Mechanics and energetics of swinging the human leg
1 Department of Mechanical Engineering, University of Michigan, Ann Arbor,
MI 48109-2125 USA
2 Department of Physiology, University of Alberta, Edmonton, AB T6G 2H7
Canada
* Author for correspondence (e-mail: jdokeh{at}umich.edu)
Accepted 25 November 2004
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Summary |
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Key words: metabolic energy, locomotion, biomechanics, muscle, force production
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Introduction |
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The metabolic cost of active leg motion has previously been considered
mostly in running animals. Taylor et al.
(1980) argued that the cost of
running is dominated by the generation of force to support body weight for
short durations of ground contact (Kram
and Taylor, 1990
), rather than to move the legs
(Taylor, 1994
). But loading
the limbs of running humans (Myers and
Steudel, 1985
) or dogs
(Steudel, 1990
) causes
metabolic cost to increase more than for the same loads applied to the center
of mass, suggesting that moving the limbs does require energy. Marsh et al.
(2004
) used more direct
measurements of blood flow to estimate energy expenditure in the swing-phase
muscles of guinea fowl. They estimated that 26% of the energy used by the
limbs was for the swing phase.
The cost of driving the legs back and forth relative to the body may be
significant during human walking. Griffin et al.
(2003) proposed that little
energy is needed to move the legs during walking because human energy
expenditure increases in proportion to carried load. But again, expenditure
increases several times more when the limbs are loaded (e.g.
Soule and Goldman, 1969
) as
opposed to the trunk, therefore implying the opposite. Another argument for a
cost for moving the legs is derived from a mathematical model of walking
(Kuo, 2001
). We hypothesized
that mechanical work must be performed to redirect the center of mass from the
pendular arc dictated by the stance leg, especially in the transition from one
step to the next (Kuo, 2002
).
Metabolic energy is needed to perform this work (Donelan et al.,
2002a
,b
),
which itself could be minimized by taking short steps. But the actual
metabolic minimum for a given speed occurs at a longer step length, indicating
a separate cost for short but fast steps
(Kuo, 2001
). To account for
this trade-off, our model required a metabolic cost for walking at high step
frequencies increasing roughly with the fourth power of step frequency. The
force and work needed to move the legs relative to the body might explain this
proposed cost of high step frequencies. In particular, a cost for producing
force over short durations - applied to fast leg motions and called the
`force/time hypothesis' here - could potentially account for the trade-off
against high step frequencies. Regardless of the specific dependency on
magnitude or duration of work or force, our model predicted a substantial cost
for moving the legs relative to the body, associated with neither center of
mass redirection nor body weight support.
A simple approach for estimating this cost is to study leg swinging itself without walking. The loading conditions must necessarily differ between isolated leg swinging and actual walking, but the range of hip torques and leg angles can roughly be matched. The metabolic cost of leg swinging could potentially depend on the work produced by muscles, and possibly even the force/time cost predicted for walking. But regardless of the particular cause, both of these possibilities predict a sharply increasing metabolic cost for swinging at higher than the leg's natural frequency.
The purpose of the present study was to measure the mechanics and metabolic energetics of swinging the human leg by itself. We tested how much metabolic rate increases with frequency of swinging and considered possible contributions to the cost of moving the legs.
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Materials and methods |
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Model
A simple pendulum model (Fig.
1) illustrates the mechanics of moving the leg. Employing a small
angle approximation, and measuring the angular displacement from
vertical, the equations of motion are
![]() | (1) |
![]() | (2) |
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Active movement of the leg requires muscle force or torque, increasing with
the square of swing frequency. Combining
(1) and
(2), the torque is
![]() | (3) |
![]() | (4) |
The most obvious potential metabolic cost is for performing work on the
limb, increasing with the cube of swing frequency. The mean rate of work
performed on the pendulum is
![]() | (5) |
Each cycle of pendulum swing involves both positive and negative work, both
exacting a positive metabolic cost (Hill,
1938). Substituting Equations
(2) and
(3) into
(5), the mean rate of positive
work,
(+), for the pendulum
model is
![]() | (6) |
Another possible contributor to metabolic cost is the force/time cost
derived from our model of walking, increasing with the fourth power of swing
frequency. This exponent was required to explain the preferred step length
vs speed relationship. In our formulation of the force/time
hypothesis, when muscle force is produced in bursts, metabolic cost increases
with force but with an economy inversely proportional to burst duration time
(Kuo, 2001). The force in
question is proportional to hip torque amplitude, and the burst duration is
proportional to swing period
= 1/f. The proposed metabolic
cost, labeled `rate of force/time' or
, is
![]() | (7) |
Substituting Equations (2),
(3),
(4) into
(7) yields the model prediction
![]() | (8) |
The mechanics and metabolic energetics of isolated leg swinging can be measured experimentally. It is straightforward to compare leg-swinging mechanics against the pendulum model, but it is more difficult to differentiate between contributions to metabolic cost, because metabolic rate may depend not only on work and force but also other factors not considered. Rather than attempting to test for one potential cost against another, we tested for an increase in metabolic rate proportional to the larger (fourth power) component in a combined cost including both rate of work and rate of force/time.
Experimental procedure
We measured mechanical and metabolic costs of swinging the leg at different
frequencies in twelve young adults. All subjects (six males, six females; body
mass M=64.8±8.3 kg, leg length l=0.88±0.07 m,
mean ± S.D.) were healthy and exhibited no clinical gait
abnormalities. They gave their informed consent to participate in this study
prior to the experiment. Seven different swing frequencies, f,
ranging from approximately 0.5-1.1 Hz, were tested on each subject's left leg,
all with a peak-to-peak amplitude 2A of approximately 45°. The
trial order was randomized to reduce fatigue effects.
We constructed an apparatus for estimating work performed on the limb through measured leg displacement and reaction forces (see Fig. 2), effectively acting as an ergometer. This apparatus consisted of a metal frame, to support the upper body, mounted atop a force platform. Subjects stood inside the frame with one leg on a raised block so that the other leg could swing freely. Their upper bodies were strapped securely to the frame, with their weight distributed between one leg and two armrests. A lightweight knee splint was used to keep the swinging leg straight. An optical encoder, rotating about an axis through the hip and attached to the swinging leg, was used to measure the leg angle with respect to vertical. This angle was also displayed to the subject on a computer screen, along with visual targets showing 45° peak-to-peak amplitude. Subjects were asked to swing the leg between the targets, in time with a metronome set to twice the swing frequency, so that there was an audible cue for swinging of the leg in each direction. Subjects typically learned to follow the metronome after a few minutes' practice.
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Reaction forces were measured using a force platform (AMTI Biomechanics
Platform Model OR6-5; Watertown, MA, USA) underneath the ergometer frame. The
platform collected forces and moments simultaneously at a sampling rate of 120
Hz. Assuming that the swing leg alone was in motion, the ground reaction
forces were equal to the hip reaction forces. We used anthropometric
measurements and regression equations
(Yeadon and Morlock, 1989) to
determine the distance from the hip to the leg center of mass, r, as
well as the leg moment of inertia. These were used, with measured leg
kinematics, in inverse dynamics equations
(Kuo, 1998
) for a single rigid
leg to calculate the hip reaction torque, T.
We used the kinematic and reaction force data to calculate the torque and
work performed on the leg. The average rate of positive mechanical work
performed on the swing leg,
(+), was found by
integrating the half-wave rectified mechanical power (product of T
and
), and dividing by the entire data collection time for the
trial. An equal magnitude of negative mechanical work was also performed,
because there was zero net work performed on the leg. We also computed the
amplitude of the first fundamental component of the hip torque,
T0, after first applying a low-pass filter with a cut-off
frequency of twice the swing frequency. The force/time was calculated from
Equation (7).
We measured the metabolic cost of swinging the leg using an open circuit respirometry system (VMax29, SensorMedics Corp., Yorba Linda, CA, USA). Each trial was 6 min long, with the first three minutes used to allow oxygen consumption to reach steady state, followed by 3 min of data collection. The first trial for each subject was used to measure the resting metabolic rate with no leg motion, with the subject standing quietly on one leg while attached to the ergometer frame. This resting rate was used as a baseline that was subtracted from each subsequent data set to yield net metabolic rate. Trials 2-8 were leg swinging trials conducted in random order, with a short resting period given between each. Finally, we conducted a walking trial, in which the subject walked at 1.3 m s-1 on a motorized treadmill.
Net metabolic rate, , was computed from the average rate of
oxygen consumption, subtracting the rate for quiet standing. We assumed a rate
of 20.9 W for 1 ml s-1 O2. Although we did not measure
lactate concentration, we did monitor the respiratory exchange ratio (RER). In
all trials, RER was <0.9, indicating that the exercise was primarily
aerobic.
To account for differences in subjects' body size, we performed our
analysis using dimensionless variables, with M, g, and
l as base units. For example, energy rates
(+) and
were made dimensionless by the factor
A2Mg1.5l0.5,
and force/time
by
AMg1.5l0.5. For convenience of
data presentation, frequencies are presented in units of Hz, and energy rates
additionally in the more commonly used units of W kg-1, converted
back by an appropriate mean non-dimensionalizing factor.
We first tested the degree to which isolated leg swinging resembled forced
motion of a pendulum. We used regression tests to compare measured
T0, (+)
and
with the amounts
given by Equations (4),
(6) and
(8), respectively. In terms of
frequencies in Hz, the regressions were
![]() | (9) |
![]() | (10) |
![]() | (11) |
We next compared the measured net metabolic rate against
the force/time hypothesis using two regressions. The first was of the form
![]() | (12) |
![]() | (13) |
Because the force/time hypothesis only applies to fast swinging of the leg, these tests were performed only for frequencies above 0.7 Hz.
We also compared leg swinging with walking. In terms of mechanics, we
compared a typical subject's hip work loops at all swing frequencies against
published data for normal walking at 1.3 m s-1
(Whittle, 1996). Metabolic
rates were compared between leg swinging and walking at 1.3 m
s-1.
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Results |
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The rate of force/time
, increased with
fourth power of swing frequency (Fig.
3c), fitting well with Equation
(11),
R2=0.95. The dimensionless regression coefficients were
CF=1.52±0.07 (CI),
DF=0.001±0.002 (CI).
Examining the metabolic rate, we found it increased substantially with
swing frequency (Fig. 4a),
fitting well with the force/time hypothesis
(Equation 12),
R2=0.92. The data ranged from 0.41±0.26 W
kg-1 (S.D.) to 2.10±0.31 W kg-1. The
regression coefficients were CE=2.04±0.23 W
s-4 kg-1 (CI), with offset
DE=0.30±0.22 W kg-1 (S.D.).
The second regression demonstrated that increased
approximately linearly with
(Fig. 4b),
R2=0.85. The coefficients were
CEF=6.62±0.74 (CI), with offset
DEF=0.015±0.005 (S.D.).
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When walking at 1.3 m s-1, subjects chose a stride frequency of about 0.9 Hz and consumed metabolic energy at net rate 2.8±0.8 W kg-1. Work loops for a typical subject showed a range of hip torques and angles for comparison with walking (Fig. 5).
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Discussion |
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The observed increases in mechanical (Fig. 3) and metabolic (Fig. 4) measurements confirm that pendulum mechanics are relevant to the leg motion. Even though no net work is performed over an entire cycle, force and work are necessary within each cycle to move the leg faster than its natural frequency. The sharp increase in mechanical demands must be met by muscle, probably causing the fourfold increase in metabolic cost.
Mechanical work is probably responsible for much of the metabolic cost.
Some active work is almost certainly performed by muscle fibers, but not
necessarily as much as the measured work performed on the limb. Series
elasticity, in tendon and other structures, can also perform work on the limb
passively (Kuo, 2001), thus
lowering the proportion performed actively. In addition, the highest forces
occur at the extremes of leg motion when speed is lowest, so that muscle
fibers can be nearly isometric. The actual muscle fiber work during leg
swinging and its true contribution to metabolic cost are unknown here.
Metabolic cost may also increase with short durations of force production,
as indicated by the observed correlation to
, consistent with the
force/time hypothesis. Others have previously observed increases in metabolic
rate with short force durations in situations as disparate as supporting body
weight in running (Roberts et al.,
1998
) and propelling the body in cross-country skiing
(Bellizzi et al., 1998
),
although with varying formulations. The cost might be attributed to increasing
recruitment of less economic fast-twitch muscle fibers for short durations of
force production (Kram and Taylor,
1990
), but this explanation alone is probably insufficient to
explain the fourfold increase in cost seen here. Isolated muscle measurements
also demonstrate a substantial increase in energetic cost of producing force
for shorter durations, even when fiber type recruitment is relatively fixed
(Hogan et al., 1998
). A
possible explanation is the energetic cost of activation-deactivation
dynamics, in particular calcium pumping associated with the sarcoplasmic
reticulum (Bergstrom and Hultman,
1988
; Hogan et al.,
1998
; Verburg et al.,
2001
).
Our results suggest that metabolic rate depends on work and force/time, but cannot distinguish between their relative contributions. The fit to the larger fourth-power cost (Fig. 4a) means that the force/time hypothesis cannot be excluded. But neither can the contribution of rate of work be excluded. In the absence of a hypothesis for how these two costs might sum - most likely in a nonlinear fashion - it would not be fruitful to add another term for work. Such a term would only add a third degree of freedom to the fit of Equation (12) without explaining the many other factors that might affect metabolic cost. Further differentiation of costs might require experiments that manipulate force and duration as separate independent variables.
The conditions of isolated leg swinging were only roughly comparable to human walking in terms of hip torque and amplitude, but with a lower frequency. Our experiment sought to separate the problem of moving the legs relative to the body from that of loading and propelling the center of mass. But lacking the actual loads of walking, isolated leg swinging cannot simultaneously match both the forces and kinematics of walking. At f=1.08 Hz, the ranges of hip torques and angles are roughly similar to that of normal walking at 1.3 m s-1 (Fig. 5), but not to the stride frequency of about 0.9 Hz. Swing and stride frequency could alternatively be matched, f=0.9 Hz, but the torques would then be considerably lower than for walking. By using similar torque and amplitude but lower frequency, our conditions conservatively involved less work than that performed on the leg during walking.
We also used a splint to restrict greatly the knee motion that would normally occur in walking. If the knee were instead allowed to bend, the leg could theoretically be moved at higher frequency for the same hip torque. But as noted above, the same hip torque at a higher speed would not be expected to require less metabolic power, and if active torque were produced at the knee it might also exact a metabolic cost. Allowing knee motion could alternatively enable the same swing frequency at lower hip torque and, therefore, lower rate of work and lower metabolic cost. But our intent was to approximate the hip torques used in walking, and doing so with a knee splint is likely to produce an underestimate of the cost of moving the leg during walking because of the lower speed.
A more significant limitation of this experiment was that subjects exerted considerable effort to hold their bodies immobile during leg swinging, despite our efforts to strap their bodies to the rigid measurement apparatus. In walking, reciprocal leg motion allows reaction forces to be produced between the legs and against each other rather than an external frame. In terms of reaction forces, isolated swinging of a single leg might be roughly comparable to moving both legs during walking.
The most conservative walking comparison is, therefore, with the condition of isolated leg swinging at f=0.9 Hz, which would cost approximately 0.95 W kg-1, or about one-third of the rate for walking at the same stride frequency. It is conservative because it likely underestimates the hip torque and work needed to move both legs in walking, it does not include possible costs of moving the knee, and it assumes that the reaction forces for swinging a single leg are similar to those for moving both legs during walking.
In actual walking, it is difficult to experimentally isolate moving the
legs from supporting body weight or redirecting the center of mass. When a leg
is in contact with the ground, it is somewhat arbitrary to assign muscle
activity to one function or another. But there might be a significant
metabolic cost even if moving the legs were narrowed to the swing phase alone,
as evidenced by the findings of Marsh et al.
(2004). Swing-phase activity
of guinea fowl hip muscles accounted for about one-fourth of metabolic cost
even at slow speed of 0.5 m s-1. Assuming a hip height of 0.2 m and
a stride frequency of 1.5 Hz (Gatesy and
Biewener, 1991
), the one-fourth estimate applies to a slightly
slower dimensionless speed and stride frequency than humans (speed 0.36
vs 0.44, stride frequency 0.21 vs 0.27, guinea fowl
vs human, respectively). Legs of guinea fowl are also a slightly
lower proportion of body mass than in humans, approximately 10% vs
16% per leg (Fedak et al.,
1982
). A comparable cost for the human swing phase alone appears
reasonable, both in relation to these data, and to our one-third estimate for
moving the legs relative to the body including both swing and stance
phases.
We do not interpret the one-third cost estimate to conflict with Mochon and
McMahon's (1980) notion that
much of the swing phase is ballistic. These authors noted that muscle activity
occurs mostly at the start and end of swing, with the motion being largely
passive in between. For fast leg motions, the highest torques are needed only
at the extremes of motion, and there could be substantial intervals of time
that need minimal muscle activity (Kuo,
2002
). Even with a high metabolic cost, the swing phase appears to
be governed by pendulum dynamics.
We originally hypothesized a cost for moving the legs to explain why humans
do not walk with short steps to minimize the costs of transitioning between
inverted pendulum arcs (Kuo,
2001). Large increases in metabolic cost for leg swinging may be
sufficient to explain the increasing cost of walking with step frequency. The
approximate fourth power exponent of frequency is also consistent with the
optimum combination of step length and frequency preferred by humans. Low
economy of force production for short durations is a potential explanation for
this cause, but more detailed physiological studies would be necessary to test
this further.
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Acknowledgments |
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