Abstract

This paper provides a comprehensive explanation of striated muscle mechanics and contraction on the basis of filament rotations. Helical proteins, particularly the coiled-coils of tropomyosin, myosin and α-actinin, shorten their H-bonds cooperatively and produce torque and filament rotations when the Coulombic net-charge repulsion of their highly charged side-chains is diminished by interaction with ions. The classical “two-component model” of active muscle differentiated a “contractile component” which stretches the “series elastic component” during force production. The contractile components are the helically shaped thin filaments of muscle that shorten the sarcomeres by clockwise drilling into the myosin cross-bridges with torque decrease (= force-deficit). Muscle stretch means drawing out the thin filament helices off the cross-bridges under passive counterclockwise rotation with torque increase (= stretch activation). Since each thin filament is anchored by four elastic α-actinin Z-filaments (provided with force-regulating sites for Ca2+ binding), the thin filament rotations change the torsional twist of the four Z-filaments as the “series elastic components”. Large scale models simulate the changes of structure and force in the Z-band by the different Z-filament twisting stages A, B, C, D, E, F and G. Stage D corresponds to the isometric state. The basic phenomena of muscle physiology, i. e. latency relaxation, Fenn-effect, the force-velocity relation, the length-tension relation, unexplained energy, shortening heat, the Huxley-Simmons phases, etc. are explained and interpreted with the help of the model experiments.

Highlights

  • The basic molecular event for filament sliding and force generationAccording to the conventional theory the subfragment S1 of the enzyme myosin supplies the force for actin filament sliding during muscle contraction by an ATP-dependent “working stroke” of the “lever arm”

  • This paper provides a comprehensive explanation of striated muscle mechanics and contraction on the basis of filament rotations

  • Since each thin filament is anchored by four elastic α-actinin Z-filaments, the thin filament rotations change the torsional twist of the four Z-filaments as the “series elastic components”

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Summary

Introduction

According to the conventional theory the subfragment S1 of the enzyme myosin supplies the force for actin filament sliding during muscle contraction by an ATP-dependent “working stroke” of the “lever arm” (see for example Holmes in Sugi's book, p. 13 [1]). For example in vitro sliding of actin filaments over a myosin lawn in the presence of ATP should depend on an effective drilling motion. When they undergo the characteristic "wiggling" motions without displacement [3] slipping against the substratum may take place under idle rotation. A basic rotational mechanism seems to work and may replace the conventional conception of the “power” or “working stroke” It will be shown by future work whether the torque production in α-helical proteins is sufficient to explain the filament rotation of the various kinds of biological motions or whether it is necessary to assume other physical forces, e.g. such as proposed by Tirosh (this volume)

Stretch activation
The twisting stages A to G of the four anchoring series elastic Z-filaments
Z-band dynamics and the “latency-relaxation”
The “Fenn-effect”
The force-velocity relation
3.12. Unloaded shortening velocity and sarcomere length
3.14. The Huxley-Simmons phases during quick length changes
3.15. Shortening after sudden load reduction
3.17. The Z-filaments in the region of high tension between stage D and G
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