The Z lattice in canine cardiac muscle

Filtered images of mammalian cardiac Z bands were reconstructed from optical diffraction patterns from electron micrographs. Reconstructed images from longitudinal sections show connecting filaments at each 38-nm axial repeat in an array consistent with cross-sectional data. Some reconstructed images from cross sections indicate two distinctly different optical diffraction patterns, one for each of two lattice forms (basket weave and small square). Other images are more complex and exhibit composite diffraction patterns. Thus, the two lattice forms co-exist, interconvert, or represent two different aspects of the same details within the lattice. Two three-dimensional models of the Z lattice are presented. Both include the following features: a double array of axial filaments spaced at 24 nm, successive layers of tetragonally arrayed connecting filaments, projected fourfold symmetry in cross section, and layers of connecting filaments spaced at intervals of 38 nm along the myofibril axis. Projected views of the models are compared to electron micrographs and optically reconstructed images of the Z lattice in successively thicker cross sections. The entire Z band is rarely a uniform lattice regardless of plane of section or section thickness. Optical reconstructions strongly suggest two types of variation in the lattice substructure: (a) in the arrangement of connecting filaments, and (b) in the arrangement of units added side-to-side to make larger myofilament bundles and/or end-to-end to make wider Z bands. We conclude that the regular arrangement of axial and connecting filaments generates a dynamic Z lattice.     

Z band dynamics as a function of sarcomere length and the contractile state of muscle

The Z band in skeletal muscle has two distinct structural states--a relaxed (small square or ss) form and a maximally activated (basket weave or bw) form. We have examined by electron microscopy and optical diffraction Z lattice forms and dimensions and A band spacings in relaxed, tetanized, stretched, and stretched-and-tetanized rat soleus muscle. We have tested the independent contributions of passive load, active tension, and sarcomere length to Z band state. As the A band spacing decreased with increasing load and increasing sarcomere length in the untetanized muscles, the Z lattice remained in the ss form and the Z spacing changed only slightly. Computer-enhanced images from digitized electron micrographs showed that the ss Z lattice resisted deformation regardless of load or method of stretching. In contrast, when the muscle was tetanized at sarcomere lengths of up to 2.7 microns, the Z lattice assumed the bw form and the Z spacing was increased by 20%. Regardless of lattice form, Z spacing did not vary significantly with sarcomere length. Images from freeze-substituted preparations showed both lattice forms comparable to those in images from glutaraldehyde-fixed muscles. Thus, Z band state appears to be a function of the presence (or absence) of active tension. Our previous three-dimensional model is compatible with these observations and with the sub-structures revealed by computer-enhanced images of both lattice forms.     

Structural states in the Z band of skeletal muscle correlate with states of active and passive tension

In skeletal muscle Z bands, the ends of the thin contractile filaments interdigitate in a tetragonal array of axial filaments held together by periodically cross-connecting Z filaments. Changes in these two sets of filaments are responsible for two distinct structural states observed in cross section, the small-square and basketweave forms. We have examined Z bands and A bands in relaxed, tetanized, stretched, and stretched and tetanized rat soleus muscles by electron microscopy and optical diffraction. In relaxed muscle, the A-band spacing decreases with increasing load and sarcomere length, but the Z lattice remains in the small-square form and the Z spacing changes only slightly. In tetanized muscle at sarcomere lengths up to 2.7 micron, the Z lattice assumes the basketweave form and the Z spacing is increased. The increased Z spacing is not the result of sarcomere shortening. Further, passive tension is not sufficient to cause this change in the Z lattice; active tension is necessary.     

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

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

The relation between Z--disk lattice spacing and sarcomere length in sartorius muscle fibres from Hyla cerulea.

Sartorius muscles from the green tree frog Hyla cerulea were set at variety of muscle lengths and fixed for electron microscopy using acrolein followed by osmium tetroxide. The sarcomere length, s, was determined in thick sections using laser-diffraction. The Z-disk lattice spacing, z, was measured in electron micrographs of thin sections from the same muscles. The Z-disk lattice was found to expand as sarcomere length decreased such that the quantity sz2 was constant at 1-05 X 10(6) nm3 for all sarcomere lengths in the range 1-9-2-9 mum. Thus, the sarcomere length dependency of the Z-disk lattice is similar to that of the myosin filament lattice. The density of thin filaments per unit cross section of fibril leaving the Z-disk is less than their density in the A band. Thus, fibrils have a smaller cross section in the I band, leaving more inter-fibrillar space there. This may explain why more mitochondria and lipid droplets are located in the I bands than in the A bands. It is suggested that the Z-disk may contributed to the short range elasticity of muscle fibres.     

Concentric intermediate filament lattice links to specialized Z-band junctional complexes in sonic muscle fibers of the type I male midshipman fish

Type I male midshipman fish produce high-frequency hums for prolonged durations using sonic muscle fibers, each of which contains a hollow tube of radially oriented thin and flat myofibrils that display extraordinarily wide ( approximately 1.2 microm) Z bands. We have revealed an elaborate cytoskeletal network of desmin filaments associated with the contractile cylinder that form interconnected concentric ring structures in the core and periphery at the level of the Z bands. Stretch and release of single fibers revealed reversible length changes in the elastic desmin lattice. This lattice is linked to Z bands via novel intracellular desmosome-like junctional complexes that collectively form a ring, termed the "Z corset," around the periphery and within the core of the cylinder. The junctional complex consists of regularly spaced parallel approximately 900-nm-long cytoskeletal rods, or "Z bars," interconnected with slender (3-4 nm) plectin-positive filaments. Z bars are linked to the Z band by plectin filaments and on the opposite side to a dense mesh of desmin filaments. Adjacent Z bands are linked by slender filaments that appear to suspend sarcotubules. We propose that the highly reinforced elastic desmin cytoskeleton and the unique Z band junctions are structural adaptations that enable the muscles' high-frequency and high-endurance activity.     

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

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

The glucan–chitin complex in Saccharomyces cerevisiae. IV. The electron diffraction of crustacean and yeast cell wall chitin

Crustacean and yeast cell wall chitin were analyzed by means of transmission electron microscopy and selected-area diffraction. Single fibrils 8–25 nm wide have been observed in the micrographs of crustacean chitin. Analysis of a series of diffraction patterns obtained from thin crustacean chitin platelets yielded results which were in a better agreement with the theoretical structural model than those measured earlier. In this respect electron diffraction is shown to be superior to the more commonly used x-ray diffraction. Yeast cell wall chitin had a less perfect structure than the crustacean chitin. Single fibrils were not observed on the micrographs and electron diffraction patterns did not show any preferred fiber orientation. The evaluation of electron-diffraction patterns of both the primary septum and the adjacent circular zone of scar ring led to the conclusion that α-chitin is present in both these parts of the mother bud scar.     

The Striated Musculature of Blood Vessels : I. General Cell Morphology

The musculature of small lung veins, of the thoracic portion of the inferior vena cava, and of other thoracic veins of the mouse have been studied in the electron microscope. Tissues were fixed in 1 per cent osmium tetroxide buffered with veronal, to which either sodium chloride or sucrose had been added. Methacrylate or araldite served as embedding matrices. Phosphotungstic acid or uranyl acetate was used to stain some of the preparations. Thin sections were examined in a Siemens and Halske Elmiskop Ib electron microscope. The entire musculature of the veins examined was of the striated type. It represents a variety of cardiac muscle, characterized by centrally located nuclei, typical mitochondria, and narrow I bands. Many I bands cannot be recognized at all. H and M bands are likewise indistinct. There is a double array of primary and secondary myofilaments. Mitochondria are large and numerous and contain many cristae. The endoplasmic reticulum consists of longitudinal tubules which run through the whole sarcomeres and bypass Z bands, and of transverse tubules which accompany Z bands. Some "triads," located at Z levels, consist of flattened vacuoles flanked by such transverse tubules. Small vesicles located at Z bands, close to the nucleus, and beneath the plasma membrane may represent still other portions of the reticulum.     

The quaternary structure of Alfalfa mosaic virus

From an analysis of electron micrographs of Alfalfa Mosaic Virus (AMV), evidence has been obtained which favors a cylindrical P₆ lattice for the protein coat of the virus. For the analysis use was made of optical diffraction and computer processing of electron images of negatively stained virus particles. The virus coat exhibits polymorphism. Two kinds of structure were found: a stacked and a helical type. In the stacked type of lattice the unit cells are arranged in staggered rings in such a way that two rings comprise a repeat distance of the structure. The selection rule for the optical diffraction patterns of the stacked form is 1 = n + 2m, in which n is an integer multiple of 3. The layerlines are equally spaced at a distance of approximately 1/80 Å^?1. In the helical type of lattice these rings of unit cells are transformed into turns of a double helix. The selection rule derived in this case is 1 = 6n ? 17m, in which n is an integer multiple of 2. The repeat of the structure is approximately 440 Å.     

Ultrastructure of skeletal muscle fibers studied by a plunge quick freezing method: myofilament lengths.

We have set up a system to rapidly freeze muscle fibers during contraction to investigate by electron microscopy the ultrastructure of active muscles. Glycerinated fiber bundles of rabbit psoas muscles were frozen in conditions of rigor, relaxation, isometric contraction, and active shortening. Freezing was carried out by plunging the bundles into liquid ethane. The frozen bundles were then freeze-substituted, plastic-embedded, and sectioned for electron microscopic observation. X-ray diffraction patterns of the embedded bundles and optical diffraction patterns of the micrographs resemble the x-ray diffraction patterns of unfixed muscles, showing the ability of the method to preserve the muscle ultrastructure. In the optical diffraction patterns layer lines up to 1/5.9 nm-1 were observed. Using this method we have investigated the myofilament lengths and concluded that there are no major changes in length in either the actin or the myosin filaments under any of the conditions explored.     

MICROTUBULE SURFACE LATTICE AND SUBUNIT STRUCTURE AND OBSERVATIONS ON REASSEMBLY

Neuronal microtubules have been reassembled from brain tissue homogenates and purified. In reassembly from purified preparations, one of the first structures formed was a flat sheet, consisting of up to 13 longitudinal filaments, which was identified as an incomplete microtubule wall. Electron micrographs of these flat sheets and intact microtubules were analyzed by optical diffraction, and the surface lattice on which the subunits are arranged was determined to be a 13 filament, 3-start helix. A similar, and probably identical, lattice was found for outer-doublet microtubules. Finally, a 2-D image of the structure and arrangement of the microtubule subunits was obtained by processing selected images with a computer filtering and averaging system. The 40 x 50 Å morphological subunit, which has previously been seen only as a globular particle and identified as the 55,000-dalton tubulin monomer, is seen in this higher resolution reconstructed image to be elongated, and split symmetrically by a longitudinal cleft into two lobes.     

Model for the capsid structure of alfalfa mosaic virus.

The coat protein of alfalfa mosaic virus is clustered in such a way as to avoid the 3 and 6-fold lattice positions of the hexagonal surface lattice. This results in a relatively open structure for the capsid, which is mainly caused by holes situated at the 6-fold positions and, to a minor extent, those present at the 3-fold lattice points. The evidence for this has been obtained by analysing electron micrographs of negatively stained virus particles by optical diffraction and digital image processing.     

Electron microscopy of thin protein crystal sections.

In continuation of an earlier publication (Hoppe et al., 1968), further experiments are described here on the preparation of thin film sections of embedded protein crystals for investigation by electron microscopy and electron diffraction. Several embedding media were compared, the best being Aquon. Periodicities were observed in electron micrographs as well as in electron diffraction patterns. In diffraction experiments the best resolution observed was approximately 10 to 11 Å.     

Three-dimensional crystals of the light-harvesting chlorophyll a/b protein complex from pea chloroplasts

Two forms of three-dimensional crystals of the light-harvesting chlorophyll a/b protein complex from pea have been obtained. Crystals of one form grew as hexagonal plates measuring up to 150 micron across and 2 to 3 micron in thickness. Electron diffraction patterns of thin hexagonal plates showed sharp reflections to a resolution of 3.7 A on a hexagonal reciprocal lattice. The unit cell in projection (a = 127.0 A) and the symmetry of the diffraction pattern (6 mm) suggested that the hexagonal plates were highly ordered stacks of two-dimensional crystals suitable for structure analysis by electron microscopy and image processing. Crystals of a second form grew as dark green octahedra measuring roughly 0.5 mm across. Low-resolution X-ray diffraction patterns suggested a large cubic unit cell (a = 390 A). SDS/polyacrylamide gel electrophoresis of single octahedral crystals showed the same polypeptide composition as the starting solution, one major band at 24,000 apparent molecular weight and two satellite bands of 23,000 and 23,500 apparent molecular weight.     

CARDIAC MUSCLE OF THE HORSESHOE CRAB, LIMULUS POLYPHEMUS : I. Ultrastructure

The fine structure of the cardiac muscle of the horseshoe crab, Limulus polyphemus, has been studied with respect to the organization of its contractile material, and the structure of its organelles and the cell junctions. Longitudinal sections show long sarcomeres (5.37 µ at L_max), wide A bands (2.7 µ), irregular Z lines, no M line, and no apparent H zone. Transverse sections through the S zone of the A band show that each thick filament is ca. 180 A in diameter, is circular in profile with a center of low density, and is surrounded by an orbit of 9–12 thin filaments, each 60 A in diameter. Thick filaments are confined to the A band: thin filaments originate at the Z band, extend through the I band, and pass into the A band between the thick filaments. The sarcolemmal surface area is increased significantly by intercellular clefts. Extending into the fiber from these clefts and from the sarcolemma, T tubules pass into the fiber at the A-I level. Each fibril is enveloped by a profuse membranous covering of sarcoplasmic reticulum (SR). Sacculations of the SR occur at the A-I boundary where they make diadic contact with longitudinal branches of the T system. These branches also extend toward the Z, enlarge at the Z line, and pass into the next sarcomere. Infrequently noted were intercalated discs possessing terminal insertion and desmosome modifications, but lacking close junctions (fasciae occludentes). These structural details are compared with those of mammalian cardiac and invertebrate muscles.     

STRUCTURE OF LIMULUS STRIATED MUSCLE : The Contractile Apparatus at Various Sarcomere Lengths

The musculature of the telson of Limulus polyphemus L. consists of three dorsal muscles: the medial and lateral telson levators and the telson abductor, and one large ventral muscle; the telson depressor, which has three major divisions: the dorsal, medioventral, and lateroventral heads. The telson muscles are composed of one type of striated muscle fiber, which has irregularly shaped myofibrils. The sarcomeres are long, with discrete A and I and discontinuous Z bands. M lines are not present. H zones can be identified easily, only in thick (1.0 µm) longitudinal sections or thin cross sections. In lengthened fibers, the Z bands are irregular and the A bands appear very long due to misalignment of constituent thick filaments. As the sarcomeres shorten, the Z lines straighten somewhat and the thick filaments become more aligned within the A band, leading to apparent decrease in A band length. Further A band shortening, seen at sarcomere lengths below 7.4 µm may be a function of conformational changes of the thick filaments, possibly brought about by alterations in the ordering of their paramyosin cores.     

MODELS OF MUSCLE Z-BAND FINE STRUCTURE BASED ON A LOOPING FILAMENT CONFIGURATION

The fine architecture of skeletal muscle Z bands is considered in view of stereo electron microscopical evidence and current biochemical and immunological concepts, and a new Z-band model is proposed. This model is based on a looping, interlinking configuration, within the Z band, of strands which emanate from I-band (actin) filaments of adjacent sarcomeres. Two versions of the model seem presently feasible: one in which the Z-band lattice is composed of actin loops; and another in which the same pattern is derived from tropomyosin. Either version satisfies actual electron micrograph images as well as or better than prior Z-band models. Moreover, the principle of looping linkage in filament-to-filament attachment can be related to similar filament patterns seen in several adhesion sites where intracellular filaments insert on cell membranes.     

Structure of actin-containing filaments from two types of non-muscle cells

Bundles of actin-containing filaments from the acrosomal process of horseshoe crab sperm and from sea urchin egg contain a second protein having a molecular weight of about 55,000. Electron micrographs of these filamentous bundles show features reminiscent of paracrystalline arrays of actin except that bundles from the sea urchin egg have distinctive transverse bands every 110 Å. From optical diffraction patterns of the micrographs, we deduced very similar models for both structures. The models consist of hexagonal arrays of actin filaments cross-linked by the second protein. The pattern of transverse bands in bundles derived from the sea urchin eggs is accounted for by postulating that the second protein is bonded to actin only at positions where cross-linking can occur, rather than being bonded to every actin. The helical symmetry of the actin requires that the bonding contacts involved in the cross-linking be slightly different at different positions along the length of the bundle. The technique of image reconstruction was used to obtain a three-dimensional map of the bundles from the acrosomal process.     

THE FINE STRUCTURE OF SHEEP MYOCARDIAL CELLS; SARCOLEMMAL INVAGINATIONS AND THE TRANSVERSE TUBULAR SYSTEM

An electron microscope study of sheep myocardial cells has demonstrated the presence of a transverse tubular system, apparently forming a network across the cell at each Z band level. The walls of these tubules resemble the sarcolemma in consisting of two dense layers—plasma membrane and basement menbrane; continuity of the tubule walls with the sarcolemma can be seen when longitudinal sections of a cell are obtained between two subsarcolemmal myofibrils and at the same time perpendicular to the cell surface. The demonstration of communication between the lumen of the transverse tubular system and the extracellular space appears to be more definite in this study than in any work hitherto published. It provides anatomical evidence of a possible direct pathway for transmission of the activating impulse from the sarcolemma to the myofibril Z bands.