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Am J Physiol Regul Integr Comp Physiol 274: R686-R693, 1998;
0363-6119/98 $5.00
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Vol. 274, Issue 3, R686-R693, March 1998

Circadian rhythms in diving behavior and ventilatory response to asphyxia in canvasback ducks

Melanie Woodin and Richard Stephenson

Department of Zoology, University of Toronto, Toronto, Ontario, Canada M5S 3G5

    ABSTRACT
Top
Abstract
Introduction
Methods
Results
Discussion
Appendix
References

Underwater feeding behavior was measured in 10 captive canvasback ducks (Aythya valisineria) for 12 days under a 12:12-h light-dark photoperiod. Feeding activity exhibited a daily rhythm, with 76% of dives occurring at night. In separate experiments on six of these ducks, a circadian rhythm was observed in the duration of voluntary dives. Dives at night (14.7 ± 0.7 s) were significantly longer than those during the day (10.7 ± 0.7 s). These day-night differences in diving behavior were accompanied by day-night differences in respiratory responses to progressive asphyxia. In the same six ducks, ventilation increased exponentially as a function of inspired CO2 concentration during rebreathing in a closed-circuit barometric plethysmograph. The exponential rate constant for inspired ventilation was significantly smaller at night (0.23 ± 0.02) than during the day (0.26 ± 0.01). We suggest that intermittent apneic exercise is facilitated by reduced respiratory chemosensitivity and that the respiratory and behavioral control systems are synchronized by the circadian timing system in diving ducks.

plethysmography; hypoxic hypercapnia; respiratory chemosensitivity; avian respiration

    INTRODUCTION
Top
Abstract
Introduction
Methods
Results
Discussion
Appendix
References

MANY SPECIES of birds and mammals forage underwater. Diving behavior, which often exhibits a distinct daily rhythmicity (4, 14, 21, 24, 33, 34), typically consists of bouts of aerobic dives (31, 35). These dives tend to be short compared with maximal breath-hold times, and they are separated by similarly brief intervals at the water surface (24, 31).

Current models of the physiological regulation of dive patterns are either explicitly based on, or implicitly incorporate, aspects of the "aerobic dive limit" concept (22). Although not discounting the potential for short-term modification of dive patterns through anaerobic mechanisms (9), the aerobic dive limit hypothesis predicts that, during routine aerobic diving behavior, dive times are directly or indirectly determined by the quantity of O2 stored in the lungs, blood, and muscle and the rate at which the O2 is consumed (22). If O2 or a correlated variable serves as a signal to terminate a dive (i.e., to resume lung ventilation), then the respiratory sensitivity to hypoxemia or a correlated variable is an integral component of this model. It has been suggested that diving species have a relatively low respiratory responsiveness to asphyxia (6), although supporting evidence is scarce. It is assumed that this adaptation would enable diving species to utilize a greater fraction of their O2 store and therefore to remain submerged for longer.

In this study, it was hypothesized that the circadian organization of avian diving behavior may reflect an underlying circadian oscillation in respiratory chemosensitivity. Day-night differences in respiratory responses to hypoxia and hypercapnia have been demonstrated in rodents (26, 27, 30) and humans (28), but no information is available for birds or diving species. To test this hypothesis, the circadian rhythm in diving behavior was monitored in captive canvasback ducks, and the ventilatory response to progressive asphyxia was measured at times corresponding to maximal and minimal dive activities.

    METHODS
Top
Abstract
Introduction
Methods
Results
Discussion
Appendix
References

Ten adult canvasback ducks (Aythya valisineria; 7 females, 3 males; body mass range 900-1,200 g) were housed in an indoor diving tank under a 12:12-h light-dark photoperiod (lights on at 6:30 AM EST). The ducks were trained to dive for food that was delivered to the floor of the tank by a semiautomatic feeder. This feeder, which was based on the design used by Bevan et al. (2), provided the ducks with unlimited access to food. The ducks were trained to activate a submerged paddle switch to deliver 1.5-2 g of food pellets. Ducks used this self-feeding system for several weeks and were observed to maintain normal body weight before recordings were initiated.

Animal preparation. Six of the ducks underwent surgery a minimum of 1 wk before experiments. All procedures were performed under general anesthesia (halothane, 1-2.5% in a 50% air-50% O2 mixture) using sterile materials. A temperature-sensitive radiotransmitter was implanted into the abdomen through a midline incision and sutured to the muscle of the abdominal wall. Care was taken to avoid damaging the abdominal plumage so that the ducks could resume diving behavior within 1 day of recovery. The ducks were then given a topical antibiotic (Cicatrin) and a broad-spectrum antibiotic (Penlong XL, Rogar/STB, 0.3 ml/kg im). The ducks were kept in postsurgical isolation for 2 h until full recovery from anesthesia and then returned to the diving tank. The six animals with radiotransmitters were used for measurement of circadian rhythms in dive duration and for plethysmographic analysis of ventilatory sensitivity to progressive asphyxia.

Diving behavior. An indirect measure of the temporal organization of diving behavior of the group of 10 ducks was obtained by recording activations of the feeding device. The circadian rhythm was first measured during a 2-wk control period during which the ducks were left undisturbed (with the exception of an experimenter filling the food hopper once every 4 days and the cleaning the tank once per week). Measurements continued during subsequent experiments to ensure that disturbance and handling did not disrupt the diving rhythm.

To characterize the circadian diving rhythm in more detail, six of the ducks were studied in pairs in a different diving tank. They continued to use a semiautomatic feeder. This diving tank was visually isolated, and the ducks were observed by videocamera. Body temperature (Tb) and diving behavior were monitored continuously for 1 mo using crystal-controlled radiotransmitters (Mini-mitter, TM-DISC). Reception of the radio signal was adjusted by manipulating loop antenna length and water conductivity (addition of sea salt). In this way, the body temperature signal could be recorded while the animal was at the water surface, but the radio signal was attenuated when the animal was submerged. The radio dropout intervals were used as a measure of dive duration. Therefore, during diving bouts [i.e., 3 or more dives in series separated by short intervals (<1 min) at surface], Tb was recorded during the intervals between successive dives.

Measurement of ventilation. A closed-circuit plethysmography system was used to measure resting lung ventilation in six animals (Fig. 1). The system operates on the principle that air is warmed and humidified during inspiration causing an expansion in volume, which in turn results in an increase in pressure within the fixed-volume animal chamber (15). The ventilatory pressure waveform was monitored using a differential pressure transducer (model DP45-14, Validyne Engineering), which measured the difference in pressure between the animal chamber and an identical reference chamber. The ventilatory pressure signal was calibrated using an animal ventilator (Columbus Instruments). Tb was continuously recorded using implantable radiotransmitters (Mini-mitter; TM-DISC or VM-FH-DISC). The transmitters weighed ~4.9 g when fully encapsulated, they had a response time constant of 77 s and a resolution of 0.1°C. Nasal temperature was also continuously recorded using a thermocouple probe (Physitemp Instruments, EXT-6) taped to the bill at the opening of the nares. Chamber temperature and humidity were recorded periodically from a small thermometer and hygrometer located in the animal chamber.


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Fig. 1.   Schematic diagram of closed-circuit plethysmograph. Dotted lines represent electrical connections. Bold lines represent primary recirculating airflow. Fine lines represent airflow for gas analysis and O2 supply. 1, Three-way stopcock used to include or exclude KOH solution (CO2 scrub) in primary air circulation; 2, 3-way stopcock used to enable CO2 analyzer to sample gas before or after KOH solution.

The animal chamber gas was recirculated at a rate of 5.8 l/min using a diaphragm pump (Cole-Parmer Instrument). O2 and CO2 concentrations in dry gas were continually monitored and recorded using electrochemical fuel cell and infrared analyzers, respectively (models S-3A/1 and CD-3A, Ametek). Small fans were placed in the chambers to keep the gases mixed.

The volume of gas in the animal chamber plus recirculating system (Vc) with a duck in place was determined by gas dilution following the injection of a known volume of pure CO2 (VCO2) directly into the experimental chamber
Vc = V<SC>co</SC><SUB>2</SUB> /&Dgr;F<SC>co</SC><SUB>2</SUB> (1)
where Delta FCO2 is the increase in fractional concentration of CO2 following injection.

Experimental protocol. At the start of each experiment, the animals were allowed to rest quietly in the chamber until all variables had reached an apparent steady state. During this period, which usually lasted ~30 min, O2 was bled into the plethysmograph at a flow rate sufficient to maintain the O2 concentration between 20.98 and 21.02%. CO2 concentration was kept at <= 0.05% by bubbling the gas through concentrated KOH solution. A recording of CO2 production and lung ventilation was made for 5 min; then the duck was exposed to progressive asphyxia during a period of rebreathing. To accomplish this, the O2 supply was turned off, and the CO2 scrubbers were temporarily bypassed. Lung ventilation, gas exchange, and temperature were recorded continuously during the rebreathing period. The experiment was terminated when CO2 concentration reached 6%. Each duck was used three times at 9 AM and three times at 9 PM, and at least 60 h separated consecutive experiments.

Analysis of plethysmography data. Tidal volume (VT, ml BTPS) was calculated as follows (18)
V<SC>t</SC> = [(Pm/Pcal) ⋅ Vcal ⋅ Ga]/[1 − (<IT>t</IT><SC>i</SC>/<IT>t</IT><SUB>tot</SUB>)(1 − Ga/Gn)] (2)
where
Ga = [T<SUB>b</SUB>(P<SC>b</SC> − Pc<SUB>H<SUB>2</SUB>O</SUB>)]
/[T<SUB>b</SUB>(P<SC>b</SC> − Pc<SUB>H<SUB>2</SUB>O</SUB>) − T<SUB>c</SUB>(P<SC>b</SC> − Pa<SUB>H<SUB>2</SUB>O</SUB>)] (3)
and
Gn = [T<SUB>b</SUB>(P<SC>b</SC> − Pn<SUB>H<SUB>2</SUB>O</SUB>)]
/[T<SUB>b</SUB>(P<SC>b</SC> − Pn<SUB>H<SUB>2</SUB>O</SUB>) − T<SUB>n</SUB>(P<SC>b</SC> − Pa<SUB>H<SUB>2</SUB>O</SUB>)] (4)
where Pm is the observed ventilatory pressure deflection; Pcal is the pressure deflection due to cyclic injection and withdrawal of a known volume, Vcal; Ga represents the ratio of tidal volume at respiratory air sac conditions to the small increase in volume that occurs when the tidal gas expands from its volume at chamber conditions; Gn is analogous to Ga but represents the volume change from air sac to nasal temperature, Tn (K); tI is the inspiratory time (s); ttot is the total breath time (s); PB is the barometric pressure (mmHg); PcH2O is the water vapor pressure of gas in the animal chamber (mmHg); PnH2O is the saturated water vapor pressure of gas at Tn (mmHg); PaH2O is the saturated water vapor pressure of gas in the respiratory air sacs (mmHg); Tb is abdominal air sac temperature (K); and Tc is the temperature (K) of gas in the animal chamber.

Respiratory frequency (fr) was calculated as 60/ttot, using an average value of ttot derived from 30 to 50 breaths. Respiratory CO2 production (VCO2, ml/min STPD) during steady-state conditions before the onset of asphyxia was calculated as follows
<A><AC>V</AC><AC>˙</AC></A><SC>co</SC><SUB>2</SUB> = <A><AC>V</AC><AC>˙</AC></A>r ⋅ (F<SC>co</SC><SUB>2,o</SUB> − F<SC>co</SC><SUB>2,i</SUB>) (5)
where Vr is the recirculating gas flow rate (ml/min STPD), FCO2,o is the fractional concentration of CO2 leaving the animal chamber and FCO2,i is the fractional concentration of CO2 entering the animal chamber.

O2 consumption (VO2, ml/min STPD) and VCO2 during rebreathing asphyxia were determined as follows
<A><AC>V</AC><AC>˙</AC></A><SC>o</SC><SUB>2</SUB> = [F<SC>o</SC><SUB>2,1</SUB> × Vc − ({F<SC>o</SC><SUB>2,2</SUB> × Vc × [1 − (F<SC>o</SC><SUB>2,1</SUB> + F<SC>co</SC><SUB>2,1</SUB>)]}
/[1 − (F<SC>o</SC><SUB>2,2</SUB> + F<SC>co</SC><SUB>2,2</SUB>)])]/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (6)
<A><AC>V</AC><AC>˙</AC></A><SC>co</SC><SUB>2</SUB> = [( {F<SC>co</SC><SUB>2,2</SUB> × Vc × [1 − (F<SC>o</SC><SUB>2,1</SUB> + F<SC>co</SC><SUB>2,1</SUB>)]}
/[1 − (F<SC>o</SC><SUB>2,2</SUB> + F<SC>co</SC><SUB>2,2</SUB>)]) − F<SC>co</SC><SUB>2,1</SUB> × Vc]/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (7)
where FO2,1, FO2,2, FCO2,1, and FCO2,2 are fractional concentrations of O2 and CO2 at the start (t1) and end (t2) of the measurement interval, respectively. This calculation accounts for the change in number of dry gas molecules in the plethysmograph due to a respiratory exchange ratio (RER) <1.0 (see APPENDIX for derivation).

Data sets were compared using paired-sample t-tests as appropriate. Differences are considered significant at the 95% confidence level (P < 0.05).

    RESULTS
Top
Abstract
Introduction
Methods
Results
Discussion
Appendix
References

Diving activity exhibited a daily rhythm (Fig. 2). In 10 undisturbed ducks, the underwater feeder was activated a total of 8,273 times in 12 days. Seventy-six percent of the dives occurred during darkness and 24% in the light. The lights-on and lights-off transitions were followed by abrupt increases in diving activity. The increase in diving activity at lights-on was transient (1-2 h), whereas that at lights-off was maintained for ~8 h (Fig. 2). Feeding dives were least frequently performed between ~8 and 11 AM, and the greatest number occurred between ~9 and 11 PM (Fig. 2). In six of the ducks, dive durations, surface intervals, and Tb during a diving bout and during nondiving intervals were analyzed over a 2-h time bin in these two time periods (Table 1). Dive durations were 37% greater at 9-11 PM than at 9-11 AM (P = 0.01). There was no significant difference in surface intervals at these two time intervals. Tb during diving bouts and nondiving periods was significantly higher at 9-11 AM than at 9-11 PM (P = 0.03). In addition, Tb was significantly higher during diving bouts than during nondiving periods at 9-11 AM and 9-11 PM (P = 0.003).


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Fig. 2.   Total number of feeding dives performed per hour by 10 ducks over 12 days. Lights came on at 6:30 AM and went out at 6:30 PM as indicated by horizontal bar.

                              
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Table 1.   Dive pattern and body temperature in undisturbed ducks during periods of minimal (9-11 AM) and maximal (9-11 PM) daily diving intensity

Respiratory variables measured during steady-state air breathing are presented in Table 2. None of the variables differed significantly between 9 AM and 9 PM. Respiratory variables measured during progressive asphyxia are presented in Table 3. There were no significant differences in metabolic rate (VO2, VCO2, RER), breathing pattern (fr, tI/ttot), or Tb between 9 AM and 9 PM in the asphyxic state. There were, however, significant differences in Tb between steady-state air breathing and asphyxia (P = 0.0002) at 9 PM but not at 9 AM. Tb decreased progressively during asphyxia to minima of 40.6 ± 0.2 and 40.8 ± 0.2°C at 9 PM and 9 AM, respectively.

                              
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Table 2.   Respiratory variables measured during a steady-state period of air breathing at 9 AM and 9 PM

                              
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Table 3.   Respiratory variables measured during progressive asphyxia at 9 AM and 9 PM

During progressive asphyxia, inspired ventilation (VI) increased exponentially with both increasing CO2 concentration (Fig. 3) and decreasing O2 concentration. The ventilatory response was analyzed as a function of CO2 concentration, and an analysis of the response as a function of O2 concentration yields the same qualitative result because RER was invariant in each experiment.


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Fig. 3.   Day and night ventilatory responses to progressive asphyxia in a representative animal. bullet , 9 AM data; open circle , 9 PM data.

VT, VI, VT/tI, and VI/VCO2 were analyzed as a function of inspired CO2 concentration (%) using an exponential model of the following type: y = a · eb[CO2], where y is a respiratory variable. The coefficient a represents the magnitude of y under air-breathing conditions, and the exponent b is interpreted as a measure of the sensitivity of y to progressive hypercapnic hypoxia. The exponent b was derived by least-squares linear regression of lny against CO2 concentration ([CO2]). The resulting r2 values were slightly, but consistently, higher than for linear regressions of the untransformed data. Furthermore, examination of plots of residuals vs. predicted values showed that untransformed data were heteroscedastic and exhibited a curved relationship to the regression. These undesirable characteristics were corrected by logarithmic transformation, indicating that the exponential model provided a better description of the data than a linear model. There were significant day-night differences (P < 0.05) in the value of the exponential rate constant b, i.e., in the slopes of lnVT/[CO2], lnVI/[CO2], ln(VI/VCO2)/[CO2], and ln(VT/tI)/[CO2] (see Table 3).

A least-squares regression of fr against [CO2] yielded a nonsignificant regression coefficient (P = 0.527), indicating that fr did not change during progressive asphyxia. Therefore an average value was calculated over the entire rebreathing period and is presented in Table 3.

There were no statistically significant differences in Tn between 9 AM and 9 PM in air or during asphyxia. In addition, Tn did not differ significantly between air and asphyxia at either time of day. The ducks often began to breathe through the open mouth when inspired CO2 rose to ~6%. When this occurred, Tn increased instantaneously by ~4°C, and experiments were terminated.

    DISCUSSION
Top
Abstract
Introduction
Methods
Results
Discussion
Appendix
References

This study, which to our knowledge represents the first continuous long-term recording of duck diving patterns, has confirmed that ducks exhibit a circadian rhythm in diving behavior. Dives were more frequent and of longer duration at night. Furthermore, the plethysmographic data support the hypothesis that the ventilatory response to asphyxia is lower at night, when the ducks are diving the most, than in the morning, when they dive the least.

All animals responded to progressive asphyxia with a nonlinear increase in ventilation and no change in fr. This corroborates other studies in birds in which hypercapnic hypoxia produced a nonlinear ventilatory response (12), with the increase in ventilation due mainly to a rise in VT with small changes in fr (7, 12). Inhalation of CO2 is known to evoke an increase in ventilation in unanesthetized birds (20, 32), although the effect on breathing pattern can be quite variable due, at least in part, to the inhibitory effect of CO2 on the intrapulmonary chemoreceptors (25). In general, the avian hypercapnic ventilatory response consists of an increase in VT with small increases or decreases in fr (1, 8, 20, 32). In addition, birds have been shown to respond to a decrease in ambient O2 with an increase in ventilation, produced by increases in both VT and fr (3, 5, 7, 8, 12, 19, 20). Comparisons of the ventilatory response to hypoxia, hypercapnia, and hypoxic hypercapnia indicate that effects of CO2 and O2 are additive in birds (20), although the data presented by Colby et al. (12) suggest that there may be a multiplicative interaction in adult bank swallows.

In the present study, it was found that simultaneous progressive hypoxia and progressive hypercapnia (asphyxia) evoked a greater ventilatory response in the day than at night. This difference in VI, which was entirely due to a difference in VT, was manifest as a difference in the exponential rate constant b. Recent studies in humans (28) and rats (26, 27, 30) have provided evidence for the existence of a circadian rhythm in mammalian respiratory chemosensitivity, but the mechanisms of interaction of the circadian timing system and the respiratory control system are unknown at present. In rodents, it appears that the interaction could be mediated indirectly via circadian modulation of metabolic rate (26, 27, 30), but this was not the case in ducks. The exponential rate constant describing the relationship between VI/VCO2 and inspired CO2 concentration differed between 9 AM and 9 PM (Table 3). Thus the metabolism-specific ventilatory response to hypoxic hypercapnia was greater during the day than during the night.

The question as to whether diving mammals and birds have a reduced respiratory sensitivity to CO2 is unresolved. Seals appear to have a lower sensitivity to CO2 than humans (13, 29), but it is not established whether diving birds are less sensitive than nondiving birds (1, 7). It has been suggested that a chemoreceptor system with low sensitivity to CO2 would allow a diving animal to remain submerged for extended periods of time (6, 13) because the drive to resurface would develop more slowly. In support of this idea, we observed a circadian difference in dive durations in the ducks in the present study, with longer dives occurring at night when respiratory sensitivity was low. Previous studies that did not convincingly demonstrate a lower chemosensitivity in aquatic birds (1, 5, 7, 25) may have been confounded by inappropriate timing of the tests. It is likely that experiments were done during the day when the respiratory system was most sensitive to chemical stimuli.

The correlation between high chemosensitivity and reduced dive times raises the question as to whether the respiratory chemosensory system plays a direct role in the control of dive times. If so, what kind of role is it? The aerobic dive limit concept is descriptive but not explanatory. That is, natural dive times of freely diving animals often fall within the predicted limit, but this does not tell us anything about whether O2 or any other correlated variables actually act to signal the animal to resurface to breathe. A threshold mechanism based on O2 content would implicate the respiratory chemosensory system, but such a scheme is likely to be too simplistic given what is known about the numerous mechanisms involved in respiratory control (11, 16).

We suggest an alternative hypothesis: that routine diving patterns are determined by the temporal characteristics of a sustained instability in the respiratory control system. The chemosensory system can be viewed as a damped feedback control loop with delay and variable feedforward drive (11, 16). Many diving vertebrates precede a series of dives with a short period of hyperventilation (6). This destabilizing maneuver is immediately followed by a step increase in metabolic rate and, through the reduction in cardiac output, a simultaneous lengthening of circulation time. Submersion of the head in water may also cause a step decrease in the central drive to breathe. The synchronized oscillations in metabolic rate (VO2, VCO2, and metabolic acid production), circulation delay, and perhaps central feedforward drive could conceivably give rise to periodic oscillations in respiratory output (11). This respiratory instability model predicts that the behavior of freely diving animals would become entrained to the natural frequency of oscillations in respiratory drive. The natural frequency of such oscillations is predicted to vary with such factors as the size of the O2 and CO2 stores, the buffering capacity of the body fluids, the intensity of the diving bradycardia, and the metabolic power input during underwater locomotion. In a feedback control system, for any given set of the above conditions, the amplitude and frequency of the oscillations would also be dependent on the gain (sensitivity) of the chemosensory system (11). Specifically, a reduction in the gain would tend to cause an increase in the period of the oscillation (i.e., increased dive times).

Some species of diving animals (e.g., whales, seals, penguins) may not show a circadian rhythm in respiratory chemosensitivity, because most of their activity budget involves diving, at least during foraging trips, which can last several weeks at a time (23, 24). Furthermore, it is likely that the control of dive times in ectothermic divers (e.g., turtles, sea snakes, crocodilians, amphibians, and air-breathing fishes) is more complicated than the proposed respiratory instability model would imply. The dependence of metabolism on such factors as water temperature and O2 tension, the increased capacity for anaerobic metabolism, the capacity for cardiac shunting and cutaneous gas exchange, and the interdependence of respiration and buoyancy all suggest that the simple model suggested above may not represent a complete or adequate description of the respiratory control process in diving ectotherms. Nevertheless, daily rhythms in dive depths and duration have been recorded in some species (e.g., leatherback sea turtle; Ref. 17), and it would be interesting to know whether this behavior is correlated with changes in respiratory chemosensitivity.

Further research is required to determine whether observed daily diving rhythms represent endogenous circadian rhythms or whether they represent a direct effect ("masking") of rhythmic stimuli, such as the light-dark cycle or food availability. For example, many diving birds and mammals exhibit a daily pattern in both the time of day that they dive and in the depth and/or duration of those dives (4, 14, 21, 23, 24, 33, 34). However, this daily pattern is often correlated with daily changes in the abundance and distribution of their prey and may not represent an endogenous circadian rhythm. This confounding variable is not likely to apply to canvasback ducks, however, because they forage for benthic invertebrates which do not show a daily rhythm in abundance. Preliminary observations in three ducks found that the day-night differences in dive durations were retained after several days in constant darkness (36).

In conclusion, this study has shown that canvasback ducks exhibit significant day-night differences in their respiratory responses to progressive asphyxia, which are correlated with circadian rhythms in diving behavior. Ducks dive most often, and for longer, at night when respiratory sensitivity to combined hypoxia and hypercapnia is lower. Further work is required to determine whether these observations bear any direct causal relationship and, if so, which mechanisms mediate these effects. The data suggest that diving performance may be facilitated by reduced respiratory sensitivity to progressive asphyxia and, furthermore, that the circadian timing system may serve to synchronize the behavioral and respiratory control systems in birds.

Perspectives

This study has confirmed and extended recent studies in rodents and humans (26-28, 30) suggesting that the respiratory control system may experience modulation by the circadian timing system. An important additional feature of the present study is that, by linking of the day-night differences in respiratory chemosensitivity to the voluntary diving behavior of the animals, it suggests an adaptive role for circadian modulation of respiratory control. If reduced chemosensitivity enables air-breathing animals to remain submerged for longer, this may increase the underwater foraging efficiency of the animals (9). The present study also raises the possibility that chemosensory characteristics favoring diving activities may not be optimal for the performance of other, nondiving behaviors. Ducks engage in numerous nondiving activities during the day. Some of these behaviors, such as swimming and flight, involve intense aerobic exercise (35), and there are data from human exercise studies to suggest that performance could be compromised by low respiratory chemosensitivity (10). Thus there may be a significant advantage to temporal separation of diving activities (apneic exercise) requiring low chemosensitivity and nondiving exercise requiring increased chemosensitivity. The present data suggest that both behavioral and respiratory rhythms are indeed synchronized in this way in ducks.

By providing a temporal organization to both behavior and physiology, the circadian timing system may serve to optimize overall locomotor performance and thereby enhance the evolutionary fitness of semiaquatic diving species.

    APPENDIX
Top
Abstract
Introduction
Methods
Results
Discussion
Appendix
References

Calculation of VO2 and VCO2 in a Closed-Circuit Plethysmograph

Rates of O2 consumption (VO2, ml/min STPD) and CO2 production (VCO2, ml/min STPD) of an animal in a closed chamber can be calculated from a knowledge of the volume of dry gas present in the chamber (Vc, ml STPD) and the instantaneous rates of change of the fractional concentrations of O2 (FO2) and CO2 (FCO2), respectively, in the dry gas. Thus
<A><AC>V</AC><AC>˙</AC></A><SC>o</SC><SUB>2</SUB> = Vc(F<SC>o</SC><SUB>2,1</SUB> − F<SC>o</SC><SUB>2,2</SUB>)/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A1a)
<A><AC>V</AC><AC>˙</AC></A><SC>co</SC><SUB>2</SUB> = Vc(F<SC>co</SC><SUB>2,2</SUB> − F<SC>co</SC><SUB>2,1</SUB>)/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A1b)
where subscripts 1 and 2 refer to quantities measured at the time at which the chamber is closed (t1) and at a later time (t2). The interval between t1 and t2 must be short enough to avoid violating the assumption of linearity that is implicit in this analysis.

Equations A1a and A1b only apply when the volume of gas within the chamber is constant over the measurement interval (t2-t1). This condition would be met if the respiratory exchange ratio (RER = VCO2/VO2) is equal to 1.0, or if an inert gas (N2) were added or removed at the appropriate rate under conditions in which RER is <1.0 or RER is >1.0, respectively. Under most circumstances, RER is <1.0, in which case the total number of gas molecules in the chamber will decrease over time, leading to a progressive overestimation of both FO2 and FCO2. Hence, the rate of decrease of FO2 (and therefore VO2) will be underestimated and the rate of increase of FCO2 (and therefore VCO2) will be overestimated by an amount that is dependent on the prevailing RER.

In the current experiments, the animal chamber was a fixed volume, so that the consequent change in the number of gas molecules resulted in a progressive decrease in pressure. However, the recirculation tubing had a significant compliance, so that the change in pressure could not be used to calculate the change in the number of dry gas molecules (using ideal gas law), nor could it be used reliably as a feedback signal for compensating infusions of N2. Therefore the following analysis was derived. For convenience, the quantities of gas are expressed as isobaric volumes (i.e., volumes that would be measured in a chamber of infinite compliance).

All equations refer to dry gas. The volume of gas (Vc) at the instant that the chamber is closed (t1) is known. The dry gas contains only O2, CO2 and inert gas (mainly N2) so that at any time
Vc = V<SC>o</SC><SUB>2</SUB> + V<SC>co</SC><SUB>2</SUB> + V<SC>n</SC><SUB>2</SUB> (A2a)
and
F<SC>o</SC><SUB>2</SUB> + F<SC>co</SC><SUB>2</SUB> + F<SC>n</SC><SUB>2</SUB> = 1 (A2b)
The volume of inert gas (VN2) is assumed to remain constant over time and is given by
V<SC>n</SC><SUB>2</SUB> = Vc ⋅ F<SC>n</SC><SUB>2</SUB> (A3a)
Rearranging and substituting Eq. A2b yields
V<SC>n</SC><SUB>2</SUB> = Vc ⋅ [1 − (F<SC>o</SC><SUB>2</SUB> + F<SC>co</SC><SUB>2</SUB>)] (A3b)
and
Vc = V<SC>n</SC><SUB>2</SUB> /[1 − (F<SC>o</SC><SUB>2</SUB> + F<SC>co</SC><SUB>2</SUB>)] (A3c)
At any time, the volumes of O2 (VO2) and CO2 (VCO2) are given by
V<SC>o</SC><SUB>2</SUB> = Vc ⋅ F<SC>o</SC><SUB>2</SUB> (A3d)
V<SC>co</SC><SUB>2</SUB> = Vc ⋅ F<SC>co</SC><SUB>2</SUB> (A3e)
and the rates of consumption of O2 and production of CO2 are
<A><AC>V</AC><AC>˙</AC></A><SC>o</SC><SUB>2</SUB> = &Dgr;V<SC>o</SC><SUB>2</SUB> /&Dgr;<IT>t</IT>   = (V<SC>o</SC><SUB>2,1</SUB> − V<SC>o</SC><SUB>2,2</SUB>)/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A4a)
<A><AC>V</AC><AC>˙</AC></A><SC>co</SC><SUB>2</SUB> = &Dgr;V<SC>co</SC><SUB>2</SUB> /&Dgr;<IT>t</IT>   = (V<SC>co</SC><SUB>2,2</SUB> − V<SC>co</SC><SUB>2,1</SUB>)/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A4b)
For situations in which RER is not equal to 1, the total volume of gas is different at t1 and t2; therefore Eqs. A4a and A4b can

be reexpressed by substituting Eqs. A3d and A3e
<A><AC>V</AC><AC>˙</AC></A><SC>o</SC><SUB>2</SUB> = (Vc ⋅ F<SC>o</SC><SUB>2,1</SUB> − Vc<SUB>2</SUB> ⋅ F<SC>o</SC><SUB>2,2</SUB>)/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A5a)
<A><AC>V</AC><AC>˙</AC></A><SC>co</SC><SUB>2</SUB> = (Vc<SUB>2</SUB> ⋅ F<SC>co</SC><SUB>2,2</SUB> − Vc ⋅ F<SC>co</SC><SUB>2,1</SUB>)/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A5b)
Substituting Eq. A3c to replace the unknown Vc2
<A><AC>V</AC><AC>˙</AC></A><SC>o</SC><SUB>2</SUB> = (F<SC>o</SC><SUB>2,1</SUB> ⋅ Vc − {F<SC>o</SC><SUB>2,2</SUB> ⋅ V<SC>n</SC><SUB>2</SUB> /[1 − (F<SC>o</SC><SUB>2,2</SUB> + F<SC>co</SC><SUB>2,2</SUB> )]})
/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A6a)
<A><AC>V</AC><AC>˙</AC></A><SC>co</SC><SUB>2</SUB> = ({F<SC>co</SC><SUB>2,2</SUB> ⋅ V<SC>n</SC><SUB>2</SUB> /[1 − (F<SC>o</SC><SUB>2,2</SUB> + F<SC>co</SC><SUB>2,2</SUB>)]} − F<SC>co</SC><SUB>2,1</SUB> ⋅ Vc)
/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A6b)
Substitute Eq. A3b to replace VN2
<A><AC>V</AC><AC>˙</AC></A><SC>o</SC><SUB>2</SUB> = [F<SC>o</SC><SUB>2,1</SUB> ⋅ Vc − ({F<SC>o</SC><SUB>2,2</SUB> ⋅ Vc ⋅ [1 − (F<SC>o</SC><SUB>2,1</SUB> + F<SC>co</SC><SUB>2,1</SUB>)]}
/[1 − (F<SC>o</SC><SUB>2,2</SUB> + F<SC>co</SC><SUB>2,2</SUB>)])]/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A7a)
<A><AC>V</AC><AC>˙</AC></A><SC>co</SC><SUB>2</SUB> = [({F<SC>co</SC><SUB>2,2</SUB> ⋅ Vc ⋅ [1 − (F<SC>o</SC><SUB>2,1</SUB> + F<SC>co</SC><SUB>2,1</SUB>)]}
/[1 − (F<SC>o</SC><SUB>2,2</SUB> + F<SC>co</SC><SUB>2,2</SUB>)]) − F<SC>co</SC><SUB>2,1</SUB> ⋅ Vc]/<IT>t</IT><SUB>2</SUB> − <IT>t</IT><SUB>1</SUB> (A7b)

    ACKNOWLEDGEMENTS

We thank Dr. C. Bluhm and the Delta Waterfowl and Wetlands Research Station, Manitoba, for providing the canvasback ducks.

    FOOTNOTES

This work was supported by the Natural Sciences and Engineering Research Council of Canada.

Address for reprint requests: R. Stephenson, Dept. of Zoology, University of Toronto, 25 Harbord St., Toronto, ON, Canada M5S 3G5.

Received 12 May 1997; accepted in final form 30 October 1997.

    REFERENCES
Top
Abstract
Introduction
Methods
Results
Discussion
Appendix
References

1.   Andersen, H. T., and A. Lovo. The effect of carbon dioxide on the respiration of avian divers (ducks). Comp. Biochem. Physiol. 12: 451-456, 1964.

2.   Bevan, R. M., E. Keijer, and P. J. Butler. A method for controlling the feeding behaviour of aquatic birds: heart rate and oxygen consumption during dives of different duration. J. Exp. Biol. 168: 199-217, 1992[Abstract/Free Full Text].

3.   Bouverot, P., and P. Sebert. O2-chemoreflex drive of ventilation in awake birds at rest. Respir. Physiol. 37: 201-218, 1979[Medline].

4.   Boyd, I. L., J. P. Y. Arnould, T. Barton, and J. P. Croxall. Foraging behaviour of Antarctic fur seals during periods of contrasting prey abundance. J. Anim. Ecol. 63: 703-713, 1994.

5.   Butler, P. J. The effect of progressive hypoxia on the respiratory and cardiovascular systems of the pigeon and duck. J. Physiol. (Lond.) 201: 527-538, 1970.

6.   Butler, P. J., and D. R. Jones. The comparative physiology of diving in vertebrates. Adv. Comp. Physiol. Biochem. 8: 179-364, 1982[Medline].

7.   Butler, P. J., and E. W. Taylor. The effect of hypercapnic hypoxia, accompanied by different levels of lung ventilation, on heart rate in the duck. Respir. Physiol. 19: 176-187, 1973[Medline].

8.   Butler, P. J., and E. W. Taylor. Responses of the respiratory and cardiovascular systems of chickens and pigeons to changes in PaO2 and PaCO2. Respir. Physiol. 21: 351-363, 1974[Medline].

9.   Carbone, C., and A. I. Houston. The optimal allocation of time over the dive cycle: an approach based on aerobic and anaerobic respiration. Anim. Behav. 51: 1247-1255, 1996.

10.   Casaburi, R., R. W. Stremal, B. J. Whipp, W. L. Beaver, and K. Wasserman. Alteration by hyperoxia of ventilatory dynamics during sinusoidal work. J. Appl. Physiol. 48: 1083-1091, 1980[Abstract/Free Full Text].

11.   Cherniack, N. S., and G. S. Longobardo. Abnormalities in respiratory rhythm. In: Handbook of Physiology. Respiratory System. Control of Breathing Bethesda, MD: Am. Physiol. Soc., 1986, sect. 3, vol. II, pt. 2, chapt. 22, p. 729-749.

12.   Colby, C., D. L. Kilgore, Jr., and S. Howe. Effects of hypoxia and hypercapnia on VT, f, and VI of nestling and adult bank swallows. Am. J. Physiol. 253 (Regulatory Integrative Comp. Physiol. 22): R854-R860, 1987[Abstract/Free Full Text].

13.   Craig, A. B., Jr., and A. Pasche. Respiratory physiology of freely diving harbor seals (Phoca vitulina). Physiol. Zool. 53: 419-432, 1980.

14.   Croxall, J. P., I. Everson, G. L. Kooyman, C. Ricketts, and R. W. Davis. Fur seal diving behaviour in relation to vertical distribution of krill. J. Anim. Ecol. 54: 1-8, 1985.

15.   Drorbaugh, J. E., and W. O. Fenn. A barometric method for measuring ventilation in newborn infants. Pediatrics 16: 81-86, 1955[Abstract/Free Full Text].

16.   Duffin, J. The chemoreflex control of breathing and its measurement. Can. J. Anaesth. 37: 933-942, 1990[Abstract/Free Full Text].

17.   Eckert, S. A., K. L. Eckert, P. Ponganis, and G. L. Kooyman. Diving and foraging behavior of leatherback sea turtles (Dermochelys coriacea). Can. J. Zool. 67: 2834-2840, 1989.

18.   Jacky, J. P. Barometric measurement of tidal volume: effects of pattern and nasal temperature. J. Appl. Physiol. 49: 319-325, 1980[Abstract/Free Full Text].

19.   Jones, D. R., and G. F. Holeton. Cardiovascular and respiratory responses of ducks to progressive hypocapnic hypoxia. J. Exp. Biol. 56: 657-666, 1972[Abstract/Free Full Text].

20.   Jones, D. R., and M. J. Purves. The effect of carotid body denervation upon the respiratory response to hypoxia and hypercapnia in the duck. J. Physiol. (Lond.) 211: 295-309, 1970[Abstract/Free Full Text].

21.   Kooyman, G. L. A comparison between day and night diving in the Weddell seal. J. Mammal. 56: 536-574, 1975.

22.   Kooyman, G. L., M. A. Castellini, R. W. Davis, and R. A. Maue. Aerobic dive limits in immature Weddell seals. J. Comp. Physiol. 151: 171-174, 1983.

23.   Kooyman, G. L., and T. G. Kooyman. Diving behaviour of Emperor penguins nurturing chicks at Coulman Island, Antarctica. Condor 97: 536-549, 1995.

24.   Le Boeuf, B. J., Y. Naito, A. C. Huntley, and T. Asaga. Prolonged, continuous, deep diving by northern elephant seals. Can. J. Zool. 67: 2514-2519, 1989.

25.   Milsom, W. K., D. R. Jones, and G. R. J. Gabbott. On chemoreceptor control of ventilatory responses to CO2 in unanesthetized ducks. J. Appl. Physiol. 50: 1121-1128, 1981[Abstract/Free Full Text].

26.   Peever, J., and R. Stephenson. Is the hypoxic ventilatory response in the rat time-of-day dependent? (Abstract). Physiologist 39: 180, 1996.

27.   Peever, J., and R. Stephenson. Day-night differences in the respiratory response to hypercapnia in awake adult rats. Respir. Physiol. 109: 241-248, 1997[Medline].

28.   Raschke, F., and K. H. Moller. Untersuchungen zur Tagesrhythmik der Chemosensitivitat und deren Beitrag zu nachtlichen Atmungsregulationsstorungen. Pneumologie 43: 568-571, 1989.

29.   Robin, E. D., V. H. Murdaugh, W. Pyron, E. Weiss, and P. Soteres. Adaptations to diving in the harbor seal---gas exchange and ventilatory response to CO2. Am. J. Physiol. 205: 1175-1177, 1963.

30.   Saiki, C., and J. P. Mortola. Hypoxia abolishes the morning-night differences of metabolism and ventilation in 6-day-old rats. Can. J. Physiol. Pharmacol. 73: 159-164, 1995[Medline].

31.   Stephenson, R. Diving energetics in lesser scaup (Aythya affinis, Eyton). J. Exp. Biol. 190: 155-178, 1994[Abstract].

32.   Tallman, R. D., Jr., and F. S. Grodins. Intrapulmonary CO2 receptors and ventilatory response to lung CO2 loading. J. Appl. Physiol. 52: 1272-1277, 1982[Abstract/Free Full Text].

33.   Thompson, D. Feeding ecology of diving ducks on Keokuk Pool, Mississippi River. J. Wildl. Manage. 37: 367-381, 1973.

34.   Thornburg, D. D. Diving duck movements on Keokuk Pool, Mississippi River. J. Wildl. Manage. 37: 382-389, 1973.

35.   Woakes, A. J., and P. J. Butler. Swimming and diving in tufted ducks, Aythya fuligula, with particular reference to heart rate and gas exchange. J. Exp. Biol. 107: 311-329, 1983[Abstract/Free Full Text].

36.   Woodin, M. A. Circadian Organization of Diving Behaviour and Respiratory Chemoreflexes in Birds (MSc thesis). Toronto, Canada: Univ. of Toronto, 1997.


AJP Regul Integr Compar Physiol 274(3):R686-R693
0363-6119/98 $5.00 Copyright © 1998 the American Physiological Society



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