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First published online February 12, 2007
Journal of Experimental Biology 210, 741-749 (2007)
Published by The Company of Biologists 2007
doi: 10.1242/jeb.02705
Cloacal evaporation: an important and previously undescribed mechanism for avian thermoregulation
School of Life Sciences, Arizona State University, Tempe, AZ 85287-4501, USA
* Author for correspondence (e-mail: tycmhoffman{at}cox.net)
Accepted 2 January 2007
| Summary |
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Key words: cloaca, cutaneous, evaporative, water loss, metabolism, bird, Inca dove, Columbina inca, Eurasian quail, Coturnix coturnix
| Introduction |
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Adjustment of evaporation can be made either by changing the evaporative
conductance of (and therefore the rate of evaporation from) any specific
epithelium or by changing the surface area of exposed epithelia. Experimental
partitioning of total evaporation into components, or evaporative routes, has
been done for many species using various methods in studies that have used a
variety of terms to describe those evaporative routes (e.g.
Bernstein, 1971a
;
Richards, 1976
;
Maloney and Dawson, 1998
;
Webster and Bernstein, 1987
;
Taylor et al., 1971
;
Arieli et al., 1999
;
Menon et al., 1986
; Lee and
Schmidt-Nielsen, 1971; McKechnie and Wolf,
2004
; Tieleman and Williams,
2002
). Birds possess three anatomically distinct epithelia from
which evaporation can occur: the mouth and pharynx, the dry skin, and the
cloaca. We therefore categorize avian evaporative routes as either
buccopharyngeal, cutaneous, or cloacal. The present study is the first to
measure avian rates of cloacal evaporation. Buccopharyngeal evaporation
includes gular fluttering and evaporation due to breathing, whether by panting
or not. For simplicity, we include ocular evaporation within cutaneous
evaporation. Because previous studies did not discriminate between evaporation
from the dry skin and from the cloaca, we describe the sum of cutaneous and
cloacal evaporation as non-buccopharyngeal evaporation.
Despite the avian lack of sweat glands, several bird species have been
shown to exhibit rates of non-buccopharyngeal evaporation that rival or exceed
buccopharyngeal rates (e.g. Hoffman and
Walsberg, 1999
; McKechnie and
Wolf, 2004
; Marder et al.,
1989
; Webster and King,
1987
; Arad et al.,
1987
; Wolf and Walsberg,
1996
; Withers and Williams,
1990
; Marder and
Gavrieli-Levin, 1987
; Smith,
1969
). Historically, workers
(Bernstein, 1969
;
Smith and Suthers, 1969
) have
assumed that all but a negligible portion of this non-buccopharyngeal
evaporation occurs from the skin or from the conjunctivae. Terms such as
`cutaneous' (Lasiewski et al.,
1971
; Bernstein,
1969
; Smith and Suthers,
1969
), `peripheral' (Dawson,
1982
) and `transepidermal'
(Hattingh, 1972
;
Menon et al., 1989
;
Muñoz-Garcia and Williams,
2005
) were thus used to describe the remainder of a bird's
evaporative output, after evaporation due to ventilation and gular fluttering
were subtracted. Though some workers (Cade
and Dybas, Jr, 1962
) have conducted hygrometric measurements in
which the avian cloaca was occluded, the rationale for such experimental
treatment was to prevent urination and defecation, either of which would
render a hygrometric measurement unusable in analyses of evaporation from the
skin. A recent study of a desert reptile, the Gila monster Heloderma
suspectum Cope (DeNardo et al.,
2004
), demonstrated for the first time in any animal that cloacal
rates of evaporation can rid the body of enough heat to be important for
thermoregulation. Those results raised the possibility that birds (which, like
reptiles, possess cloacae) are similarly able to exploit this previously
undescribed evaporative route.
Columbiform species, which can tolerate high ambient temperatures without
panting (Arieli et al., 1988
;
Marder and Arieli, 1988
;
Ophir et al., 2002
), show some
of the highest non-buccopharyngeal rates of evaporation for any bird
(Hoffman and Walsberg, 1999
;
Marder and Ben-Asher, 1983
;
McKechnie and Wolf, 2004
). We
have demonstrated previously (Hoffman and
Walsberg, 1999
) that mourning doves Zenaida macroura
Linnaeus are able to make rapid adjustments to the rate of non-buccopharyngeal
evaporation in response to an experimental suppression of evaporation from the
mouth. Here, to add insight regarding the generality of the results observed
in mourning doves, we investigate the response to suppression of
buccopharyngeal evaporation in a different columbiform, the Inca dove
Columbina inca Lesson. In addition, we refine the experimental
technique to quantify the apportionment of non-buccopharyngeal evaporation
into its cutaneous and cloacal components. For comparison, we present values
for all three evaporative rates in a gallinaceous bird, the Eurasian quail
Coturnix coturnix Linnaeus. Both of the test species are easily
obtained and are widely distributed, occurring in arid and semiarid habitats,
but they represent distinct taxonomic orders.
| Materials and methods |
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Respirohygrometry
Inca doves
We used the flow-through method to measure evaporative rates, which allowed
us also to measure rates of change in oxygen and carbon dioxide. To minimize
hygroscopicity, we constructed the test chamber of plate glass with aluminum
corner supports. The chamber included two compartments one for the
head and one for the torso separated by an aluminum partition that
supported a thin sheet of latex (4 cmx4 cm) into which a hole was cut to
allow for passage of the head and neck. With the bird in place the latex was
stretched slightly, forming a barrier between the two compartments while not
interfering with the bird's breathing. The head compartment (426 ml) was
contained by a borosilicate bell jar fitted with borosilicate ports that
accepted minimally hygroscopic tubing (3 mm i.d., Bev-a-Line IV, Thermoplastic
Processes, Inc., Stirling, NJ, USA) for both influent and effluent. Identical
ports were attached to the plate glass of the torso compartment (17.72 l)
using epoxy, and the influent port was equipped with a copperconstantan
(type T) thermocouple for measurement of ambient temperature. A steel rod
hanging from the aluminum partition was equipped to support a removable
polypropylene shackle that was placed on the bird's legs prior to placement
into the chamber. An aluminum neck stock positioned immediately below the
latex sheet prevented the bird from pulling its head through the neck hole. An
illustration of a similar chamber appears elsewhere
(Wolf and Walsberg, 1996
).
Air entering the two compartments was first passed through an industrial air purifier (PCDA11129022, Puregas, Denver, CO, USA) that removed carbon dioxide and water vapor. Flux through each of the two influent lines was controlled and measured by separate mass flow controllers (FMA-A2406 and FMA-A2409, Omega Engineering, Stamford, CT, USA) positioned upstream of the compartments. Flux into the head compartment and torso compartment was maintained at ca. 1300 ml min1 and ca. 6700 ml min1, respectively. A borosilicate U-tube containing mineral oil was interposed between tubes connecting the compartments. The U-tube served as a manometer to allow for minimization of any intercompartmental pressure gradient due to unequal flow rates, thus minimizing the possibility of a gas leak from one compartment to the other. We occasionally verified that leaking was not occurring by sending air subsampled from the torso compartment to the CO2 analyzer and ensuring that the air was virtually free of carbon dioxide. To avoid any appreciable increase of chamber air pressure beyond barometric pressure, both effluent lines were kept short and allowed to empty into spill tubes from which separate subsampling pumps drew air and delivered it to the downstream instruments.
Sample air from the two compartments was pumped to separate dewpoint hygrometers (RH100, Sable Systems International, Las Vegas, NV, USA). Effluent from the torso-compartment hygrometer was vented to the temperature-controlled room in which the test chamber sat. Effluent from the head-compartment hygrometer was sent through anhydrous calcium sulfate to rid it of water vapor, and the dried air then passed through a carbon dioxide analyzer (LI-6252, Li-Cor Biosciences, Lincoln, NE, USA) and an oxygen analyzer (FC-1B, Sable Systems International, Las Vegas, NV, USA). Prevailing barometric pressure was continuously measured using an electronic manometer.
For half of the trials, the acapnic air supplying the head compartment was diverted to a series of three copper water columns through which it was bubbled to saturate the air with water vapor. Condensate, visible in the tubing that exited the water columns, assured us of saturation. The water-saturated air was then sent to the test chamber, just as for dry air in all other trials. To avoid condensation in the mass flow controller, and because we calibrated the controller for dry air, it was placed upstream of the water columns. We used the value for saturation vapor density at the temperature of the water to calculate the volumetric rate at which water vapor was added to the air stream, and we added that rate to the flux through the mass flow controller to determine head-compartment influx for those trials.
Measurements from all sensors were sampled every second by a datalogger
(CR23X, Campbell Scientific, Logan, UT, USA) and then averaged for output
every minute. The effective volumes
(Lasiewski et al., 1966
) of
the compartments were calculated as 1960 ml (head) and 81.5 l (torso),
yielding 99% equilibration periods of 1.5 min and 12.2 min, respectively.
Eurasian quail
Because of the mass and body geometry of Eurasian quail, we were not able
to conduct trials in the compartmentalized chamber. Instead, quail were placed
in a cylindrical chamber made of borosilicate glass (5.1 l) with an aluminum
lid and a glass floor. A cylindrical, polycarbonate mask (open on one end) was
placed over the bird's head and secured at the neck by nylon twine. The distal
(closed) end of the mask was attached to a flexible tube connected to a
miniature air swivel that allowed the bird to move about the cage without
tangling the air line. The effluent line from the swivel was attached to a
pump that drew air from the chamber, through the mask, and into a dewpoint
hygrometer (Sable Systems RH100), from which it was sent through anhydrous
calcium sulfate and then through a carbon dioxide analyzer (Li-Cor 6252) and
an oxygen analyzer (Sable Systems FC-1B).
The cylindrical chamber was fitted with three borosilicate ports, each of
which connected to minimally hygroscopic tubing (Bev-a-Line IV). Thus, there
were separate air lines for chamber influent, chamber effluent and mask
effluent. The influent line was equipped with a copperconstantan
thermocouple for measurement of ambient temperature. Negative-pressure flux
through the mask was maintained by a mass flow controller (Omega Engineering
FMA-A2406) at ca. 630 ml min1, sufficient to capture the
expired air and prevent it from escaping at the junction between the mask and
the neck. Positive-pressure flux into the chamber was maintained at ca. 6730
ml min1 by a separate mass flow controller (Omega
Engineering FMA-A2409), resulting in a 3.5 min period for gaseous
equilibration (Lasiewski et al.,
1966
). Collecting all of the expired air at the mask served to
effectively partition the chamber into torso and head compartments. The
baseline gas for the torso compartment was dry, acapnic air as described above
for the Inca dove experiment. The chamber effluent provided for measurement of
non-buccopharyngeal evaporation. In addition, this effluent served as the
baseline gas for the mask, because air drawn through the mask included water
vapor added to the chamber from the bird's torso. As for the Inca dove
experiment, the chamber effluent line was allowed to empty into a spill tube
from which air was subsampled and sent to a dewpoint hygrometer (Sable Systems
RH100). This chamber effluent could also be routed to the carbon dioxide and
oxygen analyzers. By ensuring that there was a negligible change in the dried
fractions of respiratory gases sampled from the body compartment, we were
assured that leaking from the mask did not occur.
The specifics of data acquisition for Eurasian quail were the same as for Inca doves.
Experimental protocol
Inca doves
The experiment included three treatment variables: ambient temperature,
ventilatory humidity and cloacal patency (N=8 to 13; see
Table 1). Trials were conducted
at four ambient temperatures (30°C, 35°C, 40°C and 42°C), two
levels of ventilatory humidity (`dry trials' and `humid trials'), and two
levels of cloacal patency (`unsealed trials' and `sealed trials'). For humid
trials, the torso compartment was supplied with dry air, and the head
compartment was supplied with air saturated at the respective ambient
temperature with water vapor. Immediately prior to placement of the bird into
the chamber for sealed trials, the cloaca was occluded with cyanoacrylic glue.
The resulting cloacal cap remained in place throughout the trial and was
removed using acetone immediately after the trial. Any feces released during
unsealed trials fell into a layer of mineral oil on the floor of the chamber,
thereby eliminating fecal water from hygrometric measurements.
|
During unsealed trials, the hygrometers directly measured buccopharyngeal
and non-buccopharyngeal evaporation; during sealed trials, they directly
measured buccopharyngeal and cutaneous evaporation. These direct measurements
allowed us to calculate cloacal evaporation as the difference between
non-buccopharyngeal and cutaneous evaporation. During humid trials,
buccopharyngeal evaporation was eliminated (or at least severely reduced),
because the influent was already saturated with water vapor. This required the
bird to either store that extra heat or dissipate it by increasing evaporative
flux elsewhere. The bird remained in the test chamber for 2 h. For the first
60 min, dry air was delivered to both compartments. A remote switch then
triggered a re-routing of the influent without disturbing the bird, thereby
delivering water-saturated air to the head chamber for an additional 60 min,
before the bird was removed from the chamber. Data used in analyses were
averages of measurements taken over the last 10 min of each portion (dry or
wet) of the overall time spent in the chamber. All trials were conducted in
darkness during daylight hours. Darkness reduced the unnatural level of stress
experienced by the birds. Conducting trials in darkness during daylight hours
results in a modest, circadian increase in total evaporation
(MacMillen and Trost, 1967
).
We feel this is more representative of field conditions under which
thermoregulatory evaporation is employed by Inca doves.
Eurasian quail
The experiment included two treatment variables: ambient temperature and
cloacal patency (N=8). Trials were conducted at two ambient
temperatures (30°C and 32°C) and two levels of cloacal patency
(`unsealed trials' and `sealed trials'). We did not conduct trials at
Ta>32°C, because quail apparently became distressed
at higher temperatures, as evidenced by observation of persistent struggling.
Because quail were allowed to stand on the floor of the chamber, no mineral
oil was used; if defecation occurred during any trial, the resulting data were
discarded. For sealed trials, the cloaca was sealed with cyanoacrylic glue for
the duration of the trial, after which the glue was removed using acetone.
Except for differences in the method of partitioning evaporative routes and in
the ambient temperatures of trials, the protocol for the Eurasian quail
experiment was the same as for the dry trials using Inca doves. All trials
were conducted in darkness during daylight hours.
Calculations
Evaporation represents an input of gas into the chamber, so that the efflux
and influx differ. Similarly, rate of oxygen consumption,
O2, and carbon
dioxide production,
CO2, alter the
flux. To incorporate these changes into our data, we derived the following
equations for calculating evaporative rates. All symbols are defined in the
List of symbols.
![]() | (1) |
![]() | (2) |
![]() | (3) |
![]() | (4) |
![]() | (5) |
![]() | (6) |
![]() | (7) |
O2=0 and
CO2=0, thereby
simplifying Eqn 7 as:
![]() | (8) |
![]() | (9) |
![]() | (10) |
We calculated sampled water vapor pressure from the measured dewpoint,
using the eighth-order polynomial of Flatau et al.
(Flatau et al., 1992
), and we
calculated vapor density from vapor pressure using the Ideal Gas Law
(Campbell and Norman,
1998
).
Analysis of data
We used SAS (Version 9.1, SAS Institute, Cary, NC, USA) to perform all
statistical tests. For Inca doves, the MIXED procedure was used to perform
repeated-measures analyses of variance (RM-ANOVA) and TukeyKramer
post-hoc comparisons, with non-buccopharyngeal evaporation
(NBE), buccopharyngeal evaporation (BE), oxygen consumption
(
O2), and carbon
dioxide production
(
CO2) separately
defined as dependent variables. For each of these tests, the within-subjects
factors were ambient temperature, humidity of the head-chamber influent and
cloacal patency. The same tests were performed for Eurasian quail, but
humidity was not included as a within-subjects factor, because humidity was
not adjusted in trials using quail. In all tests for both species, we
specified the Compound Symmetry covariance structure, because it yielded the
lowest values for both Akaike's Information Criterion and Schwartz' Bayesian
Criterion.
| Results |
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Cloacal evaporation (CloE) was negligible at
Ta
40°C. However, at
Ta=42°C, mean values for CloE were 91.3 µg
g1 min1 during dry trials and 85.0 µg
g1 min1 during wet trials. These values
are similar to mean BE at Ta=42°C during dry
trials (90.7 µg g1 min1) and slightly
less than half of mean cutaneous evaporation (CutE, 222.4 µg
g1 min1 during dry trials, 256.6 µg
g1 min1 during wet trials). That is, for
trials at 42°C, total evaporation was apportioned as 25.4%
buccopharyngeal, 21.2% cloacal and 53.4% cutaneous
(Fig. 2). This indicates that
cloacal evaporation was thermoregulatorily important at the highest
experimental temperature, on a par with buccopharyngeal evaporation. The heat
liberated by cloacal evaporation at Ta=42°C averaged
3.7 mW g1, or 27.6% of mean metabolic heat (13.4 mW
g1) at that temperature.
|
We separately calculated the volumetric rate (µl g1
min1) of BE, so we could relate buccopharyngeal
evaporation to oxygen consumption as the dimensionless evaporespiratory ratio,
BE:
O2.
A temperature-dependent change in this ratio indicates an uncoupling of the
rate of buccopharyngeal evaporation from the rate of ventilation. This, in
turn, can be partially caused by an attempt to increase evaporation from the
rate that would occur just as a result of breathing. The evaporespiratory
ratio increased by more than threefold with ambient temperature from 30°C
to 42°C (F=62.9, P<0.0001), and the ratio at each
temperature differed significantly from that at all other temperatures
(P
0.0011 at all temperatures). This reflects the significant
decrease in
O2
as Ta increased from 30°C to 35°C
(t=8.69, adjusted P<0.0001) and the temperature-dependent
increase in BE, along with the birds' use of panting or gular
fluttering that we observed at the higher temperatures.
Eurasian quail
Table 1 provides means and
standard errors for hygrometric and respirometric measurements, along with
numbers of individuals on which measurements were made. There were no
significant effects of treatment variables on NBE
(Ta: F=0.01, P=0.9215; patency:
F=3.57, P=0.1009; Ta x patency:
F=0.02, P=0.8908). Similarly, BE did not change
with treatment (Ta: F=1.16, P=0.3163;
patency: F=0.36, P=0.5689; Ta x
patency: F=1.79, P=0.2226), nor did the evaporespiratory
ratio (Ta: F=3.77, P=0.0932; patency:
F=0.15, P=0.7075; Ta x patency:
F=1.00, P=0.3513). Despite frequent observations of panting,
cloacal evaporation remained comparatively low, accounting for only 8.3%
(Ta=30°C) and 6.4% (Ta=32°C)
of total evaporation, and CloE did not change with
Ta (F=0.01, P=0.9151). Evaporation from
the cloaca was about one-fifth to one-third of BE, the latter of
which accounted for 26.2% (Ta=30°C) and 35.4%
(Ta=32°C) of total evaporation. Thus, the majority of
evaporation from Eurasian quail was cutaneous (65.4% and 58.2% at 30°C and
32°C, respectively). The relatively constant rate of cloacal evaporation
liberated 330 µW g1 of heat at
Ta=30°C and 283 µW g1 at
Ta=32°C, corresponding to presumably negligible
portions (2.8% and 2.5%) of metabolic heat at the respective ambient
temperatures.
| Discussion |
|---|
|
|
|---|
The earliest accepted standard view of avian evaporation was driven by the
anatomical discovery that birds do not possess sweat glands; workers therefore
assumed that a lack of sweat glands indicated a corresponding lack of
evaporation from the avian integument, and that effectively all of the water
lost evaporatively from a bird's body was lost from its mouth
(Bartholomew and Cade, 1963
;
Bartholomew and Dawson, 1953
;
Bartholomew et al., 1962
;
Cowles and Dawson, 1951
;
Schmidt-Nielsen et al., 1969
;
Calder, Jr and Schmidt-Nielsen,
1966
; Lasiewski and Dawson,
1964
). This assumption was challenged by subsequent studies in
which separate hygrometric measurements were made from the head and from the
rest of the body (Bernstein,
1971a
; Bernstein,
1971b
; Smith and Suthers,
1969
; Lasiewski et al.,
1971
; Lee and Schmidt-Nielsen, 1971;
Marder and Ben-Asher, 1983
;
Taylor et al., 1971
). These
newer results threw into question the original assumption of negligible
evaporation from the skin of birds, and they prompted microanatomical
investigations (Arieli et al.,
1999
; Menon et al.,
1989
; Menon et al.,
1986
; Menon et al.,
1996
) that revealed major differences between mammalian and avian
epidermis, helping to explain the observed rates of cutaneous evaporation in
the absence of sweating. Yet with cutaneous evaporation having been clearly
established as occurring in birds, researchers continued to assume that
evaporation from the cloaca was negligible
(Marder and Ben-Asher, 1983
;
Marder, 1983
;
Crawford, Jr and Lasiewski,
1968
). That is, any measurement of avian evaporation that was not
occurring from the mouth was assumed to be a measurement of cutaneous
evaporation. Our results demonstrate that non-buccopharyngeal evaporation in
birds can be subdivided into cutaneous and cloacal components, and that avian
evaporation should now be considered on a tripartite basis.
Rates of cloacal evaporation in Eurasian quail and Inca doves differed
markedly. Unfortunately, quail became thermally stressed in the test chamber
at ambient temperatures much lower than we anticipated, and we were forced to
restrict our measurements to two, relatively low and closely spaced
temperatures. This did not afford us the experimental resolution necessary for
determining whether these birds make any thermally driven adjustment to the
rate of cloacal evaporation. Nevertheless, two interesting findings emerge.
First, evaporation is dominated just as strongly by the cutaneous route in
Eurasian quail as it is in Inca doves, despite the fact that the Eurasian
quail is a non-columbiform bird. However, despite the predominance of
cutaneous evaporation, Eurasian quail exhibited mass-specific rates of
cutaneous evaporation at 30°C that were only about 42% of those measured
in Inca doves at the same air temperature. This is in agreement with the
observation by others (Degen et al.,
1982
; Roberts and Baudinette,
1986
) that rates of evaporation and water-turnover in quail occur
near the minimum of the predicted range for bird species. Second, cloacal
evaporation accounts for about 7% of total evaporation in Eurasian quail. This
fraction is lower than the cloacal fraction observed in Inca doves, despite
the large anatomical difference between the cloacae of these species. The
Eurasian quail has a cloaca appearing as a semilunar slit, the orifice of
which is much larger in relation to the body than that of the small, circular
sphincter occurring in the Inca dove.
|
Our results suggest that Inca doves could employ a three-stage approach toward evaporative thermoregulation. At lower temperatures, at which breathing might rid the body of sufficient heat for thermostasis, cutaneous evaporation is minimized and cloacal evaporation is virtually eliminated by constricting the cloacal sphincter. As temperature increases beyond a point at which buccopharyngeal evaporation is inadequate, cutaneous evaporation is increased to make up for the thermoregulatory deficit. At still higher temperatures, when evaporation by panting and from the skin might be maximized, the cloacal epithelium is exposed to provide for increased latitude with respect to the range of survivable microenvironments.
Hoffman and Walsberg previously showed that another columbiform, the
mourning dove, is able to make temperature-dependent adjustments to rates of
non-buccopharyngeal evaporation, and that those adjustments are larger than
any that could be explained passively, or simply on the basis of a change in
skin-surface temperature (Hoffman and
Walsberg, 1999
). Because that experiment did not discriminate
between cloacal and cutaneous evaporation, it is uncertain how much of the
observed change in non-buccopharyngeal evaporation resulted from a change in
cutaneous evaporation. The present study of Inca doves is intriguing in light
of those earlier results for mourning doves, because suppression of
buccopharyngeal evaporation in Inca doves did not significantly increase
cutaneous evaporation at any individual temperature, though cutaneous
evaporation increased greatly with increasing temperature. Whether mourning
doves possess a greater capacity than Inca doves for adjusting rates of
cutaneous evaporation or whether the adjustment of evaporation in mourning
doves was largely due to adjustment of cloacal evaporation remains to be
tested.
It is interesting to note that the response of cloacal evaporation to
increase in ambient temperature is similar in Inca doves and Gila monsters
(DeNardo et al., 2004
), the
two species for which cloacal evaporation has been demonstrated at magnitudes
sufficient for thermoregulation. Both of these species are able to tolerate
very high temperatures, and in both of these species cloacal evaporation
remains negligibly low until a critically high ambient temperature prompts a
steep rise in cloacal evaporation. This is in keeping with the notion that
cloacal evaporation might be used by some animals as a last resort, when the
only alternatives are an immediate change of microenvironment or a potentially
life-threatening increase in body temperature.
These novel observations of avian cloacal evaporation raise several interesting questions. Perhaps most obvious is the question of how cloacal evaporation is controlled. Apart from simply relaxing the cloacal sphincter, is the bird everting the cloaca? If so, then how much of the cloacal surface is exposed? Whether or not the cloaca is everted, the rate of evaporation therefrom could be altered by changes in such properties as the surface temperature and degree of perfusion of the cloacal epithelium. Independent of all of these factors, a rhythmic ventilation of the cloaca could increase the rate of evaporation, as could postural adjustments that take advantage of the convective air currents to which the bird is exposed.
A second set of important questions raised by these findings involves possible trade-offs that might occur. Traditionally, the cloaca has been viewed as a fairly simple repository for excretory, digestive and reproductive products. Given its additional function of serving as an evaporative organ, perhaps the cloaca will prove to possess unforeseen complexities. Since avian urine can undergo postrenal processing, how might the resorption of water into the hindgut interfere with cloacal evaporation, and how quickly can changes be made to these seemingly competing processes? Similarly, how might the demands for cloacal evaporation affect (and be affected by) the digestive and reproductive functions of the cloaca?
Indeed, since such high rates of cloacal evaporation have now been observed in Inca doves and Gila monsters, most of these questions apply to both birds and reptiles. Further refinement of measurement techniques and testing of other taxa will provide much needed insight.
| List of symbols |
|---|
|
|
|---|
H2O
'A
A
O2
CO2
'V
V
| Acknowledgments |
|---|
| References |
|---|
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|---|
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