The contractile apparatus of striated muscle in the course of atrophy and regeneration

Summary Changes in the contractile apparatus of denervated rat soleus muscles were investigated during the course of reinnervation.As observed earlier, in the course of denervation atrophy the ratio of myosin to actin filaments decreases because myosin filaments disappear faster than actin filaments (Jakubiec-Puka et al. 1981 a). After reinnervation the amount of myosin filaments and myosin heavy chains (myosin HC) in the muscle increased during the first few days; the increment of actin content was negligible. The proportion of myosin HC to actin remained lower than normal for about 30 days. The excess of actin filaments frequently observed in the newly-formed myofibrils reflects this disproportion.The results show a lability of myosin and suggest some cytoskeletal role for actin filaments.     

Forces measured with micro-fabricated cantilevers during actomyosin interactions produced by filaments containing different myosin isoforms and loop 1 structures

Background

There is evidence that the actin-activated ATP kinetics and the mechanical work produced by muscle myosin molecules are regulated by two surface loops, located near the ATP binding pocket (loop 1), and in a region that interfaces with actin (loop 2). These loops regulate force and velocity of contraction, and have been investigated mostly in single molecules. There is a lack of information of the work produced by myosin molecules ordered in filaments and working cooperatively, which is the actual muscle environment.

Methods

We use micro-fabricated cantilevers to measure forces produced by myosin filaments isolated from mollusk muscles, skeletal muscles, and smooth muscles containing variations in the structure of loop 1 (tonic and phasic myosins). We complemented the experiments with in-vitro assays to measure the velocity of actin motility.

Results

Smooth muscle myosin filaments produced more force than skeletal and mollusk myosin filaments when normalized per filament overlap. Skeletal muscle myosin propelled actin filaments in a higher sliding velocity than smooth muscle myosin. The values for force and velocity were consistent with previous studies using myosin molecules, and suggest a close correlation with the myosin isoform and structure of surface loop 1.

General significance

The technique using micro-fabricated cantilevers to measure force of filaments allows for the investigation of the relation between myosin structure and contractility, allowing experiments to be conducted with an array of different myosin isoforms. Using the technique we observed that the work produced by myosin molecules is regulated by amino-acid sequences aligned in specific loops.     

Calcium-Dependent Myosin from Insect Flight Muscles

Calcium regulation of the insect actomyosin ATPase is associated with the thin filaments as in vertebrate muscles, and also with the myosin molecule as in mollusks. This dual regulation is demonstrated using combinations of locust thin filaments with rabbit myosin and locust myosin with rabbit actin; in each case the ATPase of the hybrid actomyosin is calcium dependent. The two regulatory systems are synergistic, the calcium dependency of the locust actomyosin ATPase being at least 10 times that of the hybrid actomyosins described above. Likewise Lethocerus myosin also contains regulatory proteins. The ATPase activity of Lethocerus myosin is labile and is stabilized by the presence of rabbit actin. Tropomyosin activates the ATPase of insect actomyosin and the activation occurs irrespective of whether the myosin is calcium dependent or rendered independent of calcium.     

Heat-induced Gelation of Myosin from Leg and Breast Muscles of Chicken

Heat-induced gelation of myosin from leg and breast muscles of chicken was studied in 0.6 m KC1. Gel strength of breast myosin was higher than that of leg myosin between pH 5.2 and 6.0. Turbidity of breast myosin increased below pH 6.0 but that of leg myosin did not increase at pH 5.7. Turbidity of leg myosin was higher than that of breast myosin below pH 5.6. Viscosity of breast myosin increased between pH 5.5 and 6.0 as the pH decreases, although that of leg myosin decreased. The breast myosin assembled to form long filaments at pH 5.7, but leg myosin failed to form long filaments. At pH 5.4, breast myosin filaments became longer and leg myosin assembled into filaments though they were shorter than breast myosin filaments. The strength of heat-induced gel formed from the filamentous leg and breast myosins at acidic region was not influenced by F-actin. These results indicate that the strength of heat-induced gel of both myosins is closely related to their morphological properties.     

Head-head interaction characterizes the relaxed state of Limulus muscle myosin filaments

Regulation of muscle contraction via the myosin filaments occurs in vertebrate smooth and many invertebrate striated muscles. Studies of unphosphorylated vertebrate smooth muscle myosin suggest that activity is switched off through an intramolecular interaction between the actin-binding region of one head and the converter and essential light chains of the other, inhibiting ATPase activity and actin interaction. The same interaction (and additional interaction with the tail) is seen in three-dimensional reconstructions of relaxed, native myosin filaments from tarantula striated muscle, suggesting that such interactions are likely to underlie the off-state of myosin across a wide spectrum of the animal kingdom. We have tested this hypothesis by carrying out cryo-electron microscopy and three-dimensional image reconstruction of myosin filaments from horseshoe crab (Limulus) muscle. The same head-head and head-tail interactions seen in tarantula are also seen in Limulus, supporting the hypothesis. Other data suggest that this motif may underlie the relaxed state of myosin II in all species (including myosin II in nonmuscle cells), with the possible exception of insect flight muscle.The molecular organization of the myosin tails in the backbone of muscle thick filaments is unknown and may differ between species. X-ray diffraction data support a general model for crustaceans in which tails associate together to form 4-nm-diameter subfilaments, with these subfilaments assembling together to form the backbone. This model is supported by direct observation of 4-nm-diameter elongated strands in the tarantula reconstruction, suggesting that it might be a general structure across the arthropods. We observe a similar backbone organization in the Limulus reconstruction, supporting the general existence of such subfilaments.     

Paramyosin content and thick filament structure in insect muscles

Summary The myosin filaments of the flight muscles of the locust Locusta migratoria, the cockchafer Melolontha melolontha and the femur muscles of L. migratoria have solid centers. Those of the flight muscles of the housefly Musca domestica and Drosophila melanogaster are tubular. Electron micrographs of myofibrils of the fleshfly Phormia terrae-novae contain both filament types within one sarcomere and suggest the existence of 4 cross-bridges per crown.Estimates of the ratios of myosin to paramyosin and of myosin to actin on sodium dodecyl sulphate-polyacrylamide gels yielded paramyosin contents of 9% of the thick filament mass for the solid and 2.6% for the tubular filaments (3.8% for P. terrae-novae). Based on the myosinactin ratios up to 6 myosin dimers per crown could be calculated.The molar ratio of actin to arthrin on SDS gels was found to be 3.37 for native and extracted myofibrils of flight muscles from P. terrae-novae. Arthrin is also present in isolated actin filaments suggesting that it is localized in or on the thin filaments. If we assume that it is constituent part of the helices of the thin filaments the number of myosin dimers per crown can be diminished to 4.5, considerably closer to the values obtained by evaluation of electron micrographs.Dedicated to Prof. Dr. Bernhard Rensch on his 85^th birthday     

General model of myosin filament structure. 3. Molecular packing arrangements in myosin filaments

Following the original proposals about myosin filament structure put forward as part of a general myosin filament model (Squire, 1971, 1972) it is here shown what the most likely molecular packing arrangements within the backbones of certain myosin filaments would be assuming that the model is correct. That this is so is already indicated by recently published experimental results which have confirmed several predictions of the model (Bullard and Reedy, 1972; Reedy et al., 1972; Tregear and Squire, 1973).The starting point in the analysis of the myosin packing arrangements is the model for the myosin ribbons in vertebrate smooth muscle proposed by Small &; Squire (1972). It is shown that there is only one reasonable type of packing arrangement for the rod portions of the myosin molecules which will account for the known structure of the ribbons and which is consistent with the known properties of myosin molecules. The dominant interactions in this packing scheme are between parallel myosin molecules which are related by axial shifts of 430 Å and 720 Å. In this analysis the myosin rods are treated as uniform rods of electron density and only the general features of two-strand coiled-coil molecules are considered.Since the general myosin filament model is based on the assumption that the structures of different types of myosin filament must be closely related, the packing scheme derived for the myosin ribbons is used to deduce the structures of the main parts (excluding the bare zones) of the myosin filaments in a variety of muscles. It is shown in each case that there is only one packing scheme consistent with all the available data on these filaments and that in each filament type exactly the same interactions between myosin rods are involved. In other words the myosin-myosin interactions involved in filament formation are specific, they involve molecular shifts of either 430 Å or 720 Å, and are virtually identical in all the different myosin filaments which have been considered. Apart from the myosin ribbons, these are the filaments in vertebrate skeletal muscle, insect flight muscle and certain molluscan muscles.In the case of the thick filaments in vertebrate skeletal muscle the form of the myosin packing arrangement in the bare zone is considered and a packing scheme proposed which involves antiparallel overlaps between myosin rods of 1300 Å and 430 Å. It is shown that this scheme readily explains the triangular profiles of the myosin filaments in the bare zone (Pepe, 1967, 1971) and many other observations on the form of these myosin filaments.Finally it is shown that the cores of several different myosin filaments, assuming they contain protein, may consist of different arrangements of one or other of two types of core subfilament.     

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.     

The Effect of Experimental Hyperthyroidism on Characteristics of Actin–Myosin Interaction in Fast and Slow Skeletal Muscles

The molecular mechanism of the failure of contractile function of skeletal muscles caused by oxidative damage to myosin in hyperthyroidism is not fully understood. Using an in vitro motility assay, we studied the effect of myosin damage caused by oxidative stress in experimental hyperthyroidism on the actin–myosin interaction and its regulation by calcium. We found that hyperthyroidism-induced oxidation of myosin is accompanied by a decrease in the sliding velocity of the regulated thin filaments in the in vitro motility assay, and this effect is increased with the duration of the pathological process.     

DAAM Is Required for Thin Filament Formation and Sarcomerogenesis during Muscle Development in Drosophila

During muscle development, myosin and actin containing filaments assemble into the highly organized sarcomeric structure critical for muscle function. Although sarcomerogenesis clearly involves the de novo formation of actin filaments, this process remained poorly understood. Here we show that mouse and Drosophila members of the DAAM formin family are sarcomere-associated actin assembly factors enriched at the Z-disc and M-band. Analysis of dDAAM mutants revealed a pivotal role in myofibrillogenesis of larval somatic muscles, indirect flight muscles and the heart. We found that loss of dDAAM function results in multiple defects in sarcomere development including thin and thick filament disorganization, Z-disc and M-band formation, and a near complete absence of the myofibrillar lattice. Collectively, our data suggest that dDAAM is required for the initial assembly of thin filaments, and subsequently it promotes filament elongation by assembling short actin polymers that anneal to the pointed end of the growing filaments, and by antagonizing the capping protein Tropomodulin.     

Three-dimensional structure of the vertebrate muscle A-band: II. The myosin filament superlattice

The three-dimensional arrangement of the myosin filaments in the A-band of frog sartorius muscle was studied using electron micrographs of very thin and accurately cut transverse sections through the bare region (on each side of the M-band) where the thick filament shafts are roughly triangular in shape. It was found that the orientations of these triangular profiles are arranged to give a superlattice of the same size and shape as that proposed by Huxley & Brown (1967) on the basis of X-ray diffraction evidence, but the contents of the superlattice may not be as they suggested. The results from detailed image analysis strongly suggest that myosin filaments (which have been shown to have 3-fold rotational symmetry, Luther, 1978; Luther, Munro and Squire, unpublished results) are arranged with one of two orientations which are 60 ° (or 180 °) apart. This arrangement of filaments with 3-fold symmetry is not that predicted for a superlattice with the symmetry suggested by Huxley & Brown.Two rules define the way in which the orientations of neighbouring filaments are defined. Rule (1): no three mutually adjacent filaments in the hexagonal array of filaments in the A-band can all have identical orientations; and rule (2): no three successive filaments along a 10$\text{1}\text{?}$ row in the filament array can have identical orientations. These two no-three-alike rules are sufficient to describe the observed arrangement of filament profiles in the frog bare region (except for some minor violations discussed in the text), and they lead automatically to the generation of the required superlattice. The A-band structure in fish muscle is different; there is no superlattice and the triangular bare region profiles have only one orientation. The frog superlattice and fish simple lattice are explained directly in terms of different interactions between the M-bridges in the M-bands of these muscles. The observed structures require that the myosin filament symmetry at the centre of the M-band is that of the dihedral point group 32. The two possible forms of interaction between filaments with this symmetry (apart from a completely random structure) give rise to the observed A-band lattices in frog and fish muscles. The 3-fold rotational symmetry of the myosin filaments required to explain the observed micrographs also requires that the myosin crossbridge arrangements around the actin filaments in frog and fish muscles will be different. It is suggested that the structure in the frog A-band (and in the A-bands of other higher vertebrates) has evolved from that in fish to improve the distribution of crossbridges around the aotin filaments. The X-ray diffraction evidence of Huxley & Brown (1967) will be accounted for in terms of the proposed A-band structure in a further paper in this series.     

Myosin filament structure in vertebrate smooth muscle

The in vivo structure of the myosin filaments in vertebrate smooth muscle is unknown. Evidence from purified smooth muscle myosin and from some studies of intact smooth muscle suggests that they may have a nonhelical, side-polar arrangement of crossbridges. However, the bipolar, helical structure characteristic of myosin filaments in striated muscle has not been disproved for smooth muscle. We have used EM to investigate this question in a functionally diverse group of smooth muscles (from the vascular, gastrointestinal, reproductive, and visual systems) from mammalian, amphibian, and avian species. Intact muscle under physiological conditions, rapidly frozen and then freeze substituted, shows many myosin filaments with a square backbone in transverse profile. Transverse sections of fixed, chemically skinned muscles also show square backbones and, in addition, reveal projections (crossbridges) on only two opposite sides of the square. Filaments gently isolated from skinned smooth muscles and observed by negative staining show crossbridges with a 14.5-nm repeat projecting in opposite directions on opposite sides of the filament. Such filaments subjected to low ionic strength conditions show bare filament ends and an antiparallel arrangement of myosin tails along the length of the filament. All of these observations are consistent with a side-polar structure and argue against a bipolar, helical crossbridge arrangement. We conclude that myosin filaments in all smooth muscles, regardless of function, are likely to be side-polar. Such a structure could be an important factor in the ability of smooth muscles to contract by large amounts.     

Organization of native and in vitro-reassembled myosin filaments from lobster tonic muscle

Tonic muscle of the crusher claw of the American lobster (Homarus amencanus) was investigated with respect to sarcomeric organization and the capacity for self-assembly of extracted myosin for comparison with the same properties of rabbit muscle. Native myosin filaments in the lobster muscle are much longer than in rabbit skeletal fibers, and differ further in sarcomeric organization in showing an actinto-myosin relationship in which two actin filaments are shared between adjacent myosins in a 12-membered orbital. The self-assembly of lobster myosin into filaments comparable in length and fine structure to the natural filament was achieved in the presence of excess Mg²⁺, a condition not required for rabbit myosin self-assembly. Results of in situ and self-assembly studies indicate a difference in molecular organization between lobster and rabbit myosin filaments and of the inferred presence of regulatory factors in the formation of these ultrastructural elements. These studies represent the groundwork for an investigation of in vitro polymerization of actin in association with the synthetic lobster myosin filament.     

Interaction of myosin and paramyosin

The interaction of myosin and paramyosin was investigated by enzymological and ultrastructural techniques. The actin-activated Mg⁺² ATPase of rabbit skeletal muscle myosin can be inhibited by clam adductor paramyosin. Both proteins must be rapidly coprecipitated to form filaments for this inhibition. Slowly formed cofilaments are fully activatable by F-actin. In both cases, the cofilaments possess unique structural characteristics when compared to homofilaments. The mode of inhibition appears to be competitive when different concentrations of paramyosin and F-actin are compared. The apparent affinity of the myosin heads for actin is reduced by the presence of paramyosin within rapidly reconstituted thick filaments. These results suggest that paramyosin may serve as part of a relaxing mechanism within invertebrate muscles. It is unlikely that paramyosin plays a role in the initiation and maintenance of catch within specialized molluscan muscles.     

Immunohistochemistry of chaetognath body wall muscles

Abstract. A light and electron immunohistochemical study was carried out on the body wall muscles of the chaetognath Sagitta friderici for the presence of a variety of contractile proteins (myosin, paramyosin, actin), regulatory proteins (tropomyosin, troponin), and structural proteins (α‐actinin, desmin, vimentin). The primary muscle (～80% of body wall volume) showed the characteristic structure of transversely striated muscles, and was comparable to that of insect asynchronous flight muscles. In addition, the body wall had a secondary muscle with a peculiar structure, displaying two sarcomere types (S1 and S2), which alternated along the myofibrils. S1 sarcomeres were similar to those in the slow striated fibers of many invertebrates. In contrast, S2 sarcomeres did not show a regular sarcomeric pattern, but instead exhibited parallel arrays of 2 filament types. The thickest filaments (～10–15 nm) were arranged to form lamellar structures, surrounded by the thinnest filaments (～6 nm). Immunoreactions to desmin and vimentin were negative in both muscle types. The primary muscle exhibited the classical distribution of muscle proteins: actin, tropomyosin, and troponin were detected along the thin filaments, whereas myosin and paramyosin were localized along the thick filaments; immunolabeling of α‐actinin was found at Z‐bands. Immunoreactions in the S1 sarcomeres of the secondary muscle were very similar to those found in the primary muscle. Interestingly, the S2 sarcomeres of this muscle were labeled with actin and tropomyosin antibodies, and presented no immunore‐actions to both myosin and paramyosin. α‐Actinin in the secondary muscle was only detected at the Z‐lines that separate S1 from S2. These findings suggest that S2 are not true sarcomeres. Although they contain actin and tropomyosin in their thinnest filaments, their thickest filaments do not show myosin or paramyosin, as the striated muscle thick myofilaments do. These peculiar S2 thick filaments might be an uncommon type of intermediate filament, which were labeled neither with desmin or vimentin antibodies.     

Assembly of thick filaments and myofibrils occurs in the absence of the myosin head

We investigated the importance of the myosin head in thick filament formation and myofibrillogenesis by generating transgenic Drosophila lines expressing either an embryonic or an adult isoform of the myosin rod in their indirect flight muscles. The headless myosin molecules retain the regulatory light-chain binding site, the alpha-helical rod and the C-terminal tailpiece. Both isoforms of headless myosin co-assemble with endogenous full-length myosin in wild-type muscle cells. However, rod polypeptides interfere with muscle function and cause a flightless phenotype. Electron microscopy demonstrates that this results from an antimorphic effect upon myofibril assembly. Thick filaments assemble when the myosin rod is expressed in mutant indirect flight muscles where no full-length myosin heavy chain is produced. These filaments show the characteristic hollow cross-section observed in wild type. The headless thick filaments can assemble with thin filaments into hexagonally packed arrays resembling normal myofibrils. However, thick filament length as well as sarcomere length and myofibril shape are abnormal. Therefore, thick filament assembly and many aspects of myofibrillogenesis are independent of the myosin head and these processes are regulated by the myosin rod and tailpiece. However, interaction of the myosin head with other myofibrillar components is necessary for defining filament length and myofibril dimensions.     

β-Filagenin, a Newly Identified Protein Coassembling with Myosin and Paramyosin in Caenorhabditis elegans

Muscle thick filaments are stable assemblies of myosin and associated proteins whose dimensions are precisely regulated. The mechanisms underlying the stability and regulation of the assembly are not understood. As an approach to these problems, we have studied the core proteins that, together with paramyosin, form the core structure of the thick filament backbone in the nematode Caenorhabditis elegans. We obtained partial peptide sequences from one of the core proteins, β-filagenin, and then identified a gene that encodes a novel protein of 201–amino acid residues from databases using these sequences. β-Filagenin has a calculated isoelectric point at 10.61 and a high percentage of aromatic amino acids. Secondary structure algorithms predict that it consists of four β-strands but no α-helices. Western blotting using an affinity-purified antibody showed that β-filagenin was associated with the cores. β-Filagenin was localized by immunofluorescence microscopy to the A bands of body–wall muscles, but not the pharynx. β-filagenin assembled with the myosin homologue paramyosin into the tubular cores of wild-type nematodes at a periodicity matching the 72-nm repeats of paramyosin, as revealed by immunoelectron microscopy. In CB1214 mutants where paramyosin is absent, β-filagenin assembled with myosin to form abnormal tubular filaments with a periodicity identical to wild type. These results verify that β-filagenin is a core protein that coassembles with either myosin or paramyosin in C. elegans to form tubular filaments.     

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.     

Ultrastructure of the contractile apparatus of rat skeletal muscle embedded in an aqueous medium

The method of tissue embedding in melamine resin was applied to rat skeletal muscle. This method does not require tissue dehydration with organic solvents; only aqueous solutions are used. Electron micrographs of muscles embedded in melamine differ from those embedded in the conventional epoxy resin. In melamine-embedded muscles the actin and myosin filaments appear larger in diameter and subunits can be recognized in cross-sectioned myosin filaments. Within the Z-line, the characteristic patterns described for muscles embedded in epoxy resin are not visible; the spaces between the actin filaments are filled with electron-dense material. This suggests that the Z-line is more compact than could be concluded from epoxy resin-embedded muscle specimens. The M-line appears to be different from what is observed in epoxy-embedded muscle. The membranes appear as several clearly delineated layers. Dehydration rather than the action of the organic solvents per se is the main reason for the differences in the structure of the contractile apparatus between melamine- and epoxy-embedded muscles.