First published online August 17, 2007
Journal of Experimental Biology 210, 2949-2960 (2007)
Published by The Company of Biologists 2007
doi: 10.1242/jeb.005801
Unsteady locomotion: integrating muscle function with whole body dynamics and neuromuscular control
Andrew A. Biewener1,*,
and
Monica A. Daley2,*
1 Concord Field Station, Department of Organismic and Evolutionary Biology,
Harvard University, Cambridge, MA 01238, USA
2 Department of Movement Science, Division of Kinesiology, University of
Michigan, Ann Arbor, MI 48109, USA

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Fig. 1. (A) Spring-mass model (or `spring-loaded inverted pendulum', SLIP) for the
dynamics of legged terrestrial locomotion. The body is represented by a point
mass m, located at the body center of mass (CoM; black circle), and
the leg by a linear compression spring with leg stiffness
kleg and contact angle o. (B) Despite
its simplicity, the spring-mass model accurately describes the fluctuations in
mechanical energy of the body during running (PEg,
gravitational potential energy; KEv and
KEh, vertical and horizontal kinetic energy, respectively;
Ecom, center of mass energy)
(Daley and Biewener, 2006 ;
Daley et al., 2006 ). (C)
Furthermore, all terrestrial animals appear to exhibit spring-mass dynamics,
whether they run on two, four, six or eight legs. Multiple legs act in concert
to produce the effective `leg-spring' dynamics
(Holmes et al., 2006 ). (D)
Similarly, a lateral spring-mass model describes well the medio-lateral
dynamics of cockroach locomotion, in which three legs operate as a single
effective `leg-spring' in the medio-lateral plane
(Full et al., 2002 ).
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Fig. 3. Proximo-distal differences in muscle architecture within the hindlimb of a
cursorial animal (similar patterns occur in the forelimb and in the limbs of
other running birds and mammals). Representative fascicle strain (red) and
myoelectric (EMG) patterns (black) recorded in vivo from muscles of
various animals are shown in relation to proximo-distal differences in
muscle–tendon architecture. For fascicle strain traces, the tick on the
scale bar indicates zero strain (the estimated resting length of the
fascicles, based on the average length during quiet standing). In
vivo forces (gray) are also shown for the two distal muscles. Fascicle
strain and time scales are the same for all muscle recordings shown. Duration
of stance phase is shaded gray.
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Fig. 4. (A) Schematic representation of regional patterns of joint work over the
course of stance summarizing patterns observed for muscle groups of various
animals during running. Curved arrows indicate the rotational motion of the
distal segment of each joint (clockwise versus counterclockwise).
Arrow color shows whether net energy is produced (red) or absorbed (blue) or
zero (gray) at that joint during stance. These joint patterns are shown in
relation to muscle work patterns in B and C. Muscle path arrows indicate
hypothesized contraction of muscle groups, undergoing net shortening and
positive work (red), lengthening and negative work (blue), or no net length
change (gray). In this example, the hip extends, doing positive work mainly
during the second half of stance (C); the knee flexes, doing negative work
(energy absorption) mainly during the first half of stance (B); the ankle
initially flexes during the first half of stance (B) and then extends during
the second half of stance (C), doing net positive work; and the TMP
(tarsometatarsal–phalangeal) joint dorsiflexes doing negative work
throughout stance, though shown in B only (overall limb work is zero,
characteristic of steady level locomotion assuming no work is done by other
pelvic and trunk muscles). In comparison, the hamstrings (biceps) shorten
while active, performing positive work (second half of stance, C); the
quadriceps (vastus) undergo net lengthening while active doing negative work
(first half of stance, B); the triceps surae [gastrocnemius (soleus, not
shown) and plantaris] contract isometrically doing zero net work throughout
stance, whereas the digital flexors are stretched and absorb energy initially
(B) and then remain isometric during the second half of stance (not shown). As
a result of their biarticular organization, the gastrocnemius, plantaris and
digital flexor act as force links and, although they do no significant net
work as a group, act to transfer energy from the hip and knee joints
(via the hamstrings and/or quadriceps) to the ankle joint. This
pattern is observed during steady level locomotion as well as during jumping
in several species. See text for additional details.
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Fig. 5. Distal-limb muscle performance during running on a slope in guinea fowl
(A,B) and turkeys (C). (A) Fascicle strain (via sonomicrometry), EMG
and muscle–tendon force in the lateral gastrocnemius (LG) of guinea fowl
during running on the level versus the incline. Although LG work
output increases by increased fascicle shortening and force development on an
incline, (B) total and mass-specific work performance of the LG (and digital
flexors) is less than if each hindlimb muscle contributed work in proportion
to its mass, and small compared to the whole-body work demand (see
Daley and Biewener, 2003 ). (C)
Patterns of fascicle strain, force and muscle work for the LG and peroneus
longus (PL) of turkeys running on the level, incline and decline show that
these muscles also modulate their mechanical work output largely by changes in
lengthening versus shortening strain [part C was originally published
in Gabaldón et al. (Gabaldón
et al., 2004 )]. In C, negative strain and velocity indicate
lengthening, filled circles are averages over stance, and open circles are
averages over the period of force production within stance.
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Fig. 7. Body CoM dynamics following perturbations in relation to spring-mass model
dynamics. (A) Computer simulation of the spring-mass trajectory following a
change from a soft to hard surface, with no change in leg stiffness
(kleg), resulting in an asymmetrical CoM path and a steep
trajectory during take-off at the end of support. (B) Actual CoM vertical
displacement of a human runner encountering an abrupt but expected change from
a soft to hard substrate. The runner maintains similar (symmetrical) CoM
motion by anticipating the change and adjusting kleg
within the first step (Ferris et al.,
1999 ). (C) Computer simulation of the spring-mass trajectory
following a sudden, unexpected drop in substrate height (40% of leg length).
In the perturbed step, the only model value that differs from the level step
is the limb contact angle ( o), which is steeper due to the
backward motion of the limb before it contacts the ground (see also
Fig. 8B). The angle used in the
simulation was that measured experimentally from guinea fowl. (D) Actual CoM
trajectory and energy changes of running guinea fowl following an unexpected
drop in substrate height equal to 40% of leg length (PEg,
solid blue line; KEv and KEh, solid
green and broken purple lines; Ecom, total center of mass
energy, solid black line). The broken vertical gray line indicates when the
foot contacted the tissue paper `false floor', and the gray box indicates the
duration of stance. The bar graph (right) shows the net energy changes during
the step (between the start and end of the traces on the left). Two response
modes were observed: in most cases the body dynamics of the bird match the
conservative spring-mass model (as shown in C), converting lost
PEg to forward KE (D, top graphs). In some cases,
however, the limb muscles absorb net energy, decreasing the total body
mechanical energy (Ecom; D, bottom graphs). The different
response modes are associated with different limb postures when the foot
contacts the ground (Daley and Biewener,
2006 ; Daley et al.,
2006 ).
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Fig. 8. Postural influences on intrinsic limb dynamics following a perturbation.
Intrinsic mechanical changes can simplify control and stabilization of running
dynamics, because these mechanisms rely on the natural dynamics of the body
and limb interacting with the environment, without the need for altered muscle
activation through central or reflex neural pathways. (A) Following an
unexpected change in substrate properties during hopping in place, humans
exhibit an intrinsic decrease in limb stiffness (kleg) due
to increased flexion of the knee in response to rapid limb loading
(Moritz and Farley, 2004 ). (B)
Upon encountering an unexpected drop in terrain height, guinea fowl exhibit an
intrinsic increase in limb contact angle ( o) due to the
normal backward motion of the limb during late swing phase just prior to
ground contact (to match foot and ground speed). If the limb acts as a simple
compression spring, limb loading (and ground reaction force) depends on the
angle between the limb and the bird's velocity ( o). The
backward motion of the limb in the drop step results in altered geometry as
shown, which is associated with an intrinsic decrease in the ground reaction
force impulse over stance (the time integral of force, Fg),
due to decreased peak force and shorter contact duration. These dynamics are
consistent with the spring-mass model
(Daley and Biewener,
2006 ).
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Fig. 9. The left panel schematically illustrates the hypothesized interplay between
feed-forward muscle activation and intrinsic mechanical effects during running
over a terrain drop (solid line) perturbation. Arrow color and direction
conventions are the same as in Fig.
4. (A) Activation of muscles in anticipation of stance results in
extension of the hip, ankle and TMP joints upon tissue paper (dotted line)
contact. Depending on the balance among multiarticular muscles at the knee
joint, the knee either flexes (A) or remains relatively extended (B). This
alters limb posture and limb loading at ground contact. When the knee is
flexed and o close to vertical (A), limb loading is low, and
the distal joints act as springs (purple and blue cumulative work curves for
the ankle and TMP joints absorb with low net work output). When the knee is
relatively extended and o is lower (B), limb loading is
greater, and the distal muscles undergo stretch, resulting in net energy
absorption (blue arrows for distal muscles, and negative cumulative work for
the ankle and TMP joints). In contrast the hip behaves uniformly, producing
energy, as if the hip extensors are under feed-forward control and insensitive
to perturbations. The knee does little net work under either condition. We
hypothesize that variation in the breaking force of the tissue paper results
in altered distal muscle contraction dynamics during the perturbation (on
left, greater and lower distal muscle work production in A and B,
respectively), leading to altered stance phase limb posture and dynamics
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© The Company of Biologists Ltd 2007