Modeling rigor cross-bridge patterns in muscle I. Initial studies of the rigor lattice of insect flight muscle.

We have undertaken some computer modeling studies of the cross-bridge observed by Reedy in insect flight muscle so that we investigate the geometric parameters that influence the attachment patterns of cross-bridges to actin filaments. We find that the appearance of double chevrons along an actin filament indicates that the cross-bridges are able to reach 10--14 nm axially, and about 90 degrees around the actin filament. Between three and five actin monomers are therefore available along each turn of one strand of actin helix for labeling by cross-bridges from an adjacent myosin filament. Reedy's flared X of four bridges, which appears rotated 60 degrees at successive levels on the thick filament, depends on the orientation of the actin filaments in the whole lattice as well as on the range of movement in each cross-bridge. Fairly accurate chevrons and flared X groupings can be modeled with a six-stranded myosin surface lattice. The 116-nm long repeat appears in our models as "beating" of the 14.5-nm myosin repeat and the 38.5-nm actin period. Fourier transforms of the labeled actin filaments indicate that the cross-bridges attach to each actin filament on average of 14.5 nm apart. The transform is sensitive to changes in the ease with which the cross-bridge can be distorted in different directions.     

Three-dimensional image reconstruction of insect flight muscle. II. The rigor actin layer

The averaged structure of rigor cross-bridges in insect flight muscle is further revealed by three-dimensional reconstruction from 25-nm sections containing a single layer of thin filaments. These exhibit two thin filament orientations that differ by 60 degrees from each other and from myac layer filaments. Data from multiple tilt views (to +/- 60 degrees) was supplemented by data from thick sections (equivalent to 90 degrees tilts). In combination with the reconstruction from the myac layer (Taylor et al., 1989), the entire unit cell is reconstructed, giving the most complete view of in situ cross-bridges yet obtained. All our reconstructions show two classes of averaged rigor cross-bridges. Lead bridges have a triangular shape with leading edge angled at approximately 45 degrees and trailing edge angled at approximately 90 degrees to the filament axis. We propose that the lead bridge contains two myosin heads of differing conformation bound along one strand of F-actin. The lead bridge is associated with a region of the thin filament that is apparently untwisted. We suggest that the untwisting may reflect the distribution of strain between myosin and actin resulting from two-headed, single filament binding in the lead bridge. Rear bridges are oriented at approximately 90 degrees to the filament axis, and are smaller and more cylindrical, suggesting that they consist of single myosin heads. The rear bridge is associated with a region of apparently normal thin filament twist. We propose that differing myosin head angles and conformations consistently observed in rigor embody different stages of the power stroke which have been trapped by a temporal sequence of rigor cross-bridge formation under the constraints of the intact filament lattice.     

Three-dimensional image reconstruction of insect flight muscle. I. The rigor myac layer

We have obtained detailed three-dimensional images of in situ cross-bridge structure in insect flight muscle by electron microscopy of multiple tilt views of single filament layers in ultrathin sections, supplemented with data from thick sections. In this report, we describe the images obtained of the myac layer, a 25-nm longitudinal section containing a single layer of alternating myosin and actin filaments. The reconstruction reveals averaged rigor cross-bridges that clearly separate into two classes constituting lead and rear chevrons within each 38.7-nm axial repeat. These two classes differ in tilt angle, size and shape, density, and slew. This new reconstruction confirms our earlier interpretation of the lead bridge as a two-headed cross-bridge and the rear bridge as a single-headed cross-bridge. The importance of complementing tilt series with additional projections outside the goniometer tilt range is demonstrated by comparison with our earlier myac layer reconstruction. Incorporation of this additional data reveals new details of rigor cross-bridge structure in situ which include clear delineation of (a) a triangular shape for the lead bridge, (b) a smaller size for the rear bridge, and (c) density continuity across the thin filament in the lead bridge. Within actin's regular 38.7-nm helical repeat, local twist variations in the thin filament that correlate with the two cross-bridge classes persist in this new reconstruction. These observations show that in situ rigor cross-bridges are not uniform, and suggest three different myosin head conformations in rigor.     

Tomographic 3D reconstruction of quick-frozen, Ca2+-activated contracting insect flight muscle

Motor actions of myosin were directly visualized by electron tomography of insect flight muscle quick-frozen during contraction. In 3D images, active cross-bridges are usually single myosin heads, bound preferentially to actin target zones sited midway between troponins. Active attached bridges (approximately 30% of all heads) depart markedly in axial and azimuthal angles from Rayment's rigor acto-S1 model, one-third requiring motor domain (MD) tilting on actin, and two-thirds keeping rigor contact with actin while the light chain domain (LCD) tilts axially from approximately 105 degrees to approximately 70 degrees. The results suggest the MD tilts and slews on actin from weak to strong binding, followed by swinging of the LCD through an approximately 35 degrees axial angle, giving an approximately 13 nm interaction distance and an approximately 4-6 nm working stroke.     

A proline shuttle in insect flight muscle.

A proline shuttle for oxidation of extramitochondrial NADH was reconstituted from soluble and mitochondrial fractions of blowfly ($\text{Phormia}$$\text{regina}$) flight muscle. The soluble fraction catalyzed reduction of Δ′-pyrroline-5-carboxylate to proline via the action of Δ′-pyrroline-5-carboxylate reductase (EC 1.5.1.2). The reaction required NADH as hydrogen donor, NAD (P) H being ineffective in this regard. Mitochondria catalyzed regeneration of Δ′-pyrroline-5-carboxylate from proline via action of proline oxidase. The capacity of the shuttle to operate under conditions of possible competition for Δ′-pyrroline-5-carboxylate between Δ′-pyrroline-5-carboxylate reductase and Δ′-pyrroline-5-carboxylate dehydrogenase (EC 1.5.1.12) was incestigated. Results of these investigations indicate that dehydrogenase activity does not significantly interfere with shuttle activity.     

COOH-terminal truncation of flightin decreases myofilament lattice organization, cross-bridge binding, and power output in Drosophila indirect flight muscle

The indirect flight muscle (IFM) of insects is characterized by a near crystalline myofilament lattice structure that likely evolved to achieve high power output. In Drosophila IFM, the myosin rod binding protein flightin plays a crucial role in thick filament organization and sarcomere integrity. Here we investigate the extent to which the COOH terminus of flightin contributes to IFM structure and mechanical performance using transgenic Drosophila expressing a truncated flightin lacking the 44 COOH-terminal amino acids (fln(ΔC44)). Electron microscopy and X-ray diffraction measurements show decreased myofilament lattice order in the fln(ΔC44) line compared with control, a transgenic flightin-null rescued line (fln(+)). fln(ΔC44) fibers produced roughly 1/3 the oscillatory work and power of fln(+), with reduced frequencies of maximum work (123 Hz vs. 154 Hz) and power (139 Hz vs. 187 Hz) output, indicating slower myosin cycling kinetics. These reductions in work and power stem from a slower rate of cross-bridge recruitment and decreased cross-bridge binding in fln(ΔC44) fibers, although the mean duration of cross-bridge attachment was not different between both lines. The decreases in lattice order and myosin kinetics resulted in fln(ΔC44) flies being unable to beat their wings. These results indicate that the COOH terminus of flightin is necessary for normal myofilament lattice organization, thereby facilitating the cross-bridge binding required to achieve high power output for flight.     

The influence of flight on the phospholipid metabolism in insect flight muscle

Males of the American cockroach, Periplaneta americana, received an injection of 32P-orthophosphates and the specific activity of phosphatidylcholine (PC), phosphatidylethanolamine (PE) and phosphatidylinositol (PI) was determined after 120 min of in vivo incorporation. If the insects were forced to fly for 10 min immediately before the end of the experiment, the specific activity (S.A.) of PC and PE was lowered by 34.3 and 31.0%, respectively, that of PI by 17.5%. If the animals were allowed to rest for 10 min after cessation of flight, the S.A. of PC and PE did not differ significantly from the controls, whereas that of PI rose by 91.0% above the control value. These effects cannot be due to changes in precursor labelling (glycerophosphate and phosphoarginine were measured) and reflect changes in the rate of phospholipid biosynthesis. The possibility is discussed that mechanisms regulating the rate of phospholipid biosynthesis are involved.     

A 3-D reconstruction of smooth muscle alpha-actinin by CryoEm reveals two different conformations at the actin-binding region

Cryoelectron microscopy was used to obtain a 3-D image at 2.0 nm resolution of 2-D arrays of smooth muscle alpha-actinin. The reconstruction reveals a well-resolved long central domain with 90 degrees of left-handed twist and near 2-fold symmetry. However, the molecular ends which contain the actin binding and calmodulin-like domains, have different structures oriented approximately 90 degrees to each other. Atomic structures for the alpha-actinin domains were built by homology modeling and assembled into an atomic model. Model building suggests that in the 2-D arrays, the two calponin homology domains that comprise the actin-binding domain have a closed conformation at one end and an open conformation at the other end due to domain swapping. The open and closed conformations of the actin-binding domain suggests flexibility that may underlie Ca2+ regulation. The approximately 90 degrees orientation difference at the molecular ends may underlie alpha-actinin's ability to crosslink actin filaments in nearly any orientation.     

Immunolocalization of ubiquitin in degenerating insect flight muscle

Summary Ubiquitin was localized by immunofluorescence microscopy during post-mating histolysis of fibrillar flight muscle in female fire ants, Solenopsis spp. Normal muscles, as well as histolysing muscles from artificially inseminated and haemolymph-injected females contained ubiquitin in association with nuclei, Z-lines, myofilaments and mitochondria. However, the density of the ubiquitin immunoreaction was markedly increased in the nuclei, Z-lines and mitochondria of degenerating tissues 6, 12 and 24 h post treatment. At these times the heaviest immunoreactivity for ubiquitin was seen in association with the nuclei, Z-lines and mitochondria. Immuno-controls, incubated in the absence of the primary antibody, showed no similar immunostaining. When insemination was preceded by the injection of actinomycin D, muscle degradation was significantly depressed after a 24-h period. Also, ubiquitin immunofluorescence was markedly reduced in tissues pre-treated with actinomycin D. These observations suggest that insemination increases the ubiquitination of specific myofibrillar proteins destined for degradation.     

Filament lattice of frog striated muscle. Radial forces, lattice stability, and filament compression in the A-band of relaxed and rigor muscle.

Repulsive pressure in the A-band filament lattice of relaxed frog skeletal muscle has been measured as a function of interfilament spacing using an osmotic shrinking technique. Much improved chemical skinning was obtained when the muscles were equilibrated in the presence of EGTA before skinning. The lattice shrank with increasing external osmotic pressure. At any specific pressure, the lattice spacing in relaxed muscle was smaller than that of muscle in rigor, except at low pressures where the reverse was found. The lattice spacing was the same in the two states at a spacing close to that found in vivo. The data were consistent with an electrostatic repulsion over most of the pressure range. For relaxed muscle, the data lay close to electrostatic pressure curves for a thick filament charge diameter of approximately 26 nm, suggesting that charges stabilizing the lattice are situated about midway along the thick filament projections (HMM-S1). At low pressures, observed spacings were larger than calculated, consistent with the idea that thick filament projections move away from the filament backbone. Under all conditions studied, relaxed and rigor, at short and very long sarcomere lengths, the filament lattice could be modeled by assuming a repulsive electrostatic pressure, a weak attractive pressure, and a radial stiffness of the thick filaments (projections) that differed between relaxed and rigor conditions. Each thick filament projection could be compressed by approximately 5 or 2.6 nm requiring a force of 1.3 or 80 pN for relaxed and rigor conditions respectively.     

On the role of arginine kinase in insect flight muscle

In the flight muscle of Locusta migratoria L., arginine kinase activity increased 10-fold when 5th instar larvae and adult animals were compared. During the onset of flight, ATP decreased slightly with the amount of phospho-l-arginine remaining constant. Thus, high arginine kinase activity characterizes the adult muscle, giving rise to the speculation that the phospho-l-arginine/l-arginine kinase system does not act only as a buffer system for high-energy phosphate but also as a shuttle mechanism for high-energy phosphate between mitochondria and myofibrils. Judged from electrophoretic mobility, only one isoenzyme exists that is not bound to subcellular structures. Calculations of the diffusive fluxes of ATP, ADP, phosphate, phospho-l-arginine and l-arginine between the sites of ATP-consumption and production, respectively, can be interpreted in such a way, that the low concentration of ADP_free might limit ATP-turnover during flight. Judging from the high arginine kinase activity, the major acceptor for high-energy phosphate at the mitochondria could be l-arginine, while phospho-l-arginine is transphosphorylated to ATP at the myofibrils, thus presumably serving as an energy shuttle.     

On the contractile mechanism of insect fibrillar flight muscle

Zusammenfassung Zur Erfassung der dynamischen Vorgänge bei der Muskelkontraktion wurde das System des fibrillären Insektenflugmuskels unter Bedingungen, die eine Linearisierung zulassen, untersucht. Um die Frequenzantwort als das Systemverhalten im sinusförmigen stationären Zustand zu erhalten, wurden die durch aufgeprägte sinusförmige Längenänderungen erzeugten Spannungsänderungen gemessen. Die Frequenzganganalysen beziehen sich auf die Annahme eines zeitinvarianten Systems mit konzentrierten Elementen. Die dominanten passiven Strukturen des Muskels, die Verbindungs-filamente und die Myosinbrücken, können in dem Frequenzbereich, der den Arbeitsfrequenzen des Insektenflugmuskels entspricht, durch ein aus drei Elementen bestehendes viscoelastisches System des Maxwell-Typs mit Zeitkonstanten vergleichbarer Größe beschrieben werden. Für die Frequenzantwort des aktivierten Muskels wurde mit hinreichender Genauigkeit die Übertragungsfunktion eines Phasenminimum-systems ermittelt. Eine theoretische Übertragungsfunktion für aktive Seite der Kontraktion ist durch Differenzbildung experimentell erhaltener Ortskurven bestätigt worden. Auf der Grundlage dieser theoretischen Differenzkurve wurde eine Beziehung zwischen oscillatorischer Arbeit und enzymatischer Hydrolyse des Adenosintriphosphates (ATP) als Energiequelle hergestellt. Bis zur optimalen Frequenz der Oscillation unter den benutzten Bedingungen wird eine Proportionalität zwischen diesen Größen festgestellt, die durch einen konstanten mechanochemischen Kopplungsfaktor bestimmt ist.