Axial disposition of myosin heads in isometrically contracting muscles

Meridional x-ray diffraction diagrams, recorded with high angular resolution, from muscles contracting at the plateau of isometric tension show that the myosin diffraction orders are clusters of peaks. These clusters are due to pronounced interference effects between the myosin diffracting units on either side of the M-line. A theoretical analysis based on the polarity of the myosin (and actin) filaments shows that it is possible to extract phase information from which the axial disposition of the myosin heads can be determined. The results show that each head in a crown pair has a distinct structural disposition. It appears that only one of the heads in the pair stereospecifically interacts with the thin filament at any one time.     

Structural changes of actin-bound myosin heads after a quick length change in frog skeletal muscle

Changes in the x-ray diffraction pattern from a frog skeletal muscle were recorded after a quick release or stretch, which was completed within one millisecond, at a time resolution of 0.53 ms using the high-flux beamline at the SPring-8 third-generation synchrotron radiation facility. Reversibility of the effects of the length changes was checked by quickly restoring the muscle length. Intensities of seven reflections were measured. A large, instantaneous intensity drop of a layer line at an axial spacing of 1/10.3 nm(-1) after a quick release and stretch, and its partial recovery by reversal of the length change, indicate a conformational change of myosin heads that are attached to actin. Intensity changes on the 14.5-nm myosin layer line suggest that the attached heads alter their radial mass distribution upon filament sliding. Intensity changes of the myosin reflections at 1/21.5 and 1/7.2 nm(-1) are not readily explained by a simple axial swing of cross-bridges. Intensity changes of the actin-based layer lines at 1/36 and 1/5.9 nm(-1) are not explained by it either, suggesting a structural change in actin molecules.     

X-ray study of myosin heads in contracting frog skeletal muscle

Using synchrotron radiation, the behaviour of the diffuse X-ray scatter was investigated in the relaxed and active phases of auxotonic and isometric contractions. Muscles were stimulated tetanically for 0.75 of a second, leaving intervals of three minutes between successive contractions. In isometric contractions the scatter is very asymmetric, which means that the myosin heads have a strongly preferred orientation. During tension rise the scatter expands in the meridional direction and contracts in the equatorial direction, the maximal local intensity change being about 20%. The shape change indicates that on average the myosin heads become oriented more perpendicularly to the fibre axis. The distribution of orientations at peak tension is quite different from that we found previously in X-ray scattering data from rigor muscles. In auxotonic contractions where muscles shorten against an increasing tension the scatter is practically circularly symmetrical. This suggests that during shortening the myosin heads go evenly through a wide range of orientations. It is concluded that the results from both the auxotonic and isometric experiments provide strong support for the rotating myosin head model. In isometric contractions the transition between the relaxed phase and peak tension is accompanied by an overall increase in scattering intensity of about 10%: this corresponds to a relative increase in the fraction of disordered myosin heads by almost 30%.     

Statistical mechanics of myosin molecular motors in skeletal muscles

Statistical mechanics provides the link between microscopic properties of matter and its bulk properties. The grand canonical ensemble formalism was applied to contracting rat skeletal muscles, the soleus (SOL, n = 30) and the extensor digitalis longus (EDL, n = 30). Huxley's equations were used to calculate force (pi) per single crossbridge (CB), probabilities of six steps of the CB cycle, and peak muscle efficiency (Eff(max)). SOL and EDL were shown to be in near-equilibrium (CB cycle affinity 2.5 kJ/mol) and stationary state (linearity between CB cycle affinity and myosin ATPase rate). The molecular partition function (z) was higher in EDL (1.126+/-0.005) than in SOL (1.050+/-0.003). Both pi and Eff(max) were lower in EDL (8.3+/-0.1 pN and 38.1+/-0.2%, respectively) than in SOL (9.2+/-0.1 pN and 42.3+/-0.2%, respectively). The most populated step of the CB cycle was the last detached state (D3) (probability P(D3): 0.890+/-0.004 in EDL and 0.953+/-0.002 in SOL). In each muscle group, both pi and Eff(max) linearly decreased with z and statistical entropy and increased with P(D3). We concluded that statistical mechanics and Huxley's formalism provided a powerful combination for establishing an analytical link between chemomechanical properties of CBs, molecular partition function and statistical entropy.     

Arrangement of myosin heads in relaxed thick filaments from frog skeletal muscle

The distribution of myosin heads on the surface of frog skeletal muscle thick filaments has been determined by computer processing of electron micrographs of isolated filaments stained with tannic acid and uranyl acetate. The heads are arranged in three strands but not in a strictly helical manner and so the structure has cylindrical symmetry. This accounts for the "forbidden" meridional reflections seen in diffraction patterns. Each layer-line therefore represents the sum of terms of Bessel orders 0, +/- 3, +/- 6, +/- 9 and so on. These terms interact so that, unlike a helical object without terms from overlapping Bessel orders, as the azimuth is changed, the amplitude on a layer-line at a particular radius varies substantially and its phase does not alter linearly. Consequently, a three-dimensional reconstruction cannot be produced from a single view. We have therefore used tilt series of three individual filaments to decompose the data on layer-lines 0 to 6 into terms of Bessel orders up to +/- 9 using a least-squares procedure. These data had a least-squares residual of 0.32 and enabled a three-dimensional reconstruction to be obtained at a nominal resolution of 6 nm. This showed, at a radius of about 10 nm, three strands of projecting morphological units with three units spaced along each strand every 42.9 nm axially. We have identified these units with pairs of myosin heads. Successive units along a strand are perturbed axially, azimuthally and radially from the positions expected if the structure was perfectly helical. This may simply be a consequence of steric restrictions in packing the heads on the thick filament surface, but could also reflect an underlying non-helical arrangement of myosin tails, which would be consistent with the thick filament shaft being constructed from three subfilaments in which the tails were arranged regularly. There was also material at a radius of about 6 nm spaced 42.9 nm axially, which we tentatively identified with accessory proteins. The filament shaft had a pronounced pattern of axial staining.     

The aggregation characteristics of column-purified rabbit skeletal myosin in the presence and absence of C-protein at pH 7.0.

The aggregation properties of column-purified rabbit skeletal myosin at pH 7.0 were investigated as functions of ionic strength, protein concentration, and time. Filaments prepared by dialysis exhibited the same average length and population distribution at 0.10 and 0.15 M KCl at protein concentrations greater than 0.10 mg/ml; similar results were obtained at .0.20 M KCl, although average filament length was approximately 0.5 micrometer shorter. Once formed, these length distributions remained virtually unchanged over an 8-d period. At and below 0.10 mg/ml, average filament length decreased as a function of protein concentration; filaments prepared from an initial concentration of 0.02 mg/ml were half the length of those prepared at 0.2 mg/ml. Filaments prepared by dilution exhibited a sharp increase in average length as the time-course increased up to 40 s, then altered only slightly over a further period of 4 min. Addition of C-protein in a molar ratio of 1-3.3 myosin molecules affected most of these results. Average filament length was affected neither by ionic strength nor by initial protein concentration down to 0.04 mg/ml or over an 8-d period. Filaments formed by dilution in the presence of C-protein exhibited a constant average length and hypersharp length distribution over variable time courses up to 7 min. It is possible that C-protein acts to stabilize the antiparallel intermediate during filamentogenesis, and may also affect subunit addition to this nucleus.     

X-ray studies of order-disorder transitions in the myosin heads of skinned rabbit psoas muscles.

Using x-rays from a laboratory source and an area detector, myosin layer lines and the diffuse scattering between them in the moderate angle region have been recorded. At full overlap, incubation of rigor muscles with S-1 greatly reduces the diffuse scattering. Also, three of the four actin-based layer lines lying close to the meridian (Huxley, H. E., and W. Brown, 1967. J. Mol. Biol. 30:384-434; Haselgrove, J. C. 1975. J. Mol. Biol. 92:113-143) increase, suggesting fuller labeling of the actin filaments. These results are consistent with the idea (Poulsen, F. R., and J. Lowy, 1983. Nature [Lond.]. 303:146-152) that some of the diffuse scattering in rigor muscles is due to a random mixture of actin monomers with and without attached myosin heads (substitution disorder). In relaxed muscles, regardless of overlap, lowering the temperature from 24 to 4 degrees C practically abolishes the myosin layer lines (a result first obtained by Wray, J.S. 1987. J. Muscle Res. Cell Motil. 8:62 (a). Abstr.), whilst the diffuse scattering between these layer lines increases appreciably. Similar changes occur in the passage from rest to peak tetanic tension in live frog muscle (Lowy, J., and F.R. Poulsen. 1990. Biophys. J. 57:977-985). Cooling the psoas demonstrates that the intensity relation between the layer lines and the diffuse scattering is of an inverse nature, and that the transition occurs over a narrow temperature range (12-14 degrees C) with a sigmoidal function. From these results it would appear that the helical arrangement of the myosin heads is very temperature sensitive, and that the disordering effect does not depend on the presence of actin. Measurements along the meridian reveal that the intensity of the diffuse scattering increases relatively little and does so in a nearly linear manner: evidently the axial order of the myosin heads is much less temperature sensitive. The combined data support the view (Poulsen, F. R., and J. Lowy. 1983. Nature [Lond.]. 303:146-152) that in relaxed muscles a significant part of the diffuse scattering originates from disordered myosin heads. The observation that the extent of the diffuse scattering is greater in the equatorial than in the meridional direction suggests that the disordered myosin heads have an orientation which is on average more parallel to the filament axis.     

Properties of the alkali light-chain-20-kilodalton fragment complex from skeletal myosin heads

We have developed a rapid and reproducible procedure widely applicable to the preparation of pure aqueous solutions of the complex between an alkali light chain and the COOH-terminal heavy-chain fragments of skeletal myosin chymotryptic subfragment 1 (S-1) split by various proteases. It was founded on the remarkable ethanol solubility of these complexes. A systematic study of the ethanol fractionation of the tryptic (27K-50K-20K)-S-1 (A2) showed the NH2-terminal 27K fragment to behave like a specific protein entity being quantitatively precipitated at a relatively low ethanol concentration. Only the 20K peptide-A2 complex remained in solution when the S-1 derivative was treated with exactly 4 volumes of ethanol in the presence of 6 M guanidinium chloride. At a lower ethanol concentration, a soluble mixture of 50K and 20K peptides together with the light chain was obtained. The isolated 20K fragment-A2 system containing a 1:1 molar ratio of each component was investigated by biochemical and 1H nuclear magnetic resonance (NMR) techniques to highlight its structure and the interaction of the 20K heavy-chain segment with F-actin and with the light chain. During the treatment of the complex with alpha-chymotrypsin, only the 20K peptide was fragmented in contrast to its stability within the whole S-1. The binding of F-actin to the complex led, however, to a strong inhibition of its chymotryptic degradation. 1-Ethyl-3-[3-(dimethylamino)propyl]carbodiimide cross-linking of F-actin to the complex produced covalent actin-20K peptide only, the amount of which was lower relative to that observed with the entire split S-1.(ABSTRACT TRUNCATED AT 250 WORDS)     

Orientational dynamics of indane dione spin-labeled myosin heads in relaxed and contracting skeletal muscle fibers.

We have used electron paramagnetic resonance (EPR) spectroscopy to study the orientation and rotational motions of spin-labeled myosin heads during steady-state relaxation and contraction of skinned rabbit psoas muscle fibers. Using an indane-dione spin label, we obtained EPR spectra corresponding specifically to probes attached to Cys 707 (SH1) on the catalytic domain of myosin heads. The probe is rigidly immobilized, so that it reports the global rotation of the myosin head, and the probe's principal axis is aligned almost parallel with the fiber axis in rigor, making it directly sensitive to axial rotation of the head. Numerical simulations of EPR spectra showed that the labeled heads are highly oriented in rigor, but in relaxation they have at least 90 degrees (Gaussian full width) of axial disorder, centered at an angle approximately equal to that in rigor. Spectra obtained in isometric contraction are fit quite well by assuming that 79 +/- 2% of the myosin heads are disordered as in relaxation, whereas the remaining 21 +/- 2% have the same orientation as in rigor. Computer-simulated spectra confirm that there is no significant population (> 5%) of heads having a distinct orientation substantially different (> 10 degrees) from that in rigor, and even the large disordered population of heads has a mean orientation that is similar to that in rigor. Because this spin label reports axial head rotations directly, these results suggest strongly that the catalytic domain of myosin does not undergo a transition between two distinct axial orientations during force generation. Saturation transfer EPR shows that the rotational disorder is dynamic on the microsecond time scale in both relaxation and contraction. These results are consistent with models of contraction involving 1) a transition from a dynamically disordered preforce state to an ordered (rigorlike) force-generating state and/or 2) domain movements within the myosin head that do not change the axial orientation of the SH1-containing catalytic domain relative to actin.     

Structural dynamics of actin during active interaction with myosin: different effects of weakly and strongly bound myosin heads

We have used optical spectroscopy (transient phosphorescence anisotropy, TPA, and fluorescence resonance energy transfer, FRET) to detect the effects of weakly bound myosin S1 on actin during the actomyosin ATPase cycle. The changes in actin were reported by (a) a phosphorescent probe (ErIA) attached to Cys 374 and (b) a FRET donor-acceptor pair, IAEDANS attached to Cys 374 and a nucleotide analogue (TNPADP) in the nucleotide-binding cleft. Strong interactions were detected in the absence of ATP, and weak interactions were detected in the presence of ATP or its slowly hydrolyzed analogue ATP-gamma-S, under conditions where a significant fraction of weakly bound acto-S1 complex was present and the rate of nucleotide hydrolysis was low enough to enable steady-state measurements. The results show that actin in the weakly bound complex with S1 assumes a new structural state in which (a) the actin filament has microsecond rotational dynamics intermediate between that of free actin and the strongly bound complex and (b) S1-induced changes are not propagated along the actin filament, in contrast to the highly cooperative changes due to the strongly bound complex. We propose that the transition on the acto-myosin interface from weak to strong binding is accompanied by transitions in the structural dynamics of actin parallel to transitions in the dynamics of interacting myosin heads.     

Measurement of the fraction of myosin heads bound to actin in rabbit skeletal myofibrils in rigor

Tryptic digestion of rabbit skeletal myofibrils at physiological ionic strength and pH results in cleavage of the myosin heavy chain at one site giving two bands (M_r = 200,000 and 26,000) on sodium dodecyl sulfate/polyacrylamide gels. Following addition of sodium pyrophosphate (to 1 mm) to dissociate the myosin heads from actin, tryptic proteolysis results in production of three bands, 160K², 51K and 26K, with a 74K band appearing as a precursor of the 51K and 26K species. Under these conditions, there is insignificant cleavage of heavy chain to the heavy and light meromyosins. Trypsin-digested myofibrils yield the same amount of rod as native myofibrils when digested with papain. These results indicate that actin blocks tryptic cleavage of the myosin heavy chain at a site 74K from the N terminus. From measurements of the amount of 51K species formed by digestion of rigor fibers at various sarcomere lengths, we estimate that at least 95% of the myosin heads are bound to actin at 100% overlap of thick and thin filaments. Hence all myosin molecules can bind to actin, and consequently both heads of a myosin molecule can interact simultaneously with actin filaments under rigor conditions.     

Changes in myosin ATPase activity in skeletal muscles of rat during cold stress

Three skeletal muscles viz., gastrocnemius, pectoralis and diaphragm from rats acclimated to a low temperature (4 +/- 1 degrees C; 16 hr daily; maximum for 8 weeks) exhibit an increased myosin ATPase activity. An analysis of native myosin from these muscles under non-dissociating conditions reveals two myosin isozymes instead of a single isozyme expressed in control muscles. Isoelectric focusing (IEF) coupled with two dimensional sodium dodecyl sulfate polyacrylamide gel electrophoresis (2-D SDS-PAGE) confirms an increased phosphorylation of myosin light chain 2 (MLC2) in muscles from cold acclimated rats.     

Shape and length of myosin heads.

There is controversy concerning the shape and length of myosin heads. In the present paper we try to analyse the data and to draw clear conclusions in this field. When the myosin heads are isolated (S1) from the rest of the molecule, their length is approximately 12 nm and their shape is close to that of a prolate ellipsoid with an axial ratio approximately 2.3 (in solution) or close to that of a comma when attached to F-actin (with a length of 12-13 nm). When the myosin heads are observed on a whole molecule, their length is approximately 19 nm and they are pear-shaped. Here we suggest that all these observations are compatible. We believe that, for a whole myosin molecule, a large part of the head-rod joint (S1/S2 joint) is measured with the head, owing to a particularly heavy staining or shadowing of this joint. On the other hand, S1 is probably built up of a head part plus the S1/S2 joint, which is not revealed by the usual techniques (hydrodynamics, X-ray and neutron scattering). Finally, the comma shape would be related to a flexible part in the head region of S1, which is significantly bent when S1 is attached to F-actin, but which would be less bent for S1 in solution. A similar bending also occurs in crystalline S1.     

Dystonia musculorum mutation and myosin heavy chain expression in skeletal and cardiac muscles.

This study evaluated the influence of dystonia musculorum (dt) mutation, characterized by spinocerebellar fibers degeneration, on cardiac and skeletal muscles: one respiratory (diaphragm, Dia), three masticatory (anterior temporalis, AT; masseter superficialis, MS; and anterior digastric, AD), one hindlimb (soleus, S), tongue (T), and one cardiac (ventricle, V). Body and muscle weight, muscle protein content, and myosin heavy chain (MHC) isoforms relative expression were then compared in dt mutant mice and in normal mice, according to sex. Male body and muscle weight was always greater than that of females, but there was no specific muscle difference in females. dt mutant mice showed a reduced whole body growth but no specific muscle atrophy, as well as a global decrease in muscle protein content that made muscles more fragile. dt mutation induced a global reduction of muscle protein concentration, whereas a general influence of sex could not be disclosed. Concerning MHC relative composition, all the muscles were fast-twitch: Dia, AT, MS, AD, S, and T expressed predominantly the fast type 2 MHC isoforms, whereas V contained only MHC alpha, also a fast MHC. Female muscles were slower than male muscles, except for S, which was faster. However, classification of muscles in terms of shortening velocity was very different in normal males and females. In other respects, dt mutant muscles were slower and consequently more fatigue resistant than normal, except for S, which became faster and less fatigue resistant. dt mutation exhibits then a specific effect on this continually active postural muscle. In the other muscles, global increased fatigue resistance could constitute an adaptive response to work requirements modifications linked to the muscle damage. It should be noted that a developmental MHC (neonatal) was present in female dt AD. Innervation, which influences muscle structure, is altered in dt mutant and could be another causal factor of the fast-to-slow MHC switches. It appears that dystonin, the dt gene product, is very important in maintaining the structural integrity of both cardiac and skeletal muscle and in its absence, the muscle becomes more fragile and is damaged by modified activity.     

Two non-identical heads of myosin molecules

Four different preparations of skeletal subfragment-1, denoted in this report as S1(Aa), S1(Ab), S1(Ba), and S1(Bb), and two different preparations of cardiac subfragment-1, denoted as S1(A) and S1(B), were obtained as described in our recent report (J. Biochem. 97, 965, 1985). (i) The four preparations were obtained from chicken breast myosin trinitrophenylated with 2,4,6-trinitrobenzene sulfonate in the absence of inorganic pyrophosphate (-PPi), and they were all shown to be trinitrophenylated. Addition of PPi caused change in the absorption spectra of trinitrophenyl(TNP)-S1(Aa) and TNP-S1(Ba), but not in those of TNP-S1(Ab) and TNP-S1(Bb). (ii) The two preparations of S1 were obtained from cardiac myosin trinitrophenylated either in the absence (-) or presence (+) of PPi. S1(B) was trinitrophenylated, whereas S1(A) was not. Specifically emphasized is the observation that the yield of cardiac S1(A) was practically equal to that of cardiac S1(B). On the basis of these results, we propose the hypothesis of "two iso-myosins with non-identical heads," which is essentially a combination of the hypothesis of isoenzymes and that of non-identical heads.     

Molecular movements promoted by metal nucleotides in the heavy-chain regions of myosin heads from skeletal muscle

Molecular movements generated in the heavy-chain regions (27-50-20(X 10(3)) Mr) of myosin S1 on interaction with nucleotides ATP, AMPPNP, ADP and PPi were investigated by limited proteolysis of several enzyme-metal nucleotide complexes in the absence and presence of reversibly bound and crosslinked F-actin. The rate and extent of the nucleotide-promoted conversion of the NH2-terminal 27 X 10(3) Mr and 50 X 10(3) Mr segments into products of 22 X 10(3) Mr and 45 X 10(3) Mr, respectively, were estimated to determine the amplitude of the molecular movements. The 22 X 10(3) Mr peptide was identified by amino acid sequence studies as being derived from cleavage of the peptide bond between Arg and Ile (at position 23 to 24). The 45 X 10(3) Mr peptide, previously shown to represent the NH2-terminal part of the 50 X 10(3) Mr region, would be connected to the adjacent C-terminal 20 X 10(3) Mr region by a pre-existing loop segment of about 5 X 10(3) Mr; the proteolytic sensitivity of the latter region is increased particularly by nucleotide binding. The tryptic reaction proved to be a sensitive indicator of the conformational state of the liganded heavy chain as the rate of peptide bond cleavage in the two regions is dependent on the nature of the bound ligand; it decreases in the order: ATP greater than AMPPNP greater than ADP greater than PPi. It depends also on the nature of the metal present, Mg2+ and Ca2+ being much more effective than K+. Binding of F-actin to the S1-MgAMPPNP complex affords significant protection against breakdown of 27 X 10(3) Mr and 50 X 10(3) Mr peptides, but with concomitant hydrolysis of the 50 X 10(3) Mr-20 X 10(3) Mr junction. Additionally, interaction of MgATP with HMM modulates the tryptic fission of the S1-S2 region. The overall data provide a molecular support for the two-state model of the myosin head and emphasize the involvement of the 50 X 10(3) Mr unit in the mechanism of coupling between the actin and nucleotide binding sites.     

Heterogeneity and distribution of fast myosin heavy chains in some adult vertebrate skeletal muscles.

Three monoclonal antibodies, LM5, F2 and F39 raised to chicken fast skeletal muscle myosin, specific for myosin heavy chain (MHC) subunit, were used to study the composition and distribution of this protein in some vertebrate skeletal muscles. These antibodies in immunohistochemical investigations did not react with the majority of the type I fibres in most muscles. Antibodies LM5 and F39 stained all the type II fibres in all the adult chicken skeletal muscles studied. Antibody F2 also stained all the type II fibres in most chicken skeletal muscles tested except in gastrocnemius in which a proportion of both the type IIA and IIB fibres either did not stain or stained only weakly. Antibody F2 unlike LM5 and F39 stained most of the type IIIB fibres in anterior latissimus dorsi (ALD) and IB fibres in red strip of chicken Pectoralis muscle. Antibodies LM5 and F2 in the rat diaphragm reacted with all the type IIA and IIB fibres, while antibody F39 stained only the type IIB fibres darkly with most IIA fibres being either not stained or only weakly stained. In the rat extensor digitorum longus (EDL) and tibialis anterior (TA) muscles, antibody LM5 stained all the IIA and IIB fibres. Antibody F2 in these muscles stained all the type IIA fibres but only a proportion of the IIB fibres. The remaining IIB fibres were either unstained or only weakly positive. Antibody F39 in rat EDL and TA muscles did not only distinguish subgroups of IIB fibres (dark, intermediate and negative or very weak) but also of the IIA fibres. These three antibodies used together therefore detected a great deal of heterogeneity in the myosin heavy chain composition and muscle fibre types of several skeletal muscles.