New design aspects of a locomotory rehabilitation mechatronic system.
Seiciu, Petre Lucian ; Laurian, Tiberiu ; Filipoiu, Ioan Dan 等
1. INTRODUCTION
Walking is one of the most important features of humans. Walking
failure leads to serious problems in fulfilling the most common daily
activities such as stair climbing, sidewalk walking and street crossing
leading in time to total loss of the limb control. Therefore the
scientific study of the human movement is mandatory both for its
theoretical understanding and for medical purposes. The mechatronic
technology and virtual reality in rehabilitation proved to be promising
research directions. The modern rehabilitation methods were used only in
the last period at a small level, due to a lack of equipments. The use
of the gait trainers, as a new method appeared like an alternative to
the classical rehabilitation. The results are similar to the classical
methods. A consistent difference appeared with the use of the
mechatronic gait simulation systems. In this moment there are only a few
systems operating (in Germany, Switzerland and USA).
The designing and assembling of the state-of-art mechatronic system
(MS) presented in this paper lead the authors to the conclusion that a
more thorough scientific study of the walking is needed in order to
improve MS functioning (Filipoiu et al., 2007). The main goal is a new
design of the foot driving system (FDS), since this is the most complex
feature of the MS, mainly due to the foot complex movement.
2. WALKING--PEDALING ANALOGY
The most difficult task in the design of the FDS (figure 1) is to
replicate human walking as close to reality as possible.
That is why walking is studied intensely by scientists world-wide.
There are several theories that study walking (six determinants of
gait, inverted pendulum, dynamic walking etc.) but none of them is fully
applicable for design purposes.
Figure 2 presents a comparison of kinetic parameters from a
dynamical simulation with the experiments (Zajac et al., 2003). The
black lines (kinetic trajectories) are plotted from the simulation and
the grey lines (average kinetic trajectories) are plotted from
experimental subjects. VGF and HGF are the vertical and horizontal
ground reaction forces from subject measurements. AM and AP are the
ankle moment and power computed from inverse dynamics by using
subjects' measurements of ground reaction forces and kinematics.
The forces are normalized by body weight; moment and power by body
mass.
[FIGURE 1 OMITTED]
[FIGURE 2 OMITTED]
In pedalling, muscles have to produce energy over the crank cycle
and deliver the energy to the crank to overcome crank resistance and
inertia. Muscles deliver power to the crank by developing a tangential crank force. Power delivered to the crank is calculated by (Zajak et
al., 2002, 2003).
P = [omega] x T = [omega] x r x [F.sub.t] = [omega] x r x F x cos
[alpha] (1)
where co is the crank angular velocity, T is the crank torque, r is
the crank arm length, [F.sub.t] is the tangential crank force, F is the
normal force on the pedal and [alpha] is the instant angle. All the
terms are determined or measurable. The energy delivered to the crank
over the crank cycle (0 - 360[degrees], figure 3), which is the external
work done on the environment in a cycle, can be calculated by
integrating crank power over the cycle.
A comparison between simulated and experimental hip, knee and ankle
powers, during the crank cycle, is presented in figure 4 (Zajak et al.,
2002). Experimental data are plotted as grey lines and simulation data
as solid lines. Propulsive energy to the crank occurs during leg
extension (the area above 0 line, during 0 / 180[degrees] crank angle)
is positive.
If we consider the ankle diagrams in figure 3 and 4 we can observe
easily that the 2 lines are almost similar.
[FIGURE 3 OMITTED]
[FIGURE 4 OMITTED]
This can lead to the conclusion that the study of pedalling, under
some conditions is similar to the study of walking.
3. MECHANICAL WALKING ENERGY ASPECTS
Human walking is theoretically explained by two prevailing, but
contradictory theories. The first theory called "The Six
Determinants of Gait" (SDG) aims to minimize the energetic cost of
locomotion by reducing the vertical displacement of the body centre of
mass (COM). The second theory called "The Inverted Pendulum
Analogy" (IPA) suggests that walking is a movement combination of
two pendulums: the inverted pendulum for the stance leg and a direct
pendulum for the swing leg. Walking efficiency is considered for these
two theories in order to design properly the mechatronic system.
According to the SDG theory, the cost of transport depends on the
relative proportions of single and double support. The most economical
flat COM trajectory is achieved with single support dominating the step
and with an instantaneous double support phase. The dimensionless work
rate is (Kuo et al., 2007)
WR = [s.sup.2] x f/4 x [square root of 4 - [s.sup.2]] (2)
The IPA theory states that the dimensionless positive work rate is
(Kuo et al., 2007)
WR = 1/8 x [f.sup.2] x [s.sup.2] (3)
where s is the step length and f is step frequency, normalized by
the natural frequency of the leg.
The theoretical lower limit for the cost of transport (Collins et
al., 2005) in walking models is [c.sub.mt] = 0. This can be achieved by
swaying the upper body with springs in such a manner as to totally
eliminate the collision losses. Without swaying the upper body, a rough
lower bound on energetic cost can be estimated from the point-mass
small-angle model
[c.sub.et] [greater than or equal to] [c.sub.mt] [greater than or
equal to] J [(s - [s.sub.f]).sup.2] x [v.sup.2]/2 x g x d x [l.sup.2]
[approximately equal to] 0.0003 (4)
where J is the collision reduction factor, which is 1/4 for pushoff
before heel-strike, s [approximately equal to] 0.4 m is the step length
, [s.sub.f] [approximately equal to] 0.2 m is the foot length, l
[approximately equal to] 0.8 m is the leg length, v = 0.4 m/s is the
average velocity, and g [approximately equal to] 10 m/s2 is the gravity
constant.
Another dynamical model (Kuo et al., 2002) find out that [c.sub.et]
= 0.003. Other values of [c.sub.et] for real models (Collins et al.,
2005) are presented in table 1.
4. CONCLUSIONS
The most significant conclusion is that the analogy between walking
and seated pedalling is very useful for FDS design, due to the
simplicity of the pedalling model.
A total new conclusion is that the SDG theory applies best for the
new MS design, since it uses a flat COM trajectory.
The cost of transport can be estimated easily, but the results vary
largely from one application to another. We aim to reach low cost of
transport values with the above conclusions applied in the newly
designed MS.
All these conclusions will lead to a newly designed MS which will
simulate walking closer to reality and, hence, a better and more
efficient recovery of the persons with locomotory disabilities.
5. REFERENCES
Collins, S.; Ruina, A.; Tedrake, R. & Wisse M. (2005).
Efficient Bipedal Based on Passive-Dynamic Walkers, Science Magazine,
Vol. 307, no. 5712, February 2005 p. 1082-1805, ISSN: 0036-8075
Filipoiu, I. D.; Seiciu P. L.; Laurian, T. & Carutasu, N.
(2007). Mechatronic System for Neuro-Motor Disabled Persons: Computer
Simulation, Ann. DAAM proc. Int. DAAM Symposium, Katalinic, B. (Ed.),
pp. 281-282, ISBN 3901509-58-5, Zadar, Croatia, 24-27th. October 2007,
DAAAM International Vienna, Vienna
Filipoiu, I. D.; Seiciu P. L.; Laurian, T. & Carutasu, N.
(2007). SIMESIM--The Mechatronic System For Neuro-Motor Disabled
Persons, In.: DAAM International Scientific Book 2007, Katalinic, B.
(Ed.), pp. 387-398, DAAAM International Publishing, ISBN: 3-901509-60-7,
Vienna
Kuo, A. D. (2002). Energetics Of Actively Powered Locomotion Using
the Simplest Walking Model, Journal Of Biomechanical Engineering, ASME,
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Zajak, F. E.; Neptune, R. R. & Kautz, S. A. (2002).
Biomechanics and Muscle Coordination of Human Walking. Part I. Gait and
Posture, Vol.16, Issue 3, December 2002, pp. 215-232, Elsevier, ISSN:
0966-6362
Zajak, F. E.; Neptune, R. R. & Kautz, S. A. (2003).
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Table 1. Estimated cost of transportation for various robots.
Cornel biped Deft robot MIT learning
biped
0.2 5.3 10.5