4.5 Article

The 3D trajectory of the body centre of mass during adult human walking: Evidence for a speed-curvature power law

Journal

JOURNAL OF BIOMECHANICS
Volume 44, Issue 4, Pages 732-740

Publisher

ELSEVIER SCI LTD
DOI: 10.1016/j.jbiomech.2010.10.035

Keywords

Centre of mass; Walking; Gait; 3D-trajectory; Power law

Funding

  1. Universita degli Studi di Milano
  2. Italian Foundation for Multiple Sclerosis [2005/R/20]
  3. Italian Ministry of Health

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During straight walking, the body centre of mass (CM) follows a 3D figure-of-eight (bow-tie) trajectory about 0.2 m long and with sizes around 0.05 m on each orthogonal axis. This was shown in 18 healthy adults walking at 0.3 to 1.4 m s(-1) on a force-treadmill (Tesio and Rota, 2008). Double integration of force signals can provide both the changes of mechanical energy of the CM and its 3D displacements (Tesio et al., 2010). In the same subjects, the relationship between the tangential speed of the CM, Vt, the curvature. C, and its inverse-the radius of curvature, re were analyzed. A power law (PL) model was applied, i.e. log Vt was regressed over log r(c). A PL is known to apply to the most various goal-directed planar movements (e.g. drawing), where the coefficient of log r(c), beta, usually takes values around 1/3. When the PL was fitted to the whole dataset, beta was 0.346 and variance explanation, R-2, was 59.8%. However, when the data were split into low- and high-curvature subsets (LC, HC, arbitrary cut-off of C=0.05 mm r(c)=20 mm), beta was 0.185 in the LC (R-2 0.214) and 0.486 in the HC (R-2 0.536) tracts. R-2 on the whole dataset increased to 0.763 if the LC-HC classification of the forward speed and their interaction entered the model. The beta coefficient, the curvature C, and the pendulum-like recovery of mechanical energy were lower during the double foot-ground contact phase, compared to the single contact. Along the CM trajectory, curvature and muscle power output peaked together around the inversions of lateral direction. Non-zero torsion values were randomly distributed along 60% of the trajectory, suggesting that this is not segmented into piecewise planar tracts. It is proposed that the trajectory can be segmented into one tract that is more actively controlled (tie) where a PL fits poorly and another tract which is more ballistic (bow) where a PL fits well. Results need confirmation through more appropriate 3D PL modelling. (C) 2010 Elsevier Ltd. All rights reserved.

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