An internal viscous element limits unloaded velocity of sarcomere shortening in rat myocardium.

1. Peak twitch force (F0) and sarcomere length (SL) were measured in trabeculae that had been dissected from the right ventricle of rat heart and that were superfused with a modified Krebs‐Henseleit solution at 25 degrees C. Sarcomere length was measured by laser diffraction techniques. Force was measured with a silicone strain gauge. Unloaded velocity of sarcomere shortening (V0) was measured by the ‘isovelocity release’ technique. 2. At [Ca2+]o = 1.5 mM and SL below 1.9 microns, V0 increased in proportion to SL, while V0 was independent of SL above 1.9 microns. At [Ca2+]o = 0.5 mM, V0 was proportional to SL up to 2.2 microns. At [Ca2+]o = 0.2 mM, V0 was proportional to SL up to 2.3 microns which is the longest SL that we were able to study in our trabeculae. 3. A unique relationship was observed between V0 and F0, irrespective of whether F0 was altered by variation of [Ca2+]o or sarcomere length above slack length. 4. Passive viscosity (Fv) was measured during the pause between contractions in the presence of 1.5 mM [Ca2+bdo and in the range SL = 2.0‐2.1 microns by applying 0.1 micron stretches at various velocities up to v = 30 microns s‐1. The force response to stretch, corrected for the contribution of parallel elastic force, showed viscoelastic characteristics with an exponential increase to a maximum (Fv) during stretch and an exponential decline after the end of the stretch. Fv increased, by 0.3%F0 microns‐1 s‐1, in proportion to v < 5 microns s‐1; the increase of Fv was smaller at higher v, suggesting non‐Newtonian viscous properties. 5. The time constant of the increase of force during the stretch decreased (tau rise congruent to 7 ms to tau rise congruent to 4 ms) with increases in v (congruent to 4 microns s‐1 to v congruent to 10 microns s‐1; P = 0.02). The time constant of decay of force at the end of the stretch also decreased with increases in v (tau decay congruent to 8 ms at v congruent to 4 microns s‐1 to tau decay congruent to 3 ms at v congruent to 30 microns s‐1; P < 0.001). Calculated stiffness of the elastic term of the viscoelastic element was independent of v, i.e. 45‐50 N mm‐3.(ABSTRACT TRUNCATED AT 400 WORDS)

[1]  B. R. Jewell,et al.  Calcium‐ and length‐dependent force production in rat ventricular muscle , 1982, The Journal of physiology.

[2]  K. Edman The velocity of unloaded shortening and its relation to sarcomere length and isometric force in vertebrate muscle fibres. , 1979, The Journal of physiology.

[3]  A. Huxley,et al.  Tension transients during steady shortening of frog muscle fibres. , 1985, The Journal of physiology.

[4]  Y. Chiu,et al.  Force, velocity, and power changes during normal and potentiated contractions of cat papillary muscle. , 1987, Circulation research.

[5]  A. Huxley Muscle structure and theories of contraction. , 1957, Progress in biophysics and biophysical chemistry.

[6]  A. Huxley,et al.  Tension responses to sudden length change in stimulated frog muscle fibres near slack length , 1977, The Journal of physiology.

[7]  H. Keurs,et al.  Lack of effect of isoproterenol on unloaded velocity of sarcomere shortening in rat cardiac trabeculae. , 1991 .

[8]  H. T. ter Keurs,et al.  Tension Development and Sarcomere Length in Rat Cardiac Trabeculae: Evidence of Length‐Dependent Activation , 1980, Circulation research.

[9]  B. R. Jewell,et al.  Length‐Dependent Activation: Its Effect on the Length‐Tension Relation in Cat Ventricular Muscle , 1977, Circulation research.

[10]  P. Hofmann,et al.  Bound calcium and force development in skinned cardiac muscle bundles: effect of sarcomere length. , 1988, Journal of molecular and cellular cardiology.

[11]  K. Wang,et al.  Architecture of the sarcomere matrix of skeletal muscle: immunoelectron microscopic evidence that suggests a set of parallel inextensible nebulin filaments anchored at the Z line , 1988, The Journal of cell biology.

[12]  H. T. ter Keurs,et al.  Sarcolemma, sarcoplasmic reticulum, and sarcomeres as limiting factors in force production in rat heart. , 1990, Circulation research.

[13]  H. T. ter Keurs,et al.  Restoring forces and relaxation of rat cardiac muscle. , 1980, European heart journal.

[14]  E. Eisenberg,et al.  Evidence for cross-bridge attachment in relaxed muscle at low ionic strength. , 1982, Proceedings of the National Academy of Sciences of the United States of America.

[15]  F. Julian,et al.  Variation of muscle stiffness with force at increasing speeds of shortening , 1975, The Journal of general physiology.

[16]  H. Keurs,et al.  Force and velocity of sarcomere shortening in trabeculae from rat heart. Effects of temperature. , 1990 .

[17]  J. Haselgrove X-ray evidence for conformational changes in the myosin filaments of vertebrate striated muscle. , 1975, Journal of molecular biology.

[18]  K. Edman Mechanical deactivation induced by active shortening in isolated muscle fibres of the frog. , 1975, The Journal of physiology.

[19]  J. Murray,et al.  Molecular control mechanisms in muscle contraction. , 1973, Physiological reviews.

[20]  H. Keurs,et al.  Sarcomere dynamics in cat cardiac trabeculae. , 1991 .

[21]  A. Fabiato,et al.  Myoplasmic free calcium concentration reached during the twitch of an intact isolated cardiac cell and during calcium-induced release of calcium from the sarcoplasmic reticulum of a skinned cardiac cell from the adult rat or rabbit ventricle , 1981, The Journal of general physiology.

[22]  D. Allen,et al.  Calcium transients in mammalian ventricular muscle. , 1980, European heart journal.

[23]  A. Huxley,et al.  The relation between stiffness and filament overlap in stimulated frog muscle fibres. , 1981, The Journal of physiology.

[24]  V A Claes,et al.  Velocity of Shortening of Unloaded Heart Muscle and the Length‐Tension Relation , 1971, Circulation research.

[25]  G. M. Briggs,et al.  Modulation by the Thyroid State of Intracellular Calcium and Contractility in Ferret Ventricular Muscle , 1988, Circulation research.

[26]  H. T. ter Keurs,et al.  Comparison between the Sarcomere Length‐Force Relations of Intact and Skinned Trabeculae from Rat Right Ventricle: Influence of Calcium Concentrations on These Relations , 1986, Circulation research.

[27]  A. J. Brady,et al.  Mechanical properties of isolated cardiac myocytes. , 1991, Physiological reviews.

[28]  D L Morgan,et al.  Variation of muscle stiffness with tension during tension transients and constant velocity shortening in the frog. , 1981, The Journal of physiology.

[29]  L. E. Ford,et al.  Internal viscoelastic loading in cat papillary muscle. , 1982, Biophysical journal.

[30]  Myocardial segment velocity at a low load: time, length, and calcium dependence. , 1983, The American journal of physiology.

[31]  H. T. ter Keurs,et al.  Velocity of sarcomere shortening in rat cardiac muscle: relationship to force, sarcomere length, calcium and time. , 1984, The Journal of physiology.

[32]  L. E. Ford,et al.  Velocity transients and viscoelastic resistance to active shortening in cat papillary muscle. , 1982, Biophysical journal.

[33]  E. Sonnenblick,et al.  Instantaneous Force‐Velocity‐Length Determinants in the Contraction of Heart Muscle , 1965, Circulation research.

[34]  M. Noble,et al.  The Diastolic Viscous Properties of Cat Papillary Muscle , 1977, Circulation research.

[35]  W. Lehman Thick-filament-linked calcium regulation in vertebrate striated muscle , 1978, Nature.

[36]  P Haugen,et al.  The stiffness under isotonic releases during a twitch of a frog muscle fibre. , 1988, Advances in experimental medicine and biology.

[37]  N. Curtin,et al.  Energetic aspects of muscle contraction. , 1985, Monographs of the Physiological Society.