Evidence for Unique Structural Change of Thin Filaments upon Calcium Activation of Insect Flight Muscle

Upon activation of living or skinned vertebrate skeletal muscle fibers, the sixth X-ray layer-line reflection from actin (6th ALL) is known to intensify, without a shift of its peak position along the layer line. Since myosin attachment to actin is expected to shift the peak towards the meridian, this intensification is considered to reflect the structural change of individual actin monomers in the thin filament. Here, we show that the 6th ALL of skinned insect flight muscles (IFMs) is rather weakened upon isometric calcium activation, and its peak shifts away from the meridian. This suggests that the actin monomers in the two types of muscles change their structures in substantially different manners. The changes that occurred in the 6th ALL of IFM were not diminished by lowering the temperature from 20 to 5 °C, while active force was greatly reduced. The inclusion of 100 μM blebbistatin (a myosin inhibitor) did not affect the changes either. This suggests that calcium binding to troponin C, rather than myosin binding to actin, causes the structural change of IFM actin.     

X-ray diffraction evidence for the lack of stereospecific protein interactions in highly activated actomyosin complex

The structure of actomyosin complex while hydrolyzing ATP was investigated by recording X-ray diffraction patterns from rabbit skeletal muscle fibers, in which exogenously introduced rabbit skeletal subfragment-1 (S1) was covalently cross-linked to the endogenous actin filaments in rigor by 1-ethyl-3-(3-dimethylaminopropyl) carbodiimide (EDC). Approximately two-thirds of the introduced S1 was cross-linked. The cross-linking procedure did not affect the profile of the S1-induced enhancement of the actin-based layer line reflections in rigor, indicating that the acto-S1 interactions remained highly stereospecific. In the presence of ATP, the MgATPase of the S1 was highly activated regardless of calcium levels, presumably because the availability of the stereospecific binding sites for both proteins was maximized by the cross-linking. However, the diffraction pattern in the presence of ATP was striking in that the intensity profile of the strong 1/5.9 nm(-1) layer lines was indistinguishable from that from bare actin filaments, despite the fact that the majority of the S1 was still associated with actin. The change of the intensity profiles upon addition of ATP was completely reversible. Model calculations showed that this result can be explained if the S1 is not only swinging around its pivoting point, but the pivoting point itself is also moving on the actin surface in a range of a few nanometers. The results suggest that the stereospecific binding sites, which have been considered important for actomyosin cycling, are paradoxically left unoccupied for most of the time in this highly activated actomyosin complex.     

X-ray diffraction patterns from mammalian heart muscle

We have obtained light and X-ray diffraction patterns from trabecular and papillary muscles of various mammalian hearts in the living resting state and in rigor. Equatorial X-ray diffraction patterns from living muscles show the 1,0 and 1,1 reflections from a hexagonal lattice of filaments. The lattice spacing varies with sarcomere length over the observable range (2·0 to 2·5 μm) in such a manner that the lattice volume remains constant. In the living resting state the 1,0 reflection is stronger than the 1,1 reflection, whereas in rigor the 1,1 reflection is almost as strong as the 1,0 reflection. These intensity changes are similar to those found in vertebrate skeletal muscle, suggesting that the mechanism of cross-bridge attachment to actin is similar in both muscles.Two types of meridional X-ray diffraction pattern were observed in muscles in different conditions. One type, obtained from dead or glycerol-extracted muscles or from muscles treated with iodoacetate, showed a strong actin-related pattern but only a weak pattern associated with myosin. This type of pattern was similar to that from vertebrate skeletal muscle in rigor. The other type, obtained from living, resting muscle, showed a weaker actin pattern but a stronger myosin pattern. The myosin pattern included layer-line reflections associated with projections from the thick filaments. This second type of pattern was similar to that from resting vertebrate skeletal muscle, but the layer lines were weaker. The weakness of the myosin layer lines may indicate that part of the high resting tension found in heart muscle arises from a small amount of actin-myosin interaction in the resting state. Such interaction could provide a mechanism for varying the diastolic length of heart muscle and thereby the diastolic volume of the heart.     

X-ray diffraction evidence for the extensibility of actin and myosin filaments during muscle contraction.

To clarify the extensibility of thin actin and thick myosin filaments in muscle, we examined the spacings of actin and myosin filament-based reflections in x-ray diffraction patterns at high resolution during isometric contraction of frog skeletal muscles and steady lengthening of the active muscles using synchrotron radiation as an intense x-ray source and a storage phosphor plate as a high sensitivity, high resolution area detector. Spacing of the actin meridional reflection at approximately 1/2.7 nm-1, which corresponds to the axial rise per actin subunit in the thin filament, increased about 0.25% during isometric contraction of muscles at full overlap length of thick and thin filaments. The changes in muscles stretched to approximately half overlap of the filaments, when they were scaled linearly up to the full isometric tension, gave an increase of approximately 0.3%. Conversely, the spacing decreased by approximately 0.1% upon activation of muscles at nonoverlap length. Slow stretching of a contracting muscle increased tension and increased this spacing over the isometric contraction value. Scaled up to a 100% tension increase, this corresponds to a approximately 0.26% additional change, consistent with that of the initial isometric contraction. Taken together, the extensibility of the actin filament amounts to 3-4 nm of elongation when a muscle switches from relaxation to maximum isometric contraction. Axial spacings of the layer-line reflections at approximately 1/5.1 nm-1 and approximately 1/5.9 nm-1 corresponding to the pitches of the right- and left-handed genetic helices of the actin filament, showed similar changes to that of the meridional reflection during isometric contraction of muscles at full overlap. The spacing changes of these reflections, which also depend on the mechanical load on the muscle, indicate that elongation is accompanied by slight changes of the actin helical structure possibly because of the axial force exerted by the actomyosin cross-bridges. Additional small spacing changes of the myosin meridional reflections during length changes applied to contracting muscles represented an increase of approximately 0.26% (scaled up to a 100% tension increase) in the myosin periodicity, suggesting that such spacing changes correspond to a tension-related extension of the myosin filaments. Elongation of the myosin filament backbone amounts to approximately 2.1 nm per half sarcomere. The results indicate that a large part (approximately 70%) of the sarcomere compliance of an active muscle is caused by the extensibility of the actin and myosin filaments; 42% of the compliance resides in the actin filaments, and 27% of it is in the myosin filaments.     

Enhanced stability of isolated muscles and actomyosin due to the action of anesthetics in subnarcotic concentrations

Subnarcotic concentrations of anesthetics and model anesthetics prolong the survival time of isolated living frog skeletal muscles, the time of contractile ability of the same glycerinated muscles, and the time of frog skeleton muscle actomyosin denaturation. The mode of anesthetic action involves hydrophobic interactions of anesthetics with the investigated biosystems. According to the quantitative analysis, physico-chemical parameters of the anesthetic-binding sites are identical in muscle and in muscle models. This result is interpreted as an evidence that anesthetic-evoked rising of contractile protein stability may be involved in the mechanism of stabilization of isolated muscles.     

Denaturation time of actomyosin exposed to different chemicals]

The frog sceleton muscle actomyosin denaturation time dependence on the concentration of salts (NaCl and CaCl2) and organic chemicals (carbohydrates, narcotics and alcohols) was investigated. The following effects were detected: phase change in denaturation time associated with the rise of concentration of chemicals under study; actomyosin stabilization effect; coincidence of concentrations giving rise to protein stability with those increasing the survival time of isolated frog sceleton muscles in vitro (literature data); denaturation effect of alcohols used, both in high and very low concentrations.     

Structural changes during activation of frog muscle studied by time-resolved X-ray diffraction

The pattern given by contracting frog muscle can be followed with high time resolution using synchrotron radiation as a high-intensity X-ray source. We have studied the behaviour of the second actin layer-line (axial spacing of approximately 179 A) at an off-meridional spacing of approximately 0.023 A-1, a region of the diagram that is sensitive to the position of tropomyosin in the thin filaments. In confirmation of earlier work, we find that there is a substantial increase in the intensity of this part of the pattern during contraction. We find that the reflection reaches half its final intensity about 17 milliseconds after the stimulus at 6 degrees C. The changes in the equatorial reflections, which arise from movement of crossbridges towards the thin filaments, occur with a delay of about 12 to 17 milliseconds relative to this change in the actin pattern. In over-stretched muscle, where thick and thin filaments no longer overlap, the changes in the actin second layer-line still take place upon stimulation with a time course and intensity similar to that observed at full overlap. This indicates that tropomyosin movement, in response to calcium binding to troponin, is the first structural step in muscular contraction, and is the prerequisite for myosin binding. A change in intensity similar to that found in contracting muscle is seen in rigor, where tropomyosin is probably locked in the active position. During relaxation the earlier stages in the decrease in intensity of the second actin layer-line take place significantly sooner after the last stimulus than tension decay. In over-stretched muscles the intensity decay is appreciably faster than in the same muscles at rest length, where attached crossbridges may interfere with the return of tropomyosin to its resting position.     

STUDIES ON MUSCLE DIFFERENTIATION. V. ANTIGENICITIES OF MYOSIN AND OF ACTIN FROM FROG SKELETAL MUSCLES1

Both intact and denatured preparations of myosin and actin from frog skeletal muscles produced in rabbits antisera containing antibodies against authentic myosin and actin, respectively, though being contaminated with antibodies against other proteins. Antigenicity of our frog myosin as revealed in agar diffusion tests was indistinguishable from that of cardiac muscle myosin from the same species. Similarly, skeletal muscle myosins from other amphibians shared to a certain extent immunological characteristics with our frog myosin, but those from avian and mammalian materials did not. Similarity in antigenicity was also demonstrated among our skeletal muscle actin, cardiac muscle actin from the same species and skeletal muscle actin from the other anurans studied. However, skeletal muscle actin from an urodele could not clearly be correlated in its immunological properties with our frog actin, and those from avian and mammalian materials were antigenically different from our frog actin. Thus, the degree of antigenic similarity of these muscle proteins seemed to be correlated with the phylogenic relationship of the animals so far studied. The results also indicated that our antisera could only be applied to immuno-cytological and immuno-embryological studies of myosin and actin when the antisera absorbed with the corresponding antigen preparations were used as negative controls.     

Dependence of energy transduction in intact skeletal muscles on the time in tension.

In intact single crayfish muscle fibers and frog semitendinosus muscles we have studied the tension response to sinusoidal length changes in the frequency range of 0.25-133 Hz. By this method we have resolved three processes in the interaction of myosin cross-bridges with actin in fully activated preparations. They are (A) a low-frequency phase advance, (B) a middle-frequency delay, and (C) a high-frequency advance. These processes can be used as probes to study the chemomechanical coupling of contractility. Process (B) represents net power output from the muscle preparation (oscillatory work). With maximal K or caffeine activation of crayfish muscle at 20 degrees C, it decreases to zero in the initial 45 s of maintained tension. Similar results were obtained with frog semitendinosus whole muscles. We interpret this decrease of (B) with time as a gradual decrease in actomyosin ATP-hydrolysis rate.     

X-ray diffraction studies on muscle regulation

Using the intensity of the outer part of the second actin layer line as an indicator of thin filament conformation in vertebrate muscle we were able to identify the four different states of rest, and the three states induced by the presence of Ca²⁺ ions, rigor bridge attachment and actively cycling bridges, respectively. These findings are in qualitative agreement with a number of biochemical studies by Eisenberg and Greene and others, indicating that activation of the thin filament depends both on Ca²⁺ ions and crossbridge binding. Yet quantitatively, the biochemical data and our structural data are contradictory. Whereas the biochemical studies suggest a strong coupling between structural changes of the thin filament and the ATPase activity, the structural studies indicate that this is not necessarily the case.Troponin molecules also change their conformation upon activation depending on both Ca²⁺ ions and crossbridge binding as demonstrated by the early part of the time course of the thin filament meridional reflections in contracting frog muscle.Low ionic strength which has been shown by Brenner and collaborators to increase weakly binding crossbridges in relaxed rabbit psoas muscle does not influence the intensity of the second actin layer line in this muscle. Yet in contracting frog muscle the increase of the second actin layer line increases very rapidly in one step, suggesting that weak binding bridges which are attached to actin prior to force production may indeed influence the thin filament conformation. It therefore appears that weakly bound bridges in the low ionic strength state do not have the same effect on the thin filament conformation as weakly bound bridges in an actively contracting muscle.Arthropod muscles like the thin filament regulated lobster muscles differ from vertebrate muscle in not showing an increase of the second layer line during contraction, which may have to do with differences in crossbridge attachment. The myosin-regulated molluscan muscle ABRM shows a large increase on the second actin layer line upon phasic contraction and a much smaller increase in catch or rigor, indicating that actively cycling bridges influence the thin filament conformation differently than catch or rigor bridges.Several pieces of evidence which we have briefly outlined in this paper suggest that the thin filament conformational changes we have observed do not arise solely from tropomyosin movements and that conformational changes of actin domains should be considered.     

Non-specific termination of simian virus 40 DNA replication.

Axial X-ray diffraction patterns have been studied from relaxed, contracted and rigor vertebrate striated muscles at different sarcomere lengths to determine which features of the patterns depend on the interaction of actin and myosin. The intensity of the myosin layer lines in a live, relaxed muscle is sometimes less in a stretched muscle than in the muscle at rest-length; the intensity depends not only on the sarcomere length but on the time that has elapsed since dissection of the muscle. The movement of cross-bridges giving rise to these intensity changes are not caused solely by the withdrawal of actin from the A-band.When a muscle contracts or passes into rigor many changes occur that are independent of the sarcomere length: the myosin layer lines decrease in intensity to about 30% of their initial value when the muscle contracts, and disappear completely when the muscle passes into rigor. Both in contracting and rigor muscles at all sarcomere lengths the spacings of the meridional reflections at 143 Å and 72 Å are 1% greater than from a live relaxed muscle at rest-length. It is deduced that the initial movement of cross-bridges from their positions in resting muscle does not depend on the interaction of each cross-bridge with actin, but on a conformational change in the backbone of the myosin filament: occurring as a result of activation. The possibility is discussed that the conformational change occurs because the myosin filament, like the actin filament, has an activation control mechanism. Finally, all the X-ray diffraction patterns are interpreted on a model in which the myosin filament can exist in one of two possible states: a relaxed state which gives a diffraction pattern with strong myosin layer lines and an axial spacing of 143.4 Å, and an activated state which gives no layer lines but a meridional spacing of 144.8 Å.     

AMP and IMP Dissociate Actomyosin into Actin and Myosin

We investigated to determine why heating of squid muscle at 60 °C induced the liberation of actin from myofibrils. When a mixture of a myofibrillar fraction and a low-molecular sarcoplasmic fraction prepared from squid muscle was heated at 60 °C, actin liberation occurred. When a myofibrillar fraction was heated with ATP, AMP, or IMP, actin liberation occurred. Hence, AMP is perhaps one of the factors causing actin liberation in postmortem squid muscle. It was found that AMP and IMP reversibly dissociated actomyosin of chicken, bovine, and porcine skeletal muscles into actin and myosin on incubation at 0 °C at pH 7.2 in 0.2 M KCl. These results led us to conclude that AMP and IMP were the most responsible factors causing actin liberation from myofibrils in the heated muscle and causing reversible dissociation of actomyosin on storage of skeletal muscle at a low temperature. Hence, AMP and IMP are possible factors causing the resolution of rigor mortis in muscles.     

AMP and IMP dissociate actomyosin into actin and myosin

We investigated to determine why heating of squid muscle at 60 degrees C induced the liberation of actin from myofibrils. When a mixture of a myofibrillar fraction and a low-molecular sarcoplasmic fraction prepared from squid muscle was heated at 60 degrees C, actin liberation occurred. When a myofibrillar fraction was heated with ATP, AMP, or IMP, actin liberation occurred. Hence, AMP is perhaps one of the factors causing actin liberation in postmortem squid muscle. It was found that AMP and IMP reversibly dissociated actomyosin of chicken, bovine, and porcine skeletal muscles into actin and myosin on incubation at 0 degrees C at pH 7.2 in 0.2 M KCl. These results led us to conclude that AMP and IMP were the most responsible factors causing actin liberation from myofibrils in the heated muscle and causing reversible dissociation of actomyosin on storage of skeletal muscle at a low temperature. Hence, AMP and IMP are possible factors causing the resolution of rigor mortis in muscles.     

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.     

Time-resolved x-ray diffraction studies on the intensity changes of the 5.9 and 5.1 nm actin layer lines from frog skeletal muscle during an isometric tetanus using synchrotron radiation.

Time-resolved x-ray diffraction studies have been made on the 5.9- and 5.1-nm actin layer lines from frog skeletal muscles during an isometric tetanus at 6 degrees C, using synchrotron radiation. The integrated intensities of these actin layer lines were found to increase during a tetanus by 30-50% for the 5.9-nm reflection and approximately 70% for the 5.1-nm reflection of the resting values. The intensity increase of both reflections was greater than that taking place in the transition from rest to rigor state. The intensity change of the 5.9-nm reflection preceded those of the myosin 42.9-nm off-meridional reflection and of the equatorial reflections, as well as the isometric tension development. The intensity profile of the 5.9-nm layer line during contraction was found to be different from that observed in the rigor state.     

The nature of the changes in the activity of water-soluble enzymes in action on the muscles of damaging agents. VI. Glyceraldehyde-3-phosphate dehydrogenase binding and enzyme adsorption by F-actin in ghost muscle fiber]

A possibility of binding glyceraldehyde-3-phosphate dehydrogenase (GAPhDG) in frog (Rana temporaria L.) skeletal muscles was studied by measuring its solubilization in 0.15 M KCl and by its presence in isolated actomyosin. Using a 0.15 M KCl solution, more GAPhDG was extracted from intact muscles and muscles treated with heat at 38, 42 and 46 degrees C for 15 min than in a non-electrolyte medium. Actomyosin isolated from muscles reveals GAPhDG activity which cannot be removed by actomyosin reprecipitation. In myosin-, troponin- and tropomyosin-free single glycerinated muscle fibres (ghost fibres) GAPhDG absorption to F-actin was shown. It is suggested that under thermal injure of muscle cells, the increase in GAPhDG binding with thermolabile proteins of actomyosin complex may occur.     

Age peculiarities of actin polymerization in calves]

Studies have been made on the developmental changes in the polymerization degree of unfractionated actin extracts from skeletal muscles of 3-8-month calf embryos and adult cattle. It was shown that during the development, the polymerization capacity of actin increases, the increase being accompanied by a significant rise in the molecular weight of the protein. The pattern of age changes in the degree of polymerization of actin is similar to that in the molecular weight of actomyosin. Differences in fractional composition of actin extracts from skeletal muscles at various stages of embryonic development were observed. These differences may be responsible for age peculiarities of actin polymerization and may be associated with the formation of contractile activity in ontogenesis.     

"Crystalline" myosin cross-bridge array in relaxed bony fish muscle. Low-angle x-ray diffraction from plaice fin muscle and its interpretation

Detailed structural analysis of muscles normally used to study myosin cross-bridge behavior (e.g., frog sartorius muscle, insect flight muscle) is extremely difficult due to the statistical disorder inherent in their myosin filament arrays. Bony fish muscle is different from all other muscle types in having a myosin filament (A-Band) array with good three-dimensional (crystalline) regularity that is coherent right across each myofibril. Rigorous structure analysis is feasible with fish muscle. We show that low-angle x-ray diffraction patterns from plaice fin muscle contain characteristic vertebrate layer lines at orders of 429 (+/- 0.2) A, that these layer lines are well sampled by row-lines from a simple hexagonal lattice of a-spacing 470 (+/- 2.0) A at rest length and that there are meridional reflections, due to axial perturbations of the basic helix of myosin heads, similar in position to those from frog muscle but differing in relative intensities. Clear trends based on modeling to a resolution of 130 A of the observed intensities in the low angle x-ray diffraction pattern from relaxed plaice fin muscle suggest that: (a) the pattern out to 130 A is more sensitive to the distribution of the two heads than it is to details of the head shape, (b) both heads in one myosin molecule probably tilt axially in the same direction by approximately 20-40 degrees relative to a normal to the thick filament backbone, (c) the center of mass of the heads is at 145 to 160 A radius, and (d) the two heads form a compact structure by lying closely adjacent to each other and almost parallel. Little rotational disorder of the heads can occur. Because of its crystallinity, bony fish muscle provides a uniquely useful structural probe of myosin cross-bridge behavior in other muscle states such as rigor and active contraction.     

The Regulation of Catch in Molluscan Muscle

Molluscan catch muscles are smooth muscles. As with mammalian smooth muscles, there is no transverse ordering of filaments or dense bodies. In contrast to mammalian smooth muscles, two size ranges of filaments are present. The thick filaments are long as well as large in diameter and contain paramyosin. The thin filaments contain actin and appear to run into and join the dense bodies. Vesicles are present which may be part of a sarcoplasmic reticulum. Neural activation of contraction in Mytilus muscle is similar to that observed in mammalian smooth muscles, and in some respects to frog striated muscle. The relaxing nerves, which reduce catch, are unique to catch muscles. 5-Hydroxytryptamine, which appears to mediate relaxation, specifically blocks catch tension but increases the ability of the muscle to fire spikes. It is speculated that Mytilus muscle actomyosin is activated by a Ca⁺⁺-releasing mechanism, and that 5-hydroxytryptamine may reduce catch and increase excitability by influencing the rate of removal of intracellular free Ca⁺⁺.     

Changes in the X-ray diffraction pattern from rigor muscles by application of external length changes

The effect of external force on the X-ray pattern from frog muscles in rigor was studied by a time-resolved diffraction technique. When sinusoidal length changes (1.5–3% of the muscle length, 5Hz) were applied to the muscle, the 14.3 nm intensity decreased during the releasing phase and increased during the stretching phase. The intensity ratio of the equatorial 1,0 and 1,1 reflections did not change, nor were there any appreciable intensity changes in the 5.9 nm and 5.1 nm reflections during the length change. Experiments were also done with the relaxed muscles and no change was seen in any reflection, indicating that the rigor linkages are needed to produce the 14.3 nm intensity change. Thus the distinct effect of the length change was detected only on the 14.3 nm reflection. These results suggest no large conformational changes are induced in both the distal part of the myosin head attached to actin and the actin filament during the oscillation. It is therefore most probable that the proximal portion of myosin heads including S-2 contributes to the intensity change in response to the length change (see, also ref.21). When the muscle was stretched beyond the filament overlap, the 14.3 nm intensity change was suppressed to less than 50% of that of the slack length. It was also found that the tension change delayed the intensity change during the length oscillation. However, this delay of the tension change as observed in the muscle at the slack length was lacking in the overstretched muscle, indicating that the 14.3 nm intensity change may arise partly from a portion other than the crossbridges.