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Table 1 Model parameters used in the simulations with the Huxley’57 model

From: Thermodynamic properties of muscle contraction models and associated discrete-time principles

Model parameters
\(\mu \hbox {T}\)\(100\hbox { zJ}\)
\(s^{+}\)\(20\hbox { nm}\)
\(s^{-}\)\(-20\hbox { nm}\)
\(s^{*}\)0
\(\tilde{s}\)\(9\hbox { nm}\)
\({\bar{s}}\)\(5\hbox { nm}\)
\(\kappa _{w}\)\(1.1\hbox { pN nm}^{-1}\)
\(k_{\mathrm{max}}\)\(41.3 \times 10^{-3}\hbox { ms}^{-1}\)
\(k_{\mathrm{min}}\)\(10 \times 10^{-3}\hbox { ms}^{-1}\)
\(k_{\mathrm{mid}}\)\(30 \,k_{\mathrm{max}}\)
\(\lambda _{1}\)\(6.21 \times 10^{-5}\hbox { nm}^{-8}\)
\(\lambda _{2}\)\(3\, \lambda _{1}\)
\(\alpha _{w}\)\(\frac{1}{2} \kappa _{w}\,({\tilde{s}} - {\bar{s}})^{2}\)
\(\alpha _{{k}_{1}}\)\(k_{\mathrm{mid}}/ \lambda _{1}\)
\(\alpha _{{k}_{2}}\)\(k_{\mathrm{mid}}\)