A study on the structure of paracrystals of F-actin.

The structure of three types of paracrystals formed by a muscle protein, actin, was studied by electron microscopy using the technique of optical diffraction and filtering methods.The type I paracrystal of F-actin⁴ had a flat net structure and each thread of the net appeared to be made of a single double-stranded filament of F-actin. Its unit cell was rhombic with sides of about 340 Å in length. The narrower angle of the rhomb was about 30 °. A side of the rhomb corresponded to one repeating unit of F-actin. The cross-connecting point of the net appeared to occur at a cross-over point of the double helical F-actin filament when the paracrystal plane was observed perpendicularly. A set of parallel filaments running in one direction seem to simply overlie another set of parallel filaments running in another direction.The type II paracrystal also had a flat net structure with a unit cell of the same size and shape as type I, but had twice the amount of material in the unit cell in comparison with that of type I; a thread of type II was made of a pair of F-actin filaments. The type II paracrystal seemed to be made by attaching the F-actin filaments side-by-side to filaments of the type I paracrystal. These newly associated filaments cross-connected with each other in the same manner as those of the type I paracrystal.The type III paracrystal was a side-by-side aggregate of F-actin filaments. There was no lateral order between the neighbouring filaments.     

Structure of actin paracrystals induced by nerve growth factor

When nerve growth factor is added to F-actin, well-ordered bundles of filaments are formed. These bundles are observed even at low concentrations of NGF²¹, but when N-bromosuccinimide-treated NGF, a biologically inactive form of the protein is used, a much higher concentration is required to produce aggregation. Moreover, the bundles induced by the modified NGF are not very well ordered and show amorphous aggregates attached at various points.Electron microscopy of paracrystals induced by native NGF shows that, although they resemble pure actin paracrystals induced by Mg²⁺, the interfilament spacing is larger and bridges connect the filaments. Optical diffraction patterns show, in addition to the off-meridional reflections characteristic of the actin helix, meridional reflections on the first and fourth layer-lines, at axial spacings of 37 and 9 nm. Measurements of the axial positions of the layer-lines show that the actin helical symmetry is not significantly different from that in pure actin paracrystals. The presence of the meridional reflections indicates that groups of two or three bridges with spacing 9 nm or nearly 9 nm are arranged along the bundles at a repeating interval of 37 nm.Actin filament bundles have been observed in several non-muscle cells, and specific actin-binding proteins have been identified as responsible for this aggregation. Our in vitro observations show that the biologically active form of NGF interacts with actin and organizes it into well-ordered paracrystalline arrays. The in vitro formation of NGF-actin complexes may be related to the in vivo mechanism of action of this growth factor.     

Mg2+-paracrystal formation of tropomyosin as a condensation phenomenon. Effects of pH, salt, temperature, and troponin binding.

Tropomyosin (Tm) paracrystal formation induced by Mg2+ was studied by monitoring increases in light scattering. Paracrystals formed above a critical Tm concentration with lag phases in the time courses at pH 7.5 and 6.0, indicating that condensation polymerization processes are involved. The kinetic data at pH 7.5 reasonably fit a model in which nucleation and elongation are taken into account. The rate and extent of light scattering increased at low [Mg2+] and decreased at high [Mg2+] with a maximum at [Mg2+] = 15 mM, indicating different effects of Mg2+ in the two [Mg2+] ranges. The paracrystals were destabilized by increasing the salt concentration and decreasing the temperature. Mg2+ produces paracrystals at pH 6.0 and pH 7.5 by different kinetic mechanisms. Different Tm intermolecular interactions at the two pH values were indicated by studies of the excimer fluorescence of pyrene-labeled Tm and by effects of salt and temperature on the kinetics. At pH 6.0 Tm more readily formed paracrystals with decreased electrostatic effects. Effects of troponin on Mg2+-paracrystal formation of Tm at the two pH values correlated with the known differences in paracrystal structure when troponin is bound to Tm.     

Polymorphism of actin paracrystals induced by polylysine

We describe a method for the induction of different polymorphic forms of actin filament paracrystals. This polymorphism is probably based on differences in the stagger and/or polarity of adjacent filaments in single-layered paracrystals and by superposition of different layers in multilayered paracrystals. The helical parameters defining the filament geometry are indistinguishable for the different polymorphic forms observed and for the four different actins used. Analysis of these paracrystals, some of which are ordered to better than 2.5 nm, should provide a reference structure suitable for alignment and orientation within the actin filament of high resolution models of the actin monomer obtained from crystal data.     

Actin and myosin-linked calcium regulation in the nematode Caenorhabditis elegans. Biochemical and structural properties of native filaments and purified proteins.

Calcium regulation of actomyosin activity in the nematode, Caenorhabditis elegans, has been studied with purified proteins and crude thin filaments. Actin and tropomyosin have been purified from C. elegans and shown to be similar in most respects to actin and tropomyosin from rabbit skeletal muscle. The actin comigrates with rabbit actin on polyacrylamide-sodium dodecyl sulfate gel electrophoresis, forms similar filaments and paracrystals, and activates the Mg2+-ATPase of rabbit myosin heads as efficiently as rabbit actin. Nematode tropomyosin has a greater apparent molecular weight (estimated by mobility on polyacrylamide-sodium dodecyl sulfate gels) than the rabbit protein, yet it forms Mg2+-paracrystals with a slightly shorter periodicity. Native thin filaments extracted from nematodes activate rabbit myosin subfragment 1 Mg2+-ATPase in a calcium sensitive manner; the extent of activation is threefold greater in 0.2 mM CaCl2 than in the absence of calcium. This observation suggests that the thin filaments contain components which are functionally equivalent to vertebrate troponins. Calcium is also required for maximal activation of the Mg2+-ATPase of purified nematode myosin by pure rabbit F-actin. C. elegans therefore has both myosin and thin filament-linked calcium regulatory systems. The origin of the actin, tropomyosin, and myosin from different tissues and the use of genetic analysis to answer questions about assembly and function in vivo are discussed.     

Effect of H-protein on the formation of myosin filaments and light meromyosin paracrystals

H-protein is a component of the thick filaments of skeletal myofibrils. Its effects on the assembly of myosin into filaments and on the formation of light meromyosin (LMM) paracrystals at low ionic strength have been investigated. H-protein reduced the turbidities of myosin filament and LMM paracrystal suspensions. Electron microscopic observation showed that the appearances of the filaments prepared in the presence and absence of H-protein were different. The filament length was not substantially changed by H-protein, but the diameter of the myosin filament was markedly reduced. H-protein bound to LMM and co-sedimented with it at low ionic strength upon centrifugation. Two types of paracrystals, spindle-shaped and sheet-like, were observed in LMM suspensions. H-protein altered the structure of the LMM paracrystals, especially the spindle-shaped ones. The thickness of the spindle-shaped paracrystals was reduced when H-protein was present during LMM paracrystal formation. On the other hand, periodic features along the long axis of the sheet-like paracrystals were retained even at high ratios of H-protein to LMM. However, there were fewer sheet-like paracrystals in the LMM suspensions containing H-protein than in the control. These results suggest that H-protein interferes with self-association of myosin molecule into filaments due to its binding to the tail portion of the myosin. However, H-protein does not have a length-determining effect on the formation of myosin filaments.     

Comparative electron microscopic study on projectin and titin binding to F-actin

Using the system of F-actin paracrystals, we have obtained electron microscopic evidence that projectin from synchronous flight muscles of Locusta migratoria binds to actin filaments in the same fashion as skeletal titin. Control actin paracrystals formed in the presence of Mg(2+) ions have great width and length and blunted ends. The addition of either projectin or titin results in disruption of compact ordered packing of F-actin in paracrystals and leads to the formation of loose filament bundles with smaller diameters and tapered ends. It is also accompanied with the appearance of individual actin filaments in considerable amounts. The effect becomes more pronounced with the increase in concentrations of added projectin or titin. Possible physiological implications of projectin-actin interactions are discussed.     

Arthrin: a new actin-like protein in insect flight muscle

There are one or more proteins of 50,000 to 60,000 Mr in the thin filaments of insect flight muscle. A protein of 55,000 Mr has been isolated from insect fibrillar flight muscle and called arthrin. Despite its higher molecular weight, arthrin is in many ways like actin. The amino acid composition of arthrin was similar to that of actin. There were similarities in the peptides produced by digesting the denatured proteins and mild digestion of polymerized proteins cleaved similar-sized fragments from arthrin and actin. Polymerized arthrin activated the Mg2+ ATPase of myosin to the same extent as actin and the ATPase was regulated by rabbit or Lethocerus troponin and tropomyosin. Arthrin did not itself act as troponin-T. Electron microscopy of negatively stained specimens showed that arthrin and actin filaments were similar in structure and that arthrin could be decorated by rabbit subfragment-1 to form normal-looking arrowheads. Arthrin formed paracrystals at an optimum concentration of MgCl2 (25 mM) that was somewhat lower than the optimum for actin paracrystals. Optical diffraction showed that the structure of the paracrystals was similar to those formed from actin. The mass of arthrin and actin filaments relative to phage fd was measured by scanning transmission electron microscopy; the relative mass of arthrin and actin was 1.33, in agreement with molecular weight estimations. Therefore arthrin has the properties of a heavy form of actin. The proportion of actin, arthrin and troponin-T in Lethocerus myofibrils was six moles of actin to one mole of arthrin and one mole of troponin-T. The function of arthrin is not known.     

The axial repeats in paracrystals of light meromyosin and its complex with C-protein

We examined the axial repeats in electron micrographs of three types of negatively stained paracrystals (two tactoid- and one sheet-like type) of rabbit light meromyosin (LMM) and its complex with C-protein characterized previously by similar axial period of about 43.0 nm. Assuming for the axial repeat in type II tactoids the value of 42.93 +/- 0.05 nm as it was determined by X-ray diffraction technique (Yagi and Offer 1981), we found average axial repeats in type I tactoid and in sheet-like paracrystal of 42.93 +/- 0.75 nm and 43.50 +/- 0.62 nm respectively. Analyzing the micrographs where the two types paracrystals are located side-by-side we determined rather accurately the average ratio of axial repeat in sheet-like paracrystal to that in type I tactoid (1.013 +/- 0.002). Taking 42.93 nm as the axial repeat in type I tactoid, the axial repeat in sheet-like paracrystal was found to be 43.50 +/- 0.08 nm. C-protein binds to LMM with the period of the underlying LMM paracrystals and independently of the value of their axial repeats. Two different axial repeats (42.9 nm and 43.5 nm) revealed for LMM paracrystals in this study precisely coincide with the average repeat periods of myosin crossbridges along the thick filaments found for different physiological states of skeletal muscles (Lednev and Kornev 1987). Molecular basis for the appearance of two structural states in LMM paracrystals and in the shafts of thick filaments are discussed.     

Interaction of aldolase with actin-containing filaments. Structural studies.

Electron micrographs of the paracrystals formed when fructose bisphosphate aldolase (EC 4.1.2.13) is added to actin-containing filaments were analysed by computer methods so that ultrastructural changes could be correlated with the various stoicheiometries of binding determined in the preceding paper [Walsh, Winzor, Clarke, Masters & Morton (1980) Biochem. J. 186, 89-98]. Paracrystals formed with aldolase and either F-actin or F-actin-tropomyosin have a single light transverse band every 38 nm, which is due to aldolase molecules cross-linking the filaments. In contrast, the paracrystals formed between aldolase and F-actin-tropomyosin-troponin filaments show two transverse bands every 38 nm: a major band, interpreted as aldolase binding to troponin, and a minor band, interpreted as aldolase cross-linking the filaments. The intensity of the minor band varies with Ca2+ concentration, being greatest when the Ca2+ concentration is low. A model for the different paracrystal structures which relates the various patterns and binding stoicheiometries to structural changes in the actin-containing filaments is proposed.     

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.     

A polymorphism peculiar to bipolar actin bundles.

Both muscle and nonmuscle actins produced magnesium paracrystals which we found indistinguishable from one another. Contrary to some previous reports, calcium ions caused no change in filament organization for either type of actin. The most ordered paracrystals consisted of hexagonally packed filaments with opposite polarities. We suggest that this mode of packing permits a form of disorder not previously described, which may account for some puzzling aspects of earlier observations and may prove useful in analyzing actin bundles formed, for example, with erythrocyte band 4.9 protein.     

Evidence for the non-filamentous aggregation of actin induced by lanthanide ions.

We varied the molar ratio of added lanthanide ion to skeletal muscle actin (M3+/A) and observed their effects on the change in reduced viscosity (Nred) in the presence of polymerizing quantities of salt (0.1 M KC1). Once the concentration of the lanthanide ion exceeds the concentration of the nucleotide present (0.2 mM ATP), we noted that with M3+/A ratios up to 4: (a) there was a sharp peak in the observed Nred above the level achieved by control F-actin; (b) the magnitude of (a) was shown to be a function of the initial G-actin concentration. With an M3+/A ratio of greater than 4 we observed: (i) a sharp fall in the observed Nred; (ii) the formation of an insoluble aggregate of actin; (iii) the formation of (ii) was completely reversed by removal of the M3+; (iv) a complete inhibition of the ATP hydrolysis which always accompanies the G- to F-actin transition; (v) the number of mol of M3+ required to completely inhibit the rise in Nred (above the viscosity of G-actin) was a function of the ionic radii of the 11 lanthanide ions tested; and (vi) the effects described in (i) were not mimicked when the initial protein was in the F form. In the absence of added KCI, divalent cations (e.g. Mg2+) polymerize G-actin but this effect is not mimicked by the addition of the lanthanide ions. However, under these conditions the lanthanide ions cause the formation of an insoluble aggregate of actin. We conclude that with greater than 4 mol of lanthanide ions, G-actin aggregates in a form which contains little or no F-actin and that the lanthanide ion-induced aggregates are therefore different from the Mg2+-induced F-actin paracrystals.     

Orientation of skeletal muscle actin in strong magnetic fields

Measurement of birefringence is used to follow actin filament and paracrystal formation in a strong magnetic field. Both F-actin and paracrystals orientate parallel to the field. This confirms that globular proteins arranged in filamentous assemblies can orientate in magnetic fields. This is consistent with the alpha-helical component of the actin subunits being approximately aligned along the actin filament.     

The structure of spindle-shaped paracrystals of light meromyosin

Light meromyosin paracrystals have been studied by electron microscopy combined with optical diffraction in order to understand how the tails of the myosin molecules might pack in the backbone of muscle thick filaments. The forms of paracrystal investigated were all spindle-shaped structures with an axial periodicity of either 43 nm or 14.3 nm or hybrids involving aspects of both repeats. Transverse sections show that they are not smooth but polygonal in outline. Analysis of the band patterns in negatively stained specimens indicates that the molecular arrangement in the paracrystals involves both parallel and antiparallel interactions. A parallel axial displacement of the molecules by 43 nm is intrinsic to all forms of paracrystal investigated. The principal antiparallel overlap between molecules appears to be one of 84 nm, and it is suggested that an antiparallel dimer is the structural unit in the paracrystals. The role of the interactions leading to these displacements in the formation of the thick filament backbone is discussed.     

Instability of pleomorphic tubulin paracrystals artificially induced by Vinca alkaloids in tissue-cultured cells

The processes of tubulin paracrystal induction in Chinese hamster ovary cells treated with a Vinca alkaloid, ie, vinblastine or vincristine, and treated simultaneously with one of the Vinca alkaloids and colcemid or colchicine were followed by four different microscopic techniques, in particular by tubulin-immunofluorescence. Vinca alkaloid alone, in lower concentrations, induced basically tactoid or needle-shaped (N-shaped) paracrystals. However, the formation of crystalloid was greatly enhanced by increasing the concentration of Vinca alkaloid. Square or barrel-shaped (S-shaped) and hexagonal paracrystals were also commonly induced by simultaneous treatment with a Vinca alkaloid and colcemid or colchicine. Large rectangular paracrystals often displayed fibrillar or lamellar fine structures which ran perpendicular to the long axis but tended to cleave into fragments by spontaneous splitting. Electron micrographs revealed the fine structure of crystalloids to be aggregates of numerous filaments. The growth of paracrystals, particularly N-shaped crystals, was markedly inhibited when cells were exposed to drug(s) at a low temperature (4 degrees C). We confirmed that both N- and S-shaped paracrystals dissociated rapidly after the culture medium was replaced with fresh, drug-free medium. Glutaraldehyde-fixed paracrystals treated with RNase solution were stained with acridine orange, showing a weak orange color. Possible factors involved in the assembly and disassembly of tubulin paracrystals are discussed.     

Organization of an actin filament-membrane complex. Filament polarity and membrane attachment in the microvilli of intestinal epithelial cells

The association of actin filaments with membranes is now recognized as an important parameter in the motility of nonmuscle cells. We have investigated the organization of one of the most extensive and highly ordered actin filament-membrane complexes in nature, the brush border of intestinal epithelial cells. Through the analysis of isolated, demembranated brush borders decorated with the myosin subfragment, S1, we have determined that all the microvillar actin filaments have the same polarity. The S1 arrowhead complexes point away from the site of attachment of actin filaments at the apical tip of the microvillar membrane. In addition to the end-on attachment of actin filaments at the tip of the microvillus, these filaments are also connected to the plasma membrane all along their lengths by periodic (33 nm) cross bridges. These bridges were best observed in isolated brush borders incubated in high concentrations of Mg++. Their visibility is attributed to the induction of actin paracrystals in the filament bundles of the microvilli. Finally, we present evidence for the presence of myosinlike filaments in the terminal web region of the brush border. A model for the functional organization of actin and myosin in the brush border is presented.     

The polyelectrolyte behavior of actin filaments: a 25Mg NMR study.

Under physiological conditions, filamentous actin (F-actin) is a polyanionic protein filament. Key features of the behavior of F-actin are shared with other well-characterized polyelectrolytes, in particular, duplex DNA. For example, the bundle formation of F-actin by polyvalent cations, including divalent metal ions such as Mg2+, has been proposed to be a natural consequence of the polyelectrolyte nature of actin filaments [Tang and Janmey (1996) J. Biol. Chem. 271, 8556-8563]. This recently proposed model also suggests that weak interactions between F-actin and Mg2+ ions reflect a nonspecific trapping of counterions in the electric field surrounding F-actin due to its polyelectrolyte nature. To test this hypothesis, we have performed 25Mg NMR measurements in F-actin solutions. Based on the NMR data, we estimate that the rotational correlation times of Mg2+ are independent of the overall rotational dynamics of the actin filaments. Moreover, competitive binding experiments demonstrate a facile displacement of F-actin-bound Mg2+ by Co(NH3)63+. At higher Co(NH3)63+ concentrations, a fraction of the magnesium ions are trapped as actin filaments aggregate. ATP also competes effectively with actin filaments for binding to Mg2+. These results support the hypothesis that magnesium ions bind loosely and nonspecifically to actin filaments, and thus show a behavior typical of counterions in polyelectrolyte solutions. The observed features mimic to some extent the well-documented behavior of counterions in DNA solutions.     

The structure of divalent cation-induced aggregates of PIP2 and their alteration by gelsolin and tau.

Phosphatidylinositol bisphosphate (PIP2) serves as a precursor for diacylglycerol and inositol trisphosphate in signal transduction cascades and regulates the activities of several actin binding proteins that influence the organization of the actin cytoskeleton. Molecules of PIP2 form 6-nm diameter micelles in water, but aggregate into larger, multilamellar structures in physiological concentrations of divalent cations. Electron microscopic analysis of these aggregates reveals that they are clusters of striated filaments, suggesting that PIP2 aggregates form stacks of discoid micelles rather than multilamellar vesicles or inverted hexagonal arrays as previously inferred from indirect observations. The distance between striations within the filaments varies from 4.2 to 5.4 nm and the diameter of the filaments depends on the dehydrated ionic radius of the divalent cation, with average diameters of 19, 12, and 10 nm for filaments formed by Mg2+, Ca2+, and Ba2+, respectively. The structure of the divalent cation-induced aggregates can be altered by PIP2 binding proteins. Gelsolin and the microtubule associated protein tau both affect the formation of aggregates, indicating that tau acts as a PIP2 binding protein in a manner similar to gelsolin. In contrast, another PIP2 binding protein, profilin, does not modify the aggregates.     

Conformation changes of actin during formation of filaments and paracrystals and upon interaction with DNase I, cytochalasin B, and phalloidin

Spin labels attached to rabbit muscle actin became more immobilized upon conversion of actin from the G state to the F state with 50 mM KCl. Titration of G-actin with MgCl2 produced F-actin-like EPR spectra between 2 and 5 mM-actin filaments by electron microscopy. Higher concentrations of MgCl2 produced bundles of actin and eventually paracrystals, accompanied by further immobilization of spin labels. The effects of MgCl2 and KCl were competitive: addition of MgCl2 to 50 mM could convert F-actin (50 mM KCl) to paracrystalline (P) actin; the reverse titration (0 to 200 mM KCl in the presence of 20 mM MgCl2) was less complete. Addition of DNase I to G- or F-actin gave the expected amorphous electron micrographic pattern, and the actin was not sedimentable at (400,000 x g x h). EPR showed that the actin was in the G conformation. Addition of DNase I to paracrystalline actin gave the F conformation (EPR) but the actin was "G" by electron microscopy. Phalloidin converted G-actin to F-actin, had no effect on F-actin, and converted P-actin to the F state by electron microscopy but maintained the P conformation by EPR. Cytochalasin B produced no effects observable by EPR or centrifugation but "untwisted" paracrystals into nets. Since actin retained its P conformation by EPR in two states which were morphologically not P, we conclude that the P state is a distinct conformation of the actin molecule and that actin filaments aggregate to form bundles (and eventually paracrystals) when actin monomers are able to enter the P conformation.