Unidirectional sliding of myosin filaments along the bundle of F-actin filaments spontaneously formed during superprecipitation

I reported previously (Higashi-Fujime, S., 1982, Cold Spring Harbor Symp. Quant. Biol., 46:69-75) that active movements of fibrils composed of F-actin and myosin filaments occurred after superprecipitation in the presence of ATP at low ionic strengths. When the concentration of MgCl2 in the medium used in the above experiment was raised to 20-26 mM, bundles of F-actin filaments, in addition to large precipitates, were formed spontaneously both during and after superprecipitation. Along these bundles, many myosin filaments were observed to slide unidirectionally and successively through the bundle, from one end to the other. The sliding of myosin filaments continued for approximately 1 h at room temperature at a mean rate of 6.0 micron/s, as long as ATP remained in the medium. By electron microscopy, it was found that most F-actin filaments decorated with heavy meromyosin pointed to the same direction in the bundle. Myosin filaments moved actively not only along the F-actin bundle but also in the medium. Such movement probably occurred along F-actin filaments that did not form the bundle but were dispersed in the medium, although dispersed F-actin filaments were not visible under the microscope. In this case, myosin filament could have moved in a reverse direction, changing from one F-actin filament to the other. These results suggested that the direction of movement of myosin filament, which has a bipolar structure and the potentiality to move in both directions, was determined by the polarity of F-actin filament in action.     

Formation of two-dimensional complexes of F-actin and crosslinking proteins on lipid monolayers: demonstration of unipolar alpha-actinin-F-actin crosslinking.

A method is described for forming two-dimensional (2-D) paracrystalline complexes of F-actin and bundling/gelation proteins on positively charged lipid monolayers. These arrays facilitate detailed structural studies of protein interactions with F-actin by eliminating superposition effects present in 3-D bundles. Bundles of F-actin have been produced using the glycolytic enzymes aldolase and glyceraldehyde-3-phosphate dehydrogenase, the cytoskeletal protein erythrocyte adducin as well as smooth muscle alpha-actinin from chicken gizzard. All of the 2-D bundles formed contain F-actin with a 13/6 helical structure. F-actin-aldolase bundles have an interfilament spacing of 12.6 nm and a superlattice arrangement of actin filaments that can be explained by expression of a local twofold axis in the neighborhood of the aldolase. Well ordered F-actin-alpha-actinin 2-D bundles have an interfilament spacing of 36 nm and contain crosslinks 33 nm in length angled approximately 25-35 degrees to the filament axis. Images and optical diffraction patterns of these bundles suggest that they consist of parallel, unipolar arrays of actin filaments. This observation is consistent with an actin crosslinking function at adhesion plaques where actin filaments are bound to the cell membrane with uniform polarity.     

Polarized actin bundles formed by human fascin-1: their sliding and disassembly on myosin II and myosin V in vitro

Fascin-1 is a putative bundling factor of actin filaments in the filopodia of neuronal growth cones. Here, we examined the structure of the actin bundle formed by human fascin-1 (actin/fascin bundle), and its mode of interaction with myosin in vitro. The distance between cross-linked filaments in the actin/bundle was 8-9 nm, and the bundle showed the transverse periodicity of 36 nm perpendicular to the bundle axis, which was confirmed by electron microscopy. Decoration of the actin/fascin bundle with heavy meromyosin revealed that the arrowheads of filaments in the bundle pointed in the same direction, indicating that the bundle has polarity. This result suggested that fascin-1 plays an essential role in polarity of actin bundles in filopodia. In the in vitro motility assay, actin/fascin bundles slid as fast as single actin filaments on myosin II and myosin V. When myosin was attached to the surface at high density, the actin/fascin bundle disassembled to single filaments at the pointed end of the bundle during sliding. These results suggest that myosins may drive filopodial actin bundles backward by interacting with actin filaments on the surface, and may induce disassembly of the bundle at the basal region of filopodia.     

Tetrahymena eukaryotic translation elongation factor 1A (eEF1A) bundles filamentous actin through dimer formation

Eukaryotic translation elongation factor 1A (eEF1A) is known to be a multifunctional protein. In Tetrahymena, eEF1A is localized to the division furrow and has the character to bundle filamentous actin (F-actin). eEF1A binds F-actin and the ratio of eEF1A and actin is approximately 1:1 (Kurasawa et al., 1996). In this study, we revealed that eEF1A itself exists as monomer and dimer, using gel filtration column chromatography. Next, eEF1A monomer and eEF1A dimer were separated using gel filtration column, and their interaction with F-actin was examined with cosedimentation assay and electron microscopy. In the absence of Ca2+/calmodulin (CaM), eEF1A dimer bundled F-actin and coprecipitated with F-actin at low-speed centrifugation, but eEF1A monomer did not. In the presence of Ca2+/CaM, eEF1A monomer increased, while dimer decreased. To examine that Ca2+/CaM alters eEF1A dimer into monomer and inhibits bundle formation of F-actin, Ca2+/CaM was added to F-actin bundles formed by eEF1A dimer. Ca2+/CaM separated eEF1A dimer to monomer, loosened F-actin bundles and then dispersed actin filaments. Simultaneously, Ca2+/CaM/ eEF1A monomer complexes were dissociated from actin filaments. Therefore, Ca2+/CaM reversibly regulates the F-actin bundling activity of eEF1A.     

Banding and polarity of actin filaments in interphase and cleaving cells

Heavy meromyosin (HMM) decoration of actin filaments was used to detect the polarity of microfilaments in interphase and cleaving rat kangaroo (PtK2) cells. Ethanol at -20 degrees C was used to make the cells permeable to HMM followed by tannic acid-glutaraldehyde fixation for electron microscopy. Uniform polarity of actin filaments was observed at cell junctions and central attachment plaques with the HMM arrowheads always pointing away from the junction or plaque. Stress fibers were banded in appearance with their component microfilaments exhibiting both parallel and antiparallel orientation with respect to one another. Identical banding of microfilament bundles was also seen in cleavage furrows with the same variation in filament polarity as found in stress fibers. Similarly banded fibers were not seen outside the cleavage furrow in mitotic cells. By the time that a mid-body was present, the actin filaments in the cleavage furrow were no longer in banded fibers. The alternating dark and light bands of both the stress fibers and cleavage furrow fibers are approximately equal in length, each measuring approximately 0.16 micrometer. Actin filaments were present in both bands, and individual decorated filaments could sometimes be traced through four band lengths. Undecorated filaments, 10 nm in diameter, could often be seen within the light bands. A model is proposed to explain the arrangement of filaments in stress fibers and cleavage furrows based on the striations observed with tannic acid and the polarity of the actin filaments.     

The 135-kDa actin-bundling protein from lily pollen tubes arranges F-actin into bundles with uniform polarity

 A plant 135-kDa actin-bundling protein (P-135-ABP) isolated from pollen tubes of Lilium longiflorum (Thunb.) binds stoichiometrically to F-actin filaments and bundles them in vitro (E. Yokota et al., 1998, Plant Physiol. 116: 1421–1429). To further understand the mechanism of actin-filament bundle formation by P-135-ABP, the polarity of each F-actin filament in bundles was examined using myosin subfragment 1 (S-1). Dissociation of F-actin filaments from bundles organized by P-135-ABP was induced by S-1. However, F-actin filaments that remained in a bundle and decorated by S-1 showed uniform polarity. These results indicate that P-135-ABP arranges F-actin filaments into bundles with uniform polarity and consequently plays a key role in the orientation of cytoplasmic streaming in pollen tubes. Received: 23 February 1999 / Accepted: 22 April 1999     

Intermonomer cross-linking of F-actin alters the dynamics of its interaction with H-meromyosin in the weak-binding state

Previous cross-linking studies [Kim E, Bobkova E, Hegyi G, Muhlrad A & Reisler E (2002) Biochemistry 41, 86-93] have shown that site-specific cross-linking among F-actin monomers inhibits the motion and force generation of actomyosin. However, it does not change the steady-state ATPase parameters of actomyosin. These apparently contradictory findings have been attributed to the uncoupling of force generation from other processes of actomyosin interaction as a consequence of reduced flexibility at the interface between actin subdomains-1 and -2. In this study, we use EPR spectroscopy to investigate the effects of cross-linking constituent monomers upon the molecular dynamics of the F-actin complex. We show that cross-linking reduces the rotational mobility of an attached probe. It is consistent with the filaments becoming more rigid. Addition of heavy meromyosin (HMM) to the cross-linked filaments further restricts the rotational mobility of the probe. The effect of HMM on the actin filaments is highly cooperative: even a 1 : 10 molar ratio of HMM to actin strongly restricts the dynamics of the filaments. More interesting results are obtained when nucleotides are also added. In the presence of HMM and ADP, similar strongly reduced mobility of the probe was found than in a rigor state. In the presence of adenosine 5'[betagamma-imido] triphosphate (AMPPNP), a nonhydrolyzable analogue of ATP, weak binding of HMM to either cross-linked or native F-actin increases probe mobility. By contrast, weak binding by the HMM/ADP/AlF4 complex has different effects upon the two systems. This protein-nucleotide complex increases probe mobility in native actin filaments, as does HMM + AMPPNP. However, its addition to cross-linked filaments leaves probe mobility as constrained as in the rigor state. These findings suggest that the dynamic change upon weak binding by HMM/ADP/AlF4 which is inhibited by cross-linking is essential to the proper mechanical behaviour of the filaments during movement.     

A 27,000-D core of the Dictyostelium 34,000-D protein retains Ca(2+)- regulated actin cross-linking but lacks bundling activity

Actin cross-linking proteins are important for formation of isotropic F- actin networks and anisotropic bundles of filaments in the cytoplasm of eucaryotic cells. A 34,000-D protein from the cellular slime mold Dictyostelium discoideum mediates formation of actin bundles in vitro, and is specifically incorporated into filopodia. The actin cross- linking activity of this protein is inhibited by the presence of micromolar calcium. A 27,000-D fragment obtained by digestion with alpha-chymotrypsin lacks the amino-terminal six amino acids and the carboxyl-terminal 7,000 D of the intact polypeptide. The 27,000-D fragment retains F-actin binding activity assessed by cosedimentation assays and by 125I-[F-actin] blot overlay technique, F-actin cross- linking activity as assessed by viscometry, and calcium binding activity. Ultrastructural analyses indicate that the 27,000-D fragment is deficient in the bundling activity characteristic of the intact 34,000-D protein. Actin filaments are aggregated into microdomains but not bundle in the presence of the 27,000-D fragment. A polarized light scattering assay was used to demonstrate that the 34,000-D protein increases the orientational correlation among F-actin filaments. The 27,000-D fragment does not increase the orientation of the actin filaments as assessed by this technique. A terminal segment(s) of the 34,000-D protein, lacking in the 27,000-D fragment, contributes significantly to the ability to cross-link actin filaments into bundles.     

In vivo identification of Tetrahymena actin probed by DMSO induction of nuclear bundles

We report the first successful identification of actin, an ubiquitous contractile protein, in Tetrahymena pyriformis (strain W). We employed dimethyl sulfoxide (DMSO) as a probe to induce the formation of actin bundles in the cell nucleus [1, 2] through disruption of cytoplasmic microfilament organization [3, 4]. The cells were incubated for 30 min at 22 °C in the inorganic medium of Prescott & James [5] containing 10% DMSO, and observed under a transmission electron microscope (TEM). Microfilarment bundles were formed in interphase macronuclei, and these microfilaments, approx. 6 nm in diameter, could be decorated by rabbit skeletal muscle heavy meromyosin (HMM) in the glycerinated model. In many cases, the bundles formed closely parallel to natively existing bundles of microtubules. Interestingly, these microtubules had prominent striation with 15–16 nm periodicity. SDS-polyacrylamide gel electrophoresis was designed to show the low actin content of Tetrahymena cells in comparison with that of Dictyostelium. Actin was suggested to comprise less than 1.7% of the total protein in Tetrahymena, whereas as much as 6% was actin in Dictyostelium cells. In assessing the physiological significance of the bundle formation, we further performed HMM and myosin subfragment-1 (S1)-binding studies to clarify the organization process and the polarity of the DMSO-induced nuclear actin filaments by using the tannic acid staining technique [6]. Randomly oriented short filaments appeared in the nucleus treated with 10% DMSO for 10 min. These filaments became elongated and associated with each other to form loose bundles in the following 10 min. With 30-min treatment, the filaments were organized and large bundles with single axes developed. With these well-developed bundles, the Student's t-test was performed on 172 pairs of neighboring filaments and the probability (p) of the deviation from random polarity was 0.08, suggesting that the filaments were organized in an anti-parallel manner. The results show that the DMSO induction of nuclear actin is a powerful tool to demonstrate the existence of cellular actin in vivo and to study the mechanism of microfilament organization in relation to cell physiological activities.     

Regeneration of actin bundles in Chara: polarized growth and orientation by endoplasmic flow

Strong irradiation of localized areas of the alga Chara produces chloroplast damage and extensive loss of the actin bundles responsible for cytoplasmic streaming. Immunofluorescence using a monoclonal antibody binding to the actin bundles has been used to follow their regrowth. Bundle regeneration is polarized so that new bundles develop from the ends of the actin bundles delivering endoplasm to the damaged area and not from bundles removing endoplasm. According to the previously established polarity of the actin filaments this growth is occurring from the "barbed" but not the "pointed" ends of the component filaments. The frequently irregular orientation of the regenerated bundles contrasts with the straight, parallel arrangement of the bundles before destruction. The arrangement of the regenerated bundles is suggested to depend on orientation by passive endoplasmic flow rather than a cortical template. As a result, bundles follow sweeping curves and can form a U-turn connecting oppositely polarized bundles normally separated by the neutral line. In addition to development in continuity with the free ends of pre-existing bundles, visualization of small, discrete fluorescent structures suggests that bundles can begin to form in isolation within the damaged areas. The results are discussed in terms of the polarized actin polymerisation seen in vitro, additional controls which may operate on bundle growth in vivo, and the ability of flow to orient F-actin. The relevance of the findings to normal cell ontogeny is assessed.     

Bundling of actin filaments by alpha-actinin depends on its molecular length

Cross-linking of actin filaments (F-actin) into bundles and networks was investigated with three different isoforms of the dumbbell-shaped alpha-actinin homodimer under identical reaction conditions. These were isolated from chicken gizzard smooth muscle, Acanthamoeba, and Dictyostelium, respectively. Examination in the electron microscope revealed that each isoform was able to cross-link F-actin into networks. In addition, F-actin bundles were obtained with chicken gizzard and Acanthamoeba alpha-actinin, but not Dictyostelium alpha-actinin under conditions where actin by itself polymerized into disperse filaments. This F-actin bundle formation critically depended on the proper molar ratio of alpha-actinin to actin, and hence F-actin bundles immediately disappeared when free alpha-actinin was withdrawn from the surrounding medium. The apparent dissociation constants (Kds) at half-saturation of the actin binding sites were 0.4 microM at 22 degrees C and 1.2 microM at 37 degrees C for chicken gizzard, and 2.7 microM at 22 degrees C for both Acanthamoeba and Dictyostelium alpha-actinin. Chicken gizzard and Dictyostelium alpha-actinin predominantly cross-linked actin filaments in an antiparallel fashion, whereas Acanthamoeba alpha-actinin cross-linked actin filaments preferentially in a parallel fashion. The average molecular length of free alpha-actinin was 37 nm for glycerol-sprayed/rotary metal-shadowed and 35 nm for negatively stained chicken gizzard; 46 and 44 nm, respectively, for Acanthamoeba; and 34 and 31 nm, respectively, for Dictyostelium alpha-actinin. In negatively stained preparations we also evaluated the average molecular length of alpha-actinin when bound to actin filaments: 36 nm for chicken gizzard and 35 nm for Acanthamoeba alpha-actinin, a molecular length roughly coinciding with the crossover repeat of the two-stranded F-actin helix (i.e., 36 nm), but only 28 nm for Dictyostelium alpha-actinin. Furthermore, the minimal spacing between cross-linking alpha-actinin molecules along actin filaments was close to 36 nm for both smooth muscle and Acanthamoeba alpha-actinin, but only 31 nm for Dictyostelium alpha-actinin. This observation suggests that the molecular length of the alpha-actinin homodimer may determine its spacing along the actin filament, and hence F-actin bundle formation may require "tight" (i.e., one molecule after the other) and "untwisted" (i.e., the long axis of the molecule being parallel to the actin filament axis) packing of alpha-actinin molecules along the actin filaments.     

Fluorescence properties and contraction characteristics of ANM (N-(1-anilinonaphthyl-4)maleimide)-labeled rabbit psoas muscle fibers

Fluorescence spectra of ANM-labeled, glycerinated rabbit psoas muscle fibers were recorded in relaxed, contracted, and rigor states. SDS polyacrylamide gel electrophoresis of the ANM-labeled muscle fibers indicated that proteins labeled with ANM were myosin heavy chain, C protein, and actin. In a relaxed state in the presence of ATP, myosin heavy chain was mainly labeled. During the transition from rigor to the relaxed or contracted state, there was a blue shift (about 5 nm) of the ANM emission spectrum. Similar experiments with FAM (N-(3-fluoranthyl)-maleimide)-labeled muscle fibers showed that these fluorescence changes were not artifacts due to the movement of muscle fibers. The fibers labeled in the ATP relaxing solution showed a marked decrease in both isometric force and unloaded shortening velocity (Vo), while in the fibers labeled in the rigor solution isometric tension was not markedly suppressed, though Vo decreased to the same extent as in the fibers labeled in the ATP relaxing solution. Fluorescence spectra of ANM-labeled HMM in different states were also measured. A fluorescence enhancement and a blue shift (about 5 nm) of the emission maximum were observed in HMM + MgATP or HMM + MgATP + F-actin in comparison with HMM + F-actin. These results suggest that the fluorescence spectra of the ANM-labeled muscle fibers reflect their conformational changes between the rigor state (in the absence of MgATP) and the relaxed or contracted state (in the presence of MgATP).     

Binding of actin filaments to connectin

The binding of actin filaments to connectin, a muscle elastic protein, was investigated by means of turbidity and sedimentation measurements and electron microscopy. In the presence of less than 0.12 M KCl at pH 7.0, actin filaments bound to connectin. Long actin filaments formed bundles. Short actin filaments also aggregated into irregular bundles or a meshwork, and were frequently attached perpendicularly to long bundles. The binding of F-actin to connectin was saturated at an equal weight ratio (molar ratio, 50 : 1), as determined by a cosedimentation assay. Larger amounts of sonicated short actin filaments appeared to bind to connectin than intact F-actin. Myosin S1-decorated actin filaments did not bind to connectin. The addition of S1 to connectin-induced actin bundles resulted in partial disaggregation. Thus, connectin does not appear to interfere with actin-myosin interactions, since myosin S1 binds to actin more strongly than connectin.     

Identification of Novel Graded Polarity Actin Filament Bundles in Locomoting Heart Fibroblasts: Implications for the Generation of Motile Force

We have determined the structural organization and dynamic behavior of actin filaments in entire primary locomoting heart fibroblasts by S1 decoration, serial section EM, and photoactivation of fluorescence. As expected, actin filaments in the lamellipodium of these cells have uniform polarity with barbed ends facing forward. In the lamella, cell body, and tail there are two observable types of actin filament organization. A less abundant type is located on the inner surface of the plasma membrane and is composed of short, overlapping actin bundles (0.25–2.5 μm) that repeatedly alternate in polarity from uniform barbed ends forward to uniform pointed ends forward. This type of organization is similar to the organization we show for actin filament bundles (stress fibers) in nonlocomoting cells (PtK2 cells) and to the known organization of muscle sarcomeres. The more abundant type of actin filament organization in locomoting heart fibroblasts is mostly ventrally located and is composed of long, overlapping bundles (average 13 μm, but can reach up to about 30 μm) which span the length of the cell. This more abundant type has a novel graded polarity organization. In each actin bundle, polarity gradually changes along the length of the bundle. Actual actin filament polarity at any given point in the bundle is determined by position in the cell; the closer to the front of the cell the more barbed ends of actin filaments face forward.

By photoactivation marking in locomoting heart fibroblasts, as expected in the lamellipodium, actin filaments flow rearward with respect to substrate. In the lamella, all marked and observed actin filaments remain stationary with respect to substrate as the fibroblast locomotes. In the cell body of locomoting fibroblasts there are two dynamic populations of actin filaments: one remains stationary and the other moves forward with respect to substrate at the rate of the cell body.

This is the first time that the structural organization and dynamics of actin filaments have been determined in an entire locomoting cell. The organization, dynamics, and relative abundance of graded polarity actin filament bundles have important implications for the generation of motile force during primary heart fibroblast locomotion.

     

Evaluation of mechanical parameters of the mechanochemically 'active state' of actin filaments on the basis of purely chemical data

Oosawa and his collaborators (cf. F. Oosawa, Biophys. Chem. 11 (1980) 443), employing various optical techniques, have shown that the flexibility of actin filaments increases upon interacting with the enzymatically active myosin fragments, particularly heavy meromyosin (HMM). It has been reported (S. Hitchock, L. Carlsson and U. Lindberg, Cell 7 (1976) 53) that HMM can accelerate the DNase 1-induced depolymerization of F-actin, provided MgATP is also present. Since, as we have demonstrated (cf. J. Borejdo myosin, is endowed with mechanochemical capability, we made an attempt to correlate the enhanced rate of depolymerization with the decrease in rigidity of the G-G bonds in F-actin. On the basis of the chemical kinetic data of Hitchcock et al. we could derive the approximate value of the HMM-MgATP-induced change in rigidity which is a mechanical molecular parameter. Since interaction between HMM or HMM subfragment-1 and F-actin in the presence of MgATP leads to the movement of the myosin heads along the actin filaments, it is argued that the enzymic behavior of this system should not be analyzed on the basis of simple, equilibrium, complex formation.     

Retrograde flow and myosin II activity within the leading cell edge deliver F-actin to the lamella to seed the formation of graded polarity actomyosin II filament bundles in migrating fibroblasts

In migrating fibroblasts actomyosin II bundles are graded polarity (GP) bundles, a distinct organization to stress fibers. GP bundles are important for powering cell migration, yet have an unknown mechanism of formation. Electron microscopy and the fate of photobleached marks show actin filaments undergoing retrograde flow in filopodia, and the lamellipodium are structurally and dynamically linked with stationary GP bundles within the lamella. An individual filopodium initially protrudes, but then becomes separated from the tip of the lamellipodium and seeds the formation of a new GP bundle within the lamella. In individual live cells expressing both GFP-myosin II and RFP-actin, myosin II puncta localize to the base of an individual filopodium an average 28 s before the filopodium seeds the formation of a new GP bundle. Associated myosin II is stationary with respect to the substratum in new GP bundles. Inhibition of myosin II motor activity in live cells blocks appearance of new GP bundles in the lamella, without inhibition of cell protrusion in the same timescale. We conclude retrograde F-actin flow and myosin II activity within the leading cell edge delivers F-actin to the lamella to seed the formation of new GP bundles.     

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.     

The two actin-binding regions on the myosin heads of cardiac muscle

In the presence of myosin S1 or myosin heads, actin filaments tend to form bundles. The biological meaning of the bundling of actin filaments has been unclear. In this study, we found that the cardiac myosin heads can form the bundles of actin filaments more rapidly than can skeletal S1, as monitored by light scattering and electron microscopy. Moreover, the actin bundles formed by cardiac S1 were found to be more stable against mechanical agitation. The distance between actin filaments in the bundles was approximately 20 nm, which is comparable to the length of a myosin head and two actin molecules. This suggests the direct binding of S1 tails to the adjacent actin filament. The "essential" light chain of cardiac myosin could be cross-linked to the actin molecule in the bundle. When monomeric actin molecules were added to the bundle, the bundles could be dispersed into individual filaments. The three-dimensional structure of the dispersed actin filaments was reconstructed from electron cryo-microscopic images of the single actin filaments dispersed by monomer actin. We were able to demonstrate that cardiac myosin heads bind to two actin molecules: one actin molecule at the conventional actin-binding region and the other at the essential light-chain-binding region. This capability of cardiac myosin heads to bind two actin molecules is discussed in view of lower ATPase activity and slower shortening velocity than those of skeletal ones.     

Actin in Tetrahymena paravorax: Ultrastructural Localization of HMM-Binding Filaments in Glycerinated Cells1,2

Actin has been identified in the ciliated protozoon Tetrahymena paravorax on the basis of the ultrastructural detection of filaments typically decorated with heavy meromyosin (HMM) in glycerinated microstome cells. These filaments are widely distributed in endoplasmic and cortical regions and can form bundles. They are particularly numerous in elongating cells; HMM-binding filaments run approximately parallel to rib microtubules in the ectoplasm of the right wall of the buccal cavity and seem to extend to the cytopharyngeal region, suggesting some role of actin in maintenance of the crest-trough pattern of ribbed wall and/or in formation of food vacuoles. Extensive actin bundles are observed below some membranellar areas and are thought to follow the course of the microtubular “deep fiber bundle.” The “fine filamentous reticulum” underlying the oral ribs and the “apical ring” extending beneath kinetosomes of ciliary couplets display filaments that do not bind HMM and are ? 14 nm in diameter. No evidence for actin in these structures was obtained in the present study. The “specialized cytoplasm” of the cytostome-cytopharyngeal region appears as an undecorated reticulum with 20 nm-spaced nodes. Occasionally HMM-binding filaments were found inside the macronucleus, just beneath its envelope. Actin is suggested to be involved in cell shaping and in control of the transport of food vacuoles.     

Isoforms of alpha-actinin from cardiac, smooth, and skeletal muscle form polar arrays of actin filaments

We have used a positively charged lipid monolayer to form two-dimensional bundles of F-actin cross-linked by alpha-actinin to investigate the relative orientation of the actin filaments within them. This method prevents growth of the bundles perpendicular to the monolayer plane, thereby facilitating interpretation of the electron micrographs. Using alpha-actinin isoforms isolated from the three types of vertebrate muscle, i.e., cardiac, skeletal, and smooth, we have observed almost exclusively cross-linking between polar arrays of filaments, i.e., actin filaments with their plus ends oriented in the same direction. One type of bundle can be classified as an Archimedian spiral consisting of a single actin filament that spirals inward as the filament grows and the bundle is formed. These spirals have a consistent hand and grow to a limiting internal diameter of 0.4-0.7 microm, where the filaments appear to break and spiral formation ceases. These results, using isoforms usually characterized as cross-linkers of bipolar actin filament bundles, suggest that alpha-actinin is capable of cross-linking actin filaments in any orientation. Formation of specifically bipolar or polar filament arrays cross-linked by alpha-actinin may require additional factors that either determine the filament orientation or restrict the cross-linking capabilities of alpha-actinin.