The force developed by actively lengthened muscle depends on different structures
across different scales of lengthening. For small perturbations, the active response of muscle is well
captured by a linear-time-invariant (LTI) system: a stiff spring in parallel with a light damper. The
force response of muscle to longer stretches is better represented by a compliant spring that can fix
its end when activated. Experimental work has shown that the stiffness and damping (impedance)
of muscle in response to small perturbations is of fundamental importance to motor learning and
mechanical stability, while the huge forces developed during long active stretches are critical for
simulating and predicting injury. Outside of motor learning and injury, muscle is actively lengthened
as a part of nearly all terrestrial locomotion. Despite the functional importance of impedance and
active lengthening, no single muscle model has all these mechanical properties. In this work, we
present the viscoelastic-crossbridge active-titin (VEXAT) model that can replicate the response of
muscle to length changes great and small. To evaluate the VEXAT model, we compare its response
to biological muscle by simulating experiments that measure the impedance of muscle, and the
forces developed during long active stretches. In addition, we have also compared the responses of
the VEXAT model to a popular Hill-type muscle model. The VEXAT model more accurately captures
the impedance of biological muscle and its responses to long active stretches than a Hill-type model
and can still reproduce the force-velocity and force-length relations of muscle. While the comparison
between the VEXAT model and biological muscle is favorable, there are some phenomena that can
be improved: the low frequency phase response of the model, and a mechanism to support passive
force enhancement.
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The force developed by actively lengthened muscle depends on different structures
across different scales of lengthening. For small perturbations, the active response of muscle is well
captured by a linear-time-invariant (LTI) system: a stiff spring in parallel with a light damper. The
force response of muscle to longer stretches is better represented by a compliant spring that can fix
its end when activated. Experimental work has shown that the stiffness and damping (impedance)
of mus...
»