Changes in crossbridge attachment in a myosin-regulated muscle

Invertebrate muscles: thin and thick filament structure; molecular basis of contraction and its regulation, catch and asynchronous muscle

This is the second in a series of canonical reviews on invertebrate muscle. We cover here thin and thick filament structure, the molecular basis of force generation and its regulation, and two special properties of some invertebrate muscle, catch and asynchronous muscle. Invertebrate thin filaments resemble vertebrate thin filaments, although helix structure and tropomyosin arrangement show small differences. Invertebrate thick filaments, alternatively, are very different from vertebrate striated thick filaments and show great variation within invertebrates. Part of this diversity stems from variation in paramyosin content, which is greatly increased in very large diameter invertebrate thick filaments. Other of it arises from relatively small changes in filament backbone structure, which results in filaments with grossly similar myosin head placements (rotating crowns of heads every 14.5 nm) but large changes in detail (distances between heads in azimuthal registration varying from three to thousands of crowns). The lever arm basis of force generation is common to both vertebrates and invertebrates, and in some invertebrates this process is understood on the near atomic level. Invertebrate actomyosin is both thin (tropomyosin:troponin) and thick (primarily via direct Ca(++) binding to myosin) filament regulated, and most invertebrate muscles are dually regulated. These mechanisms are well understood on the molecular level, but the behavioral utility of dual regulation is less so. The phosphorylation state of the thick filament associated giant protein, twitchin, has been recently shown to be the molecular basis of catch. The molecular basis of the stretch activation underlying asynchronous muscle activity, however, remains unresolved.

A mechanical study of regulation in the striated adductor muscle of the scallop

Chemically skinned fibre bundles were prepared from the striated adductor muscle of the sea scallop, Placopecten magellanicus. The relation between tension and calcium concentration was determined in activating solutions containing 5 mM-MgATP, ionic strength 0.2, pH 7.1 at 20 degrees C. The isometric tension rose from zero to its maximum value between pCa 6.0 and 5.2. The steepness of the relation cannot be accounted for in terms of the binding of calcium to the two known sites on myosin and suggests that there must be an additional, co-operative mechanism. The regulatory light chain content of the fibre bundles was determined by urea gel electrophoresis and was found to be approximately 2 light chains per myosin molecule. The regulatory light chains were removed completely by treatment with EDTA at 25-30 degrees C. Fibre bundles then showed a total loss of control over contraction; a high tension was generated whether or not calcium was present in the bathing solution. Complete removal of the regulatory light chains did not greatly affect the tension generated or the stiffness in the rigor state. Control of contraction could be restored completely by the addition of regulatory light chains from scallop muscle. Treatment with EDTA at 0-12 degrees C resulted in the removal of 0.76-2.0 regulatory light chains per myosin molecule. Fibre bundles for which removal was less than complete were partially sensitive to calcium, i.e. tension was higher in the presence of calcium than in its absence. The results indicate that the normal mechanism of tension generation in scallop muscle is mediated primarily through myosin and not thin filament control. This finding is consistent with previous studies of the ATPase activity of myofibrils from scallop muscle.

Electron microscopy of scallop myosin. Location of regulatory light chains

The heads of the Ca2+-sensitive myosin molecules from scallop muscle, contrasted for electron microscopy by rotary shadowing, display two appearances depending on the presence or absence of the regulatory light chains. The heads of intact myosin appear "pear-shaped" as described for vertebrate myosin (Elliott & Offer, 1978): they are widest at the end remote from the tail and taper to a narrower neck near their junction with the tail. In contrast, myosin heads that lack the regulatory light chains appear more globular. The neck region is no longer visible: the rounded heads appear directly attached to the tail or there is an apparent gap between the head and the tail. Two preparations of myosin subfragment-1 that differ in light chain content show a similar difference in appearance. Fab fragments of antibodies specific for the light chains bind to the myosin heads and can also be visualized in the electron microscope using rotary shadowing. Both Fab fragments specific for the regulatory light chains and Fab fragments specific for the essential light chains bind preferentially to intact scallop myosin in the narrow region of the myosin head near its junction with the tail.

Electron microscopy and image analysis of myosin filaments from scallop striated muscle

Thick filaments have been isolated from the striated adductor muscle of the scallop and examined by electron microscopy after negative staining. Many filaments appear intact, and reveal a centrally located bare-zone and a well-defined helical surface array of myosin crossbridges characterized by a 145 A axial period and prominent helical tracks of pitch 480 A. Heavy-metal shadowing shows that these helices are right-handed. A small perturbation of alternate crossbridge levels produces an axial period of 290 A, which is most prominent in a region on either side of the bare-zone. Image analysis reveals that the crossbridge array has 7-fold rotational symmetry, one of the possibilities suggested by earlier X-ray diffraction studies of native filaments in scallop muscle. A low-resolution three-dimensional reconstruction shows elongated surface projections ("crossbridges") that probably represent unresolved pairs of myosin heads. They run almost parallel to the filament surface, but are slewed slightly from the axis so that they lie along the right-handed helical tracks of pitch 480 A. The connection to the filament backbone probably occurs at the end of the crossbridges nearer the bare-zone; thus, their sense of tilt appears to be opposite to that of rigor attachment to actin. The 290 A period arises from a different distribution of crossbridge density at alternate levels; in addition, there are weak connections between the top of one crossbridge and the bottom of the next, 145 A away. The prominence of the 290 A period near the bare-zone suggests that anti-parallel molecular interactions are mainly responsible for this perturbation.

Segmental flexibility and head-head interaction in scallop myosin. A study using saturation transfer electron paramagnetic resonance spectroscopy

Saturation transfer electron paramagnetic resonance spectroscopy was used to investigate the rotational motion of the head domains of native and desensitized scallop myosin and its proteolytic subfragments. Scallop myosin was spin-labelled with 4-(2-iodoacetamido)-2,2,6,6-tetramethylpiperidinooxyl, which reacted with a heavy chain residue in the subfragment 1 domain. As previously shown for rabbit skeletal muscle myosin (Thomas et al., 1975), the two head domains of native scallop myosin appear to have independent motion (rotational correlation time, pi, = 0.8 X 10(-7) s for subfragment 1; 1.4 X 10(-7) s for myosin). However, removal of a regulatory light chain, to effect desensitization of the actin-activated ATPase, was associated with an increase in pi for myosin to a value of 2.4 X 10(-6) s. The Ca2+ sensitivity and initial correlation time were restored on recombination of the regulatory light chain in the presence of Mg2+. Sedimentation velocity profiles in an analytical ultracentrifuge indicated that the desensitized myosin preparations were largely monomeric and therefore the change in pi appears to reflect an intramolecular event. Addition of EDTA to spin-labelled scallop heavy meromyosin caused an immediate 2.5 to 4-fold increase in pi and a partial desensitization of the ATPase activity. Comparable experiments with subfragment 1 yielded a barely detectable increase in pi (1.5-fold) in the first ten minutes. The restricted rotational motion observed in desensitized myosin and heavy meromyosin could arise by a conformational change in the subfragment 1-subfragment 2 hinge region or by an association of one head with its partner. The latter mechanism, involving the exposed light chain binding site, would also explain the preferential release of one regulatory light chain from scallop myosin, and might account for some other co-operative effects observed in this molecule (Bagshaw, 1980).

Mechanics and energetics of contraction in striated muscle of the sea scallop, Placopecten magellanicus

1. Mechanics and energetics of contraction in the striated adductor muscle of the sea scallop, Placopecten magellanicus, were determined and compared to a more conventional muscle preparation, the semitendinosus muscle of the frog, Rana pipiens. Experiments were conducted at 10 degrees C. 2. Scallop and frog striated muscle exhibited similar isometric twitch kinetics, heat coefficients (ratio of force produced to energy liberated), and twitch to tetanus ratios. 3. There were significant differences between scallop and frog muscle in that scallop muscle demonstrated a 30% lower isometric force, an inability to maintain force during a tetanus, and a transient decrease in economy of force development in a twitch after a tetanus, i.e. a decrease in the isometric heat coefficient.