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X-ray diffraction studies of muscle have provided a wealth of information on muscle structure and physiology, and the meridian of the diffraction pattern is particularly informative. Reconditi et al. (2014. J. Physiol.https://doi.org/10.1113/jphysiol.2013.267849) performed superb experiments on changes to the M3 meridional peak as a function of sarcomere length (SL). They found that the M3 intensity dropped almost linearly as sarcomere length increased at least to about SL = 3.0 µm, and that it followed the same track as tension, pointing toward zero at the end of overlap at ∼3.6 µm. They concluded that, just as tension could only be generated by overlapped myosin heads, so ordered myosin heads contributing to the M3 intensity could only occur in the overlap region of the A-band, and that nonoverlapped heads must be highly disordered. Here we show that this conclusion is not consistent with x-ray diffraction theory; it would not explain their observations. We discuss one possible reason for the change in M3 intensity with increasing sarcomere length in terms of increasing axial misalignment of the myosin filaments that at longer sarcomere lengths is limited by the elastic stretching of the M-band and titin., (© 2021 Squire and Knupp.)

Microtubules and filamentous (F-) actin engage in complex interactions to drive many cellular processes from subcellular organization to cell division and migration. This is thought to be largely controlled by proteins that interface between the two structurally distinct cytoskeletal components. Here, we use cryo-electron tomography to demonstrate that the microtubule lumen can be occupied by extended segments of F-actin in small molecule-induced, microtubule-based, cellular projections. We uncover an unexpected versatility in cytoskeletal form that may prompt a significant development of our current models of cellular architecture and offer a new experimental approach for the in situ study of microtubule structure and contents., (© 2020 Paul et al.)

The structures of muscle thin filaments reconstituted using skeletal actin and cardiac troponin and tropomyosin have been determined with and without bound Ca 2+ using electron microscopy and reference-free single particle analysis. The resulting density maps have been fitted with atomic models of actin, tropomyosin and troponin showing that: (i) the polarity of the troponin complex is consistent with our 2009 findings, with large shape changes in troponin between the two states; (ii) without Ca 2+ the tropomyosin pseudo-repeats all lie at almost equivalent positions in the 'blocked' position on actin (over subdomains 1 and 2); (iii) in the active state the tropomyosin pseudo-repeats are all displaced towards subdomains 3 and 4 of actin, but the extent of displacement varies within the regulatory unit depending upon the axial location of the pseudo-repeats with respect to troponin. Individual pseudo-repeats with Ca 2+ bound to troponin can be assigned either to the 'closed' state, a partly activated conformation, or the 'M-state', a fully activated conformation which has previously been thought to occur only when myosin heads bind. These results lead to a modified view of the steric blocking model of thin filament regulation in which cooperative activation is governed by troponin-mediated local interactions of the pseudo-repeats of tropomyosin with actin., (Copyright © 2017 The Authors. Published by Elsevier Inc. All rights reserved.)

Myosin-binding protein C (MyBP-C) is a thick filament protein playing an essential role in muscle contraction, and MyBP-C mutations cause heart and skeletal muscle disease in millions worldwide. Despite its discovery 40 y ago, the mechanism of MyBP-C function remains unknown. In vitro studies suggest that MyBP-C could regulate contraction in a unique way--by bridging thick and thin filaments--but there has been no evidence for this in vivo. Here we use electron tomography of exceptionally well preserved muscle to demonstrate that MyBP-C does indeed bind to actin in intact muscle. This binding implies a physical mechanism for communicating the relative sliding between thick and thin filaments that does not involve myosin and which could modulate the contractile process.

We describe a novel set of single particle based procedures for the structural analysis of electron microscope images of muscle thin filaments and other partially decorated actin based filaments. The thin filament comprises actin and the regulatory proteins tropomyosin and troponin in a 7:1:1M ratio. Prior to our work, structure analysis from electron microscope images of the thin filament has largely involved either helical averaging defined by the underlying actin helix or the use of single particle analysis but using a starting model as a reference structure. Our single particle based approach yields an accurate structure for the complete thin filament by avoiding the loss of information from troponin and tropomyosin associated with helical averaging and also removing the potential reference bias associated with the use of a starting model. The approach is more widely applicable to sub-stoichiometric complexes of F-actin and actin-binding proteins., (Copyright 2009 Elsevier Inc. All rights reserved.)

C-protein (MyBP-C) is a myosin-binding protein that is usually seen in two sets of seven to nine positions in the C-zones in each half of the vertebrate striated muscle A-band. Skeletal muscle C-protein is a modular structure containing ten sub-domains (C1 to C10) of which seven are immunoglobulin-type domains and three (C6, C7 and C9) are fibronectin-like domains. Cardiac muscle C-protein has an extra N-terminal domain (C0) and also some sequence insertions, one of which provides phosphorylation sites. It is conceivable that C-protein has both a structural and regulatory role within the sarcomere. The precise mode of binding of C-protein to the myosin filament has not been determined. However, detailed ultrastructural studies have suggested that C-protein, which binds to myosin, can give rise to a longer periodicity (about 435A) than the intrinsic myosin filament repeat of 429A. The reason for this has remained a puzzle for over 25 years. Here we show by modelling and computation that the presence of this longer periodicity could be explained if the myosin-binding part of C-protein binds to myosin with the expected 429A repeat, but if there are systematic interactions of the N-terminal end of C-protein with the neighbouring actin filaments in the hexagonal lattice of filaments in the A-band. We also show that if they occur these interactions would probably only arise in defined muscle states. Further analysis of the MyBP-C sequence identifies a possible actin-binding domain in the Pro-Ala-rich sequence found at the N terminus of skeletal MyBP-C and between domains C0 and C1 in the cardiac sequence.

It is 30 years since Ebashi and colleagues showed that Ca2+ ions directly affect regulation of the myosin-actin interaction in muscle through the action of tropomyosin and troponin on muscle thin filaments. It is more than 20 years since the idea was put forward that tropomyosin might act, at least in part, by changing its position on actin, thus uncovering or modifying the myosin binding site on actin when troponin molecules take up Ca2+. Since that time, a great deal of evidence for and against this steric blocking mechanism has been published: a structure for actin filaments at close to atomic resolution has been proposed, and the whole regulation story has become both more complicated and more subtle. Here we review structural and biochemical aspects of regulation in vertebrate skeletal muscle. We show that some basic ideas of the steric blocking mechanism remain valid. We also show that additional factors, such as troponin movements and structural changes within the actin monomers themselves, may be crucial. A number of the resulting regulation scenarios need to be distinguished.

The arrangement and shape of myosin heads in relaxed muscle have been determined by analysis of low-angle X-ray diffraction data from a very highly ordered vertebrate muscle in bony fish. This reveals the arrangement and interactions between the two heads of the same myosin molecule, the shape of the resting myosin head (M.ADP.Pi) assuming a putative hinge between the myosin catalytic domain and the light chain binding-domain, and the way that the actin-binding sites on myosin are arrayed around the actin filaments in the bony fish muscle A-band cell unit. The results are discussed in terms of possible force-generating mechanisms. Changes in myosin head shape or tilt have been implicated in the mechanism of force generation. The myosin head arrangement, including perturbations from perfect helical symmetry, has all heads oriented roughly the same way up (there is only a small range of rotations around the head long axis). X-ray data do not define the absolute polarity of the myosin head array. The resting head rotation is either similar to (65 degrees difference) or opposite to (115 degrees difference) the rotation in the rigor state. If the rotations are similar, probably the more likely possibility, then the average relative axial displacement of the inner and outer ends of the heads from the resting state to rigor is about 140 to 150 A. If (less likely) the resting head rotation is opposite to rigor, then the heads would need to turn over (i.e. rotate about 115 degrees around their own long axes) and the mean relative axial displacement from relaxed to rigor would only be 20 to 30 A., (Copyright 1997 Academic Press Limited.)

The crystal structure of G-actin monomer has been used together with tropomyosin in a filament model to explain the low-angle X-ray diffraction data from relaxed and activated actin filaments. The four-subdomain actin monomer can be approximated quite well by a four-sphere unit. Orienting this unit and tropomyosin into a filament by searching for the best fit between the computed Fourier transform and the observed vertebrate skeletal muscle low-angle actin layer-lines from muscles at non-overlap sarcomere lengths produced models for the structural changes within the thin filaments (actin plus tropomyosin) between the resting state and the active states, which occur as a result of calcium-activation and independent of myosin interaction with actin. The models are very sensitive to changes in the positions of the centres of mass of the subdomains, but not to the exact shape of the objects used to represent them (e.g. spheres, ellipsoids etc.), as long as the volume is fixed, at the resolution here considered. It is concluded that, even with a four-subdomain structure for the actin molecules, the observed low-angle X-ray diffraction patterns cannot be explained without a substantial azimuthal swing of the tropomyosin strands when resting filaments are calcium-activated. The direction of this swing upon calcium-activation is away from a position close to the proposed major binding site of the myosin head on actin; a result consistent with the original "steric blocking model" of thin filament-based regulation in which the tropomyosin position on actin is crucial for regulation of the myosin crossbridge cycle on actin. Tropomyosin sterically hindering myosin attachment in the "off" state remains a possibility. However, even in the "on" state, the tropomyosin position is close enough to the myosin-binding site to have an effect, where it could regulate the transition of the head from a weak to a strong state. In addition to this tropomyosin movement there are small, but plausible, actin subdomain movements. A tropomyosin shift on its own will not explain the data. Allowance for possible movement of actin subdomain 2 along with the tropomyosin shift still does not explain the data. An additional small movement of subdomain 1; the main myosin-binding subdomain, is postulated.

Images of shadowed F-actin filaments on mica surfaces obtained using a quick-freeze, freeze-fracture, deep-etch technique were subjected to conventional 3-D helical reconstruction methods. Although the shadowing must vary systematically from subunit to subunit, the computed transforms of isolated filaments were characteristic of the helical actin transform. Helical reconstruction was therefore judged to be valid. The theoretical basis for such reconstruction is outlined. The reconstructions showed an average thin (about 3 nm) layer of shadow on the filament surface and both the outer and the inner surfaces of the shadow layer could be visualized. By comparison with the F-actin structure postulated by Holmes et al. (1990) on the basis of the known structure of the actin monomer, it is shown that, at the resolution considered, the inner surface of the shadow provides a reasonably faithful outline of the molecular surface. This, in turn, confirms that the original 3-D structure of the protein molecules has been well preserved throughout the whole preparation procedure up to the final replica. The "shadowed" filaments can thus be correlated axially and azimuthally with known actin structures and, in principle, features such as myosin head location on decorated filaments can be determined. The result emphasizes the amount of detail present in good quality images of shadowed particles and, in this case, shows that detailed evaluation of molecules labeling actin can be made.

Using data from fast time-resolved x-ray diffraction experiments on the synchrotrons at Daresbury and (Deutsches Elektronen Synchrotron [DESY]), it is shown that during contraction of fish muscle there are at least two distinct configurations of myosin cross-bridges on actin, that they appear to have different tension producing properties and that they probably differ in the axial tilt of the cross-bridges on actin. Evidence is presented for newly observed myosin-based layer lines in patterns from active fish muscle, together with intensity changes of the actin layer lines. On the equator, the 110 reflection changes much faster (time for 50% change t1/2 = 21 +/- 4 ms after activation) than the 100 reflection (t1/2 = 35 +/- 8 ms) and tension (t1/2 = 41 +/- 3 ms) during the rising phase of tetanic contractions. These and higher order reflections have been used to show the time course of mass attachment at actin during this rising phase. Mass arrival (t1/2 = 25 ms) precedes tension by approximately 15 ms. Analysis has been carried out to evaluate the effects of changes in sarcomere length during the tetanus. It is shown that any such effects are very small. Difference "equatorial" electron density maps between active muscle at a time when mass arrival at actin is just complete, but the tension is still rising, and at a later time well into the tension plateau, show that the structural difference between the lower and higher force states corresponds to mass movement consistent with axial swinging of heads from a nonstereospecific actin attached state (low force) to a more stereospecific (high force) state.

We have previously shown that time-resolved X-ray diffraction studies of the 2-D pattern from isometrically contracting flatfish (turbot) fin muscle have considerable advantages over similar studies of other vertebrate muscles due to the simple lattice and the better long-range order in these muscles (5, 24). Here we show not only that two structurally different myosin head to actin attached states must exist in the crossbridge cycle but that we are also able to define the likely crossbridge configurations in these states. A non-force producing "weak-binding" state is evident from the lead of the (11) equatorial reflections (and actin mass) time-course relative to that of tension (and the (10) equatorial reflection decrease) by about 30 msec. The first myosin layer line at 429 A has a weakened but altered intensity distribution, with no change in axial spacing, in patterns from active muscle. We show this to be consistent with myosin heads binding in the non-specific manner envisaged for the "weak-binding" state. Evidence for the second force-producing attached state, or series of states, comes from the observation of only a small increase in the intensity of the 360 A actin layer line between resting and active muscle patterns. It might be thought that a substantial increase in this layer line would be expected if myosin heads were even transiently attached to the thin filaments in a force-producing state. However, this is not so because internal changes in the structure of the thin filaments in active muscle have the opposite effect of causing this layer line to decrease in intensity. Observation of a small net intensity increase is therefore evidence for myosin head attachment with the symmetry of the actin helix. From the equatorial diffraction pattern, Fourier synthesis maps were computed at 10 msec intervals throughout the isometric tetanus, enabling changes in the mass distribution to be visualised between the force- and non-force producing populations of crossbridges. This difference map shows that in the force-producing state myosin heads have their centres of mass on average at a smaller radius from the thin filament axis compared to the case for non-force producing myosin heads. Since there is good evidence that there is no substantial change in myosin head shape during contraction (30) these observations are consistent with myosin heads swinging on actin as fairly rigid structures.

In order to investigate the geometry of the interactions which myosin molecules make with actin filaments we have studied thick (0.2--0.5 micrometer) transverse sections of striated muscles in the 1 Me V electron microscope at Imperial College. Sections obtained from fixed relaxed frog sartorius muscle and both fixed relaxed and fixed rigor insect flight muscles, show regular electron opaque features between the thick and thin filament profiles. These are thought to be the overlapping images of the many levels of myosin heads that occur in such sections. From the appearances of these images, together with studies of thin transverse sections, it appears that of the possible interactions which one myosin molecule can make, namely that its two component heads interact with the same thin filament or with two different thin filaments, it is the former interaction (both heads on the same filament) which is predominant. Nevertheless appearances have been seen similar to those expected if an interaction of one molecule with two thin filaments occurs. It is concluded that both single filament and two filament interactions can occur depending on the steric convenience of the available actin subunits, but that the single filament interaction occurs in the majority of cases in the muscle states we have studied. Finally it is shown that the myosin filament profiles seen in thick transverse sections may be a very misleading guide to thick filament structure because of the influence which the myosin crossbridge have on the appearance of the profiles.

The structures of vertebrate skeletal muscles (particularly from frog and fish) in the rigor state are analysed in terms of the concept of target areas on actin filaments. Assuming that 100% of the heads are to be attached to actin in rigor, then satisfactory qualitative low-resolution modelling of observed X-ray diffraction data is obtained if the outer ends of these myosin heads can move axially (total range about 200A) and azimuthally (total range less than 60 degrees) from their original lattice sites on the myosin filament surface to attach in defined target areas on the actin filaments. On this basis, each actin target area comprises about four actin monomers along one of the two long-pitched helical strands of the actin filament (about 200 A) or an azimuthal range of actin binding sites of about 100 degrees around the thin filament axis. If myosin heads simply label in a non-specific way the nearest actin monomers to them, as could occur with non-specific transient attachment in a 'weak binding' state, then the predicted X-ray diffraction pattern would comprise layer lines at the same axial spacings (orders of 429 A) as those seen in patterns from resting muscle. It is shown that actin target areas in vertebrate skeletal muscles are probably arranged on an approximate 62 (right-handed) helix of pitch (P) of about 720 A, subunit translation P/6 and near repeat P/2. Troponin position need not be considered in defining the labelling pattern of cross-bridges on this 62 helix of target areas; the target areas appear to be defined solely by the azimuthal position of the actin binding sites. The distribution of actin filament labelling patterns could be regular in fish muscle which has a 'crystalline' A-band, but will be irregular in higher vertebrate muscles such as frog sartorius muscle.