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EasiestBigBen

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UOW College Australia

Dr Jon Shemell

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human locomotion human biomechanics gait analysis neuromuscular control

Summary

This document provides an overview of human locomotion, including kinetics of gait, neural control, and the process of replicating human gait. It details external and internal forces, along with examples of phase-based modeling.

Full Transcript

Locomotion II DR JON SHEMMELL MEDI258: HUMAN NEUROMECHANICS Learning objectives: Locomotion 2 u Kinetics of gait u Joint moments (torques) u Neural control of locomotion u Replicating human gait Kinetics of gait Kinetics of gait u External forces u gravity u fr...

Locomotion II DR JON SHEMMELL MEDI258: HUMAN NEUROMECHANICS Learning objectives: Locomotion 2 u Kinetics of gait u Joint moments (torques) u Neural control of locomotion u Replicating human gait Kinetics of gait Kinetics of gait u External forces u gravity u friction u ground reaction forces u Internal forces u muscles u friction Stance phase of walking modeled as an inverted pendulum High P.E. Low P.E. Low K.E. High K.E. u Forward momentum of the body provides angular rotation for rising phase of stance u Potential energy is transformed into kinetic energy during the falling phase u At toe-off, the axis of rotation is transferred from the ankle to the hip Potential energy (near Earth gravity) Ep (J) = mass (kg) x gravitational acc (m/s/s) x height (m) Kinetic energy (non-rotating mass) Ek (J) = ½ x mass (kg) x velocity (m/s)2 Swing phase of walking modeled as a conventional pendulum u The swing phase involves legs moving as conventional pendulums u Use of mechanical energy reduces the need for muscle activation u Potential energy at toe-off is converted to kinetic energy during the falling phase High P.E. of swing Low K.E. u The inverse occurs during the rising phase u Pendulum (leg) length accounts for the ”natural” frequency of human gait Low P.E. High K.E. Ground reaction force 1st half of loading response phase (Norkin & Levangie, 1992, p 476) 2nd half of loading response phase (Norkin & Levangie, 1992, p 476 1st part of terminal stance phase (Norkin & Levangie, 1992, p 477) 2nd part of Terminal stance phase (Norkin & Levangie, 1992, p 477) Ground reaction forces during walking Distributing ground reaction force u Pressure = Force/Area [N/m2] u Distributing force reduces the likelihood of injury u Centre of Pressure: “… the centre of the resultant forces.” (Richards et al., 2008, p 40) u Path of COP can reflect the efficiency of weight transfer and indicate potential for excessive tissue loading during gait Mechanical power during walking P(j) = M(j). w(j) (Watts) Positive joint power: concentric muscle action M(j) w(j) Energy (generation) >0 >0 Generation

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