Insect Flight Muscle Research Articles

Effects of diet and metamorphosis upon the sterol composition of the butterfly Morpho peleides

Whole body sterol metabolism in insects has seldom been studied. We were able to design an appropriate study at a butterfly farm in Belize. We collected six larvas of butterfly (Morpho peleides), their food (leaves of Pterocarpus bayessii), and their excretions. In addition, six adult butterflies were collected. The sterols of the diet, the larva, and adult butterfly were analyzed by gas-liquid chromatography. The structures of these sterols were identified by digitonin precipitation, GC-MS, and NMR. Four sterols (cholesterol, campesterol, stigmasterol, and sitosterol) and a sterol mixture were found in the food, the body, and the excreta of the larva. The tissue sterol content of the larva was 326 microg. They consumed 276 microg of sterols per day. Their excretion was 185 microg per day as sterols. The total tissue sterol contents of the larva and butterfly were similar, but they had different sterol compositions, which indicated interconversion of sterols during development. There was a progressive increase in the cholesterol content from larva to butterfly and a decrease in the content of sitosterol and other plant sterols, which were likely converted to cholesterol. Our data indicated an active sterol metabolism in butterfly larva. Diet played an important role in determining its sterol composition. During metamorphosis, there was an interconversion of sterols. This is the first paper documenting the fecal sterol excretion in insects as related to dietary intakes.

When Is a Fly in the Ointment a Solution and not a Problem?

See related article, pages 1212–1218 You never know from where and when the next clue to any particular scientific problem will arise. In the case of cardiac function, it may have been in 1948 from Professor J.W.S. Pringle, who was trying to figure out how flies manage to fly upside down.1 Having mounted a truncated fly wing apparatus on a gyroscopic base, he serendipitously noted that when inertial and damping conditions were just right, the truncated wings oscillated at more than 100 s−1 independent of neuronal innervation (Figure, A). This, he surmised, was attributable to matching an intrinsic resonant property of insect flight muscle to the elastic and inertial properties of the wing and exoskeletal structure, producing a resonant system generating oscillatory power. He called this intrinsic property of insect flight muscle “stretch–activation” because it is a recurrent stretching in the face of persistent Ca2+ levels, not Ca2+ pulses, that activate the actomyosin interaction in these insect flight muscles. This resonant system resembles a parent pushing a child on a swing. The parent must push at the correct time; that is, the addition of energy to the system must be matched to the intrinsic resonance of the system. A, Graph of what Pringle called “free oscillation” of the truncated wing apparatus. The work loop is counter-clockwise, so that as the muscle oscillates, tension is greater during shortening than at the same length during the stretch part of the cycle. The muscle is performing work on the apparatus during shortening. Adapted from Pringle1 with permission of the publisher. B, Abstract tracing of an isometrically contracting rabbit slow muscle fiber after an imposed stretch showing the immediate spike in tension, decay, and second rise in tension. The resonant system in flight muscle can also be …

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.

The molecular elasticity of the insect flight muscle proteins projectin and kettin

Projectin and kettin are titin-like proteins mainly responsible for the high passive stiffness of insect indirect flight muscles, which is needed to generate oscillatory work during flight. Here we report the mechanical properties of kettin and projectin by single-molecule force spectroscopy. Force-extension and force-clamp curves obtained from Lethocerus projectin and Drosophila recombinant projectin or kettin fragments revealed that fibronectin type III domains in projectin are mechanically weaker (unfolding force, F(u) approximately 50-150 pN) than Ig-domains (F(u) approximately 150-250 pN). Among Ig domains in Sls/kettin, the domains near the N terminus are less stable than those near the C terminus. Projectin domains refolded very fast [85% at 15 s(-1) (25 degrees C)] and even under high forces (15-30 pN). Temperature affected the unfolding forces with a Q(10) of 1.3, whereas the refolding speed had a Q(10) of 2-3, probably reflecting the cooperative nature of the folding mechanism. High bending rigidities of projectin and kettin indicated that straightening the proteins requires low forces. Our results suggest that titin-like proteins in indirect flight muscles could function according to a folding-based-spring mechanism.

The function of elastic proteins in the oscillatory contraction of insect flight muscle

Oscillatory contraction of asynchronous insect flight muscle is activated by periodic stretches at constant low concentrations of Ca2+. The fibres must be relatively stiff to respond to small length changes occurring at high frequency. Several proteins in the flight muscle may determine the overall stiffness of the fibres. The Drosophila sallimus (sls) gene codes for multiple isoforms with a modular structure made up of immunoglobulin (Ig) and elastic PEVK domains, unique sequence, and a few fibronectin (Fn) domains at the end of the molecule. Kettin, derived from the sls gene, has Ig domains separated by linker sequences and is bound to actin near the Z-disc; the C-terminus is associated with the end of the A-band. Flight muscle also has longer isoforms of Sls, with extensible PEVK sequence, and C-terminal Fn domains; all extend from the Z-disc to the end of the A-band. Projectin, from a different gene, has repeating modules of Fn and Ig domains, and is associated with the end of thick filaments; tandem Ig and PEVK domains at the N-terminus are in the I-band. Projectin, kettin and other Sls isoforms form a mechanical link between thick and thin filaments; all are probably part of the connecting filaments, which branch from the thick filaments and are linked to actin near the Z-disc. The elasticity of fibres may depend on the relative amounts of those isoforms with extensible PEVK sequence. Flightin is bound on the outside of thick filaments and maintains the stiffness necessary for the transmission of stress along the filaments. Insect flight muscle has multiple elastic proteins to give the sarcomere the optimum compliance necessary for high frequency oscillatory contraction.

Functions of Stretch Activation in Heart Muscle

Stretch activation is an intrinsic length-sensing mechanism that allows muscle to function with an autonomous regulation that reduces reliance on extrinsic regulatory systems. This autonomous regulation is most dramatic in asynchronous insect flight muscle and gives rise to wing beat frequencies

1P247 Molecular mechanism of stretch activation in insect flight muscle as examined by X-ray diffraction(8. Muscle contraction and muscle protein,Poster Session,Abstract,Meeting Program of EABS & BSJ 2006)

1P247 Molecular mechanism of stretch activation in insect flight muscle as examined by X-ray diffraction(8. Muscle contraction and muscle protein,Poster Session,Abstract,Meeting Program of EABS & BSJ 2006)

マイクロビームを用いた昆虫飛翔筋の進化の過程に関する構造研究

マイクロビームを用いた昆虫飛翔筋の進化の過程に関する構造研究

Evolution of long-range myofibrillar crystallinity in insect flight muscle as examined by X-ray cryomicrodiffraction.

Insect flight muscle is known for its crystal-quality regularity of contractile protein arrangement within a sarcomere. We have previously shown by X-ray microdiffraction that the crystal-quality regularity in bumble-bee flight muscle is not confined within a sarcomere, but extends over the entire length of a myofibril (>1000 sarcomeres connected in series). Because of this, the whole myofibril may be regarded as a millimetre-long, natural single protein crystal. Using bright X-ray beams from a synchrotron radiation source, we examined how this long-range crystallinity has evolved among winged insects. We analysed >4600 microdiffraction patterns of quick-frozen myofibrils from 50 insect species, covering all the major winged insect orders. The results show that the occurrence of such long-range crystallinity largely coincides with insect orders with asynchronous muscle operation. However, a few of the more skilled fliers among lower-order insects apparently have developed various degrees of structural regularity, suggesting that the demand for skillful flight has driven the lattice structure towards increased regularity.

Paramyosin phosphorylation site disruption affects indirect flight muscle stiffness and power generation in Drosophila melanogaster

The phosphoprotein paramyosin is a major structural component of invertebrate muscle thick filaments. To investigate the importance of paramyosin phosphorylation, we produced transgenic Drosophila melanogaster in which one, three, or four phosphorylatable serine residues in the N-terminal nonhelical domain were replaced by alanines. Depending on the residues mutated, transgenic lines were either unaffected or severely flight impaired. Flight-impaired strains had decreases in the most acidic paramyosin isoforms, with a corresponding increase in more basic isoforms. Surprisingly, ultrastructure of indirect flight muscle myofibrils was normal, indicating N-terminal phosphorylation is not important for myofibril assembly. However, mechanical studies of active indirect flight muscle fibers revealed that phosphorylation site mutations reduced elastic and viscous moduli by 21-59% and maximum power output by up to 42%. Significant reductions also occurred under relaxed and rigor conditions, indicating that the phosphorylation-dependent changes are independent of strong crossbridge attachment and likely arise from alterations in thick filament backbone properties. Further, normal crossbridge kinetics were observed, demonstrating that myosin motor function is unaffected in the mutants. We conclude that N-terminal phosphorylation of Drosophila paramyosin is essential for optimal force and oscillatory power transduction within the muscle fiber and is key to the high passive stiffness of asynchronous insect flight muscles. Phosphorylation may reinforce interactions between myosin rod domains, enhance thick filament connections to the central M-line of the sarcomere and/or stabilize thick filament interactions with proteins that contribute to fiber stiffness.

X-ray microdiffraction and conventional diffraction from frozen-hydrated biological specimens

A system for recording microdiffraction patterns from micrometer-sized quick-frozen hydrated biological specimens at the high-flux beamline BL40XU of SPring-8 is described. The optics consists of a pair of pinholes drilled into tantalum substratum, with a defining aperture of diameter 2 microm. The frozen specimens are placed in an in-vacuum cryochamber mounted on a three-axis goniometer, where the specimens are stably held at a liquid-nitrogen temperature ( approximately 74 K). A beam size of 1.5 microm (full width at half-maximum) is attained at the sample position. By using this system, diffraction patterns have been recorded from an isolated single myofibril (diameter approximately 3 microm) of an insect flight muscle in an area equivalent to a single sarcomere (length approximately 3 microm). The technique is potentially applicable to other micrometer-sized hydrated biological specimens, which are more susceptible to radiation damage than dry synthetic polymers or biopolymers. The quick-freezing of biological specimens has also been proven useful in reducing the specimen volume in the beam in conventional diffraction recordings.

Myofilin, a protein in the thick filaments of insect muscle

Thick filaments in striated muscle are myosin polymers with a length and diameter that depend on the fibre type. In invertebrates, the length of the thick filaments varies widely in different muscles and additional proteins control filament assembly. Thick filaments in asynchronous insect flight muscle have an extremely regular structure, which is likely to be essential for the oscillatory contraction of these muscles. The factors controlling the assembly of thick filaments in insect flight muscle are not known. We previously identified a thick filament core protein, zeelin 1, in Lethocerus flight and non-flight muscles. This has been sequenced, and the corresponding proteins in Drosophila and Anopheles have been identified. The protein has been re-named myofilin. Zeelin 2, which is on the outside of Lethocerus flight muscle thick filaments, has been sequenced and because of the similarity to Drosophila flightin, is re-named flightin. In Drosophila flight muscle, myofilin has a molecular weight of 20 kDa and is one of five isoforms produced from a single gene. In situ hybridisation of Drosophila embryos showed that myofilin RNA is first expressed late in embryogenesis at stage 15, a little later than myosin. Antibody to myofilin labelled the entire A-band, except for the H-zone, in cryosections of flight and non-flight muscle. The periodicity of myofilin in Drosophila flight muscle thick filaments was found to be 30 nm by measuring the spacing of gold particles in labelled cryosections; this is about twice the 14.5 nm spacing of myosin molecules. The molar ratio of myofilin to myosin in indirect flight muscle is 1:2, which is the same as that of flightin. We propose a model for the association of these proteins in thick filaments, which is consistent with the periodicity and stoichiometry. Myofilin is probably needed for filament assembly in all muscles, and flightin for stability of flight muscle thick filaments in adult flies.

Molecular dynamics of cyclically contracting insect flight muscle in vivo

Flight in insects--which constitute the largest group of species in the animal kingdom--is powered by specialized muscles located within the thorax. In most insects each contraction is triggered not by a motor neuron spike but by mechanical stretch imposed by antagonistic muscles. Whereas 'stretch activation' and its reciprocal phenomenon 'shortening deactivation' are observed to varying extents in all striated muscles, both are particularly prominent in the indirect flight muscles of insects. Here we show changes in thick-filament structure and actin-myosin interactions in living, flying Drosophila with the use of synchrotron small-angle X-ray diffraction. To elicit stable flight behaviour and permit the capture of images at specific phases within the 5-ms wingbeat cycle, we tethered flies within a visual flight simulator. We recorded images of 340 micros duration every 625 micros to create an eight-frame diffraction movie, with each frame reflecting the instantaneous structure of the contractile apparatus. These time-resolved measurements of molecular-level structure provide new insight into the unique ability of insect flight muscle to generate elevated power at high frequency.

Submaximal power output from the dorsolongitudinal flight muscles of the hawkmothManduca sexta

To assess the extent to which the power output of a synchronous insect flight muscle is maximized during flight, we compared the maximum potential power output of the mesothoracic dorsolongitudinal (dl1) muscles of Manduca sexta to their power output in vivo. Holding temperature and cycle frequency constant at 36 degrees C and 25 Hz, respectively, we varied the phase of activation, mean length and strain amplitude. Under in vivo conditions measured in tethered flight, the dl1 muscles generated only 40-67% of their maximum potential power output. Compared to the in vivo phase of activation, the phase that maximized power output was advanced by 12% of the cycle period, and the length that maximized power output was 10% longer than the in vivo operating length.

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.

FLIGHT CONTROL

Despite a century of manned flight, when it comes to aerobatics, we're still a long way behind insects. And even though their agility can be extremely frustrating when evicting an unwanted guest, insects can teach us a great deal about the complex forces that keep them aloft and the mechanisms that control them. Michael Dickinson is fascinated by all aspects of insect flight: from the aerodynamic forces they generate to the complex neural systems that control each intricate wing beat. But it hadn't been possible to correlate variations in insect wing beats and the muscles that control them,with the effects they have on a flight path until recent technical developments allowed Claire Balint, a student in the Dickinson lab, to simultaneously monitor flight muscle activity and wing movements to see how flies steer their erratic path(p. 3813).But flies are notoriously mobile; the only way for Balint to collect the high speed flight recordings she needed to analyse the insect's wing movements was to tether the insect in a flight arena while focusing three ultra-high speed cameras on the flapping insect to capture its intricate manoeuvres. And by skilfully inserting microscopic electrodes into five of the insect's flight muscles, she could record flight muscle activity simultaneously as they flew into a mild headwind. But Balint also needed to measure the aerodynamic forces generated by each wing beat before she could begin correlating the insect's muscle activity with the forces generated. Digitising the positions of both right and left wings over a total of almost 870 wingbeats, Balint was able to calculate the forces generated by the wings as they moved through the air, as well as measuring them on a scaled-up mechanical model, before beginning the painstaking task of correlating the forces that keep the insect aloft with individual muscle activity.Balint explains that `although a reasonably robust theory exists for predicting the forces resulting from an arbitrary change in wing motion, the link between aerodynamically relevant changes in wing kinematics and the activity of specific steering muscles was less clear'. She and Dickinson also knew that certain muscle groups were responsible for three individual aspects of the insect's wing beat movements; the downstroke deviation, the dorsal amplitude and a shift in the ventral amplitude known as `mode'. Undaunted by the enormous amount of data generated by the flapping insects, Balint began analysing the aerodynamic forces generated by the insects according to each of these wing beat features, to see how they affected the insect's aerodynamic performance. Thanks to this novel approach, the team soon realised that specific sets of muscles were responsible for different aspects of the insect's aerobatic armoury. `The basalare muscles primarily control lift and roll by varying the downstroke force, the muscles of pteralae III and I control thrust and yaw by controlling the upstroke force and an unknown muscle group controls lift and roll by varying the upstroke force inclination',explains Balint.Having found that it's the flies' ability to control several force generating mechanisms in concert that allows them to dodge and weave so effectively, Dickinson is keen to know more about the elusive insect's flight and pursuit strategies.

Ca-Activation and Stretch-Activation in Insect Flight Muscle

Asynchronous insect flight muscle is specialized for myogenic oscillatory work, but can also produce isometric tetanic contraction. In skinned insect flight muscle fibers from Lethocerus, with sarcomere length monitored by a striation follower, we determined the relation between isometric force ( F 0) at serial increments of [Ca 2+] and the additional active force recruited at each [Ca 2+] by a stretch of ∼12 nm per half-sarcomere ( F SA). The isometric force-pCa relation shows that 1.5–2 units of pCa are necessary to raise isometric force from its threshold (pCa ∼6.5) to its maximum ( F 0,max). The amplitude of F SA depends only on the preceding baseline level of isometric force, which must reach at least 0.05 F 0,max to enable stretch-activation. F SA rises very steeply to its maximum as F 0 reaches ∼0.2 F 0,max, then decreases as F 0 increases so as to produce a constant sum ( F 0 + F SA) = F max. Thus Ca- and stretch-activation are complementary pathways that trigger a common process of cross-bridge attachment and force production. We suggest that stretch-induced distortion of attached cross-bridges relieves the steric blocking by tropomyosin of additional binding sites on actin, thereby enabling maximum force even at low [Ca 2+].

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.

Cross-Bridge Number, Position, and Angle in Target Zones of Cryofixed Isometrically Active Insect Flight Muscle

Electron micrographic tomograms of isometrically active insect flight muscle, freeze substituted after rapid freezing, show binding of single myosin heads at varying angles that is largely restricted to actin target zones every 38.7 nm. To quantify the parameters that govern this pattern, we measured the number and position of attached myosin heads by tracing cross-bridges through the three-dimensional tomogram from their origins on 14.5-nm-spaced shelves along the thick filament to their thin filament attachments in the target zones. The relationship between the probability of cross-bridge formation and axial offset between the shelf and target zone center was well fitted by a Gaussian distribution. One head of each myosin whose origin is close to an actin target zone forms a cross-bridge most of the time. The probability of cross-bridge formation remains high for myosin heads originating within 8 nm axially of the target zone center and is low outside 12 nm. We infer that most target zone cross-bridges are nearly perpendicular to the filaments (60% within 11°). The results suggest that in isometric contraction, most cross-bridges maintain tension near the beginning of their working stroke at angles near perpendicular to the filament axis. Moreover, in the absence of filament sliding, cross-bridges cannot change tilt angle while attached nor reach other target zones while detached, so may cycle repeatedly on and off the same actin target monomer.

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.