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Department of Exercise and Sport Science, Crewe and Alsager Faculty, Manchester Metropolitan University, Alsager ST7 2HL, United Kingdom
Batterham, Alan M., Keith Tolfrey, and Keith P. George.
Nevill's explanation of Kleiber's 0.75 mass exponent: an
artifact of collinearity problems in least squares models?
J. Appl. Physiol. 82(2): 693-697, 1997.
Intraspecific allometric modeling
(Y = a · massb,
where Y is the physiological dependent
variable and a is the proportionality
coefficient) of peak oxygen uptake
(
O2 peak) has
frequently revealed a mass exponent
(b) greater than that predicted from
dimensionality theory, approximating Kleiber's 3/4 exponent for basal
metabolic rate. Nevill (J. Appl.
Physiol. 77: 2870-2873, 1994
[Medline]
) proposed an
explanation and a method that restores the inflated exponent to the
anticipated 2/3. In human subjects, the method involves the addition of
"stature" as a continuous predictor variable in a multiple
log-linear regression model: ln Y = ln
a + c · ln stature + b · ln mass + ln
, where c is the general body size
exponent and
is the error term. It is likely that
serious collinearity confounds may adversely affect the reliability and validity of the model. The aim of this study was to
critically examine Nevill's method in modeling
O2 peak in
prepubertal, teenage, and adult men. A mean exponent of 0.81 (95%
confidence interval, 0.65-0.97) was found when scaling by mass
alone. Nevill's method reduced the mean mass exponent to 0.67 (95%
confidence interval, 0.44-0.9). However, variance inflation factors and tolerance for the log-transformed stature and mass variables exceeded published criteria for severe collinearity. Principal components analysis also diagnosed severe collinearity in two
principal components, with condition indexes >30 and variance decomposition proportions exceeding 50% for two regression
coefficients. The derived exponents may thus be numerically inaccurate
and unstable. In conclusion, the restoration of the mean mass exponent
to the anticipated 2/3 may be a fortuitous statistical artifact.
allometry; multiple regression; log-linear models
RECENTLY, IN THE HUMAN SCIENCES, there has been
a renewed interest in the influence of body size on selected
physiological measurements. Several authors (20, 21, 29) have
demonstrated the statistical and physiological validity of allometric
equations in modeling such relationships. Huxley's general allometric
equation (11)
has
been most often employed, where Y,
m, and
(1)
represent the physiological
dependent variable, body mass, and the multiplicative error term,
respectively. When modeling the intraspecific relationship between
maximal oxygen uptake
(
O2 max; in l/min) and
body mass, dimensionality theory predicts a mass exponent
(b) of 2/3 (3). A number of studies
(2, 23, 28), however, have reported mean mass exponents greater than
anticipated, often closer to the 0.75 exponent identified by Kleiber
for basal metabolic rate (14).
Nevill (18) proposed an explanation for these findings derived from
Alexander et al. (1), who found that larger mammals have a greater
proportion of proximal leg muscle mass in relation to their total body
mass (leg muscle mass proportional to
m1.1). Nevill
(18) suggested that, in humans, this would inflate the derived mass
exponent because of the disproportionate increase in metabolically
active musculature within the sample, resulting in a higher
O2 max than anticipated
from body mass. To accommodate this confound when modeling
physiological variables in human subjects, Nevill argued that
"stature" be entered together with body mass in a multiple
allometric regression model
|
(2) |
|
(3) |
As the theoretical basis for Nevill's method (18) is derived from the work of Alexander et al. (1), it depends on the validity of stature as a proxy for body mass to accurately reflect "general body size" (6). Alexander et al. (1) did not provide data to evaluate the strength of the relationship between linear dimensions and mass in their sample. However, it can safely be assumed that, in humans, there is a strong relationship between stature and mass (3). Unfortunately, whereas Nevill's method (18) depends on high collinearity between the two body size variables, paradoxically, this is its primary flaw. Two predictor variables are collinear with each other if the data vectors representing them lie on, or close to, the same line (22). If collinearity is severe, multiple allometric regression equations may be unstable and unreliable, and the exponents derived may be numerically inaccurate (4). It has been demonstrated that severe collinearity may even result in exponent sign changes, indicating a directional relationship contrary to the investigator's knowledgeable expectations (17). Clearly, such concerns are especially important when attempting to distinguish within 95% confidence limits between 0.67 and 0.75 mass exponents, and they reduce confidence in the interpretation of least squares multiple-regression models.
Berlin and Antman (5) identified three early warning signs for
collinearity: large pairwise correlations between predictor variables,
large changes in coefficients caused by the addition or deletion of
other variables, and inflated SE values for coefficients. Mandel (16)
stated that collinearity is the greatest problem encountered when using
least squares regression models. It is curious, therefore, that despite
the widespread use of multiple-regression techniques physiologists in
the exercise sciences have paid little attention to the diagnosis and
treatment of collinearity. McGiffen et al. (17) have urged that
collinearity diagnostics be calculated and reported for all
applications of multiple least squares regression models. Although
Nevill's method (18) has been employed with apparent success in three
previous studies, it is plausible that the restoration of the mass
exponent to the "anticipated" 2/3 is a fortuitous statistical
artifact resulting from collinearity confounds. The aim of this study
was to critically examine Nevill's explanation of Kleiber's 3/4 mass
exponent in modeling peak oxygen uptake
(
O2 peak) in
prepubertal, teenage, and adult males.
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O2 peak.
O2 peak was
determined via a discontinuous, incremental treadmill protocol. After a
5-min warm-up, the subjects began the test at the following speeds at
zero incline: prepubertal subjects 1.94 m/s; teenage subjects 2.22 m/s;
and adult subjects 2.78 m/s. After a belt speed of 2.78 m/s was
attained, speed was held constant and grade increased by 2.5%
increments for each 3-min stage (stages separated by 1 min), to
volitional exhaustion. Expired air was monitored throughout the test
via on-line indirect calorimetry (Oxyconsigma, Mijnhardt). The system
was calibrated before each testing session according to the
manufacturers' instructions. End-of-stage oxygen uptake was determined
from the last 30 s of each stage. Heart rate was monitored throughout
by using a Rigel (Morden, UK) electrocardiogram. Criteria for
O2 peak were
1) a heart rate plateau before the
final exercise intensity, or attainment of 95% of age-predicted
maximum; and/or 2) a
respiratory exchange ratio of 1.0 or above (24).
Allometric analyses. All analyses were
carried out by using the statistical package SPSS 6.0 for Windows
(SPSS, Chicago, IL). The allometric relationships between
O2 peak and body size
variables (stature and body mass) were derived via log transformations
of the absolute data. The general curvilinear allometric equation Y = a · X b
can be linearized by taking natural logarithms of both sides: ln
Y = ln
a + b
lnX. The exponent
b is simply the slope of the log-linear plot, and a is derived from
the antilogue of the Y intercept.
After first establishing commonality of slopes between groups (30),
single exponents (separately for body mass and stature) common to all
groups were fitted by including "group" as a class variable. This
was achieved by creating two discrete dummy variables,
"prepubertal" and "adult" (coded "1" for belonging to
that group and "0" for not). The reference class
("teenage") was thus represented by a coding of 0, 0
|
|
(4) |
|
|
(5) |
R2, where
R2 represents the
correlation of one predictor variable with the others in the model.
Hence, low tolerance signifies variable redundancy. The VIF is a
standardized and dimensionless measure of a regression coefficient's
contribution to the total variance of the coefficients. If predictor
variables are orthogonal (uncorrelated), the VIF = 1. A VIF value in
excess of 10 indicates severe collinearity (10).
A more sophisticated diagnosis was achieved via a principal components
analysis of the standardized predictor variables. The first principal
component represents the linear combination of predictor variables that
explains the most variance within the set (17). Subsequent principal
components are orthogonal (uncorrelated with) to those determined
previously. Condition indexes (CI) and variance decomposition
proportions (VDP) were calculated for each principal component. The VDP
is defined as the percentage of the variability in a parameter estimate
due to a specific principal component (17). Belsey et al. (4) suggested
that a principal component with a CI >30 and a VDP of >50% for two
or more regression coefficients indicates severe collinearity that
should be corrected.
Testing for the commonality of slopes revealed no differences between
groups (P > 0.05) for either body
mass or stature. Multivariate log-linear regression revealed common
slopes of 0.81 (SE = 0.08, 95% confidence interval 0.65-0.97;
R2 = 0.93, P < 0.05) for body mass and 2.33 (SE = 0.33, 95% confidence interval 1.68-2.98;
R2 = 0.91, P < 0.05) for stature for the three
groups. Log-linear modeling including stature alongside mass as
predictor variables (Eq. 5) reduced the mass exponent to 0.67 (SE = 0.12, 95% confidence interval 0.44-0.9) and the stature exponent to
0.66 (SE = 0.4, 95% confidence interval
0.13-1.46). Analysis of the standardized regression
coefficients (beta weights) indicated that only the contribution of the
mass exponent was significant (P < 0.05).
Pairwise comparisons between log-transformed stature and mass revealed a strong positive correlation (r = 0.96, P < 0.05). For Nevill's method (18) (Eq. 5), tolerance and VIF for stature and body mass were 0.08 and 11.5 and 0.07 and 13.7, respectively. The results of the principal components diagnostics are displayed in Table 2.
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The values attained for
O2 peak
(l/min; Table 1) are consistent with previous treadmill-derived
O2 peak in similar
samples (2, 28). The mean mass exponent common to all three groups of
0.81 approximates the 3/4 mass exponent identified by Kleiber (14) for
basal metabolic rate in a range of mammals. Similar common mass
exponents for
O2 peak
have been reported previously for children and adults (2, 23, 28).
These mass exponents appear higher than the 2/3 exponent anticipated
from dimensionality theory and have led some investigators to postulate
mechanisms to explain why theoretical principles have failed to provide
an adequate account (18, 28). In the present study, however, it is
noteworthy that the 95% confidence interval for the mass exponent
includes both 2/3 and 3/4. It is, therefore, impossible to confidently
reject dimensionality theory predictions. Many investigators fail to
report confidence intervals for the derived mass exponents. This
information is essential if meaningful interpretations are to be made.
The confidence intervals for mass exponents for
O2 peak in human
studies appear wider than those cited in investigations with the use of
animals. Taylor et al. (26) reported a mean mass exponent of 0.79 (95% confidence interval, 0.75-0.83) in a range of wild mammals
for treadmill-derived
O2 peak. This finding precludes the anticipated 2/3 exponent and indicates that
O2 peak scales
similarly to basal metabolism.
If the true mass exponent for
O2 peak in humans is
>2/3, it is possible that the body size ranges commonly studied are
insufficient to detect it within 95% confidence limits. Kleiber (15)
required a ninefold size ratio to distinguish between the 3/4 and 2/3
mass exponents. Interestingly, the mean stature exponent in the present study of 2.33 (95% confidence interval, 1.68-2.98) also conformed to dimensionality theory predictions
(
O2 peak
mass2/3
stature2).
Despite the relatively wide confidence intervals, it is clear that the
mean mass exponent more closely approximates 3/4 than the anticipated
2/3. Nevill's method (18) of including stature as a continuous
covariate to restore the mean mass exponent to 2/3 appears to have a
sound physiological basis (1). The results of the collinearity
diagnostics in the present study, however, indicate that the method may
be numerically inaccurate, unreliable, and, therefore, invalid. Low
tolerances and high VIFs were evident for both mass and stature
predictor variables, with values exceeding published criteria for
severe collinearity (10). Nevill's approach (18) assumes that stature
is an effective proxy for mass to reflect the "general size" of
the body. This assumption is supported by the strong pairwise
correlation between the log-transformed mass and stature variables
(r = 0.96, P < 0.05). Unfortunately, however,
this also alerts the investigator to potential collinearity problems
(5) and indicates variable redundancy. With stature and mass included
in the same multiple log-linear regression (Eq. 5), the SE values for the exponents were inflated
considerably, in comparison with those generated when modeling stature
and mass separately (Eq. 4).
Nevill's method (18) also reduced the mean stature exponent
dramatically from 2.33 to 0.66. Hence, the three early warning signs
for collinearity problems identified by Berlin and Antman (5) are all
present. Moreover, it is noteworthy that the analysis of the beta
weights revealed that the stature exponent no longer contributed to the
prediction of
O2 peak (P > 0.05), even though stature has
a strong positive bivariate correlation with the dependent variable.
Inclusion of stature alone as a body size variable explained 91% of
the variance in
O2 peak. The
lack of significance for the stature exponent in Eq. 5 is due to its inflated variance and may lead to the
erroneous conclusion that stature is not important in determining
O2 peak. In addition,
Nevill's method (18) provides a stature exponent that is
physiologically and theoretically implausible.
The mass exponent was reduced from the original mean of 0.81 to 0.67, exactly the value predicted from theoretical considerations. Without due consideration of collinearity confounds, this would, again, appear to support Nevill's method, adding a further study to those included in his meta-analysis (18). Due to variance inflation, however, the confidence interval for the "restored" 0.67 exponent was widened to 0.44-0.9, a range that includes 2/3, 3/4, and the original 0.81 exponent. Similarly, in the most recent of the three studies where the method has been applied (28), the confidence interval for the restored mean mass exponent of 0.71 (calculated from the SE provided) was 0.59-0.83. Notwithstanding the collinearity problems, the method is clearly unable to distinguish between theoretically predicted and empirically derived mass exponents within reasonable confidence limits.
The results of the collinearity diagnostics derived from the principal components analysis raise further doubts about the reliability and validity of Nevill's method (18). Severe collinearity was detected, with values exceeding the criterion defined by Belsey et al. (4). CI values of 32.3 and 98.8, and VDPs >50% for two coefficients, were obtained in principal components 4 and 5, respectively (Table 2).
The warning signs for collinearity, the preliminary diagnostics via tolerance and VIFs, and the specific principal components diagnostics, all indicate that little confidence can be placed in Nevill's method (18). The overlap between stature and mass is such that including both in the model (Eq. 5) is a somewhat redundant method of indicating body size. Among their suggestions for coping with collinearity, Berlin and Antman (5) include removing redundant variables from the model and reducing reliance on interpretation of coefficients for confounding variables. Both these suggestions have serious implications for Nevill's method (18). A further suggestion for coping with collinearity is to form a "summary" variable (5). With body size, this is a difficult task, as variables such as stature, mass, and surface area are expressed in different units and are highly interrelated. Indeed, the selection of an appropriate size variable has been described as the fundamental problem confronting all studies of allometry (12). As stated by Nevill (18), a fundamental assumption is that the physiological variable is influenced by active muscle mass, with body mass usually used as a proxy in the absence of muscle mass estimates. Although body mass and muscle mass are related (8), differences in body composition within samples can severely distort derived mass exponents (9). Where possible, therefore, measurements or estimates of involved musculature should be the scaling variable of choice (31).
Notwithstanding these considerations, with a large sample size and a body size range sufficient to overwhelm body composition variance (7), meaningful mass exponents may be derived, offering an advantage in practicality over sophisticated muscle mass measurement methods (27). The fact that the mean mass exponents reported in the literature frequently exceed theoretical predictions should not encourage a confirmatory bias in research. Recent attempts to account for apparent inconsistencies with theoretical predictions are a modern parallel to the process identified by Kleiber 50 years ago (14). The belief in the "surface law" for basal metabolism was so well established that empirical deviations were explained by particular conditions or measurement error. For example, when rabbits failed to comply with predicted daily heat production, their ear surface was removed from the model to restore the theoretical relationship (14).
The present study has demonstrated that Nevill's (18) explanation of
Kleiber's 3/4 mass exponent is confounded by the severe collinearity
problems detected in the multiple least squares regression model
(Eq. 5). Empirical evidence in
humans appears unable to distinguish between the 2/3 and 3/4 exponent
for
O2 peak,
as both are supported by the data. Further research, using large sample
sizes selected for body size heterogeneity, is required to more fully
elucidate the relationship between body size and
O2 peak in humans.
Address for reprint requests: A. M. Batterham, Dept. of Exercise and Sport Science, Manchester Metropolitan Univ., Crewe and Alsager Faculty, Hassall Rd., Alsager ST7 2HL, UK (E-mail: A.Batterham{at}mmu.ac.uk).
Received 26 April 1996; accepted in final form 4 October 1996.
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