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.     

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 myosin filament. XIII. The sensitivity of LMM assembly to Mg.ATP

An LMM fragment (Mr 62,000) of myosin has been prepared which has aggregation properties that are sensitive to the presence of Mg.ATP. Aggregation of the LMM by reducing the ionic strength in the presence of 1 mM Mg.ATP produces non-periodic aggregates which gradually rearrange to paracrystals with a 43 nm axial repeat pattern. This fragment includes the C-terminal end of the myosin rod starting at residue 1376. Therefore, at least one of the Mg.ATP binding sites responsible for this effect is located somewhere along this region of the myosin rod. Although assembly of the rod fragment of myosin into paracrystals does not show sensitivity to Mg.ATP, assembly of intact myosin molecules to form filaments does show sensitivity to Mg.ATP. For myosin filaments, assembly initially gives a broad distribution around a mean length of 1.5 microns, which sharpens around the mean length with time. The rearrangement of the LMM rods and intact myosin molecules both induced by the presence of Mg.ATP are probably related. These findings highlight the complexity of the cooperative interactions between different portions of the myosin molecule that are involved in determining the assembly properties of the intact molecule.     

Myosin thick filaments from adult rabbit skeletal muscles

Myosin subfragment 1 (S1) forms dimers in the presence of Mg(2+) or MgADP or MgATP. The entire myosin molecule forms head-head dimers in the presence of MgATP. The angle between the two subunits in the S1 dimer is 95 degrees. Assuming that the length of the globular part of S1 is approximately 12 nm and that the S1/S2 joint (lever arm approximately 7 nm) is clearly bent, the cylinder tangent to this dimer should have a diameter of approximately 18 nm, close to the approximately 16-20 nm suggested by many studies for the diameter of thick filaments in situ. These conclusions led us to re-examine our previous model, according to which two heads from two opposite myosin molecules are inserted into the filament core and interact as dimers. We studied synthetic filaments by electron microscopy, enzyme activity assays, controlled digestion and filament-filament interaction analysis. Synthetic filaments formed by rapid dilution in the presence of 1 mM EDTA at room temperature ( approximately 22 degrees C) had all their myosin heads outside the backbone. These filaments are called superfilaments (SF). Synthetic filaments formed by slow dilution, in the presence of either 2 mM Mg(2+) or 0.5 mM MgATP and at low temperature ( approximately 0 degrees C) had one myosin head outside the backbone and one head inside. These filaments are called filaments (F). Synthetic filaments formed by slow dilution, in the presence of 4 mM MgATP at low temperature ( approximately 0 degrees C) had most of their heads inserted in the filament core. These filaments are called antifilaments (AF). These experimental results provide important new information about myosin synthetic filaments. In particular, we found that myosin heads were involved in filament assembly and that filament-filament interactions can occur via the external heads. Native filaments (NF) from rabbit psoas muscle were also studied by enzyme assays. Their structure depended on the age of the rabbit. NF from 4-month-old rabbits were three-stranded, i.e. six myosin heads per crown, two of which were inside the core and four outside. NF from 18-month-old rabbits were two-stranded (similar to F).     

Direct observation of molecular motility by light microscopy

We used video-fluorescence microscopy to directly observe the sliding movement of single fluorescently labeled actin filaments along myosin fixed on a glass surface. Single actin filaments labeled with phalloidin-tetramethyl-rhodamine, which stabilizes the filament structure of actin, could be seen very clearly and continuously for at least 60 min in 02-free solution, and the sensitivity was high enough to see very short actin filaments less than 40 nm long that contained less than eight dye molecules. The actin filaments were observed to move along double-headed and, similarly, single-headed myosin filaments on which the density of the heads varied widely in the presence of ATP, showing that the cooperative interaction between the two heads of the myosin molecule is not essential to produce the sliding movement. The velocity of actin filament independent of filament length (greater than 1 micron) was almost unchanged until the density of myosin heads along the thick filament was decreased from six heads/14.3 nm to 1 head/34 nm. This result suggests that five to ten heads are sufficient to support the maximum sliding velocity of actin filaments (5 micron/s) under unloaded conditions. In order for five to ten myosin heads to achieve the observed maximum velocity, the sliding distance of actin filaments during one ATP cycle must be more than 60 nm.     

Role of the regulatory light chains in skeletal muscle actomyosin ATPase and in minifilament formation

Incubation of myosin with myopathic hamster protease results in substantial (more than 80%) removal of light chain 2 (LC2) with limited breakdown of the heavy chains. LC2-deficient myosin, purified by ion exchange chromatography, migrates as a single, monodisperse boundary in the analytical ultracentrifuge. The Ca2+- and EDTA-activated ATPases of LC2-deficient myosin are similar to those of the control and LC2-recombined myosins indicating that no denaturation occurred in its preparation. Double reciprocal plots for LC2-deficient, control, and LC2-recombined myosins reveal a biphasic behavior i.e. at actin concentrations above 11 microM, there is a sharp break in the 1/V versus 1/[actin] plots for all samples. The Vm values for LC2-deficient myosin are 50% lower (at low actin, Vm = 3.0 s-1, and at high actin, Vm = 4.2 s-1) than those for control myosin (Vm = 5.3 s-1 at low actin and 8.3 s-1 at high actin). Readdition of LC2 to LC2-deficient myosin restores the actin-activated ATPase to control levels. Electron microscopy of shadow cast preparations reveals a subtle difference between LC2-deficient myosin, and control or recombined myosin. In control and recombined myosins, S1 heads appear "pear"-shaped, whereas in LC2-deficient myosin, the S1 heads are rounder and display a "thinning" of mass in the "neck" region, suggesting that LC2 binds at the S1/S2 junction. Furthermore, removal of LC2 apparently influences the assembly of myosin into minifilaments, as revealed to a certain degree, by an increase in the width of the bare zone, accompanied by a decrease in the stability of these minifilaments.     

Substructure and accessory proteins in scallop myosin filaments

Native myosin filaments from scallop striated muscle fray into subfilaments of approximately 100-A diameter when exposed to solutions of low ionic strength. The number of subfilaments appears to be five to seven (close to the sevenfold rotational symmetry of the native filament), and the subfilaments probably coil around one another. Synthetic filaments assembled from purified scallop myosin at roughly physiological ionic strength have diameters similar to those of native filaments, but are much longer. They too can be frayed into subfilaments at low ionic strength. Synthetic filaments share what may be an important regulatory property with native filaments: an order-disorder transition in the helical arrangement of myosin cross-bridges that is induced on activation by calcium, removal of nucleotide, or modification of a myosin head sulfhydryl. Some native filaments from scallop striated muscle carry short "end filaments" protruding from their tips, comparable to the structures associated with vertebrate striated muscle myosin filaments. Gell electrophoresis of scallop muscle homogenates reveals the presence of high molecular weight proteins that may include the invertebrate counterpart of titin, a component of the vertebrate end filament. Although the myosin molecule itself may contain much of the information required to direct its assembly, other factors acting in vivo, including interactions with accessory proteins, probably contribute to the assembly of a precisely defined thick filament during myofibrillogenesis.     

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.     

Enhancement of actin-activated myosin ATPase by an 84K Mr actin-binding protein in vertebrate smooth muscle

A Ca2+-dependent actin-severing 84K Mr protein prepared from bovine aorta caused four-fold activation of smooth muscle actin-activated myosin ATPase at a 1/10(2) molar ratio to actin in the presence of tropomyosin and light chain kinase-calmodulin in a Ca2+-dependent manner, while it inhibited it markedly at a 1/5 molar ratio. Purified actin-tropomyosin filaments under the experimental ATPase conditions were distributed in a range of more than 10 micron in length and the addition of the 84K Mr protein changed the filament length to around 1 micron at a 1/10(2) molar ratio to actin or less than 50 nm at a 1/5 molar ratio in the presence of Ca2+. However, the apparent length of actin filaments alone does not appear to be responsible for the activation of ATPase activity, since in the absence of tropomyosin, the ATPase activation was much less in spite of actin filament length changes. These results indicate the possibility that the 84K Mr protein plays an important role with tropomyosin in at least in vitro smooth muscle actin-myosin interaction.     

A nucleation--elongation mechanism for the self-assembly of side polar sheets of smooth muscle myosin.

Self-assembled filaments of smooth muscle myosin were observed by low dose electron microscopy to be flat side-polar sheets, in which the component molecules appeared straight and close-packed. Fraying experiments released small oligomers, in which molecules were staggered in parallel by about +/- 14 nm relative to two immediate neighbours, and were bound also to an antiparallel partner via a approximately 14 nm overlap at the very tip of the tail. We suggest a filament model which preserves these packing relationships. Adding stoichiometric amounts of MgATP to the filaments caused them to disassemble completely by progressive loss of material from their ends, at a limiting rate equivalent to about 2 monomers per second per end in physiological saline. The rate of the competing association reaction varied linearly with the monomer concentration, as determined in pressure-jump experiments. This suggests that myosin monomers, rather than dimers or higher oligomers, are the building blocks of these filaments. Shearing and annealing of assembled filaments appeared negligible on a time scale of a few hours. In consequence, filament number and filament length were dependent on the rate at which monomers were supplied to the assembly reaction, and on the number of filaments already present at the start of the assembly reaction.     

Distribution of myosin and relationship to actin organization in cortical and subcortical areas of antibody-labelled, quick-frozen, deep-etched fibroblast cytoskeletons

In this study I describe the ultrastructural distribution of myosin in cortical and subcortical areas of antibody-labelled, quick-frozen fibroblasts. In many cells myosin was present in small variably spaced and sized (0.23-0.39 micron long), nonaligned patches, while in other cells much larger periodically spaced patches of more uniform length (0.27 micron) were found. In all regions of the cytoskeleton myosin was found, primarily on linear bundles of actin filaments running parallel to the cell's long axis. Myosin was absent from single actin filaments, actin filaments perpendicular to actin bundles aligned with the cell's long axis, and actin filaments, such as geodome vertices and parts of the cortex, which had a complex interwoven appearance. These data indicate that in motile non-muscle cells myosin exerts force only in a unidirectional manner. Recognisable myosin filaments were never observed even in cells incubated either in N-ethylmaleimide or sodium azide. The presence of myosin in, and almost to the very edge of, the cortex suggests that the cellular control of actomyosin based movement is direct and over short-range distances. Large numbers of small cross-linking filaments were found in association with cortical and subcortical actin. Their relationship to myosin and overall actin geometry is discussed.     

Sequential assembly of collagen revealed by atomic force microscopy.

Most polymers which comprise biological filaments assemble by two mechanisms: nucleation and elongation or a sequential, stepwise process involving a hierarchy of intermediate species. We report the application of atomic force microscopy (AFM) to the study of the early events in the sequential or stepwise mode of assembly of a macromolecular filament. Collagen monomers were assembled in vitro and the early structural intermediates of the assembly process were examined by AFM and correlated with turbidimetric alterations in the assembly mixture. The assembly of collagen involved a sequence of distinctive filamentous species which increased in both diameter and length over the time course of assembly. The first discrete population of collagen oligomers were 1-2 nm in diameter (300-500 nm in length); at later time points, filaments approximately 2-6 nm in diameter (> 10 microns in length) many with a conspicuous approximately 67-nm axial period were observed. Occasional mature collagen fibrils with a approximately 67-nm axial repeat were found late in the course of assembly. Our results are consistent with initial end-to-end axial association of monomers to form oligomers followed by lateral association into higher-order filaments. On this basis, there appears to be at least two distinctive types of structural interactions (axial and lateral) which are operative at different levels in the assembly hierarchy of collagen.     

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.     

Effects of actin filament cross-linking and filament length on actin- myosin interaction

We have used two actin-binding proteins of the intestinal brush border, TW 260/240 and villin, to examine the effects of filament cross-linking and filament length on myosin-actin interactions. TW 260/240 is a nonerythroid spectrin that is a potent cross-linker of actin filaments. In the presence of this cross-linker we observed a concentration- dependent enhancement of skeletal muscle actomyosin ATPase activity (150-560% of control; maximum enhancement at a 1:70-80 TW 260/240:actin molar ratio). TW 260/240 did not cause a similar enhancement of either acto-heavy meromyosin (HMM) ATPase or acto-myosin subfragment-one (S1) ATPase. Villin, a Ca2+-dependent filament capping and severing protein of the intestinal microvillus, was used to generate populations of actin filaments of various lengths from less than 20 nm to 2.0 microns; (villin:actin ratios of 1:2 to 1:4,000). The effect of filament length on actomyosin ATPase was biphasic. At villin:actin molar ratios of 1:2- 25 actin-activated myosin ATPase activity was inhibited to 20-80% of control values, with maximum inhibition observed at the highest villin:actin ratio. The ATPase activities of acto-HMM and acto-S1 were also inhibited at these short filament lengths. At intermediate filament lengths generated at villin:actin ratios of 1:40-400 (average lengths 0.26-1.1 micron) an enhancement of actomyosin ATPase was observed (130-260% of controls), with a maximum enhancement at average filament lengths of 0.5 micron. The levels of actomyosin ATPase fell off to control values at low concentrations of villin where filament length distributions were almost those of controls. Unlike intact myosin, the actin-activated ATPase of neither HMM nor S1 showed an enhancement at these intermediate actin filament lengths.     

Reversible dissociation of dog cardiac myosin regulatory light chain 2 and its influence on ATP hydrolysis

The regulatory light chains of dog heart myosin were removed by digestion with myopathic hamster neutral protease. The heavy chains were also cleaved to an extent of 15%, but a homogeneous, rod-free LC2-deficient myosin was obtained by ion-exchange chromatography. A similar approach was used to prepare LC2-deficient heavy meromyosin. Neither Ca2+- nor K+-EDTA-activated ATPases were affected by LC2 removal. The Lineweaver-Burk plots for actin-activated ATPase in 25 mM KCl were biphasic giving a Vmax of 1.54 s-1 for control and LC2-recombined myosins and 1.08 s-1 for LC2-deficient myosin at low actin concentrations. At high actin concentrations, the Vmax for control and recombined myosins was 2.33 s-1 and 1.39 s-1 for LC2-deficient myosin. Increasing the KCl concentration in the reaction mixtures resulted in more linear plots without suppressing the 35-45% decrease in Vmax that accompanied LC2 removal. The results from assays with control and LC2-deficient heavy meromyosin performed in the absence of KCl, paralleled those obtained with myosin. The latter was also assayed in the presence of equimolar concentrations of C-protein in 50 mM KCl: C-protein induced a significant increase in the actin-activated ATPase of both control and LC2-recombined myosins, with no effect on LC2-deficient myosin. The Vmax for actin-activation in the presence of C-protein was 2.38 s-1, 0.83 s-1, and 1.71 s-1 for control, LC2-deficient, and recombined myosins, respectively. The enhancement of actin-activation in both the control and LC2-recombined myosins represents a possible role for C-protein in a LC2-mediated potentiation of actomyosin ATPase.     

Myosin filaments in cytoskeletons of Dictyostelium amoebae

Cytoskeletons were prepared from vegetative amoebae of Dictyostelium discoideum by extraction with Triton X-100. The cytoskeletons were suspended in buffers known to induce the assembly or disassembly of myosin filaments. The samples were fixed, and thin sections were examined by transmission electron microscopy. In both types of buffers, myosin-containing cytoskeletons exhibited a ring of densely staining proteinaceous material within the cortical filament matrix; this ring was not observed in myosin-free cytoskeletons. When myosin-containing cytoskeletons were placed in buffers that induced myosin polymerization, the ring appeared as an array of rodlike filaments approximately 13 nm wide and up to 0.5 micron in length--dimensions appropriate for myosin thick filaments. If ATP was added to cytoskeletons containing such filaments, the cytoskeletons contracted and the ring of filaments disappeared. ATP-induced contraction of cytoskeletons was also visualized by indirect immunofluorescence by using monoclonal antibodies to Dictyostelium myosin. All data were consistent with the identification of the protein ring seen by electron microscopy as cortical myosin. Its location and organization were appropriate for the production of cortical contraction through a sliding filament mechanism.     

Interaction of C-protein with myosin

The effect of C-protein on the assembly reaction of myosin was studied by flow birefringence, electron microscopy, and ultracentrifugation. Myosin filaments were formed by dilution to a lower ionic strength. Thinner filaments of 70-110 A in diameter were formed in the presence of C-protein. When dilution was effected by moderately slow dilution (dilution time of 0.5-2 min) or by stepwise dilution, C-protein favored the formation of longer filaments. When dilution was effected by even slower dilution (dilution time above 2 min), C-protein favored the formation of shorter filaments. Longer filaments formed by slow dilution incorporated more C-protein than shorter ones formed by faster dilution. Addition of C-protein to a solution of myosin filaments caused association of the filaments into longer filaments. The elongation effect was slower and stronger for longer filaments.     

Effects of light chain phosphorylation and skeletal myosin on the stability of non-muscle myosin filaments

The effect of light chain phosphorylation and the presence of skeletal muscle myosin on the stability of non-phosphorylated non-muscle myosin filaments was investigated. Purified skeletal, brush border and thymus myosins were assembled in vitro into hybrid filaments consisting of varying proportions of (1) non-muscle and skeletal myosins, or (2) phosphorylated and non-phosphorylated non-muscle myosins. The stability of these hetero- and homopolymers in the presence of MgATP was determined using sedimentation, gel electrophoresis and immunochemical techniques. In addition, the effect of a monoclonal antibody, binding to the tip of brush border myosin tail, on the assembly of the homo- and heteropolymers, was tested. Filamentous non-phosphorylated non-muscle myosin was disassembled by MgATP to the same extent whether in homo- or heteropolymers, indicating that skeletal myosin has no stabilising effect on the hybrid filaments. The presence of small amounts of phosphorylated non-muscle myosin was, however, found to prevent the complete disassembly by MgATP of non-phosphorylated non-muscle myosin filaments, indicating that light chain phosphorylation stabilizes co-operatively non-muscle myosin filaments. The monoclonal antibody prevented the assembly of brush border myosin into both homo- and heteropolymers, and its effect on the filaments was compared with that of MgATP.     

Under physiological conditions actin disassembles slowly from the nonpreferred end of an actin filament

Incubation of the isolated acrosomal bundles of Limulus sperm with skeletal muscle actin results in assembly of actin onto both ends of the bundles. Because of the taper of these cross-linked bundles of actin filaments, one can distinguish directly the preferred end for assembly from the nonpreferred end. Loss of growth with time from the nonpreferred end was directly assessed by electron microscopy and found to be dependent upon salt concentration. Under physiological conditions (100 mM KCl, 1 mM MgCl2) and excess ATP (0.5 mM), depolymerization of the newly assembled actin filaments at the nonpreferred end over an 8-h period was 0.024 micron/h. Thus, even after 8 h, 63% of the bundles retained significant growth on their nonpreferred ends, the average length being 0.21 micron +/- 0.04. However, in the presence of 1.2 mM CaCl2, disassembly of actin monomers from the nonpreferred end increased substantially. By 8 h, only 7% of the bundles retained any actin growth on the nonpreferred ends, and the depolymerization rate off the nonpreferred end was 0.087 micron/h. From these results we conclude that, in the absence of other cellular factors, disassembly of actin subunits from actin filaments (subunit exchange) is too slow to influence most of the motile events that occur in cells. We discuss how this relates to treadmilling.     

Giant mitochondria in the A cells of the pancreas of a lizard: Varanus niloticus

Pancreatic A cells of the lizard Varanus niloticus are characterized by the presence of two types of mitochondria: (a) normal, small mitochondria (about 0.4 X 1 micron), and (b) giant mitochondria, measuring up to 9 micron in length and 1 micron in diameter. Giant mitochondria show various shapes. Their matrix is filled with tubules, filaments, and dense granules. Transverse sections of tubules are polygonal in shape and about 20 nm in diameter. They are grouped in bundles. The filaments, about 9-10 nm in diameter, are arranged in parallel layers crossing each other at a 57 degree angle. In a closely related species, Varanus exanthematicus, pancreatic A cells do not show these peculiar features.