The myosin filament XV assembly: contributions of 195 residue segments of the myosin rod and the eight C-terminal residues.

A mixture of two peptides of approximately M(r) 13000 has been isolated from a papain digest of LC2 deficient myosin. The peptides assemble into highly ordered aggregates which in one view are made up of strands of pairs of dots with an average side to side spacing of 13.0 nm and an average axial repeat of 9.0 nm. In another view there are strands of single dots with a side-to-side spacing of 7.8 nm and an axial repeat of 9.1 nm. From N-terminal peptide sequencing, the two peptides have been shown to come from regions of the myosin rod displaced by 195 residues. We have shown that either peptide alone can assemble to form the same aggregates. The 195 residue displacement of the M(r) 13000 peptides corresponds closely to the 196 residue repeat of charges along the myosin rod. This finding permits us to designate 195 residue segments of the myosin rod and to relate assembly characteristics directly to the similar 195 residue segments and 196 residue charge repeat. The most C-terminal 195 residue segment carries information for assembly into helical strands. The contiguous 195 residue segment, in major part, carries information for the unipolar assembly, characteristic of the assembly in each half of the myosin filament. The next contiguous 195 residue segment, in major part, carries information for bipolar assembly which is characteristic of the bare zone region of the filament; and for the transition from the bipolar bare zone to unipolar assembly. The effect of the eight C-terminal residues of the myosin rod on the assembly of the contiguous 195 residues has also been studied. The entire fragment of 195 + eight C-terminal residues assembled to form helical strands with an axial repeat of 30 nm. Successive deletion of charged residues changed the axial repeat of the helical strands suggesting that the charged residues at the C-terminus are involved in determining the pitch in the helical assembly of the contiguous 195 residues.

Substructures in the core of thick filaments: arrangement and number in relation to the paramyosin content of insect flight muscles.

Transverse sections (100-140 nm thick) of solid myosin filaments of the flight muscles of the honeybee, Apis mellifica, the fleshfly, Phormia terrae-novae and the waterbug, Lethocerus uhleri, were photographed in a JEM-200 electron microscope at 200 kV. The images were digitized and computer processed by rotational filtering. The power spectra of the images of each of these filaments showed six-fold symmetry for the outer wall region and three-fold symmetry for the inner wall region. Images of the honeybee additionally showed three-fold symmetry for the center of the filament. Considering both paramyosin content of the myosin filaments and the results of the rotational filtering, we suggest the existence of 3 paramyosin strands in the myosin filaments of the fleshfly, 6 paramyosin strands in the honeybee filaments and 5 strands in the myosin filaments of the waterbug. In the case of the honeybee, the 3 paramyosin strands of the inner wall are positioned directly opposite the myosin subfilaments, while the 3 strands of the center seem to be arranged opposite the gaps between the myosin subfilaments. The paramyosin filaments of the fleshfly wobble between 2 myosin subfilaments, without loosing their three-fold symmetry arrangement in the inner wall. The 3 paramyosin strands in the inner wall of the waterbug myosin filaments are either arranged opposite the myosin subfilaments or opposite the gaps between the subfilaments. Finally, we were able to generate a 3-dimensional reconstruction of the myosin filament of the honeybee, showing the parallel arrangement of both, myosin subfilaments and paramyosin strands, relative to the long filament axis.

Invertebrate myosin filament: Parallel subfilament arrangement in the wall of solid filaments from the honeybee, Apis mellifica.

Transverse serial sections (100-140 nm thick) of solid myosin filaments of the honeybee, Apis mellifica, were photographed in a JEM-200 electron microscope at 200 kV. The images were digitized and computer processed by rotational filtering. 87% of the myosin filaments showed 6-fold symmetry in their power spectra, confirming the results of earlier works (Beinbrech et al., 1988, 1991). To determine if the subfilaments were arranged parallel to the filament backbone, two methods were used. First, the three images of each myosin filament in the three serial sections were superimposed. 85% of the resulting images showed a strong peak for 6-fold symmetry and the averaged images showed 6 pairs of subfilaments, which gives evidence for parallel arrangement of the subfilaments relative to the filament axis. This result was confirmed by the second method in which a 3-dimensional reconstruction was made. An average image was made from the images of the same 17 myosin filaments from each of the three sections. The data for the 3-dimensional reconstruction were collected by tracing the outlines of the structures in the three successive sections. The resulting stereo image shows a parallel arrangement of the subfilaments.

The invertebrate myosin filament: subfilament arrangement of the solid filaments of insect flight muscles.

Transverse sections (approximately 140 nm thick) of solid myosin filaments of the flight muscles of the fleshfly, Phormia terrae-novae, the honey bee, Apis mellifica, and the waterbug, Lethocerus uhleri, were photographed in a JEM model 200A electron microscope at 200 kV. The images were digitized and computer processed by rotational filtering. In each of these filaments it was found that the symmetry of the core and the wall was not the same. The power spectra of the images showed sixfold symmetry for the wall and threefold symmetry for the core of the filaments. The images of the filaments in each muscle were superimposed according to the sixfold center of the wall. These averaged images for all three muscles showed six pairs of subunits in the wall similar to those found in the wall of tubular filaments. From serial sections of the fleshfly filaments, we conclude that the subunits in the wall of the filaments represent subfilaments essentially parallel to the long axis of the filament. In each muscle there are additional subunits in the core, closely related to the subunits in the wall. Evaluation of serial sections through fleshfly filaments suggests that the relationship of the three subunits observed in the core to those in the wall varies along the length of the filaments. In waterbug filaments there are three dense and three less dense subunits for a total of six all closely related to the wall. Bee filaments have three subunits related to the wall and three subunits located eccentrically in the core of the filaments. The presence of core subunits can be related to the paramyosin content of the filaments.

The myosin filament XIV backbone structure.

The substructure of the thick filaments of chemically skinned chicken pectoralis muscle was investigated by electron microscopy. Images of transverse sections of the myosin filaments were determined to have threefold symmetry by cross-correlation analysis, which gives an unbiased determination of the rotational symmetry of the images. Resolution, using the phase residual test (Frank et al. 1981. Science [Wash. DC]. 214:1353-1355), was found to be between 3.2 and 3.6 nm. Three arrangements of nine subfilaments in the backbone were found in all regions of the filament at ionic strengths of 20 and 200 mM. In the average images of two of these, there were three dense central subfilaments and three pairs of subfilaments on the surface of the thick filament. In the average image of the third arrangement, all of the protein mass of the nine subfilaments was on the surface of the filament with three of them showing less variation in position than the others. A fourth arrangement appearing to be transitional between two of these was seen often at 200 mM ionic strength and only rarely at 20 mM. On average, the myosin subfilaments were parallel to the long axis of the filament. The different arrangements of subfilaments appear to be randomly distributed among the filaments in a transverse section of the A-band. Relative rotational orientations with respect to the hexagonal filament lattice, using the three densest subfilaments as reference showed a major clustering (32%) of filaments within one 10 degrees spread, a lesser clustering (15%) at 90 degrees to the first, and the remainder scattered thinly over the rest of the 120 degrees range. There was no obvious pattern of distribution of the two predominant orientations that could define a superlattice in the filament lattice.

Effects of phosphorylation, magnesium, and filament assembly on actin-activated ATPase of pig urinary bladder myosin.

The relationship between the light-chain phosphorylation and the actin-activated ATPase activity of pig urinary bladder myosin was either linear or nonlinear depending on the free Mg2+ concentration. Varying the free [Mg2+] in the presence of 50 mM ionic strength (I) had a biphasic effect on the actin-activated ATPase. In 100 mM I, the activity increased on raising the free [Mg2+]. The activity of the phosphorylated myosin was 3-23-fold higher than that of the unphosphorylated myosin at all concentrations of free Mg2+, pH, and temperature used in this study. The increase in the turbidity and sedimentability of both phosphorylated and unphosphorylated myosins on raising the free [Mg2+] was associated with a rise in the actin-activated ATPase activity. However, myosin light-chain phosphorylation still had a remarkable effect on the actin activation. The myosin polymers formed under these conditions were sedimented by centrifugation. Experiments performed with myosin polymers formed in mixtures of unphosphorylated and phosphorylated myosins showed that the presence of phosphorylated myosin in these mixtures had a slight effect on the sedimentation of the unphosphorylated myosin but it had no effect on the actin-activated ATP hydrolysis. Electron microscopy showed that the unphosphorylated myosin formed unorganized aggregates while phosphorylated myosin molecules assembled into bipolar filaments with tapered ends. These data show that although the unphosphorylated and phosphorylated myosins have the same level of sedimentability and turbidity, the filament assembly present only with the phosphorylated myosin can be associated with the maximal actin activation of Mg-ATPase.

Orientation of the backbone structure of myosin filaments in relaxed and rigor muscles of the housefly: evidence for non-equivalent crossbridge positions at the surface of thick filaments.

The orientation of the backbone structure of myosin filaments of relaxed and rigor fibers of the flight muscles of the housefly, Musca domestica, relative to the actin filaments has been investigated. In relaxed muscles 23% of the myosin filaments have gaps in the wall of their shaft located opposite the surrounding actin filaments, while in 77% the subfilament pairs of the wall are thus located. These are the expected values if the backbone orientation is random. In rigor muscles 40% of the thick filaments have their gaps opposite the actins and 60%, the subfilament pairs are opposite the actins. This increase in the percentage of filaments with gaps opposite the actins therefore results from binding of the crossbridges in rigor with change in rotational orientation of the backbone. The findings are related to a model of Beinbrech et al. (1988) in which two populations of crossbridges have been postulated: one originating at the surface of the thick filaments, the other coming from within the gap between the subfilament pairs.

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.

LC2 involvement in the assembly of skeletal myosin filaments.

The assembly of LC2-deficient myosin was studied under conditions where control and LC2-reassociated myosin assemble around the native length of about 1.5 microns. The aim of this work was to determine how loss of LC2 affects the assembly characteristics. The findings of this study can be summarized as follows: (a) LC2-deficient myosin assembles into two populations of filaments, one around 0.5 micron in length and the other around 1 micron in length. This suggests that loss of the LC2 perturbs the length-determining mechanism. (b) The population of filaments around 0.5 micron has a diameter around 14 nm and that around 1 micron a diameter around 22 nm. Neither diameter corresponds to the 18 nm obtained with the control and LC2-reassociated myosins, suggesting that the presence of LC2 may have a role in regulating the side-to-side assembly of the myosin rods. (c) Filaments assembled from LC2-deficient myosin tend to aggregate side-by-side, but not those assembled from control and LC2-reassociated myosin. (d) The presence of MgATP has no effect on the length distribution of LC2-deficient myosin filaments in contrast to the sharpening of the distribution observed with control and reassociated myosin.

Invertebrate myosin filament: subfilament arrangement in the wall of tubular filaments of insect flight muscles.

Transverse sections (100 to 140 nm thick) of the flight muscles of the fleshfly Phormia terrae-novae and the housefly Musca domestica were studied. The images of 56 tubular myosin filaments of the fleshfly and 62 filaments of the housefly were digitized and computer processed by rotational averaging. The rotational power spectra of more than 80% of the filaments showed peaks for 6-fold rotational frequency. The average of these images for each species showed a characteristic pattern consisting of 12 subunits arranged in six pairs around the wall of the filament. This pattern was enhanced by rotationally filtering the average images using the 6-fold components of the rotational power spectrum. On tilting individual images, the subunits behaved like rods perpendicular to the plane of the transverse section and they were therefore considered to be subfilaments essentially parallel to the long axis of the filament. The center-to-center spacing between the subfilaments of a pair is 2.8 nm, and the center-to-center spacing between the adjacent subfilaments of neighboring pairs is 4.0 nm. The observation of 12 subfilaments is consistent with a four-stranded helical arrangement of myosin cross-bridges on the surface of the filaments.

Subfilament organization in myosin filaments of the fast abdominal muscles of the lobster, Homarus americanus.

The myosin filaments of the fast abdominal muscle of the lobster are about 2.7 microns long with a diameter of about 20 nm. They have a low density core in transverse sections except for a short portion in the middle of the filaments about 140 nm in length which is solid. In the solid region the diameter of the filaments is 25 nm. The wall of the filaments is made up of 12 subfilaments arranged in six pairs in a single layer around the wall. The spacing between the subfilaments of a pair is 3.4 nm and the spacing between successive pairs is 8.4 nm. An extra density is present on the inner surface of the wall of the filament along the entire length of the tubular portion of the filament. This density is always adherent to the wall and in serial transverse sections of the same filament its position changes from section to section without any apparent pattern to the change. No structural organization could be detected in this extra density.

The myosin filament. XII. Effect of MgATP on assembly.

The effect of MgATP on myosin filament assembly has been studied. Filaments were assembled by a standard dilution procedure involving two steps, dilution from 0.6 to 0.3 M KCl and from 0.3 to 0.15 M KCl with a different rate of dilution in each step. This standard dilution procedure gives filaments which are structurally similar to native filaments in that they have a sharp length distribution around 1.5 micron, a diameter of 16 nm and they vary in length with KCl concentration in a similar manner to native filaments. The addition of 1 mM MgATP leads to a sharpening of the length distribution around 1.5 micron without change in the 16 nm diameter. Filaments assembled by dialysis or by rapid dilution are not similarly affected by the presence of MgATP indicating that the standard dilution procedure produces filaments which are more closely similar to native filaments than those produced by these other methods. MgAMPPNP and magnesium pyrophosphate have the same effect as MgATP thus eliminating the possibility that phosphorylation of the myosin is involved in the effect. The effect of MgATP is not directly related to its binding to the active site of the myosin molecule since a 500:1 mole ratio of MgATP to myosin is required for the effect. It is therefore likely that the effect of MgATP is related to other binding sites on the myosin molecule. The presence of MgATP leads to molecular rearrangements which finely tune the molecular organization of the filaments formed by the standard dilution procedure in vitro.(ABSTRACT TRUNCATED AT 250 WORDS)

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. X. Observation of nine subfilaments in transverse sections.

The molecular packing of the subfilaments in muscle thick filaments has been investigated by electron microscopy. Thin (80-100 nm) transverse sections of vertebrate skeletal muscle were cut, and 129 electron microscope images of thick filaments from 15 different areas including seven to ten images in each area were analyzed by computer image processing. The transverse sections were limited to the portion of the filaments between the bare zone and the C-protein bearing region. Of the 129 images, six were discarded because they were structurally disrupted, 17 did not show evidence for the presence of subfilaments from the autocorrelation function, and four did not show evidence for three-fold rotational symmetry from the power spectrum. The remaining 102 filaments all showed evidence for three-fold rotational symmetry, consistent with other available evidence (Pepe, 1982). From the analysis of these images by rotational filtering, we have found that the vertebrate skeletal myosin filament is made up of nine subfilaments and that the image appears to have trigonal symmetry. Of these subfilaments, six are arranged with a center-to-center spacing of about 4 nm and the other three on the surface of the filament are distorted from this arrangement. Three additional densities, which together with the other nine, correspond to the pattern of 12 densities previously observed in more highly selected images (Stewart et al., 1981; Pepe and Drucker, 1972) were observed in 5% of the images. Another pattern of nine subfilaments peripherally arranged around the circumference of the filament was observed occasionally. This latter image may represent the organization of the subfilaments in the bare zone region of the filament, resulting from sampling of individual filaments displaced longitudinally relative to the other filaments in the A-band.

Non-uniform staining of myofibril a bands by a monoclonal antibody to skeletal muscle myosin S1 heavy chain.

A monoclonal antibody specific for the S1 fragment of skeletal muscle myosin has been identified. The antibody does not inhibit actin-activated Mg2+-ATPase or K+-EDTA-activated ATPase of myosin, indicating that it is not related to the portion of the S1 which carries the ATPase activity. In the absence of relaxing medium, antibody binding to the myosin filament is restricted to narrow regions on each side of the bare zone region of the filament, and to a narrow region at the tapered ends of the filament. This restricted antibody binding is not altered by the attachment of the myosin cross-bridges to the actin filaments. In the presence of relaxing medium, antibody binding occurs along the entire length of the cross-bridge-bearing region of the filament. The restricted binding to only small regions of the filament in the absence of relaxing medium suggests that the molecular packing of the myosin in different portions of the filament may be different, resulting in differences in the availability of the antigenic site on the S1 for antibody binding. The change in availability of the antigenic sites along the filament in the presence of relaxing medium may reflect a perturbation in the molecular packing of the filament, or a conformational change resulting from the binding of MgATP, both of which could affect the availability of the antigenic sites on the S1 for antibody.

The Z-band: 85,000-dalton amorphin and alpha-actinin and their relation to structure.

The conclusions arrived at as a result of this work can be summarized as follows: (a) We have found that there is an 85,000-dalton protein, which we have called 85K amorphin, associated with the Z-band of chicken pectoralis muscle myofibrils. We have isolated and purified this protein. It is not a structural component of the Z-filaments since it can be extracted completely without extraction of the Z-filaments. Extraction of 85K amorphin results in loss of specific staining of the Z-band with fluorescence specific anti-85K amorphin. (b) We have found that alpha-actinin is the structural component of the Z-filaments, since extraction of alpha-actinin is accompanied by loss of the Z-filament structure.

alpha-Actinin and membrane glycoprotein IIIa are different proteins in human blood platelets.

It has been suggested that a platelet protein that is very similar to muscle alpha-actinin is identical to the membrane glycoprotein IIIa (GPIIIa) of platelets and is responsible for anchoring actin filaments directly into the plasma membrane of platelets. To determine if alpha-actinin and GPIIIa are related in platelets, we analyzed the purified proteins on 5% sodium dodecyl sulfate/polyacrylamide gels. The two proteins differ in mobility in both the unreduced and reduced states, and they stain differently with silver stain. In addition, alpha-actinin is a prominent component of the detergent-insoluble cytoskeletons of platelets, whereas GPIIIa is absent from these structures. By using monospecific antisera to the individual proteins, it was demonstrated that alpha-actinin and GPIIIa are immunologically distinct. We conclude that alpha-actinin and GPIIIa are different proteins in human blood platelets and that it is unlikely that alpha-actinin is an integral membrane protein.

The myosin filament. VIII. Preservation of subfilament organization.

Different multistage fixation procedures patterned after the procedure described by Reedy (1976) have been evaluated with regard to preservation of subfilament structural organization along the length of the vertebrate skeletal myosin filament. The criteria used for evaluation of structural preservation include (a) the precision of subfilament organization as reflected by the quality of the optical diffraction patterns obtained from images of transverse sections of the myosin filament and (b) the clarity with which structural differences in serial transverse sections along the myosin filament could be defined.