Cross-bridge attachment during high-speed active shortening of skinned fibers of the rabbit psoas muscle: Implications for cross-bridge action duringmaximum velocity of filament sliding
R. Stehle et B. Brenner, Cross-bridge attachment during high-speed active shortening of skinned fibers of the rabbit psoas muscle: Implications for cross-bridge action duringmaximum velocity of filament sliding, BIOPHYS J, 78(3), 2000, pp. 1458-1473
To characterize the kinetics of cross-bridge attachment to actin during unl
oaded contraction (maximum velocity of filament sliding), ramp-shaped stret
ches with different stretch-velocities (2-40,000 nm per half-sarcomere per
s) were applied to actively contracting skinned fibers of the rabbit psoas
muscle. Apparent fiber stiffness observed during such stretches was plotted
versus the speed of the imposed stretch (stiffness-speed relation) to deri
ve the rate constants for cross-bridge dissociation from actin. The stiffne
ss-speed relation obtained for unloaded shortening conditions was shifted b
y about two orders of magnitude to faster stretch velocities compared to is
ometric conditions and was almost identical to the stiffness-speed relation
observed in the presence of MgATP gamma S at high Ca2+ concentrations, i.e
., under conditions where cross-bridges are weakly attached to the fully Ca
2+ activated thin filaments. These data together with several control exper
iments suggest that, in contrast to previous assumptions, most of the fiber
stiffness observed during high-speed shortening results from weak cross-br
idge attachment to actin. The fraction of strongly attached cross-bridges d
uring unloaded shortening appears to be as low as some 1-5% of the fraction
present during isometric contraction. This is about an order of magnitude
less than previous estimates in which contribution of weak cross-bridge att
achment to observed fiber stiffness was not considered. Our findings imply
that 1) the interaction distance of strongly attached cross-bridges during
high-speed shortening is well within the range consistent with conventional
cross-bridge models, i.e., that no repetitive power strokes need to be ass
umed, and 2) that a significant part of the negative forces that limit the
maximum speed of filament sliding might originate from weak cross-bridge in
teractions with actin.