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First published online February 15, 2006
Journal of Experimental Biology 209, 845-859 (2006)
Published by The Company of Biologists 2006
doi: 10.1242/jeb.02064
The effects of depth, temperature and food ingestion on the foraging energetics of a diving endotherm, the double-crested cormorant (Phalacrocorax auritus)
1 Centre d'Ecologie et Physiologie Energétiques, CNRS, 23 Rue
Becquerel, F-67087 Strasbourg Cedex 2, France
2 Department of Zoology, University of British Columbia, 6270 University
Boulevard, Vancouver, British Columbia, Canada V6T 1Z4
* Author for correspondence (e-mail: manfred.enstipp{at}c-strasbourg.fr)
Accepted 22 December 2005
| Summary |
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Key words: diving energetics, depth, double-crested cormorant, temperature, HIF, heat loss
| Introduction |
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One factor, however, that has received little attention in most studies
investigating the energetic costs of diving in endotherms is dive depth. In
avian divers, the increase in ambient pressure when diving to depth will
decrease the amount of air trapped within the plumage. The consequences are
twofold: (1) a decrease in buoyancy and, in turn, lower mechanical costs of
underwater locomotion and (2) a reduction in thermal insulation. At 10 m
depth, all air spaces will be reduced to half the surface volume, reducing
insulation from air trapped within the plumage. The resulting increase in heat
loss might outweigh any energetic advantages that might accrue from a
decreased buoyancy at greater depth, especially if water temperature is low.
We are only aware of one study to date that investigated the energetic
consequences of diving to depth. De Leeuw found that dives to 2.2 and 5.5 m
depth were equally costly in tufted ducks (Aythya fuligula)
(De Leeuw, 1996
). One possible
explanation could be that, since the depth range covered in the study was
rather small, the energetic savings in mechanical costs with an increase in
depth (reduced buoyancy) were balanced by an increase in thermoregulatory
costs. Hence, how depth shapes the energetic costs associated with diving
still remains unclear.
Double-crested cormorants (Phalacrocorax auritus Lesson) are
foot-propelled pursuit divers that forage on benthic and pelagic fish. They
target their prey in the upper part of the water column [depth range observed
= 1.57.9 m (Ross,
1974
)] in coastal and freshwater ecosystems. Owing to a partially
wettable plumage (Grémillet et al.,
2005a
), buoyancy is reduced in cormorants when compared with many
other avian divers [2.7 N kg1 at the surface for P.
auritus (Lovvorn and Jones,
1991a
)], lowering mechanical costs during diving. The accompanying
reduction in thermal insulation makes cormorants susceptible to substantial
heat loss, especially when diving in cold water. Hence, it is generally
believed that diving is very costly in cormorants when compared with other
avian divers (see table 1 in Enstipp et
al., 2005
). Grémillet et al. used a model integrating the
effects of water temperature and dive depth on energy expenditure during
diving to estimate the energetic costs of great cormorants (Phalacrocorax
carbo carbo) during foraging
(Grémillet et al.,
2001
). They calculated that dive costs will vary between 28 and 64
W kg1 [i.e. 921 times resting metabolic rate (RMR)
(Schmid et al., 1995
)] when
diving in shallow/warm water and deep/cold water, respectively. This has led
to the suggestion that poor insulating properties of their plumage and the
resulting high foraging costs might be a limiting factor for the geographic
distribution of cormorants (Gaston,
2004
). However, great cormorants winter in the Arctic and spend
considerable time foraging in almost freezing water
(Grémillet et al.,
2005c
). Similarly, European shags (Phalacrocorax
aristotelis) spend up to 7 h per day foraging in water temperatures of
56°C in Scotland (Daunt et
al., 2006
). If foraging costs in cormorants are as high as
expected, then their required daily food intake (DFI) should be high compared
with that of other seabirds. However, Grémillet et al. estimated the
DFI for great cormorants to be similar to the required intake of other,
well-insulated seabirds of comparable mass
(Grémillet et al.,
1999
). Moreover, dive costs of European shags diving in a shallow
trench have recently been measured and were considerably lower than previous
measurements for great cormorants. Dive costs of shags were, in fact, similar
to those of other foot-propelled divers and this has led to the suggestion
that dive costs might be overestimated in cormorants
(Enstipp et al., 2005
). The
depth range exploited by cormorants in the wild and their unique morphological
features (partially wettable plumage, which reduces buoyancy but also reduces
plumage insulation) make them a very interesting model to investigate the
energetic consequences of diving to depth within the constraints of a captive
setting.
Beyond these physiological considerations, measurements of
activity-specific metabolic rates and the evaluation of modifying factors are
of great importance for the calculation of timeenergy budgets. These
allow detailed estimates of individual and population energetic requirements
of seabirds, which are urgently needed for management purposes (Enstipp et
al., 2006; Boyd, 2002
). Hence,
to gain a detailed understanding of cormorant energetics we studied the
energetic costs of double-crested cormorants associated with (1) resting in
air, (2) resting in water and (3) diving. To study the importance of modifying
factors, we altered air temperature, water temperature, diving depth and
feeding status. The hypothesis that diving to depth will increase dive costs
in cormorants compared with shallow diving was tested. Also, since mechanical
and thermoregulatory costs develop in opposite directions during deep diving,
we predicted that the expected increase in dive costs during deep diving would
be less than projected from heat loss considerations alone.
| Materials and methods |
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Respirometry system
Oxygen consumption rates
(
O2) were
measured using an open-circuit respirometry system (Sable Systems, Henderson,
NV, USA). To measure the metabolic rate during diving, we used a transparent
Plexiglas dome in the shape of a truncated pyramid as a respiration chamber
(0.6 m long x 0.6 m wide x 0.4 m high; volume 50 litres), which
was partially immersed and received outside air through small holes on its
four sides just above the waterline. Similarly, to measure metabolic rate
during resting in air, we used a 55-litre bucket (0.35 m diameter x 0.65
m high) with an airtight Plexiglas lid, and air was drawn in via four
small side holes near its bottom. Air from the respiration chambers was fed
directly into the laboratory, which was set up inside a hut adjacent to the
dive tanks (Fig. 1). The main
airflow from the respiration chamber was dried using silica gel before being
led into a mass-flowmeter (Sierra Instruments Inc., Monterrey, CA, USA), which
automatically corrected the measured flow to STPD (273 K and 101.3 kPa). A
sub-sample of 10 l min1 was bled into a manifold from which
an oxygen (paramagnetic O2-analyser PA-1B, Sable Systems;
resolution 0.0001%) and CO2 analyser (Beckman LB2 Medical
CO2-analyser, Schiller Park, IL, USA; resolution 0.01%) sampled in
parallel. All connections between the various components of the respirometry
system were made with gas-impermeable TygonTM tubing.
Air flow through the respiration chamber was maintained at
10 l
min1 during the resting-in-air trials, at
45 l
min1 during the resting-in-water trials and at
80 l
min1 during the dive trials using a vacuum pump (Piston
pump, Gast Manufacturing Inc., Benton Harbour, MI, USA). Oxygen concentration
inside the respiration chamber was above 20.5%, and CO2
concentration was below 0.4% during all trials. The gas analysers were
calibrated before each trial using 99.995% pure N2, 1.03%
CO2 (PraxAir, Richmond, BC, Canada) and outside air (set to 20.95%
O2 and 0.03% CO2). Analyser drift was minimal but, if
any occurred, it was corrected for during data analysis. Before a trial, the
entire system was tested for leaks by infusing pure N2 gas. Time
delay between air leaving the respiration chamber and arriving at the
gas-analysers was calculated by dividing the total volume of the tubing and
drying columns by the flow rate. The delay was found to be 18 s (resting in
air) and 11 s (resting in water and diving) for the oxygen analyser and 21 s
(resting in air) and 11 s (resting in water and diving) for the CO2
analyser. These delay times were taken into account when calculating
O2 and
CO2 and relating
them to diving events. The time constants of the respiration chambers were
calculated to be 5.5 min for resting in air, 67 s for resting in water and
37.5 s for diving. Data from the flowmeter and the gas analysers were fed into
a universal interface (16 bits resolution, Sable Systems) and average values
were recorded every 1 s (resting in water and diving) or 5 s (resting in air)
onto a desktop computer using Datacan (Sable Systems).
Resting metabolism
Basal metabolic rate (BMR) was measured during the day (08.0018.00
h) while birds were resting, post-absorptive and within their thermo-neutral
zone (mean air temperature was 22.1±1.7°C; range
18.325.4°C; lower critical temperature for our birds, calculated
after the equation given by Ellis and
Gabrielsen, 2002
, should be 89°C). Birds were fasted
overnight (for at least 15 h) before being placed inside the metabolic
chamber. After the initial disturbance, birds calmed down quickly and sat
quietly in the darkened chamber for the remainder of the trial. A stable
O2 was typically
reached within the first hour of these 35 h-long trials. Air
temperature in the respiration chamber was monitored using a digital
thermometer (Oregon Scientific, Portland, OR, USA) and usually did not differ
from outside air temperature by more than ± 2°C. Birds were
familiarized with the procedure on at least three occasions before data
collection began. BMR was determined from at least three trials per bird. To
investigate the effect of air temperature on resting metabolism, measurements
were also conducted at various temperatures ranging from 6 to 25°C.
Resting in water
The metabolic costs associated with resting in water were measured in
separate trials during which birds floated calmly inside the dome, on the
water surface of the shallow dive tank. A metal grid mounted about 30 cm below
the base of the respiration chamber prevented birds from submerging. After the
initial disturbance, when introduced into the chamber, birds calmed down
quickly and a stable
O2 was typically
established within 10 min. Trials lasted 30 min, during which undisturbed
birds were observed from inside a hut through a tinted glass window
(Fig. 1A). Birds were
familiarized with the procedure on at least three occasions before data
collection started. To investigate the effect of water temperature on
metabolic rate when resting in water, we conducted trials in water
temperatures ranging from 7.8 to 15.6°C. The effect of feeding (heat
increment of feeding, HIF) on the metabolic rate during resting in water was
investigated in specific trials when birds were fed a known amount of food (60
g of herring) at various times (30120 min) before a trial. Mean water
temperature during these trials was 14.6°C (range
13.515.8°C).
Diving metabolism
Diving metabolic rate was measured in all birds during shallow and deep
diving at water temperatures ranging from 6.1 to 17.5°C. Water temperature
was measured 10 cm below the surface after each set of trials. At the
beginning of a trial a bird was captured, weighed and placed inside the
respiration chamber. A trap door at the bottom of the dome prevented the bird
from submerging directly. When the bird floated calmly and a stable
O2 was
established (usually within 510 min) the trap door was opened through a
remote pulley system, and diving activity began. During a trial, birds dived
continuously to the opposite end of the shallow dive tank or to the bottom of
the deep dive tank. Through the tinted glass window in the laboratory hut
(Fig. 1) it was possible to
observe the surface behaviour of the birds without causing any disturbance. To
monitor the behaviour of birds underwater, submersible cameras (Lorex,
MBrands, Scarborough, ON, Canada) were positioned within the tanks and
connected to a multiplexer (EverFocus Electronics Corp., Taipei, Taiwan) and a
video monitor inside the hut. This was especially important in the deep dive
setting, where dives were classified as deep (diving to the bottom) or shallow
(diving to less than 3 m depth). Birds typically started a dive bout with an
exploratory shallow dive before performing a series of deep dives to the
bottom of the tank. Similarly, they terminated a deep diving bout by either
remaining at the surface or by switching back to shallow diving. To avoid a
mixture of shallow and deep dives within a deep dive trial as much as
possible, the trap door was closed, preventing birds from submerging, as soon
as it became apparent that birds would not return to depth. Deep dive trials
during which birds spent more than 30% of the overall time spent submerged at
shallow depths were excluded from the analysis. All relevant behaviour of the
birds was marked onto the respirometry traces, so that behaviour as well as
dive and surface events could be related to the respirometry recordings. The
majority of shallow dive trials lasted
2030 min, during which
birds dived voluntarily and without any interference. Here, a trial was
terminated by remotely closing the trap door when a bird remained at the
surface for more than 10 min. In the deep dive setting, birds were not
motivated to dive to the bottom of the tank unless food was placed there.
Hence, birds ingested small herring pieces during all deep dive trials.
Preliminary results from experiments during which cormorants were fed a
similar amount of herring while resting in air showed that metabolic rate was
not increased during the first 10 min after ingestion (M. R. Enstipp, D.
Grémillet and D. R. Jones, unpublished data). Consequently, the
duration of deep dive trials was kept within this time frame. Therefore,
`post-absorptive deep dive trials' refers to trials where birds had been
fasted overnight (at least 15 h) beforehand but ingested small amounts of
herring during the trial.
To investigate the effect that feeding (HIF) might have on diving metabolic rate, dive trials were conducted in both the post-absorptive and absorptive state. For the absorptive trials, birds were fed a known amount of food (60 g of herring) at various times (30150 min) before a trial. Trials were conducted in the mornings and afternoons with a maximum of two dive trials per bird per day.
Stomach temperature
In parallel with the respirometry measurements, temperature loggers
(MiniTemp-xl, earth&OCEAN Technologies, Kiel, Germany; length 70 mm,
diameter 16 mm, mass 25 g, resolution 0.03K) were employed for all birds to
measure stomach temperature during the dive trials and when birds rested in
water. Stomach temperature should reflect abdominal body temperature during
post-absorptive trials if no food is ingested. Temperature loggers were
programmed to record stomach temperature every 10 s and were fed to the birds
inside a herring. The loggers were equipped with a spring crown and were not
regurgitated by the birds but retrieved when the memory was filled, after
about 10 days (Wilson and Kierspel,
1998
). After retrieval, the data were downloaded onto a laptop
computer, and the logger was cleaned, re-programmed and re-fed to the
bird.
Plumage air volume
To determine body insulation and allow comparison with other cormorant
species, we measured the total plumage air volume in six bird carcasses (mean
body mass 2.04±0.35 kg) according to previously published methods
(Grémillet et al.,
2005a
; Wilson et al.,
1992b
). The only difference in our assessment was that we
collected the water displaced by the submerged carcass in a beaker and
determined its volume using a precision balance, assuming a density of 0.9982
g ml1 for water at 20°C.
Stroke frequency and work against buoyancy
Underwater filming allowed the calculation of stroke frequencies (strokes
s1) during diving as an indicator of locomotor effort. For
deep (vertical) diving, we calculated stroke frequencies during descent (near
top and near bottom) and bottom phase, while for shallow (horizontal) diving
it was calculated for a position about halfway along the shallow dive tank. To
this end, we recorded the video signal together with the signal of a video
date time generator (RCA, resolution 0.1 s) onto VHS tape. Video analysis was
performed on 10 sequences per bird for each category by counting the total
number of strokes per sequence and dividing by the time elapsed. Duration of
selected sequences ranged between 1 and 5 s. We also estimated the mechanical
work conducted against buoyancy during deep (vertical) and shallow
(horizontal) diving. To this end, we calculated the buoyancy of a 2.1 kg
cormorant at the surface by adding the buoyancy of the respiratory system, the
plumage and body tissues. We estimated the air volume in the respiratory
system from the equation given by Lasiewski and Calder
(Lasiewski and Calder, 1971
)
(Vresp=0.1608Mb0.91), where
Mb is body mass, and used our measurement of plumage air
volume. The buoyancy of air was taken as 9.79 N l1, and the
buoyancy of body tissues as 0.659 N kg1
(Lovvorn et al., 1999
). During
descent, hydrostatic pressure increases at a constant rate of 10 kPa
m1 of depth, so that the air volume decreases by a factor of
10/(n+10), where n is depth in metres. By contrast, the
buoyancy of body tissues does not change with water depth
(Lovvorn et al., 1999
).
Mechanical work per second (W, in Joules) against buoyancy during
descent in deep (vertical) dives was calculated as:
![]() | (1) |
10 s to reach the tank bottom (10 m); hence, we assumed a
vertical descent speed of 1 m s1 to model the changes in
mechanical work against buoyancy during descent. To calculate the work against
buoyancy during shallow (horizontal) diving, we assumed that birds swam at a
depth of 1 m (which was typically observed, apart from the very short periods
of descent and ascent). The distance (Ds) that a bird
would float upward during the stroke cycle duration (t) and that has
to be offset by the bird is given by:
![]() | (2) |
Data analysis and statistics
In a preliminary analysis, oxygen consumption rates
(
O2) were
calculated using equation 3b given by Withers
(Withers, 1977
), which
indicated a respiratory exchange ratio (RER) of 0.73 in post-absorptive birds
resting in air. However, during some of the dive trials, these values seemed
unreasonably low, probably because CO2 was absorbed by the water or
because of non-pulmonary CO2 loss by our birds
(Walsberg and Wolf, 1995
).
Hence, for our analysis, we assumed a RER of 0.71 for all
post-absorptive trials and 0.8 for all absorptive trials and used equation 3a
from Withers (Withers, 1977
)
to calculate
O2.
Metabolic rate during resting in air was calculated from the lowest 15-min
running average value of
O2. Similarly,
metabolic rate during resting in water was taken as the average from the
lowest and stable 10 min section of
O2 from each 30
min trial. Our respirometry system was sufficiently fast to allow separation
of individual dive and surface events. However, since we were interested in
obtaining an estimate of the energetic costs associated with foraging
activity, we decided to calculate diving metabolic rate (MRd) as
the average value of
O2 during a dive
bout from its start until 30 s after the last dive in a bout:
![]() | (3) |
tdive and
tsurface are
the sum of all dive and surface durations in a dive bout, respectively. A dive
bout was characterised by continuous diving activity and ended, by definition,
when birds remained at the surface for longer than 100 s [using a
log-survivorship plot as bout ending criterion
(Slater and Lester, 1982
O2/60Mb
for post-absorptive trials and by
20.1
O2/60Mb
for absorptive trials, where Mb is in kg and
O2 is in ml
O2 min1. We removed the effects of body mass on
metabolic rate following Packard and Boardman
(Packard and Boardman, 1999Stomach temperatures were analysed using Multitrace (Jensen Software Systems, Laboe, Germany). Resting values during the night and day were established from periods when birds were calm. Temperature recordings were averaged over a period of 6 h during the night (between 23.00 h and 05.00 h) and over periods of at least 2 h during the day (between 08.00 h and 18.00 h). The average day temperature (`day avg') was taken as the mean stomach temperature during the hours of daylight (from sunrise to sunset). Stomach temperatures during the various phases of the dive and resting-in-water trials were taken as averages from the first and last minute of a trial (`start' and `end', respectively), as the single highest value during a trial (`peak') and as the entire trial average. We included only stomach temperature recordings from birds that had not ingested food for at least 3 h in our analysis (with the exception of `day avg' temperature), to exclude periods of decreased stomach temperature after food ingestion.
Thermal conductance (TC) was calculated when cormorants rested in
air and water and during shallow and deep diving (post-absorptive trials only)
using the following equation:
![]() | (4) |
Two-way repeated measures analysis of variance (ANOVA) with Tukey pairwise
multiple comparisons was used for comparison of metabolic rate during
different activities at various temperatures. To investigate the effect of
depth, water temperature and feeding status on cormorant diving metabolic rate
we used a repeated measure ANOVA on three factors. When single comparisons
were made, Student's paired t-test was used. The relationships
between energy expenditure/thermal conductance and air or water temperature
for the various conditions (Table
2) that take into account variability between subjects were
determined using repeated-measures multiple linear regression, with each bird
being assigned a unique index variable
(Glantz and Slinker, 1990
).
Analysis of covariance (ANCOVA) was used to compare these different
relationships. Significance was accepted at P<0.05. All mean
values are presented with standard deviation (±1 s.d.).
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| Results |
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Temperature had a significant effect on the metabolic rate of cormorants during all activities (P<0.001, F=96.24). Resting in air at an air temperature around or below their lower critical temperature significantly elevated metabolic rate (Fig. 2; mean air temperature during `cold' air trials: 8.6±1.1°C). When resting or diving in `cold' water, the metabolic rate of cormorants was significantly increased when compared with the respective `warm' water trials (Table 1; Figs 2, 3). In all cases, there was a significant negative relationship between metabolic rates of double-crested cormorants during different activities and temperature, which allowed the calculation of linear regression equations (Table 2; Fig. 3). ANCOVA comparisons revealed that the slope of these relationships for all activities in water were not significantly different from each other (P=0.43, F=0.96), while the intercepts were significantly different (P<0.001, F=42.47). However, slope and intercept for `resting in air' were significantly different from those of all other activities (P<0.001 for all comparisons, F-values between 25 and 1379).
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Diving to depth was energetically more costly than conducting shallow (horizontal) dives (Figs 2, 3). Again, this difference was significant when comparing shallow (horizontal) and deep (vertical) diving while accounting for water temperature and feeding status (P<0.001, F=83.36).
While metabolic rate was increased after feeding, this increase was not significant when the effects of temperature and activity were accounted for (P=0.072, F=5.15). In other words, metabolic rates in absorptive and post-absorptive trials during a particular activity (e.g. shallow diving) and at a particular temperature (e.g. `warm') were not significantly different from each other (Fig. 2). Furthermore, ANCOVA comparisons showed that the relationship between energy expenditure and water temperature (Table 2) was not significantly different between post-absorptive and absorptive trials during shallow (intercept, P=0.055; slope, P=0.18) and deep diving (intercept, P=0.06; slope, P=0.54). However, metabolic rates during all absorptive trials were increased by about 58% above the post-absorptive level within 30 min after feeding and remained elevated for at least 2 h.
The various factors investigated in our study (activity, temperature, depth, feeding status) were interactive and additive. While diving was more costly than resting (in water and air), descending to depth increased the energetic expenses even more. Ingesting food and decreasing water temperatures further increased the energy expenditure of cormorants. As can be seen in Table 1 and Fig. 2, the highest energy expenditure observed was during deep diving in cold water after food ingestion (absorptive), when metabolic rate increased by a factor of 6.4xBMR.
Dive durations of birds were similar for shallow and deep diving. Surface duration, however, was significantly shorter during deep diving (P=0.019, t=3.42,) resulting in a higher dive/pause ratio (Table 1). Similarly, the fraction of the dive cycle (dive and succeeding surface interval) spent underwater was higher during deep diving (60.4%) than during shallow diving (53.2%).
Stroke frequency during the early descent phase of deep dives
(3.42±0.25 strokes s1) was significantly elevated
when compared with all other phases during deep and shallow diving
(P<0.001, F=98.98;
Fig. 4A). Stroke frequency
declined with increasing depth and reached values similar to the horizontal
shallow dive situation at a depth of
10 m
(Fig. 4A). Inaccordance with
the changes in stroke frequency, glide duration between strokes increased with
increasing depth. Calculated mechanical work against buoyancy declined
considerably with depth during the descent phase of deep (vertical) dives,
ranging from 5.3 J s1 near the surface to 2.2 J
s1 at 10 m (Fig.
4B). Assuming a vertical descent speed of 1 m
s1, the cumulative mechanical work against buoyancy during
descent (10 s) would be 35.1 J. During shallow (horizontal) diving, work
against buoyancy was calculated to be 2.9 J s1, which would
result in a total of 28.6 J during an equivalent 10 s period. However, while
birds during shallow (horizontal) diving continued to stroke throughout a
dive, birds within the deep dive tank ascended passively (after a brief bottom
period) without further locomotor effort. As a consequence, total mechanical
work against buoyancy during a 20 s dive was calculated to be 57.2 J during
shallow (horizontal) diving and 36.4 J during deep (vertical) diving.
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Total plumage air volume of six double-crested cormorant carcasses was 0.13±0.04 l kg1.
| Discussion |
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Resting in air
Over the temperature range investigated in our study (625°C),
metabolic rate of cormorants increased slowly with a decline in air
temperature (Fig. 3;
Table 2). However, while
metabolic rate was relatively stable between 25 and 10°C, it increased
more rapidly at air temperatures below 10°C. Unfortunately, we were not
able to manipulate air temperature and take measurements below 6°C, so
that we could not unequivocally demonstrate the presence of a lower critical
temperature (calculated to be 89°C).
Resting in water
Resting in water increased metabolic rate of double-crested cormorants by a
factor of 2.4x and 3.2xBMR for `warm' and `cold' water,
respectively (Table 1). This is
considerably lower than that previously reported for great cormorants
[4.5xRMR (Schmid et al.,
1995
)] and European shags [4.1xBMR
(Enstipp et al., 2005
)] but
similar to Brandt's cormorants (Phalacrocorax penicillatus) resting
in 20°C water during the day and at night [2.5x and 1.6xBMR,
respectively (Ancel et al.,
2000
); BMR predicted from Ellis and Gabrielsen
(Ellis and Gabrielsen, 2002
)].
Heat loss when resting at the water surface will be less than during diving,
because the surface area exposed to water is smaller in the former. However,
when resting in water, the temperature effect on metabolic rate was even
stronger than during diving. Metabolic rate increased by
35% within the
temperature range tested (Table
1), resulting in the steepest regression slope
(Table 2; Fig. 3). This indicates that
birds might be able to use some of the heat generated by muscle activity
during diving to compensate for the heat loss in cold water. Inactive birds
floating at the surface, however, will have to spend additional energy for
thermoregulation. Similar patterns have been observed in other avian divers,
like tufted ducks (Bevan and Butler,
1992
) and macaroni penguins (Eudyptes chrysolophus)
(Barré and Roussel,
1986
). In 6°C water, body temperature of macaroni penguins
dropped when birds remained inactive at the water surface but remained stable
in birds that swam or dived (Barré
and Roussel, 1986
). While stomach temperature in our cormorants
remained stable during both diving and resting in water, mean stomach
temperature when resting in water was significantly lower than during diving
(Fig. 5), indicating that
overall heat production was greater during diving. A strong temperature
dependence of metabolic rate in birds floating on water was also observed in
tufted ducks (Bevan and Butler,
1992
; de Leeuw,
1996
), common eiders (Somateria mollissima)
(Jenssen et al., 1989
), common
murres (Uria aalge) and thick-billed murres (Uria lomvia)
(Croll and McLaren, 1993
) and
little penguins (Eudyptula minor)
(Stahel and Nicol, 1982
).
Dive behaviour
Dive patterns displayed by the cormorants in our study
(Table 1) were similar to
patterns observed in double-crested cormorants foraging in the wild. Ross
(1974
) reported mean dive and
surface durations for double-crested cormorants of 25.1 s and 10.3 s,
respectively, when foraging in water 1.57.9 m deep. In our study,
surface durations between consecutive shallow dives were longer than after
deep diving, resulting in a higher dive/pause ratio during deep diving. This
would indicate that birds dived more efficiently during deep diving since
potential underwater foraging time was increased. However, surface duration
after shallow diving was variable (see
Table 1) and might be explained
by a difference in motivation (birds were feeding on small herring pieces
during deep diving but not during shallow diving). In support of this, Enstipp
et al., working with the same individuals diving for food within both tanks,
found that surface duration was greater after deep dives
(Enstipp et al., 2001
), as one
might expect.
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Our study also shows that dive costs in double-crested cormorants are
similar to those of other avian divers
(Fig. 7). While dive costs in
cormorants as a group tend to lie above the average relationship relating
diving metabolic rate to body mass in avian divers
(Fig. 7), this is most
noticeable in the great cormorant. To allow comparison between dive cost
measurements for different Phalacrocorax species, we removed the
effect of water temperature on diving metabolic rate by recalculating the dive
costs during shallow diving for a water temperature of 12.6°C (the water
temperature for P. carbo sinensis in
Schmid et al., 1995
). Our
analysis revealed that mass-specific metabolic rates for all three cormorant
species are very similar [P. auritus, 21.64 W kg1
(present study, Table 2);
P. aristotelis, 20.01 W kg1
(Enstipp et al., 2005
); P.
carbo carbo, 22.85 W kg1 (data from
Grémillet et al.,
2001
)]. These mass-specific values are considerably below the dive
costs previously reported for P. carbo sinensis by Schmid et al.
(31.40 W kg1) (Schmid et
al., 1995
) and are similar to other foot-propelled divers (table 1
in Enstipp et al., 2005
).
The effect of dive depth on diving metabolic rate
The observed increase in metabolic rate during deep diving, when compared
with shallow diving (Table 1;
Figs 2,
3), might be caused (1) by the
distinct increase in locomotor effort during early descent
(Fig. 4) or (2) by an increase
in heat loss as a consequence of the reduced insulative properties of the
plumage.
Mechanical costs
As indicated by stroke frequency, cormorants worked the hardest during the
early descent phase of deep dives (Fig.
4A). It is important here to consider the different body
orientation of birds when descending in the deep dive tank or when diving in
the shallow tank with no changes in depth. In the shallow tank, apart from the
very short submergence and emergence to and from
1 m depth, birds swam
horizontally (with a body angle of
0°, i.e. parallel to the surface),
comparable to the bottom phase of a deep dive (albeit at a greater buoyancy).
In the deep dive tank, however, birds swam almost vertically during descent
and ascent, with a body angle of about 70° and 70°,
respectively. The higher stroke frequency we observed during descent to depth
might therefore be explained by the greater mechanical work required to
overcome buoyancy during vertical descent to depth (5.3 J s1
near the surface; Fig. 4B),
when compared with shallow (horizontal) diving (2.9 J s1)
(see also Lovvorn et al.,
1991
; Lovvorn et al.,
2004
). The increased stroke frequency could also indicate that
birds submerged with a greater air volume within their respiratory system
during deep diving than during shallow diving. Respiratory movements were
clearly visible in preparation for deep dives (brief period of
hyperventilation), while this was not the case for shallow dives. Also, deep
dives were typically initiated with a pre-dive leap
(Wilson et al., 1992a
), which
rarely occurred at the onset of shallow dives. This could indicate that
cormorants regulate their respiratory air volume in accordance with the
anticipated dive depth, as has been suggested for other avian divers, namely
penguins (Sato et al., 2002
;
Wilson, 2003
).
In this context, it is interesting to note that Enstipp et al. reported
heart rates during deep dives of double-crested cormorants (same individuals,
identical set-up) that were significantly higher than during shallow
(horizontal) dives of similar duration
(Enstipp et al., 2001
).
Similarly, Froget et al. found that heart rate during the first 6 s of
submersion in king penguins (Aptenodytes patagonicus) was higher in
long (deep) dives than in short (shallow) dives
(Froget et al., 2004
). For the
cormorants, it was argued that compression hyperoxia during descent and an
assumed reduction in energetic costs associated with reduced buoyancy during
deep dives would delay a chemoreceptor-mediated decline in heart rate.
However, based on the suggestion by Sato et al. that king penguins inhale more
air prior to deep dives (Sato et al.,
2002
), Froget et al. argued that higher heart rates during the
beginning of deep dives might be explained by the greater effort necessary to
overcome an increase in buoyancy (Froget
et al., 2004
). The high stroke frequencies we observed during the
early phase of deep dives would point in the same direction and might have
contributed to the significantly higher energetic costs we measured during
deep diving. Seen in this light, the observed higher heart rates during deep
diving in cormorants (Enstipp et al.,
2001
) might be explained by the necessity to maintain a high blood
flow to the hard-working leg muscles, at least during early descent. On the
other hand, submerging with a greater respiratory air volume and, hence, a
larger oxygen store might enable cormorants to maintain a higher arterial
oxygen tension (PaO2) in the deep diving
situation despite a higher
O2 (when
compared with shallow diving), delaying a chemoreceptor-mediated heart rate
decline.
However, the propulsive effort of cormorants was greatest during the
initial descent phase of deep dives. Stroke frequency declined with increasing
depth and was similar to the shallow dive frequency near the bottom of the 10
m tank (Fig. 4A). Furthermore,
while birds had to continue stroking throughout shallow diving, they surfaced
passively during deep diving, reducing overall locomotor costs. Watanuki et
al. found that European shags foraging in the wild descend and ascend almost
vertically (6090° relative to sea surface)
(Watanuki et al., 2005
).
Stroke frequency during descent decreased with depth, while ascent from dives
to 40 m depth was passive. In our study we only recorded stroke frequency,
while cormorants might have also altered stroke amplitude. However, in the
shag study, Watanuki et al. found that birds maintained the duration and
strength of the power stroke during descent but changed glide duration between
strokes (Watanuki et al.,
2005
). Hence, stroke frequency might be a good indicator of
locomotor effort during diving in cormorants. To get a better understanding of
locomotor effort during deep and shallow diving, we estimated the average
stroke frequency during both modes by adding the number of strokes during the
different phases of a 20 s dive and dividing by dive duration. The resulting
mean stroke frequency of 1.8 and 2.1 strokes s1 for deep and
shallow diving, respectively, indicates that overall stroke frequency was
reduced during deep diving. Similarly, calculating the cumulative work
conducted against buoyancy during a 20 s dive showed that deep (vertical)
diving required less work than shallow (horizontal) diving because of passive
ascent during the former. Hence, overall locomotor effort was probably reduced
during deep diving.
Thermoregulatory costs
Plumage air volume measured in double-crested cormorant carcasses was
similar to that of great cormorants and well below the volume of other avian
divers (Grémillet et al.,
2005a
; Wilson et al.,
1992b
), highlighting the great potential for heat loss during
dives to depth in cormorants. However, as Wilson et al. pointed out
(Wilson et al., 1992b
),
whether metabolic rate will be increased during deep diving as a direct
consequence of a compromised insulative capacity will largely depend on
peripheral heat conservation mechanisms such as vasoconstriction. In emperor
penguins (Aptenodytes forsteri), among others, such a mechanism seems
to be in place. During diving, birds maintain a high core temperature while
the outer body shell cools (Ponganis et
al., 2003
). The latter is probably a consequence of peripheral
vasoconstriction and decreased plumage insulation, which increases conductive
and convective heat loss to the water. The reduced thermal gradient between
core and peripheral tissues will decrease heat loss to the water. Whether
cormorants use a similar mechanism to reduce heat loss during diving remains
to be investigated. An indication that some mechanisms for heat conservation
are in place in double-crested cormorants comes from the observation that
TC declined significantly during both shallow and deep diving, when
water temperature decreased (Fig.
6). The decrease in TC and, hence, increase in insulation
did not completely prevent heat loss during diving, however, as can be seen by
the increase in heat production with falling water temperature
(Fig. 3). The fact that
abdominal temperature (as measured by stomach temperature loggers) did not
change significantly during post-absorptive shallow diving in double-crested
cormorants (Fig. 5) could
indicate that peripheral vasoconstriction is restricted to the skin or
adjacent tissues. Unfortunately, we did not deploy stomach temperature loggers
during deep diving, so we have no information on abdominal temperature during
these dives. If, as we will argue below, thermoregulatory costs are increased
during deep diving and if stomach temperature loggers reflect whole-body
temperature, we should have seen a temperature decline during diving that was,
in turn, countered by thermogenesis. Previous recordings (using a thermistor
positioned close to the heart alongside an electrocardiogram electrode; M. R.
Enstipp, R. A. Andrews and D. R. Jones, unpublished data) showed that core
temperature of double-crested cormorants remained stable during dives to a
depth of 10 m (water temperature
15°C). However, this does not
preclude regional heterothermy elsewhere in the body. Abdominal temperatures
of South-Georgian shags (Phalacrocorax georgianus) have been shown to
decrease during dive bouts in the wild (during which cold food was ingested)
(Bevan et al., 1997
). In a
recent study, Grémillet et al.
(Grémillet et al.,
2005b
) found that abdominal temperature declined progressively
throughout dive bouts of great cormorants foraging off Greenland (up to
2°C). Mean dive depth for these birds ranged between 2 and 18 m. The
greatest and smallest temperature drops coincided with deeper and shallower
dives, respectively. Hence, this would support the notion of increased heat
loss and, therefore, thermoregulatory costs during deep diving. In the current
study, stomach temperature initially increased during shallow diving (even in
cold water), which would imply that heat generated by the exercising muscles
exceeded heat loss to the water. However, after reaching a peak, stomach
temperature started to decline, implying that heat loss exceeded heat
generation. At the end of a trial, stomach temperature typically reached the
initial level (Fig. 5) and it
is conceivable that during longer diving activity temperature would have
fallen to lower levels. During deep diving, when insulation from air trapped
within the plumage is greatly reduced, temperature decline should be
accelerated, unless countered by thermogenesis.
When trying to investigate to what degree heat loss, and consequently
thermoregulatory costs, might have contributed to the observed difference in
diving metabolic rate between shallow and deep diving, we should also consider
the following methodological concern. De Leeuw argued
(De Leeuw, 1996
) that diving
metabolic rate (MRd), the way it is usually calculated in
respirometry studies, only reflects the mechanical costs but not the
thermoregulatory costs, which are largely paid after the end of a dive bout
and, hence, are excluded from analysis. While this raises some interesting
points, Fig. 3 clearly
illustrates that thermoregulatory costs associated with diving in
double-crested cormorants were included in our analysis. Furthermore, the
almost identical slopes of the regression equations relating dive costs to
water temperature (Table 2)
suggest that, while absolute thermoregulatory costs are different, the
relative increase with a decline in water temperature is similar during deep
and shallow diving. However, to gain a better understanding of heat loss and
potentially incurred thermoregulatory costs during diving, we conducted an
analysis similar to that of De Leeuw (De
Leeuw, 1996
). To this end we calculated the `excess diving costs'
(EDC) of cormorants during deep and shallow diving in cold water
(post-absorptive trials). EDC, the excess oxygen consumption over the resting
rate, was calculated over the period from the first dive in a bout until
metabolic rate returned to the resting level (see
De Leeuw, 1996
). Our analysis
showed that EDC during shallow diving was about 1.5xMRd,
whereas during deep diving it was about 2.6xMRd. This
indicates that heat loss and thermoregulatory costs during deep diving are in
fact substantially increased when compared with during shallow diving.
However, to study the effect of dive depth on heat loss and to evaluate how
heat loss might shape diving costs in cormorants, heat flux measurements
during diving, as have been conducted in marine mammals
(Willis and Horning, 2005
),
are urgently needed.
In the context of ecological energetics, one should also keep in mind that,
in the wild, cormorants, like other avian divers, can potentially use a number
of mechanisms to decrease thermoregulatory costs. For example, birds might be
able to use the additional heat generated by the flight muscles when leaving
the foraging area or they might be able to use heat generated from the HIF to
substitute for thermoregulatory costs
(Kaseloo and Lovvorn, 2003
).
These mechanisms might allow birds to make up for at least some of the
incurred heat loss during diving without having to spend additional energy for
thermoregulation by means of shivering or non-shivering thermogenesis.
However, in our experimental set-up, capacity for these mechanisms was
limited.
In the absence of direct measurements, thermodynamic modelling has been
used to assess the impact of dive depth on the energetic costs of diving.
Grémillet and Wilson
(Grémillet and Wilson,
1999
), for example, used a theoretical relationship between dive
depth and heat flux to incorporate the increased heat loss experienced by
great cormorants when diving to depth into their dive cost analysis. To
compare our measurements with the model predictions, we adapted the
depthheat flux relationship from Grémillet et al. for
double-crested cormorants
(Grémillet et al.,
1998
) and used the output values to calculate their energetic
costs of diving to 10 m depth, as predicted by equation 10 in Grémillet
and Wilson (Grémillet and Wilson,
1999
). This modelling approach predicts a metabolic rate for
double-crested cormorants diving to 10 m depth of 33.87 and 37.37 W
kg1 when diving in `warm' and `cold' water, respectively.
These values correspond to a 65% increase in dive costs during dives to 10 m
depth when compared with shallow dives (1 m). Our own measurements, however,
indicate an increase of
22% (Table
1). The discrepancy between our measurements and the model
predictions might be explained by the following considerations. (1) The
equation used by Grémillet and Wilson
(Grémillet and Wilson,
1999
) incorporates the theoretical heat flux experienced at a
particular depth (max. depth reached) without considering descent and ascent
phase, when heat flux will be lower. (2) The depthheat flux
relationship incorporated into the model is entirely based on physical
properties and does not take into account any ability of birds to regulate
heat flux to the environment. (3) Grémillet and Wilson
(Grémillet and Wilson,
1999
) did not consider any effect that changes in buoyancy with
depth will have on the energetic costs during deep diving. Since the required
work against buoyancy decreases with an increase in depth
(Fig. 4B), this would tend to
decrease overall mechanical costs during diving, especially if the time spent
at the bottom and during passive ascent is great compared with the descent
phase. Consequently, the model of Grémillet and Wilson
(Grémillet and Wilson,
1999
) greatly overestimates the effect that depth has on the
energetic costs of deep diving cormorants within our set-up. Nevertheless, the
discussion above confirms our prediction that the measured increase in dive
costs during deep diving in cormorants reflects a composite of mechanical and
thermoregulatory costs that develop in opposite directions.
Our study shows that depth is an important factor to consider when
assessing the energetic costs associated with underwater foraging in a diving
endotherm. By contrast, most respirometry studies to date, investigating the
energetic costs of diving in endotherms, have been conducted in shallow dive
tanks because of logistic difficulties. When diving to depth, work against
buoyancy will be greatly reduced beyond the initial 10 m, while heat loss will
be greatly increased as body insulation decreases. Divers might employ
morphological (e.g. subcutaneous fat layer) and/or physiological means (e.g.
peripheral vasoconstriction) to reduce heat loss at depth. They might also try
to counter heat loss through increased heat production or they might allow
certain tissues to cool as a potential mechanism to prolong aerobic dive
duration. However, thermoregulation during diving is a complex issue and still
awaits its full scientific appreciation. Only recently has it become possible
to record temperatures of various tissues in avian divers foraging in the wild
(Culik et al., 1996
;
Bevan et al., 1997
;
Handrich et al., 1997
) and
these studies have started to shed some light into the different strategies
employed by endotherm divers to maximise underwater foraging time.
The elevated dive costs we measured during deep diving in our cormorants are probably a consequence of the increased thermoregulatory costs associated with a greater heat loss to the water at depth. While we found some evidence that heat loss during deep diving might be substantially higher than during shallow diving, mechanisms of peripheral heat conservation in cormorants and other avian divers await further study. To this end, heat flux measurements, which would allow quantification of heat loss during diving, would be an important first step. Investigating further to what degree heat generated as a by-product of locomotion (diving, flying) or the HIF is used to make up for the heat loss incurred during diving would allow the evaluation of how heat loss shapes diving costs in avian divers.
| Acknowledgments |
|---|