Abstract
Running, walking, flying and swimming are all processes in which animals produce propulsion by executing rhythmic motions of their bodies. Dynamical stability of the locomotion is hardly automatic: millions of older people are injured by falling each year. Stability frequently requires sensory feedback. We investigate how organisms obtain the information they use in maintaining their stability. Assessing stability of a periodic orbit of a dynamical system requires information about the dynamics of the system off the orbit. For locomotion driven by a periodic orbit, perturbations that “kick” the trajectory off the orbit must occur in order to observe convergence rates toward the orbit. We propose that organisms generate excitations in order to set the gains for stabilizing feedback. We hypothesize further that these excitations are stochastic but have heavy-tailed, non-Gaussian probability distributions. Compared to Gaussian distributions, we argue that these are more effective for estimating stability characteristics of the orbit. Finally, we propose experiments to test the efficacy of these ideas.
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Notes
The vector fields are discontinuous at impacts, and their dimension may change due to different numbers of ground contacts. A slightly larger model would also describe the motion of the COM, but the periodic orbit would be replaced by a trajectory that undergoes a fixed horizontal translation each step.
The RMSE is the \(L^2\) error over the probability space of realizations. Its square has the appealing property of being the variance plus the square bias of the estimator. We use the RMSE of Floquet exponent estimates, as opposed to estimates of the Floquet multiplier, because the former has better invariance properties. In particular, the value of the exponent is the same when computed from trajectories which make different numbers of circuits around a periodic orbit. To simulate the expectation, \(10^3\) realizations are used.
In this example and the last, the intersections of the numerical solution with the cross section of interest are approximated with cubic Hermite splines. Doing so is unnecessary in the van der Pol setting—a linear interpolant is sufficiently accurate. However, that is not the case for the perturbed Lorenz system studied here (time step \(\varDelta t = 2 \times 10^{-4}\)).
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Communicated by Benjamin Lindner.
This article belongs to the Special Issue on Control Theory in Biology and Medicine. It derived from a workshop at the Mathematical Biosciences Institute, Ohio State University, Columbus, OH, USA.
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Guckenheimer, J., Javeed, A. Locomotion: exploiting noise for state estimation. Biol Cybern 113, 93–104 (2019). https://doi.org/10.1007/s00422-018-0772-z
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DOI: https://doi.org/10.1007/s00422-018-0772-z