PubMed Health⌕ Search

Biomedical subjects

John M Squire

Publications and source records attributed to John M Squire.

At least 19 recordsLinked to original sources
PubMed2006

The myosin filament superlattice in the flight muscles of flies: A-band lattice optimisation for stretch-activation?

Low-angle X-ray diffraction patterns from relaxed fruitfly (Drosophila) flight muscle recorded on the BioCat beamline at the Argonne Advanced Photon Source (APS) show many features similar to such patterns from the "classic" insect flight muscle in Lethocerus, the giant water bug, but there is a characteristically different pattern of sampling of the myosin filament layer-lines, which indicates the presence of a superlattice of myosin filaments in the Drosophila A-band. We show from analysis of the structure factor for this lattice that the sampling pattern is exactly as expected if adjacent four-stranded myosin filaments, of repeat 116 nm, are axially shifted in the hexagonal A-band lattice by one-third of the 14.5 nm axial spacing between crowns of myosin heads. In addition, electron micrographs of Drosophila and other flies (e.g. the house fly (Musca) and the flesh fly (Sarcophaga)) combined with image processing confirm that the same A-band superlattice occurs in all of these flies; it may be a general property of the Diptera. The different A-band organisation in flies compared with Lethocerus, which operates at a much lower wing beat frequency (approximately 30 Hz) and requires a warm-up period, may be a way of optimising the myosin and actin filament geometry needed both for stretch activation at the higher wing beat frequencies (50 Hz to 1000 Hz) of flies and their need for a rapid escape response.

Actin Cytoskeleton↗
PubMed2006

Refined structure of bony fish muscle myosin filaments from low-angle X-ray diffraction data.

Application of X-ray diffraction methods to the elucidation of the arrangement of the myosin heads on myosin filaments in resting muscles is made simpler when the muscles themselves are well ordered in 3D. Bony fish muscle for the vertebrates and insect flight muscle for the invertebrates are the muscles of choice for this analysis. The rich, well-sampled, low-angle X-ray diffraction pattern from bony fish muscle has previously been modelled with an R-factor of 3.4% between observed and calculated transforms on the assumption that the two heads in one myosin molecule have the same shape. However, recent evidence from other kinds of analysis of other muscles has shown that this assumption may not be valid. There is evidence that the motor domain of one head in each pair may interact with the neck region of the second head. This possibility has been tested directly in the present analysis which extends the X-ray modelling of fish muscle myosin filaments by permitting independent shape changes of the two heads in one molecule. The new model, with a computed R-factor of 1.19% against 56 independent reflections, shows that in fish muscle also there is a marked asymmetry in the organisation of each head pair.

Animals↗
PubMed2006

3D structure of relaxed fish muscle myosin filaments by single particle analysis.

To understand the structural changes involved in the force-producing myosin cross-bridge cycle in vertebrate muscle it is necessary to know the arrangement and conformation of the myosin heads at the start of the cycle (i.e. the relaxed state). Myosin filaments isolated from goldfish muscle under relaxing conditions and viewed in negative stain by electron microscopy (EM) were divided into segments and subjected to three-dimensional (3D) single particle analysis without imposing helical symmetry. This allowed the known systematic departure from helicity characteristic of vertebrate striated muscle myosin filaments to be preserved and visualised. The resulting 3D reconstruction reveals details to about 55 A resolution of the myosin head density distribution in the three non-equivalent head 'crowns' in the 429 A myosin filament repeat. The analysis maintained the well-documented axial perturbations of the myosin head crowns and revealed substantial azimuthal perturbations between crowns with relatively little radial perturbation. Azimuthal rotations between crowns were approximately 60 degrees , 60 degrees and 0 degrees , rather than the regular 40 degrees characteristic of an unperturbed helix. The new density map correlates quite well with the head conformations analysed in other EM studies and in the relaxed fish muscle myosin filament structure modelled from X-ray fibre diffraction data. The reconstruction provides information on the polarity of the myosin head array in the A-band, important in understanding the geometry of the myosin head interaction with actin during the cross-bridge cycle, and supports a number of conclusions previously inferred by other methods. The observed azimuthal head perturbations are consistent with the X-ray modelling results from intact muscle, indicating that the observed perturbations are an intrinsic property of the myosin filaments and are not induced by the proximity of actin filaments in the muscle A-band lattice. Comparison of the axial density profile derived in this study with the axial density profile of the X-ray model of the fish myosin filaments which was restricted to contributions from the myosin heads allows the identification of a non-myosin density peak associated with the azimuthally perturbed head crown which can be interpreted as a possible location for C-protein or X-protein (MyBP-C or -X). This position for C-protein is also consistent with the C-zone interference function deduced from previous analysis of the meridional X-ray pattern from frog muscle. It appears that, along with other functions, C-(X-) protein may have the role of slewing the heads of one crown so that they do not clash with the neighbouring actin filaments, but are readily available to interact with actin when the muscle is activated.

Animals↗
PubMed2006

Structural correlation between collagen VI microfibrils and collagen VI banded aggregates.

Collagen VI is a component of the extracellular matrix that is able to form structural links with cells. Collagen VI monomers cross-link into tetramers that come together to form long molecular chains known as microfibrils. Collagen VI tetramers are also the most likely candidates for the formation of banded aggregates with an axial periodicity of about 105 nm that are seen in the retinas of people suffering from age-related macular degeneration and Sorsby's fundus dystrophy, in the vitreous of patients with full thickness macular holes and in the intervertebral discs of normal individuals. Here, a protocol is developed to carry out a structural comparison between the microfibrils, which are known to be made of collagen VI tetramers, and the banded aggregates. The comparison shows that the banded aggregates are easily explained as being a lateral assembly of microfibrils, thus supporting the hypothesis that they too are made of collagen VI. Understanding the role played by the collagen VI aggregates in normal and pathological conditions will help to throw light on the pathologies with which they are associated.

Aged↗
PubMed2006

Beta-structures in fibrous proteins.

The beta-form of protein folding, one of the earliest protein structures to be defined, was originally observed in studies of silks. It was then seen in early studies of synthetic polypeptides and, of course, is now known to be present in a variety of guises as an essential component of globular protein structures. However, in the last decade or so it has become clear that the beta-conformation of chains is present not only in many of the amyloid structures associated with, for example, Alzheimer's Disease, but also in the prion structures associated with the spongiform encephalopathies. Furthermore, X-ray crystallography studies have revealed the high incidence of the beta-fibrous proteins among virulence factors of pathogenic bacteria and viruses. Here we describe the basic forms of the beta-fold, summarize the many different new forms of beta-structural fibrous arrangements that have been discovered, and review advances in structural studies of amyloid and prion fibrils. These and other issues are described in detail in later chapters.

Amyloid↗
PubMed2006

Reprint of "Structural correlation between collagen VI microfibrils and collagen VI banded aggregates" [J. Struct. Biol. 154 (2006) 312-326].

Collagen VI is a component of the extracellular matrix that is able to form structural links with cells. Collagen VI monomers cross-link into tetramers that come together to form long molecular chains known as microfibrils. Collagen VI tetramers are also the most likely candidates for the formation of banded aggregates with an axial periodicity of about 105 nm that are seen in the retinas of people suffering from age-related macular degeneration and Sorsby's fundus dystrophy, in the vitreous of patients with full thickness macular holes and in the intervertebral discs of normal individuals. Here, a protocol is developed to carry out a structural comparison between the microfibrils, which are known to be made of collagen VI tetramers, and the banded aggregates. The comparison shows that the banded aggregates are easily explained as being a lateral assembly of microfibrils, thus supporting the hypothesis that they too are made of collagen VI. Understanding the role played by the collagen VI aggregates in normal and pathological conditions will help to throw light on the pathologies with which they are associated.

Journal Article↗
PubMed2005

Skip residues and charge interactions in myosin II coiled-coils: implications for molecular packing.

Molecular packing of myosin II coiled-coil rods into myosin filaments and the role of skip residues in the heptad sequence have been investigated. Sequence comparison of rods from skeletal, smooth and non-muscle myosin II shows that different myosin II subtypes have significantly different charge distributions. Analysis of the ionic interactions between adjacent rods with changing molecular overlap relates the different patterns of charge to the different structures of skeletal and smooth muscle myosin II filaments. It is shown in the case of skeletal muscle myosin II that the skip residues have a critical role in keeping these unique patterns of charge in perfect phase. Only one of the previously suggested packing models for myosin II filaments, with a slight modification, is supported, since it satisfies all the sequence-predicted axial shifts between adjacent rods. Such analysis significantly advances understanding of myosin filament assembly properties and will help to provide a basis for the proper understanding of myosin-associated diseases.

Fourier Analysis↗
PubMed2005

Single particle analysis: a new approach to solving the 3D structure of myosin filaments.

Knowledge of the structure of muscle myosin filaments is essential for a proper understanding of sarcomere structure and how myosin heads interact with the actin filaments to produce force and movement. Two principal methods have been used to define the myosin head arrays in filaments in the relaxed state, namely modelling from low-angle X-ray diffraction data and image processing of electron micrographs of isolated filaments. Analysis of filament images by 3D helical reconstruction, which imposes total helical symmetry on the structure, is very effective in some cases, but it relies on the existence of very highly ordered preparations of straight filaments. Resolutions achieved to date are about 70 angstroms. Modelling of X-ray diffraction data recorded from whole relaxed fish or insect muscles has also been used as an independent method. Although the resolution of the diffraction data is often also about 70 angstroms, the effective resolution of the modelling is very much higher than this because additional very high resolution data (e.g. from protein crystallography) is included in the analysis. However, the X-ray diffraction method has to date provided only limited data on non-myosin thick filament proteins such as C-protein and titin and it cannot provide the polarity of the myosin head arrangement. Both the helical reconstruction and X-ray diffraction techniques have advantages and disadvantages, but their disadvantages are avoided in the new approach of single particle analysis of electron micrograph data. Even using the same micrographs as for helical reconstruction, the resolution can be extended by this method to about 50 angstroms or better. In addition, it is not necessary to assume that the myosin filaments are helical; a significant advantage in the case of vertebrate myosin filaments where there is a known crossbridge perturbation. Here we describe the principles of all these approaches, but particularly that of single particle analysis. We outline the application of single particle analysis to myosin filaments from vertebrate skeletal and insect flight (IFM) muscle myosin filaments.

Animals↗
PubMed2005

Fibrous proteins: new structural and functional aspects revealed.

Coiled-coil proteins, collagen, and elastomers together comprise an important subset of the fibrous proteins. The former group-the alpha-fibrous coiled-coil proteins-are widely distributed in nature and, indeed, the characteristic heptad motif has been recognized as an oligomerisation motif in fibril-forming collagens. This volume has selected a number of the alpha-fibrous proteins for detailed discussion, including intermediate filament proteins, the spectrin superfamily, and fibrin?fibrinogen. Of particular interest is the growing realization that the design principles governing the structures of these coiled-coil proteins are now largely discernible and can be specified with a high degree of confidence, due in large part to the wealth of crystal structure data now available. Within the connective tissues covered in this volume, two constituents of defining importance mechanically are the collagen fibrils?networks and the elastic fibers. Crystal structures of collagen peptides have been published and are described. The effects of the precise sequence of the distinct constituent triplets on molecular conformation have also become clearer. The ultrastructures of connective tissues are largely defined by the spatial arrangement of the collagen fibrils and networks, and this is elucidated here in some detail. The elastic fibers with their elastin cores and fibrillin-containing microfibril palisades are also described. A theme underlying all of the proteins discussed in this volume is the significantly increased effort to characterize the structures and functions of mutants. Some of these occur naturally and lead to various disease states, while others have been genetically engineered in order to study design principles.

Connective Tissue↗
PubMed2005

Molecular packing in network-forming collagens.

Different collagen types can vary considerably in length, molecular weight, chemical composition, and the way they interact with each other to form molecular aggregates. Collagen Types IV, VI, VIII, X, and dogfish egg case collagen make linear and lateral associations to form open networks rather than fibers. The roles played by these network-forming collagens are diverse: they can act as support and anchorage for cells and tissues, serve as molecular filters, and even provide protective permeable barriers for developing embryos. Their functional properties are intimately linked to their molecular organization. This Chapter reviews what is known about the molecular structure of this group of collagens, describes the ways the molecules interact to form networks, and-despite the large variations in molecular size-identifies common aggregation themes.

Chemical Phenomena↗
PubMed2004

New X-ray diffraction observations on vertebrate muscle: organisation of C-protein (MyBP-C) and troponin and evidence for unknown structures in the vertebrate A-band.

Previous low-angle X-ray diffraction studies of various vertebrate skeletal muscles have shown the presence of two rich layer-line patterns, one from the myosin heads and based on a 429 A axial repeat, and one from actin filaments and based on a repeat of about 360-370 A. In addition, meridional intensities have been seen from C-protein (MyBP-C; at about 440 A and its higher orders) and troponin (at about 385 A and its orders). Using preparations of intact, relaxed, bony fish fin muscles and the ID-02 low-angle X-ray camera at the ESRF with a 10 m camera length we have now seen numerous, hitherto unreported, sampled, X-ray layer-lines many of which do not fit onto the previously observed repeats and which require interpretation. The new reflections all fall on the normal ("vertical") hexagonal lattice row-lines in the highly sampled, almost "crystalline", low-angle diffraction X-ray patterns from bony fish muscle, indicating that they all arise from the muscle A-band. However, they do not fall on a single axial repeat. In direct confirmation of our previous analysis, some of these new reflections are explained by the interaction in resting muscle between the N-terminal ends of myosin-bound C-protein molecules with adjacent actin filaments, possibly through the Pro-Ala-rich region. Other newly observed reflections lie on a much longer repeat, but they are most easily interpreted in terms of the arrangement of troponin on the actin filaments. If this is so, then the implication is that the actin filaments and their troponin complexes are systematically arranged in the fish muscle A-band lattice relative to the myosin head positions, and that these newly observed X-ray reflections, when fully analysed, will report on the shape and distribution of troponin molecules in the resting muscle A-band. The less certain contributions of titin and nebulin to these new reflections have also been tested and are described. Many of the new reflections do not appear to come from these known structures. There must be structural features of the A-band that have not yet been described.

Animals↗
PubMed2004

MusLABEL: a program to model striated muscle A-band lattices, to explore crossbridge interaction geometries and to simulate muscle diffraction patterns.

The program MusLABEL has been devised as a simple aid both in understanding the origin and appearance of fibre diffraction patterns from helical structures and also to simulate the structure and some features of the diffraction patterns from striated muscles and their filament components. Helices are common as preferred conformations in both natural and synthetic macromolecules (e.g. DNA, alpha -helices, polysaccharides, synthetic polymers), and they also occur frequently in extended macromolecular aggregates (e.g. actin filaments, myosin filaments, microtubules, amyloid filaments etc). For this reason, a simple way of visualising the kinds of diffraction patterns that these filament structures can give, particularly for the actin and myosin filaments in muscle, can have educational value and can also be useful as a quick means of evaluating possible symmetries in structural interpretations of diffraction data before embarking on full helical diffraction analysis. A feature of the MusLABEL program is that, when a particular kind of A-band lattice has been set up, for example for vertebrate striated muscle or insect flight muscle, additional parameters can be defined both to describe the limits to the azimuthal and axial ranges over which a myosin head can search for an actin binding site and also to describe the size and position of an actin 'target area' assuming that the azimuthal position of an actin monomer has a large effect in determining whether or not a myosin head can bind to it. By this means the effects of lattice geometry on head attachment can be explored and the diffraction effects of specific labelling patterns on actin can be calculated and simulated. The MusLABEL program, running under Microsoft Windows, is available free on the CCP13 website (www.ccp13.ac.uk) where further documentation is given.

Animals↗
PubMed2004

Electron tomography of fast frozen, stretched rigor fibers reveals elastic distortions in the myosin crossbridges.

As a first step toward freeze-trapping and 3-D modeling of the very rapid load-induced structural responses of active myosin heads, we explored the conformational range of longer lasting force-dependent changes in rigor crossbridges of insect flight muscle (IFM). Rigor IFM fibers were slam-frozen after ramp stretch (1000 ms) of 1-2% and freeze-substituted. Tomograms were calculated from tilt series of 30 nm longitudinal sections of Araldite-embedded fibers. Modified procedures of alignment and correspondence analysis grouped self-similar crossbridge forms into 16 class averages with 4.5 nm resolution, revealing actin protomers and myosin S2 segments of some crossbridges for the first time in muscle thin sections. Acto-S1 atomic models manually fitted to crossbridge density required a range of lever arm adjustments to match variably distorted rigor crossbridges. Some lever arms were unchanged compared with low tension rigor, while others were bent and displaced M-ward by up to 4.5 nm. The average displacement was 1.6 +/- 1.0 nm. "Map back" images that replaced each unaveraged 39 nm crossbridge motif by its class average showed an ordered mix of distorted and unaltered crossbridges distributed along the 116 nm repeat that reflects differences in rigor myosin head loading even before stretch.

Animals↗
PubMed2004

Single particle analysis of filamentous and highly elongated macromolecular assemblies.

The application of single particle techniques to the three-dimensional analysis of electron microscope images of elongated or filamentous macromolecular assemblies is evaluated, taking as an example the muscle thin filament. Although the thin filament contains local helical symmetry, because of the inherent variable twist along it, the helical coherence does not extend for large enough distances to allow the symmetry to be used for full reconstruction of the tropomyosin/troponin repeat along the filament. The muscle thin filament therefore represents a general case of a filamentous object in that it is not possible to exploit symmetry in a full analysis. Due to the nature of the imaging process in the electron microscope, only projections of the thin filament around its long axis are available without tilting the grid. Crucially, projection images around a single axis do not provide enough information to assign Euler angles ab initio using current methods. Tests with a model thin filament structure indicated that an out-of-plane tilt of approximately 20 degrees was needed for ab initio angular assignment of sufficient accuracy to calculate a 3D structure to a resolution of approximately 25 A. If no out-of-plane views are available, an alternative approach is to use a prior 3D model as a reference for the initial angle assignment. Tests with the thin filament model indicated that reasonably accurate angular assignment can be made using a reference containing actin, but lacking the regulatory proteins tropomyosin and troponin. We also found that an adaptation of the exact filtered back projection method is required to allow the correct weighting of projection images in which the particle has a very large axial ratio. This adaptation resulted in significant improvements in the reconstruction.

Actin Cytoskeleton↗