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First published online July 17, 2009
Journal of Experimental Biology 212, 2313-2323 (2009)
Published by The Company of Biologists 2009
doi: 10.1242/jeb.026146
A body composition model to estimate mammalian energy stores and metabolic rates from body mass and body length, with application to polar bears
1 Centre for Mathematical Biology, Department of Mathematical and Statistical
Sciences, University of Alberta, Edmonton, AB, Canada T6G 2G1
2 Department of Biological Sciences, University of Alberta, Edmonton, AB, Canada
T6G 2E9
3 Department for Marine and Environmental Research, Ruder Bo
kovi
Institute, POB. 180, Bijeni
ka 54, HR-10002 Zagreb, Croatia
4 Wildlife Research and Development Section, Ontario Ministry of Natural
Resources, DNA Building, Trent University, 2140 East Bank Drive, Peterborough,
ON, Canada K9J 7B8
* Author for correspondence (e-mail: pmolnar{at}ualberta.ca)
Accepted 27 April 2009
| Summary |
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Key words: structure, storage, dynamic energy budgets, energy reserve, body fat, lean body mass, isotopic water dilution, bioelectrical impedance analysis, body condition index, nutritional status, Ursus maritimus
| INTRODUCTION |
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Several indices are routinely used to qualify mammalian body condition,
ranging from categorical indices that classify individuals on a fatness scale
(e.g. Lyver and Gunn, 2004
;
Stirling et al., 2008
;
Vervaecke et al., 2005
) to a
variety of continuous indices usually based on body mass and some measure of
length (e.g. Blackwell, 2002
;
Krebs and Singleton, 1993
;
Stevenson and Woods, 2006
).
Such indices may sometimes correlate with more direct measures of body
condition, such as the percentage lipid content of adipose tissue (e.g.
Stirling et al., 2008
) or the
combined mass of fat and skeletal muscle (e.g.
Cattet et al., 2002
), but they
cannot provide information on the amount of stored energy. Knowledge of
individual energy stores, however, can provide mechanistic and quantitative
insight into processes ranging from individual reproduction and survival to
population and ecosystem dynamics (Brown
et al., 2004
; Kleiber,
1975
; Kooijman,
2000
; Nisbet et al.,
2000
).
Body composition, and thus the amount of energy stored in body fat, may be
quantified by experimental methods, such as isotopic water dilution or
bioelectrical impedance analysis
(Speakman, 2001
). Water
dilution is expensive, requires prolonged immobilization of the study animal
and is impractical for large-scale field studies. Impedance analysis is less
time-consuming but has many error sources and requires extensive training to
obtain accurate measurements (Farley and
Robbins, 1994
; Parker,
2003
). Neither of these methods can be used to re-interpret
historic (mostly length and mass) data.
In the present study we develop a simple non-invasive method to estimate
energy stores in live-caught animals from mass and length data. Our approach
is based on dynamic energy budget theory, and relies on the concept that all
tissue may be characterized as either structure or storage
(Kooijman, 2000
). Storage
encompasses all materials that can be used as an energy source for growth,
maintenance and reproduction (e.g. non-structural lipids and proteins), plus
body water and ash associated with these materials. Structure consists of any
remaining tissue, body water and ash, and cannot be utilized for energy even
under extreme starvation (e.g. bones, brain, lungs, etc.). Some tissue belongs
partially to structure and partially to storage: muscle mass, for example, may
be accumulated when feeding and catabolized when fasting
(Atkinson et al., 1996a
;
Ryg et al., 1990
), but some
muscle is retained even when starving. We fully develop the method using polar
bears (Ursus maritimus Phipps) as an example, but all concepts are
general and the method is applicable to other species.
Polar bears provide a good case study, because they experience large
seasonal fluctuations in food supply and body condition, and depend on stored
energy for many aspects of their life history
(Derocher et al., 2004
;
Ramsay and Stirling, 1988
;
Stirling and Øritsland,
1995
). Pregnant females, for example, can fast up to eight months
during gestation and early lactation
(Atkinson and Ramsay, 1995
).
During this time all energy for survival, gestation and lactation must be
drawn from fat and nutrient stores, and insufficient energy stores can
negatively affect reproductive success
(Derocher et al., 2004
).
Furthermore, in the southern portions of the geographical range of this
species, bears are forced ashore in summer when the sea ice melts. Little or
no food is available on land and all bears rely on stored energy for survival
during a 4–5 month fasting period
(Derocher et al., 1993
;
Ramsay and Hobson, 1991
). Body
condition and, more specifically, energy stores thus become key variables in
polar bear population dynamics.
We first develop and parameterize a body composition model to estimate structural mass, storage mass, storage composition and storage energy of individual polar bears. Structural mass is estimated from straight-line body length, a morphometric measurement easily obtained in the field and readily available for previously handled individuals. Storage mass and storage energy are estimated from straight-line body length and total body mass. Furthermore, we apply the body composition model to estimate the metabolic rates of fasting adult polar bears from consecutive measurements of straight-line body length and total body mass only.
| MATERIALS AND METHODS |
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|
|
|---|
We first show how to estimate structural mass from an appropriately chosen
measure of length. In polar bears, straight-line body length (defined as the
dorsal straight-line distance from the tip of the nose to the end of the last
tail vertebra when the bear is lying in a sternally recumbent position) is a
natural choice for a measure of structural size, because this measure of
length is minimally affected by nutritional status and, furthermore, strongly
correlates with skeletal mass, which is a major part of structure
(Cattet et al., 2002
). We then
estimate storage mass as the difference between total body mass and structural
mass, and obtain storage energy from storage mass by accounting for storage
composition. State variables used in the model are summarized in
Table 1.
|
Model development
Total body mass, M, is by definition the sum of structural mass,
MSTR, and storage mass, MSTO (units:
kg):
![]() | (1) |
Structural mass is the product of structural volume,
VSTR (units: m3), and structural density,
STR (units: kg m–3). Due to the assumption of
isomorphic growth, VSTR is proportional to cubed
straight-line body length (Kooijman,
2000
). The relationship between structural mass and straight-line
body length (L) is therefore:
![]() | (2) |
To relate storage mass to storage energy, we need to account for storage
composition. Ignoring glycogen, a short-term energy source, we assume that
storage consists of fat (MSTO–F), protein
(MSTO–P), ash (MSTO–A) and
water (MSTO–W)
(Farley and Robbins, 1994
).
Storage mass then equals the sum of the masses of each storage constituent:
![]() | (3) |
Summarizing protein, ash and water in storage as non-structural lean (i.e.
fat-free) tissue, we write:
![]() | (4) |
![]() | (5A) |
![]() | (5B) |
![]() | (5C) |
W represents the proportion of lean body mass that is
water, and
P is the proportion of dry lean body mass that is
protein.
Because we aim to convert storage mass into energetic content, and only
protein provides an energy source from non-structural lean tissue, we use
Eqn 5A to rewrite
Eqn 4 as:
![]() | (6) |
F, and protein,
P (units: MJ kg–1), we rewrite
Eqn 6 as:
![]() | (7) |
The total energy content of storage, E, equals the sum of energy
in the fat and protein stores (i.e.
E=EF+EP). We define
as the proportion of total storage energy that is stored in body fat and
write:
![]() | (8A) |
![]() | (8B) |
![]() | (9) |
Inserting Eqn 2 and
Eqn 9 into
Eqn 1 yields the relationship
between total body mass, straight-line body length and storage energy:
![]() | (10) |
![]() | (11) |
![]() | (12) |
Moreover, storage composition is also specified by the body composition
model, and the respective proportions of storage mass that are fat, protein,
ash and water can be estimated from the following equations (see Appendix for
derivation):
![]() | (13A) |
![]() | (13B) |
![]() | (13C) |
![]() | (13D) |
Model parameterization
The model contains seven parameters
(Table 2), two of which
(
STR and k) relate straight-line body length to
structural mass. The remaining five convert storage mass into energetic
content. We used data from starved polar bears as well as literature data on
bear body composition for model parameterization, and introduce these data
more specifically when used. All bears were handled under the approval of
research permits that followed guidelines of the Canadian Council on Animal
Care. Data on two starving bears were collected by government agencies as part
of animal control actions for public safety. Statistical analyses were
performed in SYSTAT 10 (Systat Software, Chicago, IL, USA). Results were
considered significant at P
0.05. Means are presented ±
s.e.m.
|
The parameters
STR and k need not be estimated
separately, because only their product,
STRk,
determines the relationship between straight-line body length and structural
mass (cf. Eqn 2). To estimate
STRk, we used the body masses and straight-line body
lengths of two starving adult polar bears: a female (total body mass: 89.8 kg;
straight-line body length: 1.81 m; age
10 years) and a male (total body
mass: 163.3 kg; straight-line body length: 2.23 m; age: 7 years). Both bears
were in extremely poor condition, with empty stomachs, empty intestinal tracts
and no subcutaneous body fat. They were described as lethargic and the male
was hardly able to stand. We assumed that these bears had no (or only
negligible amounts of) storage energy left and set E=0. Body mass
then equals structural mass and Eqn
10 can be written as:
![]() | (14) |
STRk=15.14 kg m–3 for the female,
STRk=14.73 kg m–3 for the male, and
a mean estimate of
STRk=14.94 kg
m–3, which is used in all further calculations (the low
sample size used to estimate
STRk does not present a
major concern, cf. the Sensitivity analysis, Model validation and Discussion
sections below).
The body composition parameters
W and
P
have been estimated for black and brown bears as
W=0.734 and
P=0.835 (Farley and
Robbins, 1994
). No estimates exist for polar bears, so we adopted
these estimates for model parameterization in accordance with previous polar
bear body composition studies (Atkinson and
Ramsay, 1995
; Atkinson et al.,
1996a
). For modelling purposes, the energy densities of fat and
protein were assumed to be
F=39.3 MJ kg–1
and
P=18.0 MJ kg–1
(Schmidt-Nielsen, 1997
).
To estimate the remaining parameter,
, we rearranged
Eqn 10 as:
![]() | (15) |
. Straight-line body
lengths and adult female body fat were unreported in the respective tables so
we obtained these data from the authors
(Arnould, 1990
In polar bears, only a small fraction of body fat is structural [i.e. only
in cell membranes, the brain, and small depots in the eye sockets and foot
pads (Pond et al., 1992
)]. We
therefore simplified body composition in all further calculations by assuming
that all body fat belongs to storage. Fat measurements in Arnould and Ramsay
(Arnould and Ramsay, 1994
) and
Atkinson et al. (Atkinson et al.,
1996a
) thus provided estimates of storage fat masses. Two
measurements of storage fat mass, total body mass and straight-line body
length were available for each bear because each individual was sampled twice.
By inserting these estimates into Eqn
15 we obtained two estimates of
for each bear. No
systematic differences in
were observed within individuals, in
accordance with the strong homeostasis assumption. We therefore averaged both
estimates to obtain a single estimate of
for each individual.
Sex- and age-class had a significant effect on storage composition
(Kruskal–Wallis, H=14.61, P=0.006), with mean
highest in adult females (
=0.943±0.014), followed by yearlings
(
=0.941±0.006), subadult males (
=0.935±0.004),
cubs-of-the-year (
=0.899±0.011) and adult males
(
=0.885±0.007) (Fig.
1). Differences in storage composition may reflect sex- and
age-related differences in morphology
(Derocher et al., 2005
;
Stirling et al., 2008
;
Thiemann et al., 2006
) and
energy utilization (Atkinson et al.,
1996a
; Atkinson et al.,
1996b
), and significantly affect storage energy predictions (cf.
sensitivity analysis below). We therefore parameterized the body composition
model separately for all five sex- and age-classes, using the respective mean
estimates of
.
|
: regressing observations
against predictions and simultaneously testing for unit slope and zero
intercept (Mayer et al., 1994
,
(F2,60=11.81,
P<0.001). No such difference was found when using sex- and
age-class specific means (F2,60=0.65,
P=0.524). | RESULTS |
|---|
|
|
|---|
Structural mass can be estimated from straight-line body length (cf.
Eqn 2):
![]() | (16) |
![]() | (17) |
|
Storage energy can be estimated from total body mass and straight-line body
length (cf. Eqn 11). Predictive
equations for storage energy are presented separately for cubs-of-the-year
(C), yearlings (Y), adult females (AF), subadult males (SM) and adult males
(AM):
![]() | (18A) |
![]() | (18B) |
![]() | (18C) |
![]() | (18D) |
![]() | (18E) |
Although Eqn 18A,
18B,
18C,
18D,
18E are structurally the same,
their coefficients differ due to sex- and age-class specific differences in
storage composition. For example, comparing an adult female with an adult male
of equal body mass and length, we predict
1.34 times more storage energy
for the female (Eqn 18C,
E)
(Fig. 2C,D) due to the higher
relative fat content of storage. By contrast, the relationship between storage
energy, total body mass and straight-line body length differs little between
yearlings, adult females and subadult males (Eqn
18B,
18C,
18D), or between
cubs-of-the-year and adult males (Eqn
18A,
E), reflecting similarities in
storage composition.
|
59.76L3), an approximate upper bound to
total body mass. At this limit, body fat is estimated as 47.0% and 32.9% of
total body mass for adult females and adult males, respectively (from
Eqn 1 and
Eqn 13A), which is close to the
maximal relative body fat contents observed [females: 49%
(Atkinson and Ramsay, 1995
Model application: estimating metabolic rates
Here we show how the body composition model can be applied to estimate the
metabolic rate of fasting, resting, non-growing and non-reproducing polar
bears in a thermoneutral state, using straight-line body lengths and
consecutive measurements of total body mass only. Such bears expend storage
energy only for somatic maintenance, and storage energy decreases with a rate
of change proportional to the mass of tissue that requires maintenance
(Kooijman, 2000
). In dynamic
energy budget theory, these maintenance requirements are usually assumed to be
limited to structural mass (Kooijman,
2000
; Nisbet et al.,
2000
) whereas classical metabolic work relates changes in storage
energy to total body mass (Kleiber,
1975
). Both assumptions can be accommodated within the framework
presented here. However, for polar bears, we assume that both structural and
non-structural lean tissue requires maintenance, and that maintenance
requirements of body fat are negligible relative to those of lean tissue
(Aarseth et al., 1999
;
Atkinson and Ramsay, 1995
;
Boyd, 2002
;
Segal et al., 1989
). The rate
of change in storage energy is therefore given by the following differential
equation:
![]() | (19) |
Using Eqn 1,
Eqn 2,
Eqn 11 and
Eqn 13A to convert storage
energy and storage fat mass into functions of total body mass and
straight-line body length, and solving the resulting differential equation,
gives total body mass as a function of time t (see Appendix for
details):
![]() | (20) |
=(
)/
F represents the proportion of
storage mass that is fat (cf. Eqn
13A),
is a composite parameter given by
Eqn 12, and C is the
integration constant.
Given two measurements of body mass T time units apart,
M(0)=M0 and
M(T)=M1,
Eqn 20 can be solved to obtain
the integration constant:
![]() | (21) |
![]() | (22) |
Sensitivity analysis
Small sample sizes for model parameterization may have resulted in low
accuracy in determining the parameters
STRk and
. To understand how deviations in these parameters may affect storage
energy predictions, we varied them one at a time, while holding the other
constant at either
or at
(the across sex- and age-class mean of
). We then calculated
(E–
)/
, the resultant
proportional change in storage energy E relative to
,
the storage energy of an individual of equal body mass and length, whose
structural mass and storage composition are specified by
kg m–3 and
, respectively.
The proportional change in storage energy
(E–
)/
between two individuals
of equal body length, body mass and structural mass (specified by
) but differing storage
composition (specified by
and
, respectively)
is given by:
![]() | (23) |
), but differing structural mass (specified by
STRk and
, respectively), we obtain:
![]() | (24) |
represents the proportional increase or decrease in
STRk relative to
.
Storage energy is sensitive to storage composition and increases
monotonically with
(Fig.
3A). For instance, an average adult male (
=0.885) has 17.5%
less storage energy than an individual of equal body mass, length and
structure but with
. An average adult female
(
=0.943) of equal mass, length and structure has 10.6% more storage
energy than the reference individual with
.
The sensitivity of storage energy to
, and thus storage composition,
reflects the differing energy densities of body fat and lean tissue,
emphasizing the importance of body fat for energy storage and the need to
specify
as accurately as possible.
|
STRk (Fig.
3B). However, unlike in
, sensitivity depends on the ratio
between total body mass (M) and structural mass as specified by
and L
(Eqn 24). Sensitivity of storage
energy to
STRk is low for obese bears, increases with
decreasing storage mass and is greatest for starving bears. For instance, a
15% increase in
STRk results in a 15% decrease of
storage energy for a bear whose total body mass is twice its structural mass,
but only a 5% decrease in bears with total body mass four times their
structural mass. It is unlikely that we underestimated
STRk by more than 15%, because lean bears with
non-zero storage energy (E=0) have been observed where
M/L3 equals
1.15 times the current estimate of
STRk [A.E.D., unpublished data; cf. also the leanest
adult male in Atkinson et al. (Atkinson et
al., 1996a
STRk (cf. Eqn
14), so we limited sensitivity analyses to perturbations of
STRk not exceeding 15%.
Model validation
Full model validation is not possible because insufficient independent body
composition data exist to test model predictions. However, some tests of model
consistency for derived variables are possible using straight-line body
lengths and total body masses only. For this purpose, we obtained
straight-line body lengths and total body masses of 970 polar bears from
western Hudson Bay (all sex- and age-classes; N=505) and southern
Hudson Bay (cubs-of-the-year, yearlings, subadult and adult females;
N=465). For a description of the study populations, see Stirling et
al. (Stirling et al., 1999
)
and Obbard et al. (Obbard et al.,
2006
). Data were collected in 1989–1996 in western Hudson
Bay and in 1984–1986 and 2000–2005 in southern Hudson Bay. Total
body masses were determined by spring scale for cubs-of-the-year in spring
(±0.25 kg) and with a spring-loaded scale or an electronic load cell
otherwise (±0.5 kg). Females
4 and males
7 years old were
considered adults because polar bears in western Hudson Bay complete
structural growth at about 4 (females) and 6.5 (males) years of age,
respectively (Derocher and Stirling,
1998
). Females 2–3 years old and males 2–6 years old
were considered subadults. All capture and handling procedures were approved
annually by the Animal Care Committees of the Canadian Wildlife Service and
Ontario Ministry of Natural Resources.
We performed the following tests for model consistency. First, no bear should be lighter than its predicted structural mass. Second, estimated body compositions were compared against published body composition data. Third, estimates for storage mass and energy density were examined relative to qualitative expectations from polar bear physiology and life history. Fourth, metabolic rates were estimated for fasting adult males and compared with expected metabolic rates.
Structural mass and body composition
One implication of differentiating between structure and storage is that no
bear should be lighter than its structural mass. Our model fulfilled this
requirement for all bears regardless of sex, age or population
(Fig. 4): total body mass of
subadult and adult females ranged from 114% to 366% of their structural mass,
with a similar range for cubs-of-the-year (117–339%), yearlings
(120–317%) and subadult and adult males (115–321%). These ranges
correspond to bears with body fat constituting 7.7–45.6% of their total
body mass (adult females), 6.9–33.4% (cubs-of-the-year),
10.3–42.4% (yearlings) and 5.7–30.2% (adult males), respectively
(as estimated from Eqn 1 and
Eqn 13A). The variability in
observed body masses and estimated body fat corresponds to documented
variability in these state variables
(Atkinson and Ramsay, 1995
;
Pond et al., 1992
;
Watts and Hansen, 1987
),
largely due to seasonal changes in food availability. Upper estimates of
relative body fat content corresponded closely to previously observed maximal
values for both adult females [49%
(Atkinson and Ramsay, 1995
)]
and adult males [32% (Atkinson et al.,
1996a
)], and accordingly all bears were lighter than 4 times their
structural mass, which we considered an approximate upper bound to total body
mass.
|
Storage mass and energy density
Mean storage mass was smallest in cubs-of-the-year and increased
proportionally with structural mass (Fig.
5A,B), in accordance with patterns to be expected from
size-dependent energy acquisition and utilization
(Kooijman, 2000
). Males cease
growth later than females, and their asymptotic length exceeds that of females
(Derocher and Stirling, 1998
).
Mean structural mass is therefore largest in adult males, and so was mean
storage mass (Fig. 5A).
|
Variability in storage mass and energy density was large for all sex- and
age-classes, reflecting large seasonal fluctuations in food supply and
consequently body condition (Stirling and
Øritsland, 1995
; Watts
and Hansen, 1987
), as well as within-class differences in age and
reproductive status. Storage mass, for instance, was most variable in adult
males (Fig. 5A), probably
because males continue to accumulate body mass until
13 years old
(Derocher and Wiig, 2002
),
while structural growth is completed by
6.5 years of age. By contrast,
variability in energy density was largest in adult females
(Fig. 5C), where the
accumulation of body fat before pregnancy, an extended reproductive fast and
subsequent lactation demands result in large fluctuations in body condition
during a three-year reproductive cycle
(Arnould and Ramsay, 1994
;
Atkinson and Ramsay, 1995
;
Ramsay and Stirling,
1988
).
Metabolic rates
Adult males (N=13, ages
8 years) were measured and weighed
twice during the fasting season in western Hudson Bay. Measurements for each
bear were between 14 and 91 days apart and were obtained between late-July and
early-November. Fasting adult males in western Hudson Bay move little
(Derocher and Stirling, 1990
),
are in a thermoneutral state due to mild temperatures
(Best, 1982
) and have completed
structural growth (Derocher and Stirling,
1998
). We therefore assume that energy is solely expended for
somatic maintenance, and use Eqn
22 to estimate metabolic rates (m) from straight-line
body lengths and changes in total body mass. Metabolic rate estimates ranged
from 0.050 to 0.175 MJ per kg lean body mass per day (mean: 0.089±0.011
MJ kg–1 d–1).
Metabolic rates of these bears should by definition correspond closely to
their basal metabolic rates (Bligh and
Johnson, 1973
). However, a direct comparison between our metabolic
rate estimates and those predicted by Kleiber
(Kleiber, 1975
) is difficult.
We estimate the rate of energy expenditure relative to a unit mass lean
tissue, whereas Kleiber's law predicts the rate of energy expenditure relative
to a unit body mass, regardless of body composition. To compare our results
with Kleiber's predictions, we rescaled metabolic rate estimates for each bear
by multiplying m with the proportion of total body mass that is lean
tissue, (M–MSTO–F)/M, to
obtain the rate of energy expenditure relative to a unit body mass,
m*.
Estimates for m* ranged from 58% to 212% of the values
predicted by Kleiber's equation (mean: 107±9.0%), with
m* lower than predicted in 8 out of 13 males (range:
58–98%, mean: 76±3.1%). These results compare favourably with
previous measurements of polar bear resting metabolic rates, which were
reported as 73±8.5% relative to Kleiber's predictions for three adult
females under simulated denning conditions
(Watts et al., 1987
), as 107%
for two subadult males under similar conditions
(Watts et al., 1991
), and as
107±5.0% for pregnant and lactating females in maternity dens
(Atkinson and Ramsay, 1995
).
The higher metabolic rates found in the latter two studies indicate increased
energy expenditure towards growth and reproduction, respectively, and thus
basal metabolic rates consistent with those found here for the majority of
adult males, and those documented by Watts et al. for adult females
(Watts et al., 1987
).
Metabolic rates ranging from 141% to 212% of Kleiber's predictions (4 out of
13 males in the present study) suggest increased energy expenditure due to
movement, but these values still fall within predicted values for field
metabolic rates (Nagy et al.,
1999
).
| DISCUSSION |
|---|
|
|
|---|
The body composition model proposed in the present study provides
considerably more information on the energetic status of individuals than
currently available methods. Polar bears, for example, are routinely
classified on a subjective fatness scale from 1 to 5 as a measure of their
body condition (Stirling et al.,
2008
). This method is simple but suffers from low resolution and
potential misclassifications and inconsistencies from intra- and
inter-observer variability. For instance, assuming equal body composition, two
bears of equal mass and length should always receive the same fatness rating,
a condition that was frequently violated in our study populations for all sex-
and age-classes, and particularly for cubs-of-the-year and yearlings
(Fig. 4). Alternatively, an
objective and continuous body condition index based on standardized residuals
from regressing body mass against straight-line body length is available for
polar bears (Cattet et al.,
2002
). However, unlike our method, neither the subjective fatness
index nor the body condition index proposed by Cattet and colleagues can
provide estimates of structural mass, storage mass or storage energy.
Experimental methods, like isotopic water dilution and bioelectrical
impedance analysis, can estimate the energetic content of body fat but will
underestimate storage energy because body fat constitutes only part of
storage. The energetic content of non-structural lean tissue cannot be
estimated by these two techniques without supplemental use of a body
composition model, because they cannot differentiate between structural and
non-structural lean tissue. Furthermore, our method provides several practical
advantages over isotopic water dilution and bioelectrical impedance analysis.
Unlike impedance analysis it does not require extensive training to collect
the necessary data and is not affected by error sources like depth of
anaesthesia, limb and electrode positioning, or previous injuries of the bear
(Farley and Robbins, 1994
).
Unlike water dilution our method is quick, inexpensive, non-invasive and does
not require laboratory analyses. However, the parameterization of our model
relied heavily on body composition data obtained by isotopic water dilution,
and new data would help to validate and refine the model. We therefore
recommend our method as a supplement to these techniques.
In fact, the accuracy of the presented polar bear model is currently
limited by the low sample size of bears that was available for model
parameterization. Although the model performed well for a variety of life
history and physiological traits, model analysis revealed high sensitivity of
storage energy predictions to the storage composition parameter
. This
sensitivity is not a model artefact but reflects the differing energy
densities of body fat and lean tissue, emphasizing the necessity to estimate
as accurately as possible. Many factors could affect storage
composition, including season, age, or reproductive status of females, but we
had insufficient data to determine covariates for
other than the
proposed sex- and age-classes. Model refinements should therefore be attempted
as more data become available.
The sample size of two starved bears to estimate the structural mass
coefficient
STRk does not present a major concern for
storage energy predictions. The coefficient
STRk
usually varies little within species
(Kooijman, 2000
) (cf. also the
individual estimates for the two starving bears used to parameterize
STRk), and sensitivity of storage energy to
STRk is generally low
(Fig. 3). Furthermore, model
predictions of structural mass using the current estimate of
STRk proved robust for 970 polar bears of all sex-
and age-classes from two populations (Fig.
4). The sensitivity of storage energy to
STRk for very lean bears does not affect the
usefulness of our model because few bears reach such poor body condition (e.g.
94.7% of sampled polar bears were heavier than 1.5 times estimated structural
mass).
In some ways, model parameterization, validation and refinement may be
easier in small mammals. However, in general, our approach is applicable
across taxa and could provide the unifying approach Stevenson and Woods called
for in their recent review on body condition indices
(Stevenson and Woods, 2006
).
For instance, they note the diversity of measures used across species,
difficulties to interpret units in many currently used indices and the lack of
an underlying framework to model changes in body condition. Our method
provides a mechanistic approach towards body condition, yields easily
interpretable state variables, allows considering mammals within a dynamic
energy budget modelling framework
(Kooijman, 2000
;
Nisbet et al., 2000
) and thus
a mechanistic understanding of changes in body condition. In polar bears, for
example, the body composition model together with a dynamic energy budget
model could allow a mechanistic understanding of documented declines in body
condition, reproduction and survival, thought to result from climate change
associated reductions in sea ice and feeding opportunities
(Obbard et al., 2006
;
Regehr et al., 2007
;
Stirling et al., 1999
). Energy
density may hereby provide a natural measure of body condition, because it
relates available storage energy to the mass of tissue that requires energy
for somatic maintenance (Ross and Nisbet,
1990
).
The outlined modelling approach improves our understanding of individual bioenergetics, and could be used to link energy flow in the environment to individual body condition, survival, growth and reproduction, not just in polar bears but in many species that rely on stored energy for aspects of their life history. As the method utilizes commonly measured length and mass data, it could also be used to distinguish trends in long-term historic datasets, such as those caused by climate change and other anthropogenic influences.
| APPENDIX |
|---|
|
|
|---|
F and
P):
![]() | (A1A) |
![]() | (A1B) |
![]() | (A2A) |
![]() | (A2B) |
![]() | (A3A) |
![]() | (A3B) |
–1E for MSTO
(Eqn 9) in Eqn A3 yields
Eqn 13A and
Eqn 13B.
2. Equations 13C and 13D
By combining Eqn 5A with
Eqn 5B and
Eqn 5C, respectively, we rewrite
the masses of storage ash (MSTO–A) and storage water
(MSTO–W) as:
![]() | (A4A) |
![]() | (A4B) |
![]() | (A5A) |
![]() | (A5B) |
Derivation of Equation 20 (decline in body mass over time)
Here we provide the derivation of Eqn
20, which describes total body mass (M) as a function of
time (t) for fasting, resting, non-growing and non-reproducing polar
bears in a thermoneutral state.
For such bears, the rate of change in storage energy (E) was given
by the differential equation:
![]() | (A6) |
![]() | (A7) |
![]() | (A8) |
![]() | (A9) |
![]() | (10) |
![]() | (A11) |
=(
)/
F,
representing the proportion of storage mass that is fat (cf.
Eqn 13A). Solving Eqn A11 (a first-order, non-homogeneous linear differential equation) gives total body mass M as a function of time t as described by Eqn 20.
| Footnotes |
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