First published online September 15, 2004
Journal of Experimental Biology 207, 3797-3810 (2004)
Published by The Company of Biologists 2004
doi: 10.1242/jeb.01214
Development of pendulum mechanism and kinematic coordination from the first unsupported steps in toddlers
Yuri P. Ivanenko1,
Nadia Dominici1,2,
Germana Cappellini1,
Bernard Dan3,
Guy Cheron3 and
Francesco Lacquaniti1,2,4,*
1 Department of Neuromotor Physiology, IRCCS Fondazione Santa Lucia, via
Ardeatina 306, 00179 Rome, Italy
2 Department of Neuroscience, University of Rome Tor Vergata, Via
Montpellier 1, 00133 Rome, Italy
3 ISEPK, Université Libre de Bruxelles, Brussels 1050,
Belgium
4 Centre of Space Bio-medicine, University of Rome Tor Vergata, Via Raimondo
8, 00173 Rome, Italy

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Fig. 1. Kinematic and kinetic recordings. (A) Experimental setup. Kinematic data
were measured by monitoring markers on the gleno-humeral joint (GH), ilium
(IL), greater trochanter (GT), lateral femur epicondyle (LE), lateral
malleolus (LM), and fifth metatarso-phalangeal joint (VM). Trunk, pelvis,
thigh, shank and foot are the limb segments identified by these markers.
Elevation angles were computed relative to the vertical. Ground reaction
forces were measured by force platforms along x,y,z axes. (B)
Sagittal stick diagrams and (C) force platform measurements at two stages of
early walking in the same child (subject G.M.): at 12.5 months (first
independent steps), and at 17 months.
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Fig. 2. Kinematics of the pendulum mechanism. (A) Schematic representation of the
inverted pendulum: the hip vaults over the stance limb. (B) Ensemble averages
(± S.D., N=5 steps) of vertical hip
displacement (GTy) and knee joint angle in children of different
age, and in a representative adult walking at two different speeds (right
panels). Data are plotted vs the normalised gait cycle. Each record
begins with the right foot strike. GTy is expressed in relative
units (normalised by the limb length L). (C) Percent of variance
(± S.D.) of GTy data explained by the
second Fourier harmonic is plotted as a function of the time after the onset
of independent walking. The values for the adult group were obtained by
computing the mean (± S.D.) from the pooled data
obtained for walking at natural, freely chosen speed (on average,
3.8±0.4 km h1). (D) Correlation coefficient between
GTy data in children and the corresponding ensemble average in
adults during stance. For both C and D, the time course of changes with age
was fitted by an exponential function (r=0.93 and 0.87 in C and D,
respectively). , the corresponding time constant.
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Fig. 3. Changes of vertical hip displacement
(GTy,left+GTy,right)/2 (C), gravitational potential
energy (Ep) (B) and kinetic energy
(Ek) (A,B) of COM during walking in children of different
age, and in a representative adult. The upper three traces show the forward
(Ek,f), vertical (Ek,v) and lateral
(Ek,l) kinetic energies of COM. Ek (B)
refers to the kinetic energy in the sagittal plane (sum of
Ek,f and Ek,v) that we used to
characterize the classic pendulum behaviour in the sagittal plane. Dotted
vertical lines correspond to foot contact (FC) of one leg. For older children
and adults, the recordings of Ek and
Ep do not extend to the whole cycle. Correlation
coefficient between Ep and Ek is
indicated for each trial.
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Fig. 4. Mechanical energy of COM. Mean changes (±
S.D.) of selected parameters plotted as a function of
the time after the onset of independent walking: correlation coefficient
between Ep and Ek (A), phase shift
between Ep and Ek (B), percentage of
recovery of mechanical energy (C), external work per unit of body mass and per
unit distance (Wext; D) and internal work per unit of body
mass and per unit distance (Wint; E). The time course of
changes with age was fitted by an exponential function (r=0.93, 0.89,
0.87 and 0.92 for A, C, D and E, respectively). Data refer to walking at
natural speed.
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Fig. 5. Normalisation by the Froude number. Percentage of recovery of mechanical
energy (A) and correlation coefficients between Ep and
Ek (B) for toddlers at the first unsupported steps (blue),
15 months later (cyan), children older than 2 years of age (violet) and
adults (red). Data points for individual steps are plotted as a function of
Froude number
(Fr=V2g1L1,
where V is the average speed of locomotion, g the
acceleration of gravity, and L the lower limb length). Continuous
lines represent second-order-polynomial fittings.
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Fig. 6. Inter-segmental coordination. (A) Ensemble averages (±
S.D., N=5 steps) of thigh, shank and foot
elevation angles in children of different age and in a representative adult.
(B) Corresponding gait loops plotted in 3-D. A loop represents one gait cycle
and is obtained by plotting the thigh waveform vs shank and foot
waveforms (after mean values subtraction). Paths progress in time in the
counter-clockwise direction, foot strike and lift-off corresponding
approximately to the top and bottom of the loop, respectively (swing phase is
in red). The interpolation planes result from orthogonal planar regression.
The first eigenvector (u1) is aligned with the long axis of
the gait loops of B, the second eigenvector (u2) is aligned
with the short axis, and the third eigenvector (u3) is the
normal to the plane. uit, uis and
uif correspond to the direction cosines with the positive
semi-axis of the thigh, shank and foot angular coordinates, respectively. (C)
Changes with age of percentage of variance accounted for by
u1, u2, and u3
(PV1, PV2, PV3 respectively). (D) Direction
cosines of the plane normal. (E) Step-by-step variability of the plane normal
(exponential fitting, r=0.91).
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Fig. 7. Behaviour before and after the onset of independent walking. Percent of
variance of GTy data explained by the second Fourier harmonic (A)
and step-by-step variability of the plane normal (B) are plotted for
experimental sessions performed at different times before and after the first
unsupported steps. Triangles, subject R.D.C. data; circles, subject G.M.
data.
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© The Company of Biologists Ltd 2004