no clear dependence curve was obtained. In myosin B, Mg2+-ATPase activity was below one-tenth that of the plasma membrane ATPase with the maximum activation at 1 . 10(-2) M Mg2+ and pH 9.0 EDTA- and Ca2+-activated ATPase exhibited almost the same activity and the same KCl-dependence curve, i.e., both ATPases increased and increasing KCl concentration. With regard to pH-dependence, Ca2+-ATPase showed a U-shaped curve with the minimum at pH 7.0, wherease EDTA-activated ATPase indicated a bell-shaped curve with the maximum at pH 9.0. Based on the findings that the EDTA-activated ATPase activity was hardly detected in the plasma membrane but high in myosin B, the distribution of ATPase activity on subcellular fractions was studied and the results obtained that the myosin-ATPase activity could be directly measured using the polymorphonuclear neutrophil extract if the EDTA-activated ATPase activity was used as an enzymatic marker for myosin.     

The influence of pressure on the self-assembly of the thick filament from the myosin of vertebrate skeletal muscle.

The thick-filament-monomeric-myosin equilibrium was prepared from pure myosin at pH 8.1. The application of hydrostatic pressure to the self-assembly equilibrium resulted in a biphasic dissociation curve in which a linear decrease in turbidity (a measure of weight added to or lost from the filament) was followed by a transition to a second pressure-insensitive phase. The first phase represents the effect of hydrostatic pressure on the growth or propagation phase of filament assembly. Here is was shown that hydrostatic pressure served to shorten the filaments in concert towards the bare zone whilst maintaining the narrow length distribution seen at atmospheric pressure; the filament concentration remained constant during the experiment. A more precise definition of the delta-v for the assembly of monomer into filament was obtained than had hitherto been possible. The positioning of the bare zone at the centre of the filament seems to be one of the more obvious functions of the length-regulation mechanism. It also appears that all the basic structural elements of the native thick filament are potentially present in the pH 8.1 homopolymer; its length can be increased by physiological concentrations of MgCl2 and decreased by pressure. The monodisperse native filament could then be formed by a fine tuning of the basic length-regulation mechanism of the homopolymer by the co-polymerization of the other thick-filament proteins.     

Calorimetric studies of the ADP binding to myosin subfragment 1, heavy meromyosin, and to myosin filaments.

A calorimetric titration method was used to study the ADP binding to the chymotryptic subfragments of myosin, heavy meromyosin (HMM) and myosin subfragment 1 (S-1), and to myosin aggregated into filaments at low ionic strength. The binding constant (K) and heat of reaction (deltaH, kiloJoules (moles of ADP bound)-1) were determined. For HMM in 0.5 M KCl, 0.01 M MgCl2, 0.02 M Tris (pH 7.8) at 12 degrees, log K = 5.92 +/- 0.13 and deltaH = -70.9 +/- 3.6 kJ mol-1. These results agree with our previous findings for myosin in 0.5 M KCl at 12 degrees. When the KCl concentration was reduced to 0.1 M, the binding constant did not change significantly (log K = 6.09 +/- 0.06) but the binding was more exothermic (deltaH = -90.1 +/- 3.3 kJ mol-1). Similar results were obtained for myosin filaments in 0.1 M KCl and also for both the isoenzymes of S-1(S-1(A1) and S-1(A2) in 0.1 M KCl. In 0.5 M KCl, the binding curves suggest that about one ADP is bound per active site, but as 0.1 M KCl, the apparent stoichiometry drops from 0.7 to 0.75. The most probable explanation is that there is some site heterogeneity which is more evident at lower ionic strength.     

The bundling of actin with polyethylene glycol 8000 in the presence and absence of gelsolin.

Actin filament and bundle formation occur in the cytosol under conditions of very high total macromolecular concentration. In this study we have utilized the inert molecule polyethylene glycol 8000 (PEG) as a means of simulating crowded conditions in vitro. Column-purified Ca-actin was polymerized in the absence and presence of gelsolin (to regulate mean filament lengths between 50 and 5000 mers) and PEG (2-8%) using various concentrations of KCl and/or 2 mM divalent cations. Bundling was characterized by the scattered light intensity and mean diffusion coefficients obtained from dynamic light scattering, as well as by fluorescence and phase-contrast microscopy. The minimum concentration of KCl required for bundling decreases both with increasing concentration of PEG at a fixed mean filament length, and with decreasing filament length at a fixed concentration of PEG. In the absence of divalent cation, bundling is reversible on dilution, as determined by intensity levels, diffusion coefficients, and microscopy. However, with either 2 mM Mg2+ or Ca2+ added, bundling is irreversible under conditions of higher PEG concentrations or longer filaments, indicating that osmotic pressure effects cannot fully explain actin bundling with PEG. Weaker divalent cation-binding sites on actin as well as disulfide bonds appear to be involved in the irreversible bundling.     

Control of filament length by the regulatory light chains in skeletal and cardiac myosins

The possible role of the regulatory light chains (LC2) in in vitro assembly of rabbit skeletal and dog cardiac myosins was examined by formation of minifilaments and synthetic thick filaments. After LC2 was removed, the resulting myosin preparations exhibited little aggregation in 0.5 M KCl and 0.05 M potassium phosphate (pH 6.5). Minifilaments migrated as a single, hypersharp peak during sedimentation velocity, but electron microscopic analysis revealed a more destabilized structure for LC2-deficient minifilaments. Thick filaments were formed in buffers containing 0.15 M KCl and the following: 20 mM imidazole; 20 mM imidazole, 5 mM ATP; or 20 mM imidazole, 5 mM ATP, and 5 mM MgCl2, all at pH 7.0. Skeletal and cardiac myosin filaments formed in imidazole buffer alone were bipolar, tapered at both ends, and about 1.6 micron long. Removal of LC2 resulted in the formation of shorter thick filaments (1.2 micron long). This effect could be reversed by reassociation with LC2. Inclusion of ATP in the buffer disrupted the filament structure, resulting in irregular, short filaments (less than 0.6 micron); addition of both ATP and MgCl2 largely reversed the effects of ATP alone. In cardiac myosin filaments, the bare zone diameter increased from 16 nm as measured in control and LC2-recombined samples to 20 nm in LC2-deficient myosin assemblies. These results implicate LC2 in an active role in controlling synthetic thick filament length in both skeletal and cardiac muscles.     

Human platelet myosin. II. In vitro assembly and structure of myosin filaments

We have used electron microscopy and solubility measurements to investigate the assembly and structure of purified human platelet myosin and myosin rod into filaments. In buffers with ionic strengths of less than 0.3 M, platelet myosin forms filaments which are remarkable for their small size, being only 320 nm long and 10-11 nm wide in the center of the bare zone. The dimensions of these filaments are not affected greatly by variation of the pH between 7 and 8, variation of the ionic strength between 0.05 and 0.2 M, the presence or absence of 1 mM Mg++ or ATP, or variation of the myosin concentration between 0.05 and 0.7 mg/ml. In 1 mM Ca++ and at pH 6.5 the filaments grow slightly larger. More than 90% of purified platelet myosin molecules assemble into filaments in 0.1 M KC1 at pH 7. Purified preparations of the tail fragment of platelet myosin also form filaments. These filaments are slightly larger than myosin filaments formed under the same conditions, indicating that the size of the myosin filaments may be influenced by some interaction between the head and tail portions of myosin molecules. Calculations based on the size and shape of the myosin filaments, the dimensions of the myosin molecule and analysis of the bare zone reveal that the synthetic platelet myosin filaments consists of 28 myosin molecules arranged in a bipolar array with the heads of two myosin molecules projecting from the backbone of the filament at 14-15 nm intervals. The heads appear to be loosely attached to the backbone by a flexible portion of the myosin tail. Given the concentration of myosin in platelets and the number of myosin molecules per filament, very few of these thin myosin filaments should be present in a thin section of a platelet, even if all of the myosin molecules are aggregated into filaments.     

Optical depolarization changes in single, skinned muscle fibers. Evidence for cross-bridge involvement.

Optical ellipsometry studies of single, skinned muscle fibers conducted on the diffraction orders have yielded spectra that are sensitive to the state of the fiber. The linearly polarized light field vector becomes elliptically polarized as it passes through the fiber and may be collected at the diffraction orders. Fibers that have been subjected to extraction of myosin (0.6 M KCl) retain a weak diffraction pattern and exhibit a substantially decreased depolarization of incident linearly polarized light. A significant decrease in polarization is seen in skinned fibers that are subject to an increase in pH from 7.0 to 8.0. This increase in pH results in a decrease of approximately 30% in the depolarization angle of single fibers. The major decrease in depolarization angle that we observe at pH 8.0 is consistent with the notion that as cross-bridges move out from the shaft of the thick filament, their ability to cause depolarization of the incident linearly polarized light decreases. This interpretation is also consistent with the work of Ueno and Harrington where the decrease in the ability to cross-link S-1 and S-2 to the thick filament at pH 8.2 suggests cross-bridge movement away from the thick filament. A large decrease in birefringence, seen after treatment of skinned fibers with alpha-chymotrypsin, appears to be related to the breakdown of myosin into rod, S-1, heavy meromyosin, and light meromyosin.     

Segregated assembly of muscle myosin expressed in nonmuscle cells.

Skeletal muscle myosin cDNAs were expressed in a simian kidney cell line (COS) and a mouse myogenic cell line to investigate the mechanisms controlling early stages of myosin filament assembly. An embryonic chicken muscle myosin heavy chain (MHC) cDNA was linked to constitutive promoters from adenovirus or SV40 and transiently expressed in COS cells. These cells accumulate hybrid myosin molecules composed of muscle MHCs and endogenous, nonmuscle, myosin light chains. The muscle myosin is found associated with a Triton insoluble fraction from extracts of the COS cells by immunoprecipitation and is detected in 2.4 +/- 0.8-micron-long filamentous structures distributed throughout the cytoplasm by immunofluorescence microscopy. These structures are shown by immunoelectron microscopy to correspond to loosely organized bundles of 12-16-nm-diameter myosin filaments. The muscle and nonmuscle MHCs are segregated in the transfected cells; the endogenous nonmuscle myosin displays a normal distribution pattern along stress fibers and does not colocalize with the muscle myosin filament bundles. A similar assembly pattern and distribution are observed for expression of the muscle MHC in a myogenic cell line. The myosin assembles into filament bundles, 1.5 +/- 0.6 micron in length, that are distributed throughout the cytoplasm of the undifferentiated myoblasts and segregated from the endogenous nonmuscle myosin. In both cell lines, formation of the myosin filament bundles is dependent on the accumulation of the protein. In contrast to these results, the expression of a truncated MHC that lacks much of the rod domain produces an assembly deficient molecule. The truncated MHC is diffusely distributed throughout the cytoplasm and not associated with cellular stress fibers. These results establish that the information necessary for the segregation of myosin isotypes into distinct cellular structures is contained within the primary structure of the MHC and that other factors are not required to establish this distribution.     

Interactions between actin, myosin, and an actin-binding protein from rabbit alveolar macrophages. Alveolar macrophage myosin Mg-2+-adenosine triphosphatase requires a cofactor for activation by actin.

The interactions were analyzed between actin, myosin, and a recently discovered high molecular weight actin-binding protein (Hartwig, J. H., and Stossel, T. P. (1975) J. Biol Chem.250,5696-5705) of rabbit alveolar macrophages. Purified rabbit alveolar macrophage or rabbit skeletal muscle F-actins did not activate the Mg2+ATPase activity of purified rabbit alveolar macrophage myosin unless an additional cofactor, partially purified from macrophage extracts, was added. The Mg2+ATPase activity of cofactor-activated macrophage actomyosin was as high as 0.6 mumol of Pi/mg of myosin protein/min at 37 degrees. The macrophage cofactor increased the Mg2+ATPase activity of rabbit skeletal muscle actomyosin, and calcium regulated the Mg2+ATPase activity of cofactor-activited muscle actomyosin in the presence of muscle troponins and tropomyosin. However, the Mg2+ATPase activity of macrophage actomyosin in the presence of the cofactor was inhibited by muscle control proteins, both in the presence and absence of calcium. The Mg2+ATPase activity of the macrophage actomyosin plus cofactor, whether assembled from purified components or studied in a complex collected from crude macrophage extracts, was not influenced by the presence of absence of calcium ions. Therefore, as described for Acanthamoeba castellanii myosin (Pollard, T. D., and Korn, E. D. (1973) J. Biol. Chem. 248, 4691-4697), rabbit alveolar macrophage myosin requires a cofactor for activation of its Mg2+ATPase activity by F-actin; and no evidence was found for participation of calcium ions in the regulation of this activity.In macrophage extracts containing 0.34 M sucrose, 0.5 mM ATP, and 0.05 M KCl at pH 7.0,the actin-binding protein bound F-actin into bundles with interconnecting bridges. Purified macrophage actin-binding protein in 0.1 M KCl at pH 7.0 also bound purified macrophage F-actin into filament bundles. Macrophage myosin bound to F-actin in the absence but not the presence of Mg2+ATP, but the actin-binding protein did not bind to macrophage myosin in either the presence or absence of Mg2+ATP.     

Effect of pH on the cross-bridge arrangement in synthetic myosin filaments.

Synthetic thick filaments were cross-linked with dimethyl suberimidate at various pH values over the range pH 6.8---8.3. The rate of cross-linking myosin heads to the thick filament surface decreases significantly over a narrow pH range (7.4--8.0) despite the fact that the rate of the chemical reaction (amidination of lysine side chains) shows a positive pH dependence. The fall in rate cannot be ascribed to dissociation of the filament during the cross-linking reaction since the sedimentation boundary of the cross-linked filament (pH 8.3) remains unaltered in the presence of high salt (0.5 M). The decreased rate of cross-linking is also not caused by a shift in reactivity of a small number of highly reactive lysine groups, since the time course of cross-linking (pH 7.2) is unaffected by preincubation with a monofunctional imidate ester. Our results suggest that the heads of the myosin molecules move away from the thick filament surface at alkaline pH but are held close to the surface at neutral pH.     

Assessment of the mechanical activity of cardiac isomyosins V1 and V3 by the in vitro motility assay with regulated thin filament

The dependences of thin filament sliding velocity on the calcium concentration in solution (pCa 5 to 8) for rabbit cardiac myosin isoforms V1 and V3 were determined in a set of experiments using an in vitro motility assay with a reconstructed thin filament. The constructed pCa-versus-velocity curves had a sigmoid shape. It was demonstrated that the sliding velocity of regulated thin filament at the saturating calcium concentration (pCa 5) did not differ from the actin sliding velocity for each isoform. The determined values of Hill’s cooperativity coefficient for isomyosins V1 and V3 were 1.04 and 0.75, respectively. It was demonstrated that isomyosin V3 was more sensitive to calcium as compared with isomyosin V1. Using the same assay, the dependence of thin filament sliding velocity on the concentration of the actin-binding protein α-actinin (analog of a force-velocity dependence) was determined at the saturating calcium concentration for each myosin isoform (V1 and V3). The results suggest that the calcium regulation of V1 and V3 contractile activity follows different mechanisms.     

Nucleated polymerization of actin from the membrane-associated ends of microvillar filaments in the intestinal brush border

We examined the nucleated polymerization of actin from the two ends of filaments that comprise the microvillus (MV) core in intestinal epithelial cells by electron microscopy. Three different in vitro preparations were used to nucleate the polymerization of muscle G- actin: (a) MV core fragments containing "barbed" and "pointed" filament ends exposed by shear during isolation, (b) isolated, membrane-intact brush borders, and (c) brush borders demembranated with Triton-X 100. It has been demonstrated that MV core fragments nucleate filament growth from both ends with a strong bias for one end. Here we identify the barbed end of the core fragment as the fast growing end by decoration with myosin subfragment one. Both cytochalasin B (CB) and Acanthamoeba capping protein block filament growth from the barbed but not the pointed end of MV core fragments. To examine actin assembly from the naturally occurring, membrane-associated ends of MV core filaments, isolated membrane-intact brush borders were used to nucleate the polymerization of G-actin. Addition of salt (75 mM KCl, 1 mM MgSO4) to brush borders preincubated briefly at low ionic strength with G- actin induced the formation of 0.2-0.4 micron "growth zones" at the tips of microvilli. The dense plaque at the tip of the MV core remains associated with the membrane and the presumed growing ends of the filaments. We also observed filament growth from the pointed ends of core filaments in the terminal web. We did not observe filament growth at the membrane-associated ends of core filaments when the latter were in the presence of 2 microM CB or if the low ionic strength incubation step was omitted. Addition of G-actin to demembranated brush borders, which retain the dense plaque on their MV tips, resulted in filament growth from both ends of the MV core. Again, 2 microM CB blocked filament growth from only the barbed (tip) end of the core. The dense plaque remained associated with the tip-end of the core in the presence of CB but usually was dislodged in control preparations where nucleated polymerization from the tip-end of the core occurred. Our results support the notion that microvillar assembly and changes in microvillar length could occur by actin monomer addition/loss at the barbed, membrane-associated ends of MV core filaments.