Table 1.
Effect of TnTF88L on various contractile parameters at short and long SLs
Parameter1.9 µm2.3 µm
TnTWTTnTF88LTnTWTTnTF88L
Maximal tension (mN ⋅ mm−229.72 ± 1.25 31.63 ± 1.52a 49.07 ± 1.24 48.25 ± 0.93a 
Tension cost (pmol ⋅ mN−1 ⋅ mm−1 ⋅ s−12.56 ± 0.17 2.34 ± 0.11a 1.26 ± 0.06 1.32 ± 0.07a 
c (s−112.17 ± 0.42 10.98 ± 0.89a 7.95 ± 0.13 8.10 ± 0.38a 
b (s−14.32 ± 0.09 4.19 ± 0.09a 4.33 ± 0.11 4.37 ± 0.09a 
ktr (s−11.99 ± 0.05 1.83 ± 0.11a 1.61 ± 0.10 1.57 ± 0.05a 
Parameter1.9 µm2.3 µm
TnTWTTnTF88LTnTWTTnTF88L
Maximal tension (mN ⋅ mm−229.72 ± 1.25 31.63 ± 1.52a 49.07 ± 1.24 48.25 ± 0.93a 
Tension cost (pmol ⋅ mN−1 ⋅ mm−1 ⋅ s−12.56 ± 0.17 2.34 ± 0.11a 1.26 ± 0.06 1.32 ± 0.07a 
c (s−112.17 ± 0.42 10.98 ± 0.89a 7.95 ± 0.13 8.10 ± 0.38a 
b (s−14.32 ± 0.09 4.19 ± 0.09a 4.33 ± 0.11 4.37 ± 0.09a 
ktr (s−11.99 ± 0.05 1.83 ± 0.11a 1.61 ± 0.10 1.57 ± 0.05a 

Maximal tension was measured by exposing muscle fibers to saturating Ca2+ concentration (pCa 4.3) in a constantly stirred chamber. Tension cost was derived from the ATPase/tension relationship, as previously described (de Tombe and Stienen, 1995; Chandra et al., 2015). Parameters c and b were estimated by fitting the NLRD model to the force response phases to various amplitude stretch/release perturbations (Fig. 1; Ford et al., 2010). c represents the rate of force decay to a minimum force point following a sudden stretch in ML, and b represents the rate at which force rises at the new ML. ktr was estimated by fitting a monoexponential function to the rising phase of the force response to a large slack-restretch length maneuver and represents the rate of tension redevelopment (Brenner and Eisenberg, 1986). Estimates from several muscle fibers per group were averaged and presented as mean ± SEM. Statistical differences were analyzed using two-way ANOVA and subsequent post hoc multiple pairwise comparisons (Fisher’s LSD method). The number of fibers measured (from three hearts) for all groups was 10.

a

Not significantly different from TnTWT fibers.

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