First published online January 17, 2007
Journal of Experimental Biology 210, 383-394 (2007)
Published by The Company of Biologists 2007
doi: 10.1242/jeb.02668
Running stability is enhanced by a proximo-distal gradient in joint neuromechanical control
M. A. Daley*,
G. Felix and
A. A. Biewener
Concord Field Station, MCZ, Harvard University, 100 Old Causeway
Road, Bedford, MA 01730, USA

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Fig. 1. Still frames of a guinea fowl during an unexpected perturbation to
illustrate experimental set-up. The ground force data reported in this paper
were reported previously (Daley et al.,
2006 ), where they were used to calculate changes in mechanical
energy of the body center of mass (COM). Here, the experimental data were
analyzed further by adding limb kinematics and inverse dynamics to investigate
joint mechanics during the perturbation. A 0.6 m long force plate was placed
at the midpoint of an 8 m long runway and rested 8.5 cm below the runway
surface. White tissue paper pulled tightly across the gap created the
appearance of a uniform substrate. Kinematics and ground reaction forces were
measured through time (moving from frame A to frame B) for the perturbed step.
These data were used to (1) evaluate whole limb mechanics and (2) calculate
joint moments and work using inverse dynamics, as described in Materials and
methods.
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Fig. 2. Schematic illustration of variables used for calculation of external joint
moments and work using inverse dynamics. Joint angles for the hip, knee, ankle
and tarsometatarso-phalangeal (TMP) joints are shown in dotted blue. X marks
the force-plate center of pressure (COP); red arrow, the ground reaction force
vector (Fg). See Materials and methods for further
details.
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Fig. 4. (A) Limb angle relative to horizontal ( ) and (B) limb length as the
distance between hip and toe (L) over the course of the perturbed
step for all U trials from one individual (solid blue), with a typical C
(broken green) and V (dotted red) trial from the same individual. Thin broken
grey lines indicate the aerial phase. Thicker lines indicate the period of
ground contact. The dotted vertical line indicates the time of tissue paper
contact for U trials, and the time of ground contact for the C and V trials.
Data are shown for the period from aerial phase peak in COM height to the end
of the stance phase following the perturbation.
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Fig. 6. Joint mechanics during stance. Joint angles (left), external moments
(middle) and joint work loops (momentangle plots, right) over the
course of stance for the hip (A), knee (B), ankle (C) and TMP (D). A
representative U trial for each of the 3 response modes is shown (broken
colored lines) with a level running trial for comparison (C, solid black
line). Increasing joint angles indicate extension, and positive moments
indicate extensor moments. Arrows indicate the direction of work loops.
Counter-clockwise indicates energy production by the joint, clockwise
indicates energy absorption.
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Fig. 7. Net external mechanical work in relation to limb contact angle
( i) for (A) the hip and knee, (B) the ankle and TMP and (C)
the entire limb. Black symbols are individual U trials, grey symbols show the
mean ± s.e.m. for C trials (N=10).
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Fig. 8. Net work at each joint during C (level running), U (unexpected drop) and V
(visible drop) trials with U trials subdivided by response mode. Values are
mean ± s.e.m. (N=10, 7, 9, 3, 10, for the respective
categories).
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Fig. 9. Initial stance phase knee angle determines limb posture and the work
balance among the joints. The knee angle is the only joint angle that differs
significantly at the onset of ground contact among the U response modes. If
the knee is extended at contact (left silhouette) the limb has a lower initial
angle and longer initial length. This extended posture is associated with
larger decelerating forces, greater energy absorption by the ankle and TMP,
and net energy absorption by the limb. If the knee is flexed at contact (right
silhouette), the limb has a higher initial angle and shorter initial length.
This flexed posture is associated with lower decelerating forces, spring-like
function of the ankle and TMP, and net energy production by the limb. In cases
with an extremely flexed knee, the distal limb simply collapses without
supporting substantial weight (KEv mode, silhouette not shown).
Values are mean ± s.e.m. (N=10, 7, 9, 3, for the respective
categories).
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© The Company of Biologists Ltd 2007