Light meromyosin paracrystal formation

Studies of paracrystal formation by column purified light meromyosin (LMM) prepared in a variety of ways led to the following conclusions: (a) different portions of the myosin rod may be coded for different stagger relationships. This was concluded from observations that paracrystals with different axial repeat periodicities could be obtained either with LMM framents of different lengths prepared with the same enzyme, or with LMM fragments of identical lengths but prepared with different enzymes. (b) Paracrystals with a 14-nm axial repeat periodicity are most likely formed by the aggregation of sheets with a 44-nm axial repeat within the sheets which are staggered by 14 nm. All of the axial repeat patterns expected from one sheet or aggregates of more than one sheet, on this basis, were observed in the same electron micrograph. (c) C-protein binding probably occurs preferentially to LMM molecules related in some specific way. This was concluded from the observation that the same axial repeat pattern was obtained in paracrystals formed from different LMM preparations in the presence of C-protein, regardless of differences in the axial repeat obtained in the absence of C-protein. (d) Nucleic acid is responsible for the 43-nm axial repeat patterns observed in paracrystals formed by the ethanol-resistant fraction of LMM. In the absence of nuclei acid, paracrystals with a 14nm axial repeat are obtained. (e) The 43-nm axial repeat pattern observed with the ethanol-resistant fraction of LMM is different for LMM preparations obtained by trypsin and papain digestions.     

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.     

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.     

Interaction between vertebrate skeletal and uterine muscle myosins and light meromyosins

The specific contributions of this work may be summarized as follows: (a) No hybridization of uterine and skeletal myosin occurs at pH 6.0 although previous studies have shown that hybridization does occur at pH 6.5 (B. Kaminer et al. 1976. J. Mol. Biol. 100:379-386) or 7.0 (T. Pollard. 1975. J. Cell Biol. 67:93-104) (b) Hybridization of uterine and skeletal light meromyosins (LMM) occurs at pH 7.0 but not at pH 6.0, which is analogous to the hybridization of myosins. (c) In hybridized paracrystals there is a uniform distribution of both uterine and skeletal LMM molecules because all the paracrystals have only one axial repeat pattern. This makes it highly likely that in hybridized filaments the two myosins are also uniformly distributed throughout the filaments. (d) The 14-nm repeat of white bands observed in paracrystals of uterine LMM formed at pH 6.0, compared with the 14-nm repeat of dark bands observed with skeletal LMM under the same conditions, probably reflects differences in surface charge density along the different LMM molecules.     

Localization of C-protein isoforms in chicken skeletal muscle: ultrastructural detection using monoclonal antibodies

Monoclonal antibodies (McAbs) specific for the fast (MF-1) and slow (ALD-66) isoforms of C-protein from chicken skeletal muscle have been produced and characterized. Using these antibodies it was possible to demonstrate that skeletal muscles of varying fiber type express different isoforms of this protein and that in the posterior latissimus dorsi muscle both isoforms are co-expressed in the same myofiber (17, 18). Since we had shown that both isoforms were present in all sarcomeres, it was feasible to test whether the two isoforms co- distributed in the same 43-nm repeat within the A-band, thereby establishing a minimum number of C-proteins per repeat in the thick filaments. Here we describe the ultrastructural localization of C- protein in myofibers from three muscle types of the chicken using these same McAbs. We observed that although C-protein was present in a 43-nm repeat along the filaments in all three muscles, there were marked differences in the absolute number and position occupied by the different isoforms. Since McAbs MF-1 and ALD-66 decorated the same 43- nm repeats in the A-bands of the posterior latissimus dorsal muscle, we suggest that at least two C-proteins can co-localize at binding sites 43 nm apart along thick filaments of this muscle.     

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.     

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 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.     

Axial arrangement of the myosin rod in vertebrate thick filaments: immunoelectron microscopy with a monoclonal antibody to light meromyosin

A monoclonal antibody, MF20, which has been shown previously to bind the myosin heavy chain of vertebrate striated muscle, has been proven to bind the light meromyosin (LMM) fragment by solid phase radioimmune assay with alpha-chymotryptic digests of purified myosin. Epitope mapping by electron microscopy of rotary-shadowed, myosin-antibody complexes has localized the antibody binding site to LMM at a point approximately 92 nm from the C-terminus of the myosin heavy chain. Since this epitope in native thick filaments is accessible to monoclonal antibodies, we used this antibody as a high affinity ligand to analyze the packing of LMM along the backbone of the thick filament. By immunofluorescence microscopy, MF20 was shown to bind along the entire A-band of chicken pectoralis myofibrils, although the epitope accessibility was greater near the ends than at the center of the A-bands. Thin-section, transmission electron microscopy of myofibrils decorated with MF20 revealed 50 regularly spaced, cross-striations in each half A-band, with a repeat distance of approximately 13 nm. These were numbered consecutively, 1-50, from the A-band to the last stripe, approximately 68 nm from the filament tips. These same striations could be visualized by negative staining of native thick filaments labeled with MF20. All 50 striations were of a consecutive, uninterrupted repeat which approximated the 14-15-nm axial translation of cross-bridges. Each half M-region contained five MF20 striations (approximately 13 nm apart) with a distance between stripes 1 and 1', on each half of the bare zone, of approximately 18 nm. This is compatible with a packing model with full, antiparallel overlap of the myosin rods in the bare zone region. Differences in the spacings measured with negatively stained myofilaments and thin-sectioned myofibrils have been shown to arise from specimen shrinkage in the fixed and embedded preparations. These observations provide strong support for Huxley's original proposal for myosin packing in thick filaments of vertebrate muscle (Huxley, H. E., 1963, J. Mol. Biol., 7:281-308) and, for the first time, directly demonstrate that the 14-15-nm axial translation of LMM in the thick filament backbone corresponds to the cross-bridge repeat detected with x-ray diffraction of living muscle.     

Effects of C-protein on synthetic myosin filament structure.

In the absence of C-protein, synthetic filaments prepared from column-purified myosin exhibit the following features: individual filament diameters are uniform over a long length, but a wide distribution of diameters is apparent over the population; approximately 25% of the filaments have a frayed appearance and take up stain poorly, whereas the remaining 75% are well-stained; optical diffraction of well-stained filaments reveals a 14.3-nm subunit period and a 43-nm axial period (Koretz, 1978; Koretz, 1979). Addition of C-protein to myosin before filament formation affects all of these features in a manner related to C-protein concentration. At the physiological ratio of C-protein to myosin in the banded region of the natural thick filament, synthetic aggregates are uniform in diameter over the population and show less than 10% frays. Whereas the subunit period remains unchanged, the axial period has increased to 114.4 nm, or eight times the subunit repeat. Above and below the physiological ratio, disorder of a specific nature is apparent. Addition of C-protein after filament formation appears to coat the aggregates so that elements of backbone ultrastructure are obscured, and some evidence of axial period change is visible in diffraction patterns. A model is presented for the binding of C-protein to myosin, and its observed effects on filament structure are explained in terms of this model.     

An electron microscopic and optical diffraction analysis of the structure of Limulus telson muscle thick filaments

Long, thick filaments (greater than 4.0 micrometer) rapidly and gently isolated from fresh, unstimulated Limulus muscle by an improved procedure have been examined by electron microscopy and optical diffraction. Images of negatively stained filaments appear highly periodic with a well-preserved myosin cross-bridge array. Optical diffraction patterns of the electron micrographs show a wealth of detail and are consistent with a myosin helical repeat of 43.8 nm, similar to that observed by x-ray diffraction. Analysis of the optical diffraction patterns, in conjunction with the appearance in electron micrographs of the filaments, supports a model for the filament in which the myosin cross-bridges are arranged on a four-stranded helix, with 12 cross-bridges per turn or each helix, thus giving an axial repeat every third level of cross-bridges (43.8 nm).     

Helical disorder and the filament structure of F-actin are elucidated by the angle-layered aggregate

Angle-layered aggregates of F-actin are net-like structures induced by Mg2+ concentrations below that used to form paracrystals. These aggregates incorporate the angular disorder of subunits, which has been described elsewhere for isolated actin filaments. Because this disorder is incorporated into the aggregates in solution at the time they are formed, the possibility of negative stain preparation being responsible for the disorder is excluded. The simple two-layered geometry of the angle-layered aggregate provides information about the shape of the component actin filaments free from the superposition of large numbers of layers. A model for the filament shape, derived from single filaments and confirmed by the angle-layered aggregate, is different from those that have previously emerged from paracrystal studies. An understanding of the interfilament bond in both the angle-layered aggregate and the paracrystal allows one to reconcile these different models. We have found a bipolar bonding rule, with staggered crossover points in the angle-layered aggregate, which we suggest is also responsible for Mg2+ paracrystals. This bonding rule can explain the apparent alignment of crossover points in adjacent filaments in paracrystals as a consequence of the superposition of staggered filaments.     

X-ray diffraction and electron microscopy of a light meromyosin tactoid

The structure of a tactoid of light meromyosin with a 43-nm periodicity was studied by both X-ray diffraction and electron microscopy. Such tactoids were formed from light meromyosin prepared by a short tryptic digestion (5 min) of myosin.A strong magnetic field (6 kgauss) was employed to obtain oriented specimens of tactoids for X-ray diffraction. The oriented tactoids gave equatorial reflections from a rectangular lattice with a unit cell of 6·5 nm × 3·9 nm (at pH 6·6) in a plane perpendicular to the long axis of the tactoid. This lattice shrank anisotropically when the pH was lowered. The meridional reflections could be indexed as orders of 42·93 ± 0·05 nm.The tactoids were frequently associated with sheet-like structures termed banded sheets. In negative stain these banded sheets showed the same band pattern as the tactoids with 10 nm wide light and 33 nm wide dark bands. However, in thin banded sheets the density of neighbouring dark bands alternated so that the true axial repeat was 86 nm. Optical diffraction showed that the face-on view of the banded sheet had a unit cell of 3·6 nm × 86 nm.From these observations a plausible model for the structure of the light meromyosin tactoid has been deduced. In this model the tactoid is made by a stacking of unit layers. A unit cell (6·5 nm × 3·9 nm × 86 nm) contains four light meromyosin molecules, each 90 nm long and packed co-planar, not all of which are in an identical environment. The molecules make parallel interactions with staggers of 86 and 43 nm and antiparallel interactions with overlaps of 84 and 41 nm.     

Helical structure of Bordetella pertussis fimbriae.

The helical structures of Bordetella pertussis fimbriae of serotypes 2 and 6 were determined by optical diffraction analysis of electron micrographs of negatively stained paracrystalline bundles of purified fimbriae. The fimbrial structure is based on an axial repeat of 13 nm that contains five repeating units in two complete turns of a single-start helix. This structure was confirmed by direct measurements of mass per unit length for individual fimbriae performed by dark-field scanning transmission electron microscopy of unstained specimens. These data further established that the helically repeating unit is a monomer of fimbrial protein (Mr congruent to 22,000 for type 2 and Mr congruent to 21,500 for type 6). Radial density profiles calculated from the scanning transmission electron micrographs showed that the fimbria has peak density at its center, i.e., no axial channel, consistent with the results of conventional negative-staining electron microscopy. The radial profile gives an outermost diameter of approximately 7.5 nm, although the peripheral density is, on average, diffuse, allowing sufficient intercalation between adjacent fimbriae to give a center-to-center spacing of approximately 5.5 nm in the paracrystals. Despite serological and biochemical differences between type 2 and type 6 fimbriae, the packing arrangements of their fimbrial subunits are identical. From this observation, we infer that the respective subunits may have in common conserved regions whose packing dictates the helical geometry of the fimbria. It is plausible that a similar mechanism may underlie the phenomenon of phase variations in other systems of bacterial fimbriae.     

Towards a molecular understanding of titin.

Titin is at present the largest known protein (M(r) 3000 kDa) and its expression is restricted to vertebrate striated muscle. Single molecules span from M- to Z-lines and therefore over 1 micron. We have isolated cDNAs encoding five distant titin A-band epitopes, extended their sequences and determined 30 kb (1000 kDa) of the primary structure of titin. Sequences near the M-line encode a kinase domain and are closely related to the C-terminus of twitchin from Caenorhabditis elegans. This suggests that the function of this region in the titin/twitchin family is conserved throughout the animal kingdom. All other A-band sequences consist of 100 amino acid (aa) repeats predicting immunoglobulin-C2 and fibronectin type III globular domains. These domains are arranged into highly ordered 11 domain super-repeat patterns likely to match the myosin helix repeat in the thick filament. Expressed titin fragments bind to the LMM part of myosin and C-protein. Binding strength increases with the number of domains involved, indicating a cumulative effect of multiple binding sites for myosin along the titin molecule. We conclude that A-band titin is likely to be involved in the ordered assembly of the vertebrate thick filament.     

Three-dimensional structure of the Z band in a normal mammalian skeletal muscle

The three-dimensional structure of the vertebrate skeletal muscle Z band reflects its function as the muscle component essential for tension transmission between successive sarcomeres. We have investigated this structure as well as that of the nearby I band in a normal, unstimulated mammalian skeletal muscle by tomographic three- dimensional reconstruction from electron micrograph tilt series of sectioned tissue. The three-dimensional Z band structure consists of interdigitating axial filaments from opposite sarcomeres connected every 18 +/- 12 nm (mean +/- SD) to one to four cross-connecting Z- filaments are observed to meet the axial filaments in a fourfold symmetric arrangement. The substantial variation in the spacing between cross-connecting Z-filament to axial filament connection points suggests that the structure of the Z band is not determined solely by the arrangement of alpha-actinin to actin-binding sites along the axial filament. The cross-connecting filaments bind to or form a "relaxed interconnecting body" halfway between the axial filaments. This filamentous body is parallel to the Z band axial filaments and is observed to play an essential role in generating the small square lattice pattern seen in electron micrographs of unstimulated muscle cross sections. This structure is absent in cross section of the Z band from muscles fixed in rigor or in tetanus, suggesting that the Z band lattice must undergo dynamic rearrangement concomitant with crossbridge binding in the A band.     

New X-ray diffraction observations on vertebrate muscle: organisation of C-protein (MyBP-C) and troponin and evidence for unknown structures in the vertebrate A-band

Previous low-angle X-ray diffraction studies of various vertebrate skeletal muscles have shown the presence of two rich layer-line patterns, one from the myosin heads and based on a 429 A axial repeat, and one from actin filaments and based on a repeat of about 360-370 A. In addition, meridional intensities have been seen from C-protein (MyBP-C; at about 440 A and its higher orders) and troponin (at about 385 A and its orders). Using preparations of intact, relaxed, bony fish fin muscles and the ID-02 low-angle X-ray camera at the ESRF with a 10 m camera length we have now seen numerous, hitherto unreported, sampled, X-ray layer-lines many of which do not fit onto the previously observed repeats and which require interpretation. The new reflections all fall on the normal ("vertical") hexagonal lattice row-lines in the highly sampled, almost "crystalline", low-angle diffraction X-ray patterns from bony fish muscle, indicating that they all arise from the muscle A-band. However, they do not fall on a single axial repeat. In direct confirmation of our previous analysis, some of these new reflections are explained by the interaction in resting muscle between the N-terminal ends of myosin-bound C-protein molecules with adjacent actin filaments, possibly through the Pro-Ala-rich region. Other newly observed reflections lie on a much longer repeat, but they are most easily interpreted in terms of the arrangement of troponin on the actin filaments. If this is so, then the implication is that the actin filaments and their troponin complexes are systematically arranged in the fish muscle A-band lattice relative to the myosin head positions, and that these newly observed X-ray reflections, when fully analysed, will report on the shape and distribution of troponin molecules in the resting muscle A-band. The less certain contributions of titin and nebulin to these new reflections have also been tested and are described. Many of the new reflections do not appear to come from these known structures. There must be structural features of the A-band that have not yet been described.     

Frog skeletal muscle thick filaments are three-stranded

A procedure has been developed for isolating and negatively staining vertebrate skeletal muscle thick filaments that preserves the arrangement of the myosin crossbridges. Electron micrographs of these filaments showed a clear periodicity associated with crossbridges with an axial repeat of 42.9 nm. Optical diffraction patterns of these images showed clear layer lines and were qualitatively similar to published x-ray diffraction patterns, except that the 1/14.3-nm meridional reflection was somewhat weaker. Computer image analysis of negatively stained images of these filaments has enabled the number of strands to be established unequivocally. Both reconstructed images from layer line data and analysis of the phases of the inner maxima of the first layer line are consistent only with a three-stranded structure and cannot be reconciled with either two- or four-stranded models.     

X-ray diffraction study of the rabbit psoas muscle with extracted H-zone

Fibre bundles of glycerinated rabbit psoas muscle about 0.5-1.0 mm thick were incubated in 5 mM tris-(hydroxymethyl)-aminomethane (Tris), pH 8.0 for 5-20 hours at 4 degrees C. This treatment leads to selective removal of some proteins in the M-bands and H-zones of sarcomeres. Effects of extraction were analyzed on the basis of electron micrographs of longitudinal sections of muscle specimens, gel electrophoresis patterns of myofibrils and of the extracts, and measurements of the creatine kinase activity of myofibrils. In the X-ray diffraction patterns of the fibre bundles subjected to prolonged extraction a drastic decrease in the intensity of "442 A" and "223 A" meridional reflections and a considerably smaller decrease in the intensity of "212 A" meridional reflections were observed. The "147 A" meridional reflection remains practically unchanged. It was concluded that: (1) The reflections "442 A" and "223 A" were contributed mainly by diffraction on the minor proteins located in the central part of the thick filaments in between the C-zones. This is contrary to the widely accepted viewpoint according to which the appearance of "442 A" reflection is caused only by the C-protein component of the thick filaments. (2) The "147 A" meridional reflection is contributed mainly by C-protein and light meromyosin of the thick filaments.