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First published online January 31, 2006
Journal of Experimental Biology 209, 633-644 (2006)
Published by The Company of Biologists 2006
doi: 10.1242/jeb.02061
Effects of limb mass distribution on mechanical power outputs during quadrupedalism
Department of Anthropology, Harvard University, 11 Divinity Avenue, Cambridge, MA 02138, USA
e-mail: raichlen{at}fas.harvard.edu
Accepted 22 December 2005
| Summary |
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Key words: biomechanics, primate, locomotion, inertial properties, baboon, Papio cynocephalus
| Introduction |
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Experimental studies have generally confirmed that higher costs are
associated with distal limb loading (Myers
and Steudel, 1985
; Steudel,
1990
). However, in the only comparative experimental study of the
energetic cost of naturally occurring distal limb mass, Taylor et al.
(1974
) showed that three
mammals who differed greatly in their limb mass distributions (cheetah,
gazelle and goat) did not differ significantly in their energetic costs of
locomotion at a given velocity. Quadrupedal primates offer another example
that confounds predicted higher costs due to heavy distal limb elements
(Taylor et al., 1982
;
Heglund, 1985
;
Steudel-Numbers, 2003
).
Primates have distally heavy limb muscles that control grasping hands and
feet, yet their energetic costs do not differ from those of similarly sized
mammals (Taylor et al., 1982
;
Heglund, 1985
;
Steudel-Numbers, 2003
).
Although the results of Taylor et al.
(1974
) have been called into
question because of methodological concerns (see
Lieberman et al., 2003
), their
study, combined with the primate data, suggests that limb mass distributions
do not necessarily determine energy costs.
The purpose of the present study is to explore mechanisms used by
quadrupeds with distally heavy limbs that allow them to maintain similar
energy costs compared with mammals with more proximal limb mass
concentrations. Without a mechanism, the evolution of distally heavy limbs
could have come with a great energetic price. Any mechanism must begin by
reducing the impacts of limb mass distribution on internal power. The total
power output during quadrupedalism is, however, generally divided into two
parts: external power is the power required to lift and accelerate the body
center of mass, and internal power is the power required to move the limbs
relative to the body center of mass
(Heglund et al., 1982b
;
Minetti et al., 1999
). Taxa
with distally heavy limbs must find a way to minimize the impacts of their
limb mass on internal power and therefore maintain similar total power outputs
compared to mammals with more proximally concentrated limb mass.
Adjustments in kinematics may represent a mechanism that could mitigate the
added energy costs of distally heavy limbs, since locomotor kinematics can
have a strong impact on power outputs during locomotion
(Hildebrand and Hurley, 1985
;
Cavagna and Franzetti, 1986
;
Cavagna et al., 1991
;
Minetti et al., 1995
;
Schepens et al., 2001
;
Heglund and Schepens, 2003
;
Schepens et al., 2004
). For
example, several researchers have shown that a change in stride frequency at a
given velocity has divergent effects on internal and external power
(Cavagna and Franzetti, 1986
;
Cavagna et al., 1991
;
Minetti et al., 1995
).
Relatively low stride frequencies reduce the velocity at which muscles and
tendons must move a limb, thereby reducing internal power
(Cavagna and Franzetti, 1986
;
Cavagna et al., 1991
;
Minetti et al., 1995
;
Schepens et al., 2001
;
Heglund and Schepens, 2003
;
Schepens et al., 2004
).
Relatively low stride frequencies are associated with relatively long strides
(since velocity is the product of stride frequency and stride length), and
long strides increase external power due to larger vertical displacements of
the body center of mass (Cavagna and
Franzetti, 1986
; Cavagna et
al., 1991
; Minetti et al.,
1995
; Schepens et al.,
2001
; Heglund and Schepens,
2003
; Schepens et al.,
2004
). Interestingly, although humans walk and run with stride
frequencies that nearly minimize total power, they deviate slightly from
optimum stride frequencies (Cavagna and
Franzetti, 1986
; Cavagna et
al., 1991
; Minetti et al.,
1995
).
Although freely chosen stride frequencies do not completely minimize total
power, metabolic energy expenditure is minimized at freely chosen stride
frequencies (Zarrugh and Radcliffe,
1978
). There may be other constraints on stride frequency that
allow individuals to minimize energy expenditure despite slightly higher power
outputs. Humans' freely chosen stride frequencies closely match those
predicted by the Force Driven Harmonic Oscillator model (FDHO) described by
Holt et al. (1990
). The FDHO
models the lower limb as a harmonic oscillator whose period is dependent on
limb inertial properties, but the limb also requires a periodic driving
function (muscle activity) to maintain its oscillation amplitude
(Holt et al., 1990
;
Holt et al., 1991
). Freely
chosen combinations of stride frequencies and lengths are well predicted by
the FDHO, suggesting an optimal combination of kinematics that is related to
limb mass distribution. Any deviations from the freely chosen frequency,
either above or below, result in increased energy expenditure due to increased
muscle activity (Holt et al.,
1991
). It is likely then, that stride frequencies are constrained
by limb inertial properties so that a frequency is chosen to minimize the
driving function (Holt et al.,
1991
).
This same tuning of kinematics to inertial properties may apply to
quadrupeds as well. Stride lengths and stride frequencies appear to vary in a
predictable way with differences in limb mass distribution
(Raichlen, 2004
;
Raichlen, 2005a
). Taxa with
distally heavier limbs tend to walk with lower stride frequencies and longer
strides (Preuschoft and Günther,
1994
; Myers and Steudel,
1997
; Raichlen,
2004
; Raichlen,
2005a
), and this trend appears valid both across mammalian taxa
(Preuschoft and Günther,
1994
; Myers and Steudel,
1997
) and within ontogenetic samples where limb mass distributions
change with age (Raichlen,
2005a
). Additionally, lower stride frequencies are brought about
by a combination of longer swing durations and longer stance
durations. Thus, quadrupeds with distally heavy limbs could take advantage of
the trade-offs between kinematics and power outputs simply by virtue of the
fact that their stride frequencies are tuned to their limb inertial properties
following the FDHO model. As a by-product of this tuning, kinematics may
mitigate the energetic consequences of distally heavy limbs. If true then,
compared with more cursorial taxa, quadrupeds with distally heavy limbs using
lower stride frequencies would reduce internal power outputs (due to slower
limb velocities during both swing and stance phase), while their longer
strides would increase external power outputs so that total power outputs
would not differ among individuals regardless of limb mass distribution.
Hypothesis testing
This study tests the hypothesis that quadrupedal kinematics associated with
distally heavy limbs allows individuals to benefit from the trade-off
mechanism described above and, therefore, they can maintain similar total
power outputs compared with quadrupeds with distally lighter limbs. Two
samples are used to test this hypothesis. First, a sample of infant baboons
(Papio cynocephalus) was examined during development. Primate
ontogeny offers a natural experiment because infant primate limb mass
distributions change with age (Grand,
1977
; Turnquist and Wells,
1994
; Raichlen,
2005b
). At young ages, infant primates have distally heavy limb
muscles, used for strong grasping of their mothers fur, and limb mass becomes
more proximally concentrated with age
(Turnquist and Wells, 1994
;
Raichlen, 2005b
). As they age,
and mass becomes more proximally concentrated, the infant baboons use
relatively higher stride frequencies and shorter strides
(Raichlen, 2005a
). Therefore,
power outputs can be examined in this sample as both limb mass distributions
and kinematics change. In the second test of the trade-off mechanism, infant
baboons are compared with a sample of non-primate cursorial quadrupeds who
have more proximal limb mass concentrations. This sample of infant baboons
uses lower stride frequencies and longer strides than other mammals
(Raichlen, 2005a
) and
therefore may use these kinematic differences to maintain similar total power
outputs compared with other mammals.
Hypothesis 1. Infant baboons with distally heavy limbs (younger individuals) should have lower internal and higher external power compared with older individuals because of their lower stride frequencies and longer strides. However, age-related differences in internal and external power should lead to similar total power at all ages.
Hypothesis 2. Because of their more distally heavy limbs compared
with non-primates, the infant baboons use lower stride frequencies and longer
strides than more cursorial non-primates
(Raichlen, 2005a
). Due to
these kinematic differences, internal power should be lower, external power
should be higher, and total power should not differ significantly between the
baboons and the non-primates.
| Materials and methods |
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Inertial properties
Body segment inertial properties of the infant baboons were calculated
using a geometric modeling technique
(Raichlen, 2004
;
Raichlen, 2005b
). Briefly,
each body segment was modeled as a column with a circular cross section. Model
shapes were constructed using external circumference measurements taken at
three locations on each limb segment. From these measurements, column models
were constructed, and segment inertial properties (mass, center of mass, mass
moments of inertia) were calculated
(Raichlen, 2004
;
Raichlen, 2005b
). The natural
pendular period (NPP) of the limbs was also calculated. The
NPP is the duration of one complete oscillation of the limb if it was
swinging as a pure pendulum and is calculated according to the following
equation:
![]() | (1) |
where I is the limb's mass moment of inertia about the proximal
joint (the shoulder in the forelimb or the hip in the hindlimb), M is
the limb's mass, g is acceleration due to gravitational forces
(9.8 m s-2) and D is the distance of the center of mass
from the proximal joint. The NPP represents an important link between
limb mass distribution and kinematics because swing phase is often modeled as
an approximation of a pendulum (see Mochon
and McMahon, 1980
; Mochon and
McMahon, 1981
; Holt et al.,
1990
; Holt et al.,
1991
). Larger NPPs due to more distal limb mass imply
longer swing durations and therefore longer stride durations. Raichlen
(2005a
) has also shown that
relatively large NPPs lead to relatively long stance durations. The
use of NPP in this study is not meant to imply that swing phase is
purely passive, with no muscular action involved (see
Marsh et al., 2004
;
Modica and Kram, 2005
), but
that limb motion during swing phase is tuned to the NPP (see
Holt et al., 1990
;
Holt et al., 1991
).
NPPs were made dimensionless (dNPP) (according to
Hof, 1996
) to compare values
among individuals who differed in body size and therefore limb length
(h):
![]() | (2) |
Grouping
Individuals were grouped based on their limb inertial properties, and these
groupings did not conform to arbitrary age classes. Specifically, changes in
dNPP were used to group infants according to limb mass distributions.
Researchers have shown that limb NPPs change during swing phase due
to flexion and extension of limb joints and that this change should be taken
into account when comparing the effects of inertial properties on locomotion
(Myers and Steudel, 1997
;
Raichlen, 2004
;
Raichlen, 2005a
). When
swing-phase inertial properties are compared [by calculating the minimum
dNPP during swing phase (dNPPmin)], the infant
baboons do not show a gradual change with age
(Raichlen, 2005a
). In fact,
each individual falls into two groups: Group 1 comprises the young infants
with distally heavy limbs and dNPPmins that do not differ
significantly, and Group 2 comprises older infants who have more proximal
concentrations of limb mass and dNPPmins that do not
differ significantly (Raichlen,
2005a
). Between the two groups, dNPPmins do
differ significantly (Raichlen,
2005a
). These groupings proved robust in an examination of the
effects of inertial properties on kinematics, with Group 1 infant baboons
(more distal limb mass) using relatively lower stride frequencies and longer
strides than Group 2 infants (Raichlen,
2005a
).
Mechanical power
Three-dimensional kinematic data were obtained from each infant baboon at
regular intervals during development (Table
1). Infant baboons were allowed to walk and run at freely chosen
velocities through a Lexan tunnel made up of three removable sections
(0.61x0.91x1.22 m each). Prior to tunnel entry, spherical
reflective markers (14 mm; Oxford Metrics Inc., Oxford, UK) were glued to the
major joints of the forelimbs and hindlimbs of each infant baboon (hip, knee,
ankle, shoulder, elbow, knee). The placement of each marker was consistent
with the segment definitions used for inertial property data collection (see
Raichlen, 2005b
).
Three-dimensional marker trajectories were captured for one side of the body during each locomotor trial using a five-camera 60 Hz Vicon 250 data acquisition system (Oxford Metrics Inc.). In addition to the Vicon system, video data of each trial were collected using a digital video camera (JVC-GRDVL9800E; Wayne, NJ, USA) at 60 frames s-1. Video data were used to determine touchdown and toe-off events.
The total positive work that must be supplied by muscles and tendons during
locomotion (Wtot) can be divided into two parts
(Fenn, 1930
). The first part
is the mechanical work required to move body segments relative to the
whole-body center of mass (internal work; Wint).
Wint is calculated from changes in each segment's energy
over an entire stride (after Fedak et al.,
1982
; Willems et al.,
1995
). The second part of Wtot is external
work (Wext); the work that must be supplied to lift and
accelerate the whole body center of mass
(Cavagna et al., 1977
). Power
(
int and
ext) is simply the rate at
which internal or external work is done. Alternative approaches to calculating
ext will be discussed in a
later section.
The kinetic energy of each body segment relative to the body center of mass
was calculated from the 3-D marker positions captured by the Vicon motion
analysis system. For each stride, one side of the body (side facing cameras or
ipsilateral side) was divided into five segments (trunk, arm, forearm, thigh,
leg) that were defined by passive reflective markers at each of the major
joints. Affixing markers to define the hand and foot segments was problematic
both because of the small size of the individuals' hands and feet and because
the infant baboons were more likely to remove those markers. For this
analysis, the hands and feet were considered point masses at the distal ends
of the forearms and lower legs, respectively, and the head was considered a
point mass at the cranial end of the trunk. The positions and velocities for
segments on the contralateral side of the body were estimated assuming the
movements of the contralateral side segments during half a stride were the
same as the movements of the ipsilateral segments during the other half of the
stride (see Fedak et al.,
1982
; Willems et al.,
1995
).
Mass-specific Wint was calculated as the sum of the
positive changes in each limb's kinetic energy per stride divided by body mass
(after Willems et al., 1995
).
Dividing mass-specific Wint by stride duration gives
int. This method of
calculating internal work allows for transfers of energy between segments of a
single limb but not between limbs. To calculate Wext,
potential and kinetic energies (both horizontal and vertical) of the body
center of mass were summed at each instant in time to obtain the total energy
of the center of mass (Ecm). Center of mass position and
velocity were reconstructed based on the positions of limb segment centers of
mass (after Minetti et al.,
1999
). Mass-specific external mechanical work
(Wext) was calculated as the sum of the positive
increments in the Ecm curve over an entire stride divided
by body mass. Mass-specific external power
(
ext) was calculated as
(Wext/stride duration).
Manipulation of internal power calculations
A manipulation of inertial properties was performed to examine the
sensitivity of
int to an
individual's limb mass distribution. This manipulation consisted of scaling
the segment inertial properties of all subjects with distally light limbs to
the inertial properties of the individual with the heaviest distal limb
elements.
int was
recalculated using these scaled values for limb segment inertial properties.
The following equations were used to scale segment inertial properties of
older individuals (individual 2) to those of the subject with the heaviest
distal limb elements (individual 1):
![]() | (3) |
![]() | (4) |
![]() | (5) |
where B1 and B2 are the body masses of individuals 1 and 2, respectively, M1 and M2 are the segment masses of individuals 1 and 2, respectively, h1 and h2 are the segment lengths of individuals 1 and 2, D1 is the segment center of mass position from the proximal end of the segment for individual 1, and I1 is the segment mass moment of inertia about its center of mass for individual 1.
Data analysis
Comparisons in power outputs between Group 1 and Group 2 infant baboons
were performed in two ways. First, analyses of covariance (ANCOVAs) were used
to compare variables between groups, with velocity as the covariate since
power outputs are correlated with velocity in infant baboons. Since Group 1
and Group 2 individuals differ in size, ANCOVAs were also performed with
dimensionless velocity [velocity/(gh)0.5] as the
covariate. Significant differences were determined using Tukey-Kramer
post-hoc tests to account for multiple comparisons. In addition to
ANCOVAs, a residuals analysis was performed. Specifically, residuals were
calculated from the least-squares regression line relating dimensionless
stride frequency [stride
frequency/(g/h)0.5] and dimensionless
velocity as well as mass-specific internal power and dimensionless velocity.
Residual internal power outputs were then regressed on residual stride
frequencies. These residuals were calculated from the entire sample (Group 1
and Group 2 combined). A significant positive correlation indicates that those
individuals who use high stride frequencies relative to velocity also have
high internal power outputs. A similar analysis was performed for external
power. Residuals of external power and dimensionless velocity were regressed
on residuals of dimensionless stride length (stride length/h) and
dimensionless velocity. A significant positive correlation indicates that
those individuals using relatively long strides would also have relatively
high external power outputs. All analyses were performed on log-transformed
data since the relationship between power outputs and velocity is not
linear.
| Results |
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Hypothesis 1: ontogenetic analysis
int does not show
significant between-group differences when analyzed using velocity as the
covariate but is significantly lower in Group 1 individuals compared with
Group 2 over the dimensionless velocity range
(Fig. 1A,B;
Table 2).
int was recalculated for
each stride of all Group 2 individuals using scaled segment inertial
properties (see Materials and methods). If older individuals had the limb mass
distributions of younger individuals, but did not reduce their stride
frequencies, they would have had approximately 20% higher
int values at a given
velocity (Fig. 1C). So, by
using low stride frequencies when their mass is most distal, the infant
baboons save approximately 20% of the mechanical power they would otherwise
have had to output to move their limbs relative to their body.
|
ext over the velocity
range, but do not show significant between group differences in
ext at a given
dimensionless velocity (Fig.
1D,E; Table 2).
Finally,
tot is larger in
Group 2 individuals at a given velocity but does not show significant
between-group differences in the combined sample of infant baboons over the
dimensionless velocity range (Fig.
1F,G;Table 2).
Between-group differences in body size must be taken into account because the
same velocity has different impacts on individuals with different limb lengths
(Alexander and Jayes, 1983
int,
ext and
tot do not support a
trade-off mechanism when examined over the range of dimensionless velocities
because
ext did not differ
between groups, they do support the hypothesis that differences in kinematics
between individuals who differ in limb mass distributions will be associated
with similar total power outputs.
Individual baboon between-group comparisons generally follow the trends of
the combined sample analysis, although the differences are not always
significant (Table 3). Only
Infant 1 shows significantly lower Group 1 values of
int. Although least-squares
mean
int is lower in Group
1 for the other two individuals, these differences were not significant. For
all other variables, the individuals follow the combined-sample results.
|
Because ANCOVA results may have been compromised by only slight differences
in kinematics and power outputs, a residuals analysis was performed. Residuals
of dimensionless stride frequency and dimensionless velocity were regressed
against residuals of
int
and dimensionless velocity (Fig.
2A). A significant positive correlation (r=0.48;
P<0.001) indicates that those individuals who have relatively low
dimensionless stride frequencies at a given dimensionless velocity have
relatively low
int at a
given dimensionless velocity. Note also that groups cluster together, with
Group 1 clustering in negative residual space (both negative dimensionless
stride frequency residuals and negative
int residuals). The same
analysis of residual stride lengths and
ext also shows a slight,
but significant, positive correlation between regressed residuals
(Fig. 2B; r=0.21;
P<0.001). This relationship is, however, quite weak, suggesting
that
ext may not be
sensitive to slight differences in stride length. Infant baboons show the same
patterns when examined individually (Table
4). The residuals for
int and stride frequency
are more highly correlated than those of
ext and stride length,
although all correlations are significant.
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Hypothesis 2: comparisons with other quadrupeds
To assess the likelihood that larger differences in inertial properties and
kinematics lead to power output trade-offs, the infant baboons (combined Group
1 and Group 2) were compared with more cursorial non-primate quadrupeds. In
the following comparative analyses, dogs and horses are used because data for
inertial properties, kinematics and power outputs in these species are readily
available in the literature.
Inertial properties for dogs were taken from Myers and Steudel
(1997
) and for horses from
Buchner et al. (1997
). Stride
frequencies and stride lengths were calculated from equations in Minetti et
al. (1999
) for horses and from
Williams et al. (2002
) for
dogs. Power outputs for dogs were taken from Heglund et al.
(1982b
) and
Fedak et al. 1982
), and power
for horses was taken from Minetti et al.
(1999
). ANCOVAs cannot be used
to compare non-primate kinematics and power outputs with those of the infant
baboons because only least-squares regression equations relating kinematics
and power to velocity in dogs and horses have been reported. Therefore, the
95% confidence intervals of the regression lines for the infant baboon sample
were calculated and differences are suggested when the regression line for the
non-primate data set fell outside of this interval. The limb length used to
calculate dimensionless velocity for dogs was given in Williams et al.
(2002
) for kinematics and
Fedak et al. (1982
) for power.
For the horse data set, limb length was estimated from allometric equations in
Alexander et al. (1979
) for
mean horse body mass in Minetti et al.
(1999
) (limb length = 1.26
m).
Infant baboons have more distal forelimb and hindlimb centers of mass
compared with dogs and horses (Table
5). Following the predicted relationships between inertial
properties and kinematics, infant baboons use lower stride frequencies and
longer strides at a given dimensionless velocity than either dogs or horses
(Fig. 3A,B). The infant baboon
sample has lower
int
(Fig. 3C) and higher
ext compared with the
non-primates (Fig. 3D). The
lower
int and higher
ext in the infant baboons
lead to similar
tot in the
infant baboon sample compared with the non-primate sample
(Fig. 3E). These data are
consistent with the presence of a trade-off mechanism where low stride
frequencies are associated with relatively low internal power, long strides
are associated with high external power, and total power does not differ
significantly among the sampled taxa.
|
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| Discussion |
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int and
ext. Although relatively
low stride frequencies are associated with low
int, the relationship
between stride length and
ext appears to be less
clear.
The comparison of mechanical power in infant baboons with dogs and horses
is, however, consistent with the presence of a mechanical power trade-off
mechanism. The infant baboons have more distally heavy limbs and use longer
strides and lower stride frequencies compared with dogs and horses. The infant
baboons do less
int and
more
ext compared with the
dog and horse samples, and their values of
tot do not differ
significantly from those of the non-primate sample. It is possible that the
trade-off mechanism is only apparent when stride frequencies and stride
lengths differ greatly between taxa.
There are several possible reasons for the absence of trade-offs in the
ontogenetic sample despite the presence of a trade-off mechanism in the
inter-specific sample. First, the differences in inertial properties between
infant groups were smaller than inter-specific differences. Perhaps slight
differences in spatio-temporal kinematics simply equalize energy outputs,
rather than having the trade-off effects. This possibility seems likely given
the results of the manipulation of internal power calculations (see
Fig. 1C). If young infants,
with their relatively distally heavy limbs, used the kinematics of older aged
infants,
int would be
approximately 20% higher.
Second, it is possible that the kinematic method of calculating center of
mass displacement is not sensitive enough to make comparisons within small
differences in stride length. Future examinations of the trade-off mechanism
could use force-plate data to calculate center of mass displacements, although
Gard et al. (2004
) suggest
that differences between the two techniques are minimal.
Finally, it is possible that
ext, as calculated here,
does not fully account for the power output to produce center of mass motion.
Recently, Donelan et al.
(2002
) suggested that much of
the work required to produce center of mass motion actually occurs as the
center of mass is redirected at the end of the stance phase during walking
(e.g. collisional costs; see also Bastien
et al., 2003
for alternative method of calculating this cost).
This work done during the double-contact phase of walking may represent a
substantial portion of
ext
and should scale with step length4
(Donelan et al., 2002
). If
true, then
ext as measured
here does not fully account for the effects of longer strides on the power
required to lift and accelerate the center if mass.
Infant baboons do show between-group differences in dimensionless step
length (ANOVA results: Group 1 mean=0.94, Group 2 mean=0.88,
P<0.001, F=3.86), which should lead to higher
step-to-step costs in Group 1 infants. In fact, Group 1 step lengths raised to
the fourth power (mean=0.78) are 23% higher than those of Group 2 (mean=0.59).
This value is quite similar to the between-group difference in least-squares
means for
int (22%; see
Table 2). Although differences
in center of mass height changes associated with longer strides may not be
large enough to impact ontogenetic changes in
ext as calculated in this
study, ontogenetic differences in step-to-step costs may in fact provide the
trade-off.
Although the results presented above suggest a trade-off in mechanical
costs, the relationship between mechanical and metabolic costs remains
unclear. In a classic paper, Heglund et al. showed a disconnection between
mechanical power and metabolic costs of locomotion in a wide range of taxa
(Heglund et al., 1982a
). This
disconnection is due to the fact that muscles consume energy not only when
they do work but also when they produce force isometrically
(Kram and Taylor, 1990
).
Despite the large impact of isometric force production on metabolic costs of
locomotion, increases in mechanical power at a given speed (driven by changes
in stride frequency/length at a given speed) cause an increase in metabolic
cost (Minetti et al., 1995
).
Thus, minimizing total power should reduce the metabolic costs of locomotion
at a given speed. Minetti et al.
(1999
) suggest that a complete
description of metabolic costs should therefore include a combination of
mechanical work and power plus the costs associated with isometric muscle
force production.
Implications for mammalian limb design
These results may explain why mammals in general do not differ greatly in
energy costs despite differences in limb mass distributions. Taylor et al.
(1974
) showed that the
cheetah, the gazelle and the goat do not differ in their energetic costs
despite having different limb mass distributions. Domestic cats use relatively
longer strides than other mammalian cursors (see
fig. 3 in
Alexander and Jayes, 1983
), and
these long strides may be linked to their distally heavy limbs. If cheetahs
use similar kinematics, then low stride frequencies and long strides may
explain their similar energetic costs compared with the goat and gazelle.
Cheetahs' low stride frequencies and long strides would reduce their internal
power outputs while increasing their external power outputs, allowing them to
maintain similar total power outputs compared with other mammals.
It is possible that all mammals follow a similar trade-off pattern that is
dependent on their limb mass distributions. Alexander and Jayes
(1983
) showed that
non-cursorial mammals use longer strides at a given dimensionless velocity
compared with more cursorial mammals. Since non-cursors also have more distal
limb mass concentrations than cursors
(Grand, 1977
;
Myers and Steudel, 1997
;
Raichlen, 2004
), non-cursors
may be taking advantage of the trade-off mechanism to reduce total mechanical
power.
The trade-off mechanism may have played an important role in allowing
mammalian quadrupeds to evolve non-locomotor functions in their distal limb
elements that would increase distal mass, without having a negative impact on
their energy costs of locomotion. This type of mechanism would have been
especially important for animals such as primates, who rely on their distally
heavy limb muscles to control their grasping hands and feet. Grasping hands
and feet are a hallmark of the primate order and were an essential element of
the success of early primates (Cartmill,
1972
). The use of the trade-off mechanism would have allowed early
primates to evolve grasping hands and feet without exacting an energetic
price.
Why concentrate limb mass proximally?
Although the results from this study suggest that mechanisms exist that
reduce the impact of limb mass distributions on mechanical power outputs, the
question of why cursorial mammals concentrate limb mass proximally remains
unanswered. Based on the available evidence from studies of energy costs of
transport in mammals, proximally concentrated limb mass does not lead to
greatly reduced energy expenditures
(Taylor et al., 1974
;
Taylor et al., 1982
;
Heglund, 1985
). Other adaptive
scenarios must therefore be examined.
Reducing distal limb mass leads to a reduction in the limb's mass moment of
inertia (e.g. the limb's resistance to rotational acceleration). Limb mass
moments of inertia affect limb acceleration relative to the body and therefore
affect whole-body accelerations (Ropret et
al., 1998
; Pasi and Carrier,
2003
; Rahmani et al., 2003). Although it seems clear that the
ability to sprint at high speeds is determined mainly by the ability to
produce greater ground reaction forces
(Weyand et al., 2000
), studies
of lower limb loading show significant reductions in limb velocity and
consequently reductions in maximum sprint velocity with added distal loads
(Ropret et al., 1998
).
Accelerations are necessary to either catch prey or evade predators
(Elliott et al., 1977
), and
thus structures that enhance an individual's ability to accelerate should be
subjected to large selection pressures. Since the ability to rapidly
accelerate is a strong predictor of successful predator evasion in many taxa
(Elliott et al., 1977
), the
evolution of proximal limb mass may be the result of selection for
acceleration capabilities. Although the results from the present study
certainly cannot address why cursorial quadrupeds concentrate limb mass
proximally, the context of predator-prey interactions may provide selection
pressures for the evolution of proximally concentrated limb mass.
Summary
Infant baboons show some ontogenetic evidence of a trade-off mechanism,
although the relationship between external power and stride length appears to
be weak. Compared with dogs and horses, the infant baboon sample has lower
internal power outputs, higher external power outputs and more similar total
power outputs. These results suggest that, on a broad scale, individuals may
use a combination of stride frequency and stride length that is determined by
their limb mass distributions and that minimizes total mechanical power
outputs. These findings suggest that selection pressures for non-cursorial
activities acting on the distal limb elements of primates, and perhaps other
mammals in general, do not have to exact an energetic price. Quadrupeds may
adjust their kinematics to accommodate limb mass distribution patterns that,
superficially, seem detrimental to quadrupedal energetics. Additionally, the
results from this study suggest that researchers should explore new
explanations for the evolution of proximally concentrated limb mass in
cursorial quadrupeds.
int
ext
tot
| Acknowledgments |
|---|
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