The gas transport system of a bumblebee was investigated by measuring the oxygen partial pressure PO2 in the wing muscle. In the resting bee, PO2 showed a regular pattern of fluctuation with a typical period of 70–120s. Fluctuations in muscular PO2 were associated with intermittent abdominal pumping. Ventilation by abdominal movements may not be necessary during rest because PO2 is high (8.5–9.2kPa) in the anaesthetised bee. Thermal effects on muscular PO2 were examined by cooling the bee, causing the amplitude of PO2 fluctuations to increase. In most flight experiments, the bee started to fly after elevating muscle PO2 by abdominal pumping; muscle PO2 then decreased at the onset of flight. However, when a flight began without pre-flight ventilation, PO2 increased monotonically. During flight, muscle PO2 reached a mean level (6.36±1.83kPa) that was much higher than the lowest value recorded during discontinuous ventilation during rest. The bumblebee effectively uses abdominal movements to assist in convective gas transport not only during flight but also at rest.
Insects use the tracheal network to supply oxygen to the tissues; this network consists of air-filled tubes (tracheae), passive diaphragms (air sacs) and valves (spiracles) (Mill, 1985). The design of the tracheal system varies dramatically among species. Mechanisms of oxygen transport also differ; for example, some aquatic insects do not have spiracles but exhibit a tracheal network in appendages that function like a fish gill (e.g. mayfly larvae, Miller, 1974). In some circumstances, insects ventilate intermittently (once an hour or less), perhaps to reduce evaporative water loss (e.g. silkworm pupae, Levy and Schneiderman, 1966).
Even in flying insects, the design of the respiratory organs and the mechanisms involved vary widely. Gas transport in the hawkmoth Agrius convolvuli (Komai, 1998) has been investigated previously. While diffusive gas transport supplies sufficient oxygen at rest, the moth uses convective gas transport during flight. Contraction of the flight muscle causes a ventilating air flow in the tracheae that augments gas transport to meet increased oxygen demand. For some conditions, this increased oxygen supply is more than sufficient to meet the increased demand, and the oxygen partial pressure in the flight muscle therefore increases as flight activity increases.
A foraging bumblebee has one of the highest recorded flight metabolic rates (Wolf et al., 1996). During the short rests that may follow a flight, one can observe intense pumping movements of the abdomen. The bee’s abdomen is well equipped with muscles for both contraction and extension (Snodgrass, 1984) and the bee also has well-developed air sacs in the abdomen and in the thorax. In the present study, the oxygen partial pressure, PO2, in a wing muscle of the bumblebee Bombus hypocrita hypocruta was measured directly using a needle electrode, and the relationship between PO2 and ventilation/flight activity was investigated.
Materials and methods
A colony of the bumblebee Bombus hypocrita hypocruta (L.) was obtained from Koppert Biological Systems. The bees were kept in the nest box in which the colony had been obtained, and pollen was periodically placed in the nest box. Worker bees were used in experiments (N=47). Anatomical investigations of the thorax and muscle dimensions were carried out (as described by Komai, 1998) using frozen sections (N=10) and dissections (N=10). The muscle fibre diameter and the tracheole density were measured from microphotographs.
Oxygen partial pressure was measured by inserting an oxygen microelectrode directly into a thoracic flight muscle of a tethered bumblebee under a microscope. To avoid unnecessary damage to the bee, it was first anaesthetised using carbon dioxide. The hairs on the thoracic tergites were removed, and the back of the bee then was attached using adhesive (neoprene, G17, Konishe) to a stainless-steel pipe (1.3mm in diameter) with its head downwards. The mounting pipe was connected to a metal pole and attached to a manipulator. A segment of thoracic cuticle measuring approximately 0.3mm×0.5mm was removed, and the electrode was inserted through this opening into the dorsal longitudinal muscle (Fig.1). This route of electrode insertion was termed path 1. Beneath the thoracic tergites lie air sacs and flight muscles that attach directly to the tergites, so damage to the muscle or the air sac during removal of the cuticle or insertion of the electrode was unavoidable. A second route of electrode insertion was therefore also used to investigate the effects of the opening procedure (Fig.2). In path 1, only the muscle was potentially damaged during electrode insertion, whereas in path 2 the air sac was also punctured by the electrode. No observable differences were found between the results from the two electrode paths.
The polarographic and coaxial electrode (Pt-Ag/AgCl, −0.6V) had a tip diameter of 2–8μm (Baumgärtl, 1987). Dissolved oxygen undergoes reduction on the platinum cathode as follows:
The current produced is proportional to the oxygen partial pressure at a position just outside the recess in the electrode tip. The reduction current of the electrodes used here ranged from 200pA to 2nA in water bubbled with air and from 2 to 50pA in water bubbled with nitrogen. Taking into account the memory storage of the picoammeter, a sampling frequency of 10Hz and 16-bit resolution were chosen. The estimated response time of the electrode was shorter than 0.1s, so the time resolution in this measurement system was 0.1s. The electrode was calibrated in Theorel buffer (Baumgärtl, 1987) equilibrated by bubbling with gas mixtures of oxygen and nitrogen, and thermally regulated at 30°C. Five-point calibrations (0, 5, 10, 15 and 20% O2) were performed three times for each experimental measurement, twice before the measurement and once after it. The mean correlation coefficient (r) between the reduction current and the oxygen partial pressure was 0.9984 over 122 calibrations. The electrode surface sometimes became contaminated by tissue following an experimental measurement. In the worst case, the reduction current decreased by 20% following the measurement. Therefore, any conversion from reduction current to oxygen partial pressure was performed using the calibration curve acquired after each measurement. Room temperature was monitored using a platinum thermometer. Data from the picoammeter (M6517, Keithley Instruments) and the thermometer (M2001, Keithley Instruments) were fed into a personal computer via a general-purpose interface bus (GPIB). The bee was videotaped at 30framess−1 using a miniature CCD camera (WV-KS152, Panasonic) for later analysis of its measurements. A time code was superimposed on the video recording by the video timer (VTG-22, For.A) to synchronize the PO2 recording. Periods of flight and ventilation were identified from the wing and abdominal movements, respectively. In bees exhibiting large-amplitude abdominal ventilation, the ventilation period could be determined within an accuracy of three frames, while in bees with small, rapid abdominal movements, the period could not be determined. In flying bees with an electrode inserted along path 2, the ventilation period was determined from movements of the exposed thoracic air sac with the same accuracy. Other details of the experimental arrangement can be found in Komai (Komai, 1998).
Tissue contamination decreased the sensitivity of the electrode. Such changes after electrode insertion were monitored in paralyzed bees and showed that the electrode output decreased over approximately the first 5min following insertion and then stabilized. In all experiments, insertion at an arbitrary depth was made 10min before a measurement to minimize the effects of this sensitivity change. Each animal was subjected to only a single insertion. Experiments were limited to 2h because flight activity decreased over time in some bees. In this paper, a recording of one animal is termed a run.
Measurements of oxygen partial pressure were carried out at rest, during paralysis and during tethered flight. The measurement conditions for the figures are listed in Table1. In resting experiments, 12 animals were investigated to examine the relationship between variation in PO2 and ventilation behaviour. The electrode was inserted into the dorsal longitudinal muscle at four different depths (usually to 500, 1000, 1500 and 2000μm) for 30min each. If the bee struggled during insertion of the electrode, measurements were started when the bee became calm. Periods during which the bee moved its legs or wings during recording were excluded from analysis. During measurements, room temperature and ambient light intensity were kept constant. In one animal, behaviour after recovery from anaesthesia was recorded after the resting experiment; the bee was anaesthetised by placing a piece of chloroform-soaked paper near its head. In three animals, a cooling/rewarming experiment was performed after the resting measurement of 1h; an ice pack was placed approximately 2cm beneath the bee for 30min and was then removed; this was repeated twice.
Twenty-five animals were used in paralysis experiments to obtain a spatial profile of PO2 in the flight muscle. The bee was paralyzed by injection of 0.1ml of 10−5moll−1 tetrodotoxin into the haemolymph at the neck intersegmental membrane approximately 10min before inserting the electrode. The electrode was moved from a depth of 300μm to a depth of 2440μm in steps of 20μm (108 measurement points). PO2 was measured for 40s at each depth.
Ten animals were used in the flight experiments. Measurements were made at four different depths for 30min each: 500, 1000, 1500 and 2000μm. When the electrode had been positioned at a particular depth, the bee was allowed to rest for 10min and was then induced to fly (see below) four or five times. After a second 10min rest period, a further four or five flights were recorded at the same depth. Flight was initiated by giving the bee a piece of wet tissue paper (1cm2) to hold with its legs. The bee rotated the tissue horizontally using its feet for several seconds, then dropped the paper and usually initiated flight for 10–15s. The middle legs of the bee were removed for the flight experiment because flight activity was inhibited when the middle legs contacted or held the mounting arrangement.
Muscle PO2 showed regular fluctuations in resting bees (Fig.3A). The most common pattern was a triangular waveform with a rapid increase and a slower decrease in PO2. Movements of the abdomen dorsally and ventrally coincided with the increases in PO2. The mean amplitude of the PO2 fluctuations was 7.10±1.12kPa (mean ± s.d., N=12) and the mean duration was 79.0±1.6s (range 70–120s). During the experiment shown in Fig.3A, the bee ventilated for an average of 8.3±1.3s during each ventilation cycle, with an abdominal pumping frequency of 2.1±0.4Hz. The abdominal movements cause air to be moved towards the thorax from the abdomen, filling the thoracic air sacs with fresh air (Bailey, 1954). Eventually, PO2 in the muscle increased. In some experiments, PO2 levels fluctuated rapidly, as shown in Fig.3B. Abdominal movements in these experiments also corresponded with increases in PO2.
Fig.4 shows the relationship between the length of the non-ventilatory period and both the amplitude of the PO2 fluctuations and the minimum values of PO2. Amplitude increased and minimum PO2 decreased with increasing non-ventilatory period. Tolerance of low PO2 may reduce the cost of ventilation; for example, minimum muscle PO2 fell almost to zero in Fig.3A. It is known that diffusion alone can sustain basal metabolic rate in a resting insect (Weis-Fogh, 1964). The mean PO2 over a ventilation cycle varied widely from 1.78 to 7.65kPa (4.88±1.45kPa, mean ± s.d., N=162) and was not correlated with the length of the non-ventilatory period (r=−0.239 for run 1, r=0.365 for run 4, r=−0.738 for run 5; all P>0.05; N=49, N=80, N=33 for run 1, run 4 and run 5, respectively). In some bees, mean PO2 decreased as non-ventilatory period increased, but in others the opposite trend was found. This suggests that stabilization of muscle PO2 is not the primary function of discontinuous ventilation.
PO2 variation in a bee anaesthetised with chloroform vapour is shown in Fig.3C. In this bee, PO2 remained high (8.5–9.2kPa) even when the bee ceased abdominal ventilation. Until the bee began ventilating at around 5min, no abdominal movements were observed, although the legs occasionally moved slowly. The PO2 pattern after abdominal pumping began differed from that in an unanaesthetised bee. When abdominal pumping stopped, PO2 decreased much more slowly in the anaesthetised bee, giving the PO2 peaks a plateau. It is possible that the spiracles remain open for this period after abdominal pumping ceases in the anaesthetised bee, although spiracle movements were not observed in this study.
Many authors have proposed that discontinuous ventilation functions to reduce water or heat loss (Hadley and Quinlan, 1993; Lighton et al., 1993). Therefore, it was of interest to determine how temperature and humidity affect the pattern of muscle PO2. Fig.3D,E shows the effects of cooling and subsequent rewarming on the pattern of muscle PO2 variation. Placing an ice pack approximately 2cm beneath the bee at the onset of the recording shown in Fig.3D caused the PO2 cycle to increase in amplitude. This effect was observed in six out of six experiments from three animals. The pattern shown at the end of Fig.3D continued for a further 15min. It was clear that the bee was not cryo-anaesthetised by the cooling procedure because it could still beat its wings (data not shown). The ice pack was removed at the onset of the recording shown in Fig.3E and the rhythmic PO2 cycle disappeared (note the different time scale in Fig.3E). From the present results, we cannot determine whether the cooling or dehydrating effect of the ice pack had the greater effect on the PO2 pattern.
As described above, PO2 in the bee decreased between periods of abdominal pumping. A spatial profile of PO2 within the muscle was recorded in resting bees in preliminary experiments; however, consistent results could not be obtained because of large temporal variations in PO2. To assess how PO2 varies spatially within the muscle, the bee was paralyzed with an injection of tetrodotoxin into the haemolymph. This procedure prevented abdominal pumping, and the oxygen supply to the muscle was therefore by diffusion alone. The PO2 profile was determined by inserting the oxygen electrode into the thorax in 20μm increments (Fig.5). The PO2 profile showed a gradual decrease as depth increased; superimposed on this decrease were large, acute fluctuations. Muscle fibres in the dorsal longitudinal muscle were elliptical, measuring 38.2±6.3μm×55.1±10.1μm in transverse section (N=445 from four animals; mean ± s.d.), among which tracheae 13.5±2.8μm in diameter were located 46.6±8.8μm apart (N=16 from one animal). Tracheoles tapering to less than 1μm in diameter penetrated into each of the muscle fibres after bifurcating from the surrounding tracheae. The tracheae among the muscle fibres ran in all directions. It is likely that PO2 is uniformly high outside the muscle fibres and decreases rapidly towards the centre of each muscle fibre, thus producing the sharp PO2 peaks seen in Fig.5.
Fig.6 is a histogram of the distance between the local peaks in the vertical PO2 profiles. The interpeak distance of 60–80μm is similar to the muscle fibre diameter. Scatter within the histogram may be caused by the electrode path crossing the fibre axis at different angles or puncturing the fibre off centre.
PO2 variation in a flight muscle was measured at four different muscle depths in a single bee (Fig.7). Steady-state conditions during flight could not be achieved because the bee beat its wings for a maximum period of only 15s. However, two points should be noted. First, flight did not always result in a decrease in PO2 but instead caused it to approach asymptotically the mean value of 6.36±1.83kPa. While PO2 decreased from the onset of the flight in Fig.7A (e.g. from 8.25 to 5.85kPa in the first flight shown), in other flights PO2 increased (e.g. from 1.20 to 3.22kPa for the flight ending at 0:58min in Fig.7B) or remained unchanged (e.g. from 5.77 to 5.63kPa for the flight ending at 0:43min in Fig.7D). The most common pattern was a decrease in muscle PO2 at the onset of flight because the bee usually preceded a period of flight by elevating flight muscle PO2 using abdominal pumping. Second, mean PO2 during flight was higher than mean resting PO2 (Table2). The bee continuously contracted and expanded its abdomen during tethered flight. After flight movements ceased, the PO2 cycle gradually returned to the regular large-amplitude resting pattern (e.g. Fig.7A).
Comparison of mean PO2 among experimental conditions
Mean muscle PO2 is summarized in Table2. Resting values were divided into two groups, depending on whether the bee exhibited large- or small-amplitude PO2 fluctuations and according to whether PO2 amplitude was greater than 60% of maximum PO2 or less than 40%. Resting values were used only when the bee did not change its ventilation pattern, move its legs or beat its wings for 15min. PO2 amplitudes of 40–60% of maximum PO2 were observed only rarely (four out of 37 recordings). Flight values were used when the bee beat its wings for periods greater than 5s (mean 13.3±9.7s). PO2 during the last 2s of 2–11 flights was averaged for each animal.
The mean PO2 was highest for the small-amplitude resting category, and PO2 in the large-amplitude category was the lowest among the four conditions. Changes in oxygen consumption caused by flight or by paralysis also affected PO2.
Bees appear to use convective ventilation for gas exchange during rest and flight and exhibit abdominal pumping for approximately 11% of a ventilation cycle. Ventilation was continuous during tethered flight, so the volume of air inspired will increase approximately 10-fold. If we assume that the oxygen concentration in the expired air does not differ between rest and flight, a flying bee must consume 10 times as much oxygen as a resting bee. Kammer and Heinrich (Kammer and Heinrich, 1974) measured the oxygen consumption of the bumblebee Bombus vosnesenskii under various conditions and showed that the oxygen consumption of a flying bee was 42–50 times greater than that of a resting bee at a thoracic temperature of 25°C. They found an approximately twofold increase in oxygen consumption for every 5°C increase in thoracic temperature in resting bees. This suggests that the oxygen consumption during tethered flight in the present study was 17–30 times that during rest at a thoracic temperature of 28.5–31.5°C. These estimates suggest that the efficiency of gas exchange is higher during flight than in a resting bee because oxygen consumption increases more than 17-fold while the volume of inspired air increased only 10-fold. In resting bees, muscle PO2 changed substantially during ventilation, so the efficiency of oxygen exchange will also have varied over time because this efficiency is proportional to the PO2 difference between the inspired air and the tissues.
Effects of thoracic temperature
The sensitivity of a polarographic electrode is affected by the temperature of the surrounding medium. The sensitivity of the electrode used here increases linearly by 2.8%°C−1 with increasing temperature (Komai, 1998). In preliminary experiments, simultaneous insertion of a thermocouple was found to suppress flight activity, so thoracic temperature was not measured in the present study. However, any effects of temperature may be negligibly small. Room temperature was 28.5–31.5°C and was controlled to within 0.5°C during measurements. Analysis of the non-flight conditions excluded data where the bee moved its legs or wings, so the thoracic temperature should be equilibrated with the ambient temperature during the measurement. Muscle shivering was not observed under non-flight conditions. In the flight experiments, the bees flew briefly 4–5 times over 2–3min followed by a rest period of 10min or more before subsequent flights. Thus, heat production during the first set of flights should not affect the subsequent flights. The mean total time spent flying for the 4–5 flights was 34.5s, and the longest flight lasted 23.9s. The maximum rate of increase in thoracic temperature during flight that can be calculated from the data of Kammer and Heinrich (Kammer and Heinrich, 1974) is 2.8°Cmin−1; in the hawkmoth, this value is 3.1°Cmin−1, and the rate of decrease after a flight is 2.4°Cmin−1 (Komai, 1998), so the increase in thoracic temperature is likely to be less than 1.1°C (=2.8/60×23.9) in the flight measurements, giving a possible overestimation of PO2 of less than 3.3%. The difference in mean PO2 between flight and resting with the large-amplitude pattern is statistically significant (P<0.05) even when the temperature change of 1.1°C is taken into account.
Gas transport in resting animals
In Fig.8, the rate of change in muscle PO2 from the onset of ventilation or flight is plotted. Muscle PO2 changed asymptotically from the beginning of a series of abdominal contractions, indicating that fresh air is convected close to the muscle fibres by the ventilatory air flow but that diffusion of oxygen into the muscle fibres determines the rate of PO2 change. Old air in the tracheal network is rapidly replaced by convection within the first few abdominal contractions, and oxygen then diffuses towards the muscle fibres. At the beginning of a series of abdominal contractions, PO2 in the muscle fibres rose steeply because oxygen flux is proportional to the PO2 difference between the muscle fibre and the point to which fresh air is convected. As PO2 increases in the muscle fibre, the oxygen diffusion gradient gradually decreases. Finally, muscle PO2 will reach a plateau when the oxygen supply balances the metabolic rate. The oxygen supply to the muscle is therefore a diffusion-based phenomenon. Abdominal pumping prevents the tracheal PO2 from decreasing. The pattern of change in PO2 observed here in resting animals is consistent with the above description, although PO2 during abdominal contractions did not reach a steady state, suggesting that the bee ceases ventilation when PO2 reaches a certain level.
The time required to reach steady state can be used to determine the extent of the diffusion-dominated region around and within the muscle fibre. The time taken (δt) to diffuse a certain distance (δl) is given by the equation:
where D is diffusivity; for oxygen in water, D=2.5×10−5cm2s−1. If we take δt as 6–10s (i.e. where the change in muscle PO2 returns to zero in Fig.8), the distance δl is 120–160μm. The muscle fibre is an ellipse measuring 38.2±6.3μm×55.1±10.1μm in transverse section, and the surrounding tracheae are distributed 46.6±8.8μm apart. The calculated distance δl is therefore similar to, although slightly larger than, the expected diffusion distance based on the muscle structure. This may suggest that fresh air does not flow all the way to the muscle fibre during abdominal pumping. However, analysis is difficult without precise geometrical information because the muscle is heterogeneous, and diffusivities in the cytoplasm and across the tracheole wall, which may be a barrier to gas transport, are not known. The resting bumblebee therefore uses convective gas transport for bulk movement of air into the tracheal system, but the final step in gas exchange is diffusion-limited.
Gas transport during flight
At the onset of flight, muscle PO2 began to change immediately, irrespective of the direction of this change. The rate of oxygen consumption increases dramatically at the initiation of flight (17-fold or more), so the oxygen levels immediately surrounding a muscle fibre will be reduced as the oxygen is consumed by mitochondria. Oxygen will diffuse from the tracheole into the muscle fibre according to the PO2 gradient thus established. An initial reduction in PO2 should, therefore, occur in the flight muscle of the bumblebee as the PO2 gradient becomes established; however, this was not observed during measurements (some of the lines for flight are positive in the first second in Fig.8), implying that it may be too rapid or too small to detect using the present methods. In other words, muscle PO2 decreases until fresh air reaches the muscle fibres.
To interpret these results, gas transport phenomena must be considered. Because the tracheole is blind-ending, the concentration field near the muscle fibre is dominated by diffusive gas transport. The absence of an initial reduction in PO2 levels on flight initiation in the present recordings suggests that it occurs in less than 0.1s. In the muscle fibre, a period of less than 0.1s implies that the mitochondria are located close to the tracheoles. The exact period will depend on the time taken to develop the concentration gradient between the mitochondrion and the tracheole. For oxygen flux into the muscle fibre to increase within 0.1s, it can be estimated from equation 3 that the diffusion distance must be less than 1.5μm between the mitochondrion and the tracheole (D=2.5×10−5cm2s−1). In addition, the value 0.1s suggests that the bee can create and utilise ventilatory flow to the immediate vicinity of the muscle fibre. If unidirectional flow occurs from the abdominal air sac to the thoracic air sac, an initial reduction in PO2 should have been detected because it must take longer than 0.1s for oxygen to diffuse from a thoracic air sac to a tracheole through the trachea (δl=2–3mm, D=0.21cm2s−1). However, such flow has not been shown to exist; no specific tracheal structures have been identified that would allow unidirectional flow.
From Fig.8, approximately 10s was required for dPO2/dt to reach zero, although fresh air reached the immediate vicinity of the muscle fibre just after flight initiation. Diffusion in the muscle fibre determines the time to reach a steady-state PO2 during flight; it is not determined by diffusion from the tracheole to the mitochondrion but by diffusion from the tracheoles to the centre of the muscle fibre. In principal, the time to reach the steady state is the same as in the resting bee.
Control of the respiratory system
Alterations to ventilatory behaviour at the onset of locomotion are common in vertebrates and invertebrates. Ramirez and Pearson (Ramirez and Pearson, 1989) recorded electromyograms from the flight muscle and the respiratory muscle, and action potentials from the neurons, in a locust, Locusta migratoria, and identified an interneurone that linked flight to respiration. This interneurone, which controls the initiation of flight, resets the respiratory system at the onset of flight; respiration ceases for several seconds and then restarts with an elevated ventilation frequency. These findings indicate that the locust respiratory system is controlled by a feedforward mechanism at the initiation of flight.
The present results imply that a feedforward mechanism also controls respiratory behaviour during bumblebee flight. If a feedback mechanism were involved, a time lag should exist. In a feedback mechanism, controlling factors such as oxygen shortage, carbon dioxide excess and the presence of humoral agents must be detected by appropriate receptors in the flight muscle before respiratory behaviour can be altered. However, muscle PO2 did not always decrease at the onset of flight, and the ventilatory frequency changed simultaneously with the onset of flight.
An increase in respiration rate after exercise is commonly observed in insects, and factors such as tracheal PO2 and PCO2 and haemolymph pH are considered to be responsible. Krolikowski and Harrison (Krolikowski and Harrison, 1996) measured tracheal ventilatory pressure to evaluate precisely the respiratory rate following locomotion (continuous jumping) in a locust Melanoplus differentialsi, after injecting acid or base into the haemolymph or replacing the tracheal gas with several gas mixtures. Their results showed that post-exercise respiration rate was not affected by changes in haemolymph pH, PO2 or PCO2 or by tracheal PO2 or PCO2. They suggested that a humoral feedback mechanism was possible together with a neuronal feedforward mechanism. In the post-flight bumblebee, the PO2 cycle usually increased in amplitude to the regular large-amplitude pattern within 1min of the flight. However, a gradual transition to this pattern lasting longer than 3min (e.g. Fig.7A) and cases in which intermittent ventilation directly followed flight were occasionally observed. As can be seen from Fig.7A, muscle PO2 could be restored to pre-flight values within 15s, which is less than the time taken to restore the regular large-amplitude pattern following flight. Thus, tracheal and tracheolar PO2 will be restored before the PO2 cycle returns to the pre-flight pattern. This result suggests that humoral metabolites or a neuronal feedforward mechanism control the post-flight PO2 pattern.
Comparison with the hawkmoth
In a recent study (Komai, 1998), PO2 was measured in a hawkmoth Agrius convolvuli thorax using the same methods. The resting oxygen demands of the hawkmoth are met by diffusion, so PO2 is constant in the resting moth. The structure of the flight muscles differs between the bee and the moth, and the spatial PO2 profile therefore also differs. The dorsal longitudinal muscle of the hawkmoth consists of four layers, each 1000–1500μm thick. Tracheal trunks lie between the layers; the bifurcated tracheae penetrate the muscle layer. In hawkmoths, PO2 is highest between the muscle layers, gradually decreasing within a layer with distance from the surface. The PO2 difference between the inside and outside of the muscle layer is approximately 3kPa. The PO2 difference between the outside and inside of a muscle fibre is approximately 0.5kPa; in the paralysed bumblebee, it is 1.4kPa.
PO2 variation during flight also differs between the bumblebee and the hawkmoth. In the bumblebee, PO2 appeared rapidly to approach a constant value (6.36kPa) after the onset of flight. In contrast, PO2 in the hawkmoth dropped rapidly in the first few seconds of flight, then increased and reached a plateau after 2min. During moth flight, muscle PO2 was higher than during rest in some cases, indicating that the augmented oxygen supply exceeded the local oxygen demand. The observed differences between these species may be due to differences in their tracheal network and gas transport mechanism. The tracheal network runs uniformly throughout the bumblebee’s flight muscle, but that in the hawkmoth is dendric towards the centre of the muscle layers. While the flying bee ventilates in the same way during rest and flight, the moth switches its ventilation mechanism during flight from diffusion to convection. Since the moth does not have air sacs to contract, oxygen supply at rest occurs by diffusion. Without compressible air sacs, the hawkmoth uses deformation of the tracheae by the contracting flight muscles to drive ventilatory air flow during flight. Tidal volume is small in the moth. The ventilatory flow in the bee is a unidirectional periodic flow of large volume and low frequency (approximately 3Hz); that in the moth is an oscillatory flow of small tidal volume and high frequency (approximately 30Hz).
The bumblebee and the hawkmoth use different methods of ventilation (abdominal pumping and muscle pumping, respectively), and other large insects can use both ventilation methods. The behaviour of the spiracles of locusts (Miller, 1960), dragonflies (Miller, 1962) and beetles (Miller, 1966) was found to be synchronized with abdominal movements, suggesting unidirectional air flow in the tracheae. Weis-Fogh (Weis-Fogh, 1967) measured the volumetric change in the tracheal network as a function of wing angular position and estimated that the volumetric change was large enough to contribute to gas transport during flight in a locust. The PO2 variation in the muscles of these insects is unknown, so the degree to which the two ventilation methods contribute to gas exchange is not yet understood.
The design of the tracheal network and the ventilation method should be related to other factors too. For example, the hawkmoth Agrius convolvuli remains stationary during the day and flies only at night (Kiguchi and Shimoda, 1994). Furthermore, the adult moth rarely feeds. Respiration by diffusion alone must be economical, and the absence of movements may assist the moth to avoid predation. However, the hawkmoth will be unable to tolerate extended dry periods because the spiracles remain open.
I thank H. Baumgärtl for technical advice on the oxygen microelectrode. The electrode was produced in collaboration with K. Tanishita and K. Oka at Keio University.