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O2 peak: effects of
model choice and body composition
1 School of Social Sciences, University of Teesside, Middlesbrough, TS1 3BA, United Kingdom; 2 Department of Health and Sport Science, University of Dayton, Dayton, Ohio 45469-1210; 3 Department of Exercise and Sport Science, East Carolina University, Greenville, North Carolina 27858; and 4 Department of Health and Human Performance, University of Houston, Houston, Texas 77204-5331
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ABSTRACT |
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This study
examined the bivariate relationship between peak oxygen uptake
(
O2 peak; l/min) and
body size in adult men (n = 1,314, age 17-66
yr), using both "simple" and "full" iterative nonlinear allometric models. The simple model was described by
O2 peak = Mb (or
FFMb)
exp(c SR-PA)
exp(a + d age)
(where
M is body mass in kg; FFM is fat-free
mass in kg; SR-PA is self-reported physical activity;
is a
multiplicative error term; and exp indicates natural antilogarithms). The full model was described by
O2 peak = Mb (or
FFMb)
exp(c SR-PA)
exp(a + d age) + e (
), where
e is a permitted Y-intercept term. The
M exponent obtained from simple
allometry was 0.65 [95% confidence interval (CI),
0.59-0.71], suggestive of a curvilinear relationship
constrained to pass through the origin. This "zero
Y-intercept" assumption was
examined via the full allometric model, which revealed an
M exponent of 1.00 (95% CI,
0.7-1.31), together with a positive
Y-intercept term
(e) of 1.13 (95% CI,
0.54-1.73). The FFM exponents were not significantly different
from unity in either the simple or full allometric models. It appears
that the curvilinearity of the simple allometric model (using total
M) is fictitious and is due to the
inappropriate forcing of the regression line through the origin.
Utilizing FFM as the body-size variable revealed a linear relationship
between body size and
O2 peak, irrespective
of model choice. We conclude that the population mass exponent for
O2 peak is close to unity.
allometric scaling; nonlinear regression; log-linear modeling; body size; oxygen uptake
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INTRODUCTION |
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THE RELATIONSHIP BETWEEN body size and energy
metabolism, at rest and during exercise, has interested researchers for
over a century. In the exercise sciences, the past decade has seen a
resurgence of interest in this problem. Several authors have suggested
that allometric or power function modeling may be theoretically, physiologically, and statistically superior to alternative scaling models (27-29, 35, 36). Huxley's "simple" allometric
equation (19), Y = aMb
, has been most often employed, where
Y, M, and
represent the physiological
dependent variable, body mass, and a multiplicative error term,
respectively. Feldman (15) stated that two empirical allometric laws
for energy metabolism in adult animals operate simultaneously. These
laws are based on theoretical speculations about mechanisms of heat
loss (31, 32), biological similitude (4, 32), elastic similarity (26),
or fractal geometry (37) and predict an intraspecific (within-species)
mass exponent (b) of 2/3 and an
interspecific (between-species) value of
b = 3/4.
In humans, a wide variety of intraspecific mass exponents has been
reported for maximal or peak oxygen uptake
(
O2 peak; in l/min).
For example, Bergh et al. (9) reported
b values ranging from 0.47 to 0.86 for
maximal oxygen uptake in seven different groups of adults. The weighted
mean mass exponent of 0.71 closely approximated the anticipated 2/3
value. However, others have reported a mass exponent of 1.02 in adults,
suggestive of a linear relationship between body size and
O2 peak (30). Heil
(17) argued that a mass exponent of 0.67 was appropriate in samples
homogeneous with respect to age, training background, and body height,
whereas a 0.75 value was more applicable to more heterogeneous samples. The lack of agreement regarding the proper value of the mass exponent has provoked some lively theoretical and methodological debate (7, 27).
Rogers et al. (30) suggested that the large variation in derived
exponent values may be due to small sample sizes and/or body-size
homogeneity. In addition, failing to control, or account for, known
covariates (e.g., age, physical activity status) could also confound
empirical body size-physiological function relationships (17).
Furthermore, heterogeneity of body composition can spuriously affect
the magnitude of the obtained mass exponents (35). Indeed, over 40 years ago Döbeln (14) stated that any scaling analysis in humans
should be based ideally on body mass minus fat mass [i.e.,
fat-free mass (FFM)]. Estimated FFM has been found to be the best
single predictor of
O2 peak in several
studies (34, 35). Inasmuch as ~95% of the oxygen passing through the
lungs of a mammal exercising at
O2 peak is bound for a
"single sink" in the skeletal muscle mitochondria (25), it
follows that estimated FFM may be a judicious choice as an indicator of
body size.
Why derive a robust estimate of the population mass exponent for
O2 peak?
It is apparent that the precise numerical value of the mass exponent
for peak aerobic function has been the subject of much research and
heated scientific debate. Deriving a robust estimate of the population
mass exponent is clearly viewed as important. Most researchers in the
exercise sciences attempt to use empirical, sample-specific mass
exponents to 1) make interpretations
of their biological significance and/or
2) derive an index to remove the influence of body size from a dependent variable. Indeed, Feldman (15)
stated that, in empirical allometry studies, it is the value of the
mass exponent b that is of critical
interest, inasmuch as it may provide "insight into the biological
design of the class." As Albrecht and Gelvin (2) argued, different
numerical values for the mass exponent may result in different
biological and theoretical explanations.
Critique of allometric models.
It has been suggested (17) that, given a large sample size and
sufficient data to describe and account for known covariates, a robust
mass exponent for
O2 peak can be
obtained. However, we contend that insufficient attention has been paid
to the most appropriate statistical modeling procedures. The selection
of an allometric modeling method is not a trivial issue. A robust estimation of the position of a line of best fit through a "data cloud" requires the critical evaluation of key assumptions
underpinning the model chosen. Strauss (33) stated that, in any
empirical study of allometry, the biologist is confronted with a
confusing array of models and options. In the exercise sciences,
allometric modeling of
O2 peak has been
conducted exclusively via linear, least squares regression techniques
applied to natural log-transformed dependent and independent variables
(log
O2 peak = log
a + b log M + log
). Although this approach simplifies the
calculations greatly, it may introduce a systematic bias, resulting in
a crude estimate of the mass exponent (33). The bias is due to the fact that the least squares technique minimizes the residual error of the
linearized, log-log regression line, not that of the original untransformed data (38). Second, the equation of simple allometry, Y = aXb
,
describes a curvilinear relationship that constrains the regression line to pass through the origin. Although intuitively appealing, this
assumption has not been tested in the scaling of
O2 peak and has
no empirical basis (2). Albrecht et al. (3), in an excellent
methodological review, argued that the extrapolation of regressions
through the origin may result in fictitious curvilinearity. Hence, if
the true relationship between
O2 peak and
body mass were linear (b = 1), empirically derived mass exponents of
b < 1 (curvilinear) from simple
allometry may be an artifact of forcing the regression line to curve at
smaller values to reach the origin (1).
O2 peak may
be questionable. The purpose of the present study, therefore, was to
determine a robust estimate of the population mass exponent (body mass
and FFM) for
O2 peak in
a large sample of adult men, while controlling for some known
covariates. First, we adopt an allometric model that applies an
iterative nonlinear regression procedure to the original raw data
(rather than the customary log-linearized method). Second, we tested
the hypothesis that any obtained mass exponent of
b < 1, implying curvilinearity, would be due to imposing a "zero
Y-intercept" constraint. This simple experimental model involves manipulating the requirement for the
regression line to pass through the origin and examining the effect on
the obtained mass exponent (b). This
is achieved via a "full" allometric model (1-3, 19),
described by the equation Y = aXb + c(
), where
c is a permitted
Y-intercept term.
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METHODS |
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Subjects. The 1,314 men selected for this study were employees at the National Aeronautics and Space Adminstration Johnson Space Center (Houston, TX). With the exception of astronauts, preemployment physical screening is not compulsory. Approximately 85% of the male workforce, however, choose to have a yearly health examination and a graded exercise stress test every 3 yr. At their annual physical examination, the men in this cohort were "apparently healthy," asymptomatic, and free from cardiovascular disease. Additional exclusion criteria included the chronic use of cardiovascular medications and electrocardiographic abnormalities exhibited at rest or during the stress test. Written informed consent was obtained from all subjects before the procedures.
Test procedures. The specific protocols employed in the present study are detailed elsewhere (21). Briefly, the subjects' level of physical activity was assessed with the National Aeronautics and Space Adminstration self-report physical activity (SR-PA) scale (8). Each subject was asked to rate his physical activity during the previous month on an eight-point scale (0-7). The scale's lowest value of zero represents an almost completely sedentary lifestyle. The highest value of seven represents participation in a minimum of 3 h of regular, heavy aerobic physical activity each week.
Body fat percentage was estimated from the sum of chest, abdominal, and thigh skinfolds (23). Specific anatomic sites and procedures are described elsewhere (24). Total body mass (kg) and body fat percentage were used to partition body mass into fat mass and FFM compartments.
O2 peak was
determined during the Bruce treadmill exercise test protocol (10). A
full outline of the equipment and test procedures is provided in
another source (22). The criteria adopted for the attainment of
O2 peak were 1) volitional exhaustion;
2) a respiratory exchange ratio of
1.1; and 3) a peak exercise heart
rate
90% of the age-predicted maximum.
Allometric modeling.
All analyses were carried out by using the SPSS (release 7.5 for
Windows; SPSS, Chicago, IL) statistical software package. For
comparative purposes both "simple" and full allometric models were derived, with separate models for body mass (M )
and FFM. Subject age and SR-PA score were included in all models as
covariates. Working in the arithmetic space defined by the original raw
X and Y variables (3), we solved all model
parameters by an iterative nonlinear protocol using the
Levenberg-Marquardt algorithm (16). In this procedure, small,
successive corrections to regression parameter estimates are made until
a global solution converges (on the basis of a cutoff criterion for the
relative reduction in successive residual error of 1.0 E-08). In this
nonlinear regression program, the choice of initial values for the
parameters can influence convergence. Where possible, realistic values
should be selected close to the expected final solution as poor
starting values can result in a locally, rather than globally, optimal
solution (16). In the present study, therefore, linear multiple
regression analysis of the following log-transformed simple allometric
model was employed in an exploratory fashion to obtain starting values
for the parameters in the subsequent, nonlinear simple allometric
modeling
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1.58, b = 0.67, c = 0.05, and
d =
0.009; and
2) for the FFM model, a =
2.84,
b = 0.99, c = 0.04, and
d =
0.007.
These values were used as initial values in the confirmatory, iterative
nonlinear procedures described by the equations below. This exploratory
method could not be applied to the full allometric model, however,
inasmuch as the full model is not amenable to logarithmic
transformation (3). Therefore, it was necessary to apply the same
starting values (obtained from the simple, log-linear models) to the
nonlinear full allometric models. The initial parameter value of the
permitted Y-intercept term
(e) in the full model was defined as
zero, to test the assumption of the simple allometric model that the
regression line passes through the origin.
Simple allometric model.
The multivariable form of the general allometric model
Y = aXb
(19) is
given by
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(1) |
is a multiplicative error term.
In this model, body mass and FFM are variables assumed to relate in a
nonlinear manner to
O2 peak, whereas
SR-PA and age are linearly related to the dependent variable. The
exp(c SR-PA) exp(a + d age) term is thus the linear
coefficient applied to M or FFM
equivalent to the proportionality coefficient
a that modifies
X in the general allometric equation
Y = aXb
(19).
Full allometric model.
Similarly, the multivariable form of the full allometric model,
allowing for a Y-intercept term, is
given
by
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(2) |
O2 peak) and
X (M
or FFM) (3). The full model reduces to the simple model
(Eq. 1) if the
Y-intercept term,
e, is equal to zero. All regression
parameters were calculated as point estimates, together with the
associated estimates of uncertainty [95% confidence interval
(CI)]. The 95% CI provides important information regarding the
precision of the parameter estimates. In addition, it can be used to
test for statistical significance (if desired) at the 0.05 alpha level.
If the 95% CI for the coefficient does not cross zero, then that
parameter makes a statistically significant contribution to the
prediction of
O2 peak
(P < 0.05). Several authorities,
including the International Committee of Medical Journal Editors (20),
have urged the reporting of CI in preference to
P values, and this practice is adopted in the present study.
Regression diagnostics (5) revealed no violation of the assumptions of
allometric modeling. There were no significant interactions among the
model covariates, confirming the assumption of homogeneity of
regression. In addition, Kolmogorov-Smirnoff one-sample tests revealed
that all allometric model residuals were normally distributed (P > 0.10).
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RESULTS AND DISCUSSION |
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Table 1 presents the means, SDs, and range
for the dependent variable and all model covariates. The
subjects were heterogeneous for age, body mass, FFM,
physical activity, and
O2 peak. An ~2.5-fold
body mass size ratio was evident across the sample
(54.7-134.5 kg), with a twofold ratio for FFM (45.7-95.0 kg).
A wide size range is vital to derive meaningful scaling expressions,
and Calder (12) has urged that publication of size range should be
mandatory in all allometric studies.
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Table 2 provides the obtained regression
coefficients for the simple allometric modeling of
O2 peak by body mass.
Examination of the 95% CI reveals that all regression parameters make
a statistically significant contribution to the model
R2
(P < 0.05). This finding supports
the results of Heil (17) and Jackson et al. (21) and confirms that both
physical activity status and age are important covariates that must
always be included in the model in studies of this type. The model
R2 indicates that
~58% of the sample variance in
O2 peak is explained by
the variables entered. The simple allometric model
(Eq. 1) yielded a body mass exponent
(b) of 0.65. Table 2 confirms that the 95% CI for this point estimate included the value of 2/3
anticipated from the intraspecific empirical law for mammals (18). This 2/3 exponent is consistent with the previous findings of Nevill and
co-workers (29) using simple log-linear allometric modeling. Nevill et
al. reported a mass exponent of 0.669, common to both men and women, in
a study of 308 "recreationally active" young adults. Age and
physical activity status were not included as covariates in this study
as, presumably, the sample was homogeneous with respect to these
variables. In a larger sample of 1,732 subjects, Nevill and Holder (28)
obtained a b value of 0.66, with age and a dummy variable of "vigorous exercise" and "no vigorous
exercise" included as covariates.
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The 95% CI for the mass exponent from the simple allometric model
(Table 2) indicates that the population mass exponent is significantly
different from unity. The model implies that the relationship between
O2 peak and body mass
is curvilinear, with the regression line passing through the origin.
The results of the full allometric model (Table
3), however, suggest that this "curvilinearity" may be a fictitious artifact of an inappropriate modeling procedure. Table 3 displays a statistically significant, positive Y-intercept term
(e), together with a mass exponent
(b) equal to one. The full model
(Eq. 2) has thus reduced to a
simple, linear model (Y = aX + c). Hence, it would seem that the
curvilinearity (implied by b = 0.65)
in the simple allometric model was caused by the forcing of the curve
through the origin (1-3). Importantly, the relaxation of this
constraint revealed a very different numerical value for the mass
exponent, indicating that the critical, zero Y-intercept assumption of the simple
allometric model was untenable. This phenomenon is demonstrated
graphically in Fig. 1, which depicts the
bivariate relationship between body mass and
O2 peak. For this
analysis the dependent variable was first adjusted for the influence of
model covariates. This was achieved by regressing
O2 peak on age and
SR-PA and adding the resultant residuals to the mean
O2 peak for the sample
(3.08 l/min). Figure 1 illustrates clearly that, through the data
cloud, the relationship between body mass and
O2 peak is essentially
linear. The curvilinearity of the simple allometric fit line results
from an extrapolation of the curve well beyond the observed data. It
appears that it is possible to force simple allometric regressions on
bivariate data that are actually linear, as demonstrated previously by
Albrecht et al. (3). Permitting a
Y-intercept term revealed a different bivariate relationship between the X
and Y variables.
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To our knowledge, no similar comparison of simple vs. full allometric
models in the scaling of
O2 peak has been
published. In the anthropological literature, Albrecht and Gelvin (2) reported that mass exponents were significantly affected by model choice (simple vs. full allometric) due to non-zero
Y-intercepts obtained in the full
models. In the present study, the model
R2 and SE of the
estimate suggest that both the simple and full allometric models fit
the data about equally well. However, the exponential term
b differs significantly between the
models because of the implicit assumption in simple allometry that the
Y-intercept e = 0. If this assumption is relaxed,
as with the full allometric model, then it is found that the bivariate
relationship between
O2 peak and body mass
is described by a regression line that has a
Y-intercept
e > 0 and a mass exponent
b = 1. As can be seen in Fig. 1, this
means that the data are essentially linear within the range of
observations, not curvilinear as implied by the mass exponent
b = 0.65 from the simple allometric model.
We must emphasize that the suggestion of the addition of a constant to
the simple allometric equation is not new. Over 60 years ago, Huxley
(19) stated that the full model was the most complete and should be
taken as the theoretical basis for analysis. Indeed, Albrecht et al.
(3) argued that if the mass exponent (b) from the simple allometric model
was considered biologically meaningful, then the
b in the full model should be, also.
The problem for the researcher is that, on the basis of our findings, the two models provide different mass exponents, due to the failure to
satisfy a key assumption of the simple model. This occurred despite the
fact that the two models displayed a similar degree of
"predictive value," in terms of explained variance in
O2 peak and SE of the estimate. Hence, the mass exponent of 0.65 derived from
simple allometry may lead to theoretical expositions such as the theory
of geometric similarity (32). Conversely, exponent b in the full model implies that
O2 peak is linearly
proportional to body mass. Interestingly, the 95% CI for the body mass
exponent in the full model (Table 3), although wider than that in the simple model, did not include the anticipated intraspecific value of
2/3. It is noteworthy that several other variables (including pulmonary
diffusing capacity, heart mass, blood volume, stroke volume, and
skeletal muscle mass) in the chain of events involving the ability to
take in, transport, and utilize oxygen also scale isometrically with
body mass (albeit by using simple allometric equations) (25). Hence,
the empirically derived mass exponent b = 1 from the full model may point to
very different biological principles and connections from the
b
2/3 from the simple model. We
believe that, notwithstanding the equivalent predictive value of the
two models, the more robust estimate of the population mass exponent is
provided in this instance by the full allometric model. This assertion
is based on the fact that a key assumption of the simple model was
violated (0 Y-intercept), whereas all regression assumptions were satisfied for the full allometric model. In
the exercise sciences literature, there is no reported evidence of
checks on the validity of the zero
Y-intercept assumption in simple
allometric models.
The modeling of
O2 peak
by FFM provides additional insight. Table 4
(simple allometry) displays an obtained FFM exponent of 0.97, with the
95% CI including unity, but precluding the value of 2/3. The model
R2 indicates that
the FFM model explained ~7% more of the variance in the dependent
variable than did the body mass models. This supports earlier
contentions that FFM is a superior scaling variable for
O2 peak (13, 34, 35).
Full allometric modeling by FFM also revealed a
b exponent not significantly different
from unity (Table 5). Again, the 95% CI
precludes the value of 2/3 for the mass exponent. The point estimate
for the Y-intercept term
(e) is 0.4. However, the 95% CI for
this parameter crosses zero, suggesting that for the population there
is no statistically significant
Y-intercept. Hence, the key zero
Y-intercept assumption of the simple
allometric model has been satisfied. Both the full and simple
allometric models, therefore, indicate that the bivariate relationship
between
O2 peak and FFM
is essentially linear (b = 1) and
passes through the origin (e = 0).
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These findings are illustrated in Fig. 2,
where it is clearly shown that the simple allometric and linear
regression fit lines overlap throughout the range of observed data (in
this analysis,
O2 peak
was adjusted for the effects of SR-PA and age, as described previously). Both the full and simple allometric models have thus reduced to a simple, linear per-ratio standard model of the form Y = aX. In modeling maximal oxygen uptake
or
O2 peak, exponent values not significantly different from unity for FFM have been reported previously in children (6), adult women (35), and elderly men
(13). It is noteworthy that all of these studies (using simple,
log-linear models) reported body mass exponents significantly less than
one (implying curvilinearity), consistent with the findings of the
simple allometric modeling in the present study. None of the studies,
however, reported checks on the validity of all key model assumptions.
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The differences between the reported exponents for body mass and FFM
derived from simple allometry (Eq. 1) may relate to heterogeneity of body composition
across the sample. If there was no variance in body fat percentage, the
derived exponent values should theoretically be exactly equivalent. In
the present sample, however, a significant positive relationship was
found between body mass and body fat percentage (Pearson
r = 0.58, P < 0.05). This suggests that, as body mass increases across the sample, the proportion of total body
mass composed of FFM decreases. Inasmuch as only the metabolically active body cell mass is pertinent to the expression of
O2 peak (25, 35), this
body composition heterogeneity may artificially deflate the obtained
body mass exponents (35).
The positive Y-intercept in the full
allometric model (Eq. 2, Table 3) for
body mass may also relate to heterogeneity of body composition, in
particular to the precise relationship between body mass and FFM in
this sample. If the regression line is extrapolated to the
Y-intercept, the suggestion is that
someone of zero body mass would exhibit a
O2 peak of 1.13 l/min
(95% CI, 0.54-1.73). Recall that there was no statistically
significant Y-intercept in the full
allometric modeling by FFM (Table 5). To explore this interesting
phenomenon, we first examined the bivariate relationship between body
mass and FFM in this sample. Theoretically, there should be a linear,
proportional relationship between body mass and FFM if homogeneity of
body composition is assumed. For example, if body fat percentage was
constant at 15% across the sample, the relationship between body mass
(X) and FFM
(Y) would be described by a general
linear model, Y = 0.85 X + 0 (i.e., 0 Y-intercept). However, as stated, the
present sample is highly heterogeneous for body composition. Figure
3 illustrates the linear
(Y = aX + c) and simple allometric
(Y = aXb, for
comparison) relationships between body mass and FFM. The linear model
(dashed line) reveals a significant positive
Y-intercept of 22.9 kg of FFM. The
95% CI for this parameter was 21.3-24.6 kg. The allometric
regression (solid line) illustrates how the forcing of the curve
through the origin causes the curvilinearity implied by the obtained
body mass exponent of 0.65. Through the data cloud the regression lines
overlap, and it is clear that the relationship is essentially linear.
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The positive Y-intercept from the
linear model suggests that someone of zero body mass would exhibit FFM
of 22.9 kg. This physiologically implausible phenomenon is due to the
large variance in body fat percentage across the sample (range
3.9-39.3%, SD, 6% body fat). We next conducted a simulation of
the influence of this heterogeneity of body composition on the results
of the full allometric modeling by body mass (Eq. 2, Table 3). The 22.9 kg of FFM (the
Y-intercept, Fig. 3) were entered into
the simple allometric equation derived previously for FFM
(Eq. 1, Table 4). The simulation
predicts that a hypothetical subject presenting with 22.9 kg of FFM
would express a
O2 peak
of 1.15 l/min (95% CI, 0.41-1.89). This point estimate is almost
exactly equivalent to the significant, positive
Y-intercept of 1.13 l/min obtained from the full allometric modeling by body mass (Table 3). Hence, it is
possible that the physiologically implausible 1.13-l/min Y-intercept in Table 3 (implying that
someone of 0 body mass would still exhibit a
O2 peak value)
resulted, in part, from the specific relationship between body mass and
FFM in this sample.
Taken together, our findings suggest that "ideally," estimates of
FFM should be secured to serve as the indicator of body size. The FFM
models resulted in a larger coefficient of determination and a lower SE
of the estimate in predicting
O2 peak. When total body mass is used in scaling, the full allometric model may be preferable in situations where the
zero-Y-intercept assumption does not
hold. When FFM is used in scaling, the requirement of the regression
line to pass through the origin was a valid assumption. This resulted
in no significant difference between the FFM exponents derived from the
simple (b = 0.97) and full
(b = 1.1) allometric models.
The population body mass or FFM exponent for modeling
O2 peak appears to be
close to unity, implying a linear relationship. The 95% CIs do not
include the anticipated value of 2/3. As stated at the beginning of
this study, the intraspecific (within-species) allometric 2/3 law is an
empirical law based on studies in mammals (15, 18). Theoretical
speculations related to simple dimensionality theory or biological
similitude, however, are frequently advanced (e.g., Refs. 4, 17, 27,
29, 30). The conventional argument is that
O2 peak is a measure of
work divided by time (aerobic power). Work is equal to the product of
force (
L2,
the square of the length dimension) and distance (
L1.0). Work is
therefore proportional to
L2L1.0 = L3
M1.0. From
Newtonian mechanics, time is assumed to be proportional to the length
dimension (
M1/3) (4, 17).
Hence,
O2 peak
(metabolic work divided by time) is proportional to
L2
M2/3. Despite
intuitive appeal, however, this theory is overly simplistic and appears
to have little or no foundation (15). Butler et al. (11) argued that
energy metabolism is dependent on at least 12 dimensionally distinct
factors. In a thorough and theoretically correct dimensional analysis
of the relationship between metabolic rate and body mass, the authors
concluded that the 2/3 mass exponent does not follow logically from
dimensional reasoning. Indeed, an intrinsic 2/3 value could only be
derived theoretically if just 1 pair of the 12 contributing variables
(that does not contain a temperature dimension) were applied and held
invariant as body mass varied. Other pairs of variables would result in
completely different predicted mass exponents. Butler et al. calculated
predicted intrinsic mass exponents of 1/5, 7/6, 2/3, and 5/4 for
various pairs of invariant contributory variables. If energy metabolism depends on more than one pair of variables, in addition to mass, then
simple dimensional theory cannot predict a mass exponent at all. Hence,
the value of 2/3 is not a value anticipated from simple dimensionality theory.
The primary purpose of the present study was to determine a robust
estimate of the mass exponent in the scaling of
O2 peak. However, it is
noteworthy that the regression coefficient point estimates for the
model covariates (SR-PA and age) differ among the various analyses
(Tables 2-5). These regression coefficients provide estimates of
the independent influence of habitual physical activity and age on
O2 peak in this
cross-sectional study. The more robust estimates for these effects can
be derived from the models, including FFM as the indicator of general
body size. Recall that these models (Tables 4 and 5) explained ~7%
more of the variance in
O2 peak than the body
mass models (Tables 2 and 3). The point estimates of the covariate
regression coefficients for the simple allometric model (Table 4)
indicate that a one-unit increase in the SR-PA score is associated with
a 4.5% increase in
O2 peak
[exp(0.044 · SR-PA) = 1.045 exp(SR-PA)].
The age-associated decrease in
O2 peak predicted from
the simple FFM model (Table 4) is 0.7%/yr or 7%/decade
[exp(
0.0072 · age) = 0.993 exp(age)]. Similarly, the full allometric model (Table 5)
predicts that a one-unit increase in the SR-PA score is associated with
an increase in
O2 peak
of 5.2%, with an age-associated decrease in
O2 peak of 0.8%/yr or
8%/decade. Note that the 95% CIs for the covariate regression
estimates in the simple and full allometric models overlap, implying
that there is no statistically significant difference between them.
This is due to the fact that there is no significant Y-intercept term
(e) in the full allometric model;
the simple and full FFM models are essentially equivalent.
The present study is subject to several limitations. First, the sample is exclusively male and delimited in age range (17-66 yr). We make no attempt to extrapolate the present findings beyond the male adult population within this age range. Indeed, we would recommend that our model be also cross-validated on large, heterogeneous, and independent adult male samples. In the present study, cross-validation within the same sample via various data-splitting algorithms was avoided, as this would have reduced the precision of the sample's regression estimates. When distinguishing between mass exponent values of 2/3 and unity is attempted, for example, the sample size must be maximized to obtain an appropriately narrow (precise) 95% CI.
The limitations of the general methods employed to derive the physical
activity and body composition estimates are well documented. Clearly,
however, the adoption of criterion or "gold standard" methods for
the above variables (such as doubly labeled water and
hydrodensitometry) would have been impractical and prohibitively expensive in a cross-sectional epidemiological study of this nature. The criteria adopted for the attainment of
O2 peak may represent a
further limitation to our study. Volitional exhaustion, a respiratory exchange ratio of
1.1, and a peak exercise heart rate of
90% of
age-predicted maximum are essentially "nonphysiological"
indicators. Obtaining blood lactate data would have permitted us to
establish a physiological state of exercise intensity. The lack of
information pertaining to postexercise blood lactate concentrations is
one reason the data are described as "peak" rather than
"maximal" oxygen uptake. We are confident, however, that the
values obtained are representative of very heavy exercise.
Despite the aforementioned limitations, the advantages in increased
precision of regression parameter estimation, afforded by a large
sample size, likely far outweigh any inherent measurement errors in the
dependent variable or covariates. The present study was restricted to
one species (intraspecific). An advantage of interspecific
(between-species) allometry is an increased range of body size (e.g.,
mouse to elephant). For example, this size range, coupled with the
inclusion of data from a large number of animals, is held to overwhelm
the variability in
O2 peak because of
sources other than body size and leads to more meaningful scaling
expressions (12). To offset this advantage of interspecific allometry,
we attempted to account for a proportion of the variability due to
other sources by including important known covariates in the model. The
sample was highly heterogeneous for physical activity status, age, and
body composition. Including this information in the model covariates,
together with a large sample somewhat heterogeneous for body mass
(range from 54.7 to 134.5 kg), enabled us to distinguish (within 95%
CI) between mass exponents of 2/3 and unity.
In summary, we have demonstrated empirically, by using the most
complete (full) iterative nonlinear allometric models and controlling
for key known covariates, that the population mass exponent for
O2 peak is close to a
value of one (linearity) for adult men. This mass exponent differs from
that predicted by unfounded theoretical speculations about dimensional
consistency (4, 17, 27). The obtained
b value of 1 contradicts the empirical
2/3 scaling law derived from simple, log-linear allometry. We have
established that the curvilinearity implied by mass exponents <1 in
studies employing simple allometric models may be fictitious, due to
the inappropriate forcing of the regression line through the origin. If
simple allometric models are employed, the key assumption that the
regression line passes through the origin (Y = 0 when
X = 0) should be tested. We urge that
full allometric models be applied in large-sample scaling studies of
this type to further examine the true relationship between body size
and physiological function. If the empirically derived mass exponent value of 1.0 for
O2 peak is found to be
robust in new studies in diverse populations, then we are challenged to
understand it from a physiological and/or biological perspective.
In addition, the application of a robust population mass exponent may be preferable in studies involving small, homogeneous samples, where an index must be derived to partition out the influence of body size from a dependent variable. In such studies, calculated sample-specific mass exponents may be confounded and inaccurate, because of lack of precision and wide CI (small n), and limited between-subject variance in body size (range effects on regression estimates) (30). Moreover, attempts to apply nonlinear iterative full allometric models in small and/or homogeneous samples may be hampered by the failure of the model to converge cleanly with an optimal solution.
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FOOTNOTES |
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The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. §1734 solely to indicate this fact.
Address for reprint requests and other correspondence: A. M. Batterham, School of Social Sciences, Univ. of Teesside, Borough Road, Middlesbrough, TS1 3BA, UK (E-mail: A.Batterham{at}tees.ac.uk).
Received 14 September 1998; accepted in final form 2 June 1999.
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