Elisabetta Brunello

Skeletal muscle performance determined by modulation of number of myosin motors rather than motor force or stroke size.

Skeletal muscle can bear a high load at constant length, or shorten rapidly when the load is low. This force-velocity relationship is the primary determinant of muscle performance in vivo. Here we exploited the quasi-crystalline order of myosin II motors in muscle filaments to determine the molecular basis of this relationship by X-ray interference and mechanical measurements on intact single cells. We found that, during muscle shortening at a wide range of velocities, individual myosin motors maintain a force of about 6 pN while pulling an actin filament through a 6 nm stroke, then quickly detach when the motor reaches a critical conformation. Thus we show that the force-velocity relationship is primarily a result of a reduction in the number of motors attached to actin in each filament in proportion to the filament load. These results explain muscle performance and efficiency in terms of the molecular mechanism of the myosin motor.

Skeletal muscle resists stretch by rapid binding of the second motor domain of myosin to actin

A shortening muscle is a machine that converts metabolic energy into mechanical work, but, when a muscle is stretched, it acts as a brake, generating a high resistive force at low metabolic cost. The braking action of muscle can be activated with remarkable speed, as when the leg extensor muscles rapidly decelerate the body at the end of a jump. Here we used time-resolved x-ray and mechanical measurements on isolated muscle cells to elucidate the molecular basis of muscle braking and its rapid control. We show that a stretch of only 5 nm between each overlapping set of myosin and actin filaments in a muscle sarcomere is sufficient to double the number of myosin motors attached to actin within a few milliseconds. Each myosin molecule has two motor domains, only one of which is attached to actin during shortening or activation at constant length. A stretch strains the attached motor domain, and we propose that combined steric and mechanical coupling between the two domains promotes attachment of the second motor domain. This mechanism allows skeletal muscle to resist external stretch without increasing the force per motor and provides an answer to the longstanding question of the functional role of the dimeric structure of muscle myosin.

Force generation by skeletal muscle is controlled by mechanosensing in myosin filaments

Contraction of both skeletal muscle and the heart is thought to be controlled by a calcium-dependent structural change in the actin-containing thin filaments, which permits the binding of myosin motors from the neighbouring thick filaments to drive filament sliding. Here we show by synchrotron small-angle X-ray diffraction of frog (Rana temporaria) single skeletal muscle cells that, although the well-known thin-filament mechanism is sufficient for regulation of muscle shortening against low load, force generation against high load requires a second permissive step linked to a change in the structure of the thick filament. The resting (switched ‘OFF’) structure of the thick filament is characterized by helical tracks of myosin motors on the filament surface and a short backbone periodicity. This OFF structure is almost completely preserved during low-load shortening, which is driven by a small fraction of constitutively active (switched ‘ON’) myosin motors outside thick-filament control. At higher load, these motors generate sufficient thick-filament stress to trigger the transition to its long-periodicity ON structure, unlocking the major population of motors required for high-load contraction. This concept of the thick filament as a regulatory mechanosensor provides a novel explanation for the dynamic and energetic properties of skeletal muscle. A similar mechanism probably operates in the heart.

Structural changes in the myosin filament and cross‐bridges during active force development in single intact frog muscle fibres: stiffness and X‐ray diffraction measurements

Structural and mechanical changes occurring in the myosin filament and myosin head domains during the development of the isometric tetanus have been investigated in intact frog muscle fibres at 4°C and 2.15 μm sarcomere length, using sarcomere level mechanics and X‐ray diffraction at beamline ID2 of the European Synchrotron Radiation Facility (Grenoble, France). The time courses of changes in both the M3 and M6 myosin‐based reflections were recorded with 5 ms frames using the gas‐filled RAPID detector (MicroGap Technology). Following the end of the latent period (11 ms after the start of stimulation), force increases to the tetanus plateau value (T0) with a half‐time of 40 ms, and the spacings of the M3 and M6 reflections (SM3 and SM6) increase by 1.5% from their resting values, with time courses that lead that of force by ∼10 and ∼20 ms, respectively. These temporal relations are maintained when the increase of force is delayed by ∼10 ms by imposing, from 5 ms after the first stimulus, 50 nm (half‐sarcomere)−1 shortening at the velocity (V0) that maintains zero force. Shortening at V0 transiently reduces SM3 following the latent period and delays the subsequent increase in SM3, but only delays the SM6 increase without a transient decrease. Shortening at V0 imposed at the tetanus plateau causes an abrupt reduction of the intensity of the M3 reflection (IM3), whereas the intensity of the M6 reflection (IM6) is only slightly reduced. The changes in half‐sarcomere stiffness indicate that the isometric force at each time point is proportional to the number of myosin heads bound to actin. The different sensitivities of the intensity and spacing of the M3 and M6 reflections to the mechanical responses support the view that the M3 reflection in active muscle originates mainly from the myosin heads attached to the actin filament and the M6 reflection originates mainly from a fixed structure in the myosin filament signalling myosin filament length changes during the tetanus rise.

The mechanism of the resistance to stretch of isometrically contracting single muscle fibres.

Rapid attachment to actin of the detached motor domain of myosin dimers with one motor domain already attached has been hypothesized to explain the stretch‐induced changes in X‐ray interference and stiffness of active muscle. Here, using half‐sarcomere mechanics in single frog muscle fibres (2.15 μm sarcomere length and 4°C), we show that: (1) an increase in stiffness of the half‐sarcomere under stretch is specific to isometric contraction and does not occur in rigor, indicating that the mechanism of stiffness increase is an increase in the number of attached motors; (2) 2 ms after 100 μs stretches (amplitude 2–8 nm per half‐sarcomere) imposed during an isometric tetanus, the stiffness of the array of myosin motors in each half‐sarcomere (em) increases above the isometric value (em0); (3) em has a sigmoidal dependence on the distortion of the motor domains (Δz) attached in isometric contraction, with a maximum ∼2 em0 for a distortion of ∼6 nm; em is influenced by detachment of motors at Δz > 6 nm; (4) at the end of the 100 μs stretch the relation between em/em0 and Δz lies slightly but not significantly above that at 2 ms. These results support the idea that stretch‐induced sliding of the actin filament distorts the actin‐attached motor domain of the myosin dimers away from the centre of the sarcomere, providing the steric conditions for rapid attachment of the second motor domain. The rate of new motor attachment must be as high as 7.5 × 104 s−1 and explains the rapid and efficient increase of the resistance of active muscle to stretch.

Motion of myosin head domains during activation and force development in skeletal muscle

Muscle contraction is driven by a change in the structure of the head domain of myosin, the “working stroke” that pulls the actin filaments toward the midpoint of the myosin filaments. This movement of the myosin heads can be measured very precisely in intact muscle cells by X-ray interference, but until now this technique has not been applied to physiological activation and force generation following electrical stimulation of muscle cells. By using this approach, we show that the long axes of the myosin head domains are roughly parallel to the filaments in resting muscle, with their center of mass offset by approximately 7 nm from the C terminus of the head domain. The observed mass distribution matches that seen in electron micrographs of isolated myosin filaments in which the heads are folded back toward the filament midpoint. Following electrical stimulation, the heads move by approximately 10 nm away from the filament midpoint, in the opposite direction to the working stroke. The time course of this motion matches that of force generation, but is slower than the other structural changes in the myosin filaments on activation, including the loss of helical and axial order of the myosin heads and the change in periodicity of the filament backbone. The rate of force development is limited by that of attachment of myosin heads to actin in a conformation that is the same as that during steady-state isometric contraction; force generation in the actin-attached head is fast compared with the attachment step.

The structural basis of the increase in isometric force production with temperature in frog skeletal muscle

X‐ray diffraction patterns were recorded from isolated single fibres of frog skeletal muscle during isometric contraction at temperatures between 0 and 17°C. Isometric force was 43 ± 2% (mean ±s.e.m., n= 10) higher at 17°C than 0°C. The intensity of the first actin layer line increased by 57 ± 18% (n= 5), and the ratio of the intensities of the equatorial 1,1 and 1,0 reflections by 20 ± 7% (n= 10), signalling radial or azimuthal motions of the myosin head domains. The M3 X‐ray reflection from the axial repeat of the heads along the filaments was 27 ± 4% more intense at 17°C, suggesting that the heads became more perpendicular to the filaments. The ratio of the intensities of the higher and lower angle peaks of the M3 reflection (RM3) was 0.93 ± 0.02 (n= 5) at 0°C and 0.77 ± 0.02 at 17°C. These peaks are due to interference between the two halves of each myosin filament, and the RM3 decrease shows that heads move towards the midpoint of the myosin filament at the higher temperature. Calculations based on a crystallographic model of the heads indicated that the observed RM3 change corresponds to tilting of their light‐chain domains by 9 deg, producing an axial displacement of 1.4 nm, which is equal to that required to strain the actin and myosin filaments under the increased force. We conclude that the higher force generated by skeletal muscle at higher temperature can be accounted for by axial tilting of the myosin heads.

Sarcomere‐length dependence of myosin filament structure in skeletal muscle fibres of the frog

Contraction of skeletal muscle is thought to be regulated by a structural change in the actin‐containing thin filaments of the sarcomere, but recent results have suggested that a structural change in the myosin‐containing thick filaments may also be involved. We show that thick filament structure in resting muscle depends on the overlap with the thin filaments of the region of the thick filament containing myosin binding protein C (MyBP‐C). During isometric contraction, the regions of the thick filaments that do not overlap with thin filaments are highly disordered, in contrast to their helical order in resting muscle. The results provide strong support for the role of a structural transition in the thick filaments, mediated by an interaction between MyBP‐C and the thin filaments, in the physiological regulation of contraction in skeletal muscle.

The contributions of filaments and cross-bridges to sarcomere compliance in skeletal muscle

Muscle contraction is driven at the molecular level by a structural working stroke in the head domain of the myosin cross‐bridge linking the thick and thin filaments. Crystallographic models suggest that the working stroke corresponds to a relative movement of 11 nm between the attachments of the head domain to the thin and thick filaments. The molecular mechanism of force generation depends on the relationship between cross‐bridge force and movement, which is determined by cross‐bridge and filament compliances. Here we measured the compliance of the cross‐bridges and of the thin and thick filaments by combining mechanical and X‐ray diffraction experiments. The results show that cross‐bridge compliance is relatively low and fully accounted for by the elasticity of the myosin head, suggesting that the myosin cross‐bridge generates isometric force by a small sub‐step of the 11 nm stroke that drives filament sliding at low load.

Thick filament mechano-sensing is a calcium-independent regulatory mechanism in skeletal muscle

Recent X-ray diffraction studies on actively contracting fibres from skeletal muscle showed that the number of myosin motors available to interact with actin-containing thin filaments is controlled by the stress in the myosin-containing thick filaments. Those results suggested that thick filament mechano-sensing might constitute a novel regulatory mechanism in striated muscles that acts independently of the well-known thin filament-mediated calcium signalling pathway. Here we test that hypothesis using probes attached to the myosin regulatory light chain in demembranated muscle fibres. We show that both the extent and kinetics of thick filament activation depend on thick filament stress but are independent of intracellular calcium concentration in the physiological range. These results establish direct control of myosin motors by thick filament mechano-sensing as a general regulatory mechanism in skeletal muscle that is independent of the canonical calcium signalling pathway.