An abrupt increase in ambient CO2 resulted in a marked respiratory acidosis which took place within 30 min. During this time there was a considerable reduction in the difference between arterial blood and inspired gas caused by an increase in ventilations. Prolonged CO2 exposure (24 h) showed that there was some compensation for the acidosis in that plasma bicarbonate concentrations increased substantially. At the same time, however, the of arterial blood always rose so that the net result was usually only a small increase in pH. Upon return to air, the blood was backtitrated along a buffer line elevated above and parallel to that seen during the initial response to hypercapnia. The fall in arterial blood during the early stages of recovery often led to pH values higher than those seen in the untreated animal. After 48 h in air, recovery had gone further with pH and [HCO3] levels approaching but rarely reaching the pre-exposure values.

In vertebrates, the evolutionary transition from water to land and development of aerial gas exchange has resulted in a substantial change in acid-base regulatory mechanisms. The properties of water as a medium for gas exchange and the design of fish gills together ensure that the levels of ate low with small CO2 gradients between arterial blood and water. Mammals, on the other hand, maintain large CO, gradients in the lung and can substantially alter by changes in ventilation so as to adjust the HCO3/CO2 ratio and therefore pHa.

Amphibians occupy an intermediate position between aquatic and terrestrial vertebrates. As evidenced by many studies, pulmonary gas exchange in the Amphibia is supplemented by skin-gas transfer by directing a portion of the circulation to a highly vascularized and very permeable skin (Krogh, 1904; Hutchison, Whitford & Kohl, 1968 ; Toews, Shelton & Randall, 1971). Thus, bimodal gas exchangers such as the Anura may alter and therefore pHa by either changing their pattern of lung ventiliation or adjusting CO2 removal across the skin. In addition, renal hydrogen ion excretion (Frazier & Vanatta, 1971, 1973 ; Ludens & Fanestil, 1972), as in most terrestrial tetrapods, may also be involved in pH regulation. Finally, as in the gill epithelium of fish, Cl uptake across the frog skin is coupled to HCO3 efflux (Motais & Garcia-Romeu, 1972) so CO2 may be excreted as molecular CO2 or HCO3and either process may be modulated to regulate pHa.

The marine toad Bufo marinus lives in diverse habitats ranging from tropical rainforests to deserts (McCutcheon & Hall, 1937; Stuart, 1951) which suggests that it can adapt physiologically to a wide variety of environmental conditions. For example, under natural conditions in the Amazon, Bufo marinus may encounter very hyper capnic waters (Toews & Macintyre, 1978) where CO2 gradients could be reversed across the skin. In addition, Macintyre (1975) has studied the defensive inflation in these animals and has shown that during long periods of apnoea (up to 20 min), in lung gas progressively increases to levels reaching 35 mmHg.

Hypercapnic conditions are therefore not uncommon in the natural habitat of Bufo marinus. Exposure to similar conditions in the laboratory enabled us to observe the response to an increased acid load and describe some of the processes associated with CO2 and hydrogen ion regulation in these animals.

The animals used in this study (Bufo marinus) were collected in Mexico and supplied commercially by the Mogul-Ed. Corp., Oshkosh, Wisconsin, U.S.A. Healthy animals of both sexes, ranging in weight from 300 to 500 g were maintained at room temperature (25 ± 2 °C) in large aquaria with water at one end.

### In vivo experiments

After the animals were anaesthetized in a 1·5 g/1 solution of tricaine methane sulphonate (Sandoz MS-222), the femoral artery of one leg was occlusively cannulated in the region of the thigh with an indwelling catheter prepared from Clay-Adams polyethylene tubing (P.E. 60; i.d. 0·76 mm, o.d. 1·22 mm). Prior to insertion, catheters were filled with heparinized amphibian Ringer (250i.u./ml) to prevent clotting, and 0·1 ml/kg of the solution was injected immediately following placement of the cannula. The catheter was then secured to the surrounding tissues with nylon suture and the wound was closed with Michel skin clips. All blood samples were taken from unanaesthetized free-moving animals following a minimum recovery period of 24 h.

For experimentation, an animal was placed in a 4 1 wide-mouthed jar which provided room for limited movements. The jar was placed on its side and 3–4 cm of tap water covered the floor of the chamber. Three holes (0·5 cm diameter) were bored in the bung closing the jar to allow passage of gases and cannulae. Toads were allowed a 3–5 h period of adjustment to the chamber before the experiments began. Following a period of time while the animals were breathing water-saturated air, a 5 % CO2-95 % air mixture was introduced into the chamber. The size of the jar allowed for abrupt changes between normal and elevated levels of ambient CO2. Several samples of blood for measurement of arterial blood pH (pHa), arterial CO2 tension and total CO2 content were taken during the normal, hypercapnic and post-hypercapnic periods.

For measurements, the blood was allowed to flow, using the animal’s blood pressure, through the catheter into a Radiometer thermostatted cell and CO2 electrode (Type E5036, with silicone membrane). The output was displayed on a Radiometer PHM 72 acid-base analyzer. The electrode system reached a constant reading some 3 min after the blood sample was admitted to the cell, after which blood was again allowed to flow through the cell so that a completely fresh sample was admitted. This procedure normally resulted in a further increase in the reading. After measurement, blood was returned to the animal by applying pressure to the system with a tuberculin syringe. We have shown that certain response characteristics of Radiometer CO2 electrodes (Type E5036) necessitate the use of such sample replacement methods for accurate determinations of (Boutilier et al. 1978). The CO2 electrode was calibrated frequently using water-saturated gases of known composition, corrected each day for atmospheric pressure and temperature effects.

Measurements of pHa were made at 25 °C using a Radiometer microelectrode unit (Type E5021) coupled with a Radiometer PHM-71 acid-base analyzer. A 40 μl blood sample was drawn from the arterial catheter and following determination, the sample was discarded. The pH unit was frequently calibrated at measurement temperature against Radiometer precision buffer solutions S1500 and S1510. Both CO2 and pH electrodes were held and calibrated at the same temperature as the animal. Calculations of means were carried out directly on the pH data without converting to H+ concentration. The differences resulting from the two calculations were small and had negligible effect on data plotted in the Figures.

Total CO2 determinations were made on 100 μl blood samples using the electrode and cuvette method described by Cameron (1971). Calibration of the instrument was carried out using standard bicarbonate solutions that were prepared fresh daily. The system was maintained at 36 °C so that the response time of the CO2 electrode was reduced at this higher temperature.

The amount of blood lost from the animal following each determination of pH, and total CO2 content was 140–160 μl.

### In vitro experiments

CO2 combining curves and blood buffer lines were determined on oxygenated whole blood which was drawn from either the aortic arch or femoral artery of pithed animals. Each series of determinations required 8 ml of blood which was very often pooled from several animals. Samples of blood (0·6 ml) were immediately transferred by pipette to heparinized round-bottomed tonometers.

For each set of determinations, the tonometric vessels were placed in a temperature-controlled horizontal shaker bath maintained at 25 °C. The blood was equilibrated with gas mixtures containing 0·6 %, 1 %, 2 %, 3 %, 5 %, and 7 % CO2, the balance of which was air. All of these gas mixtures were water-saturated and were continuously supplied from Wosthoff gas mixing pumps. After 1 h of equilibration, each blood sample was taken up with a gas-tight syringe and immediately (within 15 s) introduced into the electrode chambers for determination of total CO2 content and pH. The equilibrating gases continued to flow as the blood samples were removed from the tonometers.

CO2 combining curves and buffer lines were also constructed for true plasma at 25 °C using the same methods. True plasma curves were obtained by equilibrating whole blood samples (2 ml) with the various CO2 gas mixtures and then anaerobically centrifuging off the plasma for measurement of and pH at each To avoid CO2 losses through diffusion to the air during centrifugation, the equilibrated blood samples were taken up in gas-tight Hamilton syringes and introduced into the centrifuge tubes under a thin layer of mineral oil. The tubes were then immediately sealed and the plasma was separated from the red cells in less than 90 s. Samples of the true plasma were obtained at once by puncturing the seal with the needle of a gas-tight syringe.

Because the CO2 solubility coefficient and apparent first dissociation constant of carbonic acid () were not known, an additional series of experiments were undertaken to determine these constants for Bufo marinus plasma. The solubility of CO2 in toad plasma was determined after acidification of the plasma by the addition of a small amount of pure lactic acid (Van Slyke et al. 1928 ; Bartels & Wrbitzky, 1960). Aliquots (2 ml) of the acidified plasma were placed in thermostatically controlled tonometers and equilibrated with 100% CO2 at 25 °C following the procedure of Van Slyke et al. (1928). Carbon dioxide content was measured using 50 and 100 samples by the method of Cameron (1971). The solubility coefficient of CO2 in toad plasma was found to be 0·033 m-mol.l−1.mmHg−1 (Table 1). This value is considerably lower than the value of 0 ·0404 m-mol. 1−1. mmHg for mammalian blood plasma at 25 °C (Severinghaus, 1965) and the reason for the discrepancy is not known.

Table 1.

In vivo and in vitro respiratory characteristics of Bufo marinus whole blood and plasma at 25 °C.

The of separated plasma was determined gasometrically at different pH values (Truchot, 1976; DeLaney et al. 1977) by equilibrating 2 ml aliquots in temperature controlled tonometers (25 °C) with gas mixtures containing 2, 5 and 10% CO2 in air, obtained from Wösthoff gas mixing pumps. After 30 min of equilibration, CO2 contents and pH were measured as described before. The bicarbonate concentration was estimated using the formula:
and the was then calculated using the Henderson—Hasselbalch equation ( = 6·05, Table 1). These experimentally derived constants ( and ) were then used in the in vivo experiments to calculate plasma bicarbonate concentrations of the experimental animals from measurements of pH and

### In vivo determinations on arterial blood

The relationships between the measured values of arterial blood and pH seen during the course of a typical experiment on an individual Bufo marinus are plotted in Fig. 1. Plasma bicarbonate concentrations are also shown in the diagram as diagonal lines, the positions of which were calculated using the values for (6·05) and (0·033) determined for Bufo plasma at 25 °C (Table 1). The experimental protocol adopted in all these experiments was to take samples of blood (in replicate if possible from the animal after it had been allowed to settle in the chamber and was breathing air (point A, Fig. 1). A 5% CO2-95% air mixture was then admitted and further samples taken after 30 min and, in many cases, at times during the first 3–4 h of CO2 exposure (point B). The 5 % CO2 mixture was left running for a period of approximately 24 h and further samples were taken during the final 6 h of CO2 exposure point C). Finally, air was readmitted to the chamber and, as the animal recovered, samples of blood were taken over the first 4 h (point D) and the following 24–48 h (point E) if the catheter remained patent. In Fig. 2, data from six animals have been used to determine plasma bicarbonate concentrations from meaurements of and pH. The mean (± S.E.) of these bicarbonate concentrations are plotted against pH in a Davenport diagram for each of the five experimental stages described above and labelled A-E on both Figs. 1 and 2.

Fig. 1.

A pH-log $PCO2$ diagram showing the relationships between measured values of arterial blood pH and $PCO2$ during a typical hypercapnia experiment on an individual Bufo marinus. The positions of the diagonal lines indicate the plasma bicarbonate concentrations which were calculated using the Henderson-Hasselbalch equation. Numbers adjacent to individual data points from A to C represent the CO2 exposure time in hours. Similarly, those from C to E represent the time course of movements during recovery.

Fig. 1.

A pH-log $PCO2$ diagram showing the relationships between measured values of arterial blood pH and $PCO2$ during a typical hypercapnia experiment on an individual Bufo marinus. The positions of the diagonal lines indicate the plasma bicarbonate concentrations which were calculated using the Henderson-Hasselbalch equation. Numbers adjacent to individual data points from A to C represent the CO2 exposure time in hours. Similarly, those from C to E represent the time course of movements during recovery.

Fig. 2.

Davenport diagram showing arterial blood acid-base changes that occurred in six animals during the hypercapnia experiments. Mean (±S.B.) plasma bicarbonate concentrations are plotted as a function of plasma pH for the experimental stages A to E. The curved lines are calculated $PCO2$ isopleths. Arrows indicate the major movements.

Fig. 2.

Davenport diagram showing arterial blood acid-base changes that occurred in six animals during the hypercapnia experiments. Mean (±S.B.) plasma bicarbonate concentrations are plotted as a function of plasma pH for the experimental stages A to E. The curved lines are calculated $PCO2$ isopleths. Arrows indicate the major movements.

The initial effects of hypercapnia on arterial blood (A-B in Figs. 1 and 2) were rapid and usually complete within 30 min. No consistent changes were then seen in the next 4 h. The fall in pH and elevation of plasma bicarbonate represents a shift along a whole body buffer line substantially different from that determined for whole blood samples equilibrated in vitro (Fig. 5). During this initial respiratory acidosis it seems likely that an important response by the animal was a considerable, CO2 stimulated, hyperventilation since the difference between arterial blood and inspired gas was considerably reduced (12 mmHg when the animal was breathing in air, as against 2 mmHg during the initial exposure to 5 % CO2). More prolonged exposure to 5 % CO2 led to a considerable movement of arterial blood away from the in vivo buffer line. Samples taken after 18 h of exposure to high CO2 showed that there was some compensation for the respiratory acidosis in that bicarbonate concentrations in the plasma increased substantially (point C, Figs. 1 and 2). At the same time, however, the arterial blood always increased, suggesting that changes were also taking place in respiratory regulation causing a decrease in the CO2 induced hyperventilation. The net result of these two changes was usually an increase in pH which could be substantial in some individuals (Fig. 1, B-C). Because of the rise in pH compensation was often much less marked (Fig. 2, B-C). Since the arterial pH and were measured towards the end of the 24 h period of CO2 exposure, it is difficult to be certain that complete equilibrium had been reached, especially as the changes were occurring quite slowly. No clear-cut trends were obvious in the final samples taken before air was readmitted to the chamber, however, and it is probable that the major adjustments had occurred by the end of the 24 h period.

Fig. 5.

Davenport diagram showing Bufo marinus whole blood (•) and true plasma (○) buffer lines determined in vitro at 25 °C as in Fig. 4. Data points are means from at least six measurements. Lines fitted by least squares regression analysis, whole blood (r2 = 0·99), true plasma (r2 = 0·92). Dashed line is in vivo buffer line taken from data in Fig. 3. Numbers in brackets indicate the buffering capacity (ΔHCO3/ΔpH). Curved lines are calculated $PCO2$ isopleths.

Fig. 5.

Davenport diagram showing Bufo marinus whole blood (•) and true plasma (○) buffer lines determined in vitro at 25 °C as in Fig. 4. Data points are means from at least six measurements. Lines fitted by least squares regression analysis, whole blood (r2 = 0·99), true plasma (r2 = 0·92). Dashed line is in vivo buffer line taken from data in Fig. 3. Numbers in brackets indicate the buffering capacity (ΔHCO3/ΔpH). Curved lines are calculated $PCO2$ isopleths.

When the animal was allowed to breath air, the plasma pH increased and bicarbonate decreased along an in vivo buffer line (C-D, Figs. 1 and 2), above and probably parallel to that seen during the initial response to hypercapnia. It was noticeable that the early stages of the recovery process were more gradual than those observed at the onset of hypercapnia, and during the first 3 or 4 h of air breathing, continued to fall and pH to increase. The sudden removal of a high level CO2 stimulus must cause the respiratory control system to produce a substantial hypoventilation at first, thus slowing the recovery process. The eventual fall in , levels during the early stages of recovery often led to pH values higher than those seen in the untreated animal (Fig. 1) but during this time, plasma bicarbonate concentration was also beginning to decrease and pH stabilized around the 7·7 level. After 24 h in air, recovery had gone further with pH, and bicarbonate levels approaching (Figs. 1 and 2, point E), but rarely reaching during the period monitored, those seen prior to CO2 exposure.

The changes in total CO2 of whole blood are plotted in Fig. 3, the widths of the histogram blocks indicating the time spans over which blood samples were taken that contribute to the mean values shown. The effect of breathing a 5 % CO2 mixture on the total blood CO 2 concentration was to cause changes similar in direction but different in quantitative detail from those already described for plasma. There was an initial increase of some 3–4 m-mol/1 total CO2, and as hypercapnia was prolonged so that bicarbonate-pH compensation and respiratory changes occurred, the levels increased by a further 2–3 m-mol/1 CO2. When air breathing was resumed there was an initial rapid fall in total CO2, but even in the longer term the animals were unable to bring their blood CO2 back to the original air breathing levels. Plasma bicarbonate concentrations were calculated from , and pH as before so that the distribution of CO2 between plasma and red blood cells could be determined. It was assumed that the plasma carbonate was negligible and that the haematocrit was 25 %, this being the mean value as measured in arterial blood (Table 1). The difference between total CO2 in 1 1 of blood and the sum of bicarbonate and dissolved CO2 in 750 ml plasma represented the CO2 content of 250 ml of cells. The partitioning thus calculated is shown in Fig. 3 for both air breathing and hypercapnic periods. The assumption that dematocrit remains constant during hypercapnia was not justified experimentally. It is clear that the calculations will be in error if the red cells swell when carbon dioxide concentrations rise. Under these conditions, the plasma contribution to CO2 carriage will obviously be reduced. The partitioning that would be found if the haematocrit went up to 30% during the hypercapnia has also been indicated in Fig. 3.

Fig. 3.

Histogram showing the mean (±s.E.) changes in total CO2 content ($CCO2$) as partitioned for red cells (upper part of histogram block) and plasma (lower part), during in vivo hypercapnia experiments on six Bufo marinut. Distributions were calculated on the basis of 25 % haematocrit throughout. The effect on distribution of an increase to 30 % haematocrit is indicated on histogram blocks within the 5 % CO2 period. Widths of the histogram blocks indicate the time span over which blood samples were taken that contribute to the mean values shown. The blocks are labelled A to E as described in text.

Fig. 3.

Histogram showing the mean (±s.E.) changes in total CO2 content ($CCO2$) as partitioned for red cells (upper part of histogram block) and plasma (lower part), during in vivo hypercapnia experiments on six Bufo marinut. Distributions were calculated on the basis of 25 % haematocrit throughout. The effect on distribution of an increase to 30 % haematocrit is indicated on histogram blocks within the 5 % CO2 period. Widths of the histogram blocks indicate the time span over which blood samples were taken that contribute to the mean values shown. The blocks are labelled A to E as described in text.

As Fig. 3 illustrates, much of the increase in CO2 content of the blood during the early stages of hypercapnia was due to the greatly elevated levels in the red cells. As hypercapnia continued and total CO2 increased even further, there was a substantial redistribution so that most of this later increase was reflected in the rise in plasma concentration. Following the return to air breathing, the CO2 contained in the cells fell fairly rapidly, though, as has been noted above, the recovery processes were on the whole slow and incomplete.

### In vitro determinations on pooled blood samples

Carbon dioxide combining curves for Bufo marinus whole blood and true plasma are shown in Fig. 4. The curves were obtained from three independent sets of determinations on pooled blood samples from nine animals. True plasma is that which is in equilibrium with each different gas concentration and also in equilibrium with the red blood cells and differs markedly from separated plasma which would be in equilibrium with the erythrocytes only at the time of centrifugation (Roughton, 1964). The true plasma CO2 curve is similar in shape but elevated above that of the whole blood indicating that in vitro, as was seen in vivo (Fig. 3), greater concentrations of CO2 are carried as bicarbonate in the plasma than in any form within the RBC.

Fig. 4.

CO2 combining curves for Bufo marinus whole blood (•) and true plasma (○) determined in vitro at 25 °C. Data points are means from at least six measurements. Curves fitted by eye.

Fig. 4.

CO2 combining curves for Bufo marinus whole blood (•) and true plasma (○) determined in vitro at 25 °C. Data points are means from at least six measurements. Curves fitted by eye.

The buffering capacity of the non-bicarbonate blood buffers is defined as the negative slope of the [HCO3] v. pH line (ΔHCO3/ΔpH). Over the physiological range of arterial blood in Bufo, the whole blood and true plasma bicarbonate concentrations (calculated from the , measurements in Fig. 4 and the in Table 1) were found to vary linearly with pH (Fig. 5). As determined by least squares regression analysis, the slope of the true plasma buffer curve, and thus its buffering capacity, is greater than that of whole blood (Table 1, Fig. 5).

The slope of the true plasma buffer line obtained in vivo, during whole body CO2 titration (i.e. Point A to B, Fig. 2) is markedly lower than that found in vitro (Table 1, fig. 5). Furthermore, at a given plasma pH (over the range studied), the bicarbonate concentration in vivo is always considerably elevated above that seen in vitro (Fig. 5).

Although the slope of the in vitro buffer line is higher, the levels of bicarbonate measured in vitro are considerably lower than those seen in vivo at the same pH. This depression in plasma [HCO3] is likely caused by the presence of non-respiratory (i.e. metabolic) acids which may have been added to the circulation during blood collections. Seymour (1973), for example, collected blood from toads by cardiac puncture and found that only 30 s of struggling led to a fivefold increase in blood lactate levels. In our case, the struggling activity during pithing (20–30 s) is compounded by the additional time required (2–3 min) to expose the heart and draw a sufficiently large blood sample. It should be pointed out, however, that the appearance of metabolic acids in the blood will not affect the slope of the buffer line since they do not influence the concentations of non-bicarbonate blood buffers (principally haemoglobin).

When Bufo marinus are exposed to elevated ambient CO2 tensions, there is an initial rapid increase in arterial blood to a level above that in the environment. During this time, the number of lung ventilations increase and breathing patterns are altered so that lung inflations predominate (Macintyre & Toews, 1976). This hyper ventilatory response must therefore lead to the considerable reduction in the difference between to (points A and B, Fig. 1). The slow rise in blood at constant but elevated (B-C, Fig. 1) probably occurs when changes in the carbon dioxide receptor systems diminish breathing. There can be no doubt that CO2 sensitivity exists in the respiratory control system of these animals but it seems likely that prolonged exposure to hypercapnic conditions causes some adaptive changes in the overall receptor system. Such changes are well established in the chronic hypercapnic state in the mammal where pH adjustments of the cerebrospinal fluid, by increases in [HCO3]CSF causes some decrease in ventilatory drive. It is clear that Bufo is responding in the same overall fashion.

With the onset of hypercapnia, several extracellular processes are set in motion with each of the mechanisms proceeding simultaneously over progressively lengthening time courses. Figs. 1 and 2 illustrate that the blood acid-base disturbance associated with a step increase in occurs in two distinct stages: (1) an uncompensated respiratory acidosis, and (2) a subsequent compensatory phase. The initial response (A-B) is rapid and reaches steady-state values of plasma pH, and [HCO3] by 30–60 min. This process is analogous to that seen in man during whole body CO2 titration where the time necessary for interstitial fluid to reach steady-state levels (10–60 min) is a measure of how long it takes for blood and interstitial fluids to mix (Woodbury, 1974). Unlike the in vitro buffer line, the titration curve observed in vivo has a much reduced slope (Fig. 5, Table 1) which illustrates the effect that a largely unbuffered interstitial fluid has on the distribution of plasma [HCO3].

The involvement of compensatory processes such as transmembrane ion exchange, release of fixed carbonates and renal compensation are probably slow acting, as in mammals (Woodbury, 1974), so that during the initial stage of chemical buffering and distribution (i.e. A-B, Figs. 1 and 2) they probably exert only a negligible effect on extracellular fluid bicarbonate. This appears to be the case in Bufo where the initial respiratory acidosis persists at a steady state for approximately 4 h (point B, Figs. 1 and 2) before any of the known processes giving rise to transients in pH and [HCO3] of plasma are effectively set in motion. Assuming that the blood buffering capacity stays the same, the Davenport analysis clearly illustrates that the compensatory gain of plasma bicarbonate (B-C, Fig. 2) must be caused by processes other than an increased solubility of CO2 in the blood. The origin of this plasma [HCO3] was not investigated in these experiments but additions from the tissues and hydrogen ion excretion from the plasma space represent the most likely candidates.

Figs. 3 and 4 show that a much greater proportion of the overall blood CO2 content (principally in the form of bicarbonate) is carried in the plasma than in the red blood cells, reflecting the generally lower erythrocytic pH. The proportionally greater increase in erythrocytic as compared to plasma during the early stages of hypercapnia (Fig. 3) probably reflects the enhanced capacity for bicarbonate formation in the RBC. As CO2 penetrates the erythrocyte it dissociates to form H+ and HCO3 By virtue of the buffering power of the negatively charged haemoglobin molecule, the H+ are mopped up and thus more HCO3 can be formed intracellularly; by comparison, H+ are only weakly buffered in the plasma. In mammalian erythrocytes, the majority of bicarbonate ions formed when H+ combine with haemoglobin are exchanged for plasma Cl (i.e. chloride shift). A similar outward migration of HCO3- in the blood of Bufo would serve to explain why the whole blood buffer value is lower than that of true plasma (Table 1). Because the increased RBC [HCO3] would increase the total number of osmotically active particles within the RBC it seems likely that H2O entry and swelling would also occur when blood is elevated. Although the swelling phenomenon was not investigated during these experiments, subsequent data has shown that the maximum erythrocytic volume is reached asymptotically as blood, tensions approach the 5 % level (unpublished data).

During prolonged hypercapnia (B-C), the carriage of CO2 by the RBC remained unchanged even though both and plasma [HCO3] increased considerably (Figs. 13). If we assume that CO2 can still readily penetrate the erythrocytic membrane, then upon a further increase in (B-C), it is surprising that the RBC CO2 pool does not increase as a direct result of the intracellular hydration of CO2, as was the case during the initial stages of hypercapnia (i.e. A-B). In fact, it appears that either HCO3 ions are excreted or H+ ions are taken up by the erythrocytes during this period since levels rise. What is clear is that only a small portion of the large gain in plasma [HCO3] seen during the B-C shift could be contributed by the red cells.

The blood acid-base changes accompanying the recovery period involve two processes whose time courses are different. Firstly, the plasma [HCO3] decreases such that an in vivo buffer line (C-D) develops parallel to and elevated above that of the initial response to hypercapnia (Fig. 2). In effect the animal is backtitrated along the original in vivo buffer slope to the pre-exposure pHa with the time course most likely being governed by ventilation. The redistribution of between red cells and plasma during the early stage of recovery (Fig. 3) further suggests that this initial recovery process (C-D) reflects the reverse of those interactions between blood and interstitial fluid during whole body CO2 titration. Because the differences in plasma [HCO3] between points D-A and B-C are similar, it seems likely that any further changes were slow to act and were the result of a redistribution of the base excess contributed by the tissues. Only three of the six animals studied approximated a return to original blood acid-base levels (one of which is shown in Fig. 1) and this occurred only after several days of recovery.

We should like to thank Mr D. H. Macintyre and Drs D. G. McDonald, W. W. Burggren, and D. G. Smith for their suggestions and criticisms during the preparation of the manuscript. This study was sponsored by the N.A.T.O. Research Grants Programme.

Bartels
,
H.
&
Wrbitzky
,
R.
(
1960
).
Bestimmung des CO2 - Absorptions Koeffizienten zwischen 15 und 38 °C in Wasser und Plasma
.
Pflilgert Arch. get. Physiol
.
371
,
162
168
.
Boutilier
,
R. G.
,
Randall
,
D. J.
,
Shelton
,
G.
&
Toews
,
D. P.
(
1978
).
Some response characteristics of CO2 electrodes
.
Respir. Physiol
.
32
,
381
388
.
Boutilier
,
R. G.
,
Randall
,
D. J.
,
Shelton
,
G.
&
Toews
,
D. P.
(
1979
).
Acid-base relationships in the blood of the toad. Bufo marinus. II. The effects of dehydration
.
J. exp. Biol
.
82
,
345
355
.
Cameron
,
J. N.
(
1971
).
Rapid method for determination of total carbon dioxide in small blood samples
.
J. appl. Physiol
.
31
,
632
634
.
Delaney
,
R. G.
,
Lahiri
,
S.
,
Hamilton
,
R.
&
Fishman
,
A. P.
(
1977
).
Acid-base status and plasma composition in the aestivating lungfish (Protopterus)
.
Am. J. Physiol
.
232
(
1
),
R10
R17
.
Frazier
,
L. W.
&
Vanatta
,
J. C.
(
1971
).
Excretion of H+ and NH4+ by the urinary bladder of the acidotic toad and the effect of short-circuit current on the excretion
.
Biochim. biophys. Acta
241
,
20
29
.
Frazier
,
L. W.
&
Vanatta
,
J. C.
(
1972
).
Evidence that a plasma factor(s) stimulates H+ and NH4+ excretion in the toad bladder
.
Proc. Soc. exp. Biol. Med
.
139
,
336
339
.
Frazier
,
L. W.
&
Vanatta
,
J. C.
(
1973
).
Characteristics of H+ and NH4+ excretion by the urinary bladder of the toad
.
Biochim. biophys. Acta
311
,
98
108
.
Garcia-Romeu
,
F.
,
Salibian
,
A.
&
Pezzani-Hernandez
,
S.
(
1969
).
The nature of in vivo sodium and chloride uptake mechanisms through the epithelium of the Chilean frog Calyptocephalella gayi (Dum. et Bibr., 1841)
.
J gen. Physiol
.
53
,
816
835
.
Hutchison
,
V. H.
,
Whitford
,
W. G.
&
Kohl
,
M.
(
1968
).
Relation of body size and surface area to gas exchange in anurans
.
Physiol. Zool
.
41
,
65
85
.
Krogh
,
A.
(
1904
).
On the cutaneous and pulmonary respiration of the frog
.
Skand. Archiv. Physiol
.
15
,
328
419
.
Ludens
,
J. H.
&
Fanestil
,
D. D.
(
1972
).
.
Am. J. Physiol
.
223
,
1338
1344
.
Macintyre
,
D. H.
(
1975
).
Respiratory mechanics and acid-base regulation in Bufo marinus marinus (L
.).
M.Sc. thesis
,
,
.
Macintyre
,
D. H.
&
Toews
,
D. P.
(
1976
).
The mechanics of lung ventilation and the effects of hypercapnia on respiration in Bufo marinus
.
Can. J. Zool
.
54
,
1364
1374
.
Mccutcheon
,
F. H.
&
Hall
,
F. G.
(
1937
).
Hemoglobin in the Amphibia
.
J. cell. comp. Physiol
.
9
,
191
197
.
Motais
,
R.
&
Garcia-Romeu
,
F.
(
1972
).
Transport mechanisms in the teleostean gill and amphibian skin
.
Ann. Rev. Physiol
.
34
,
141
176
.
Roughton
,
F. J. W.
(
1964
).
Transport of oxygen and carbon dioxide
.
In Handbook of Physiology
, vol.
1
(ed.
W. O.
Fenn
and
H.
Rahn
), pp.
767
825
. Am. Physiol. Soc.,
Washington, D.C
.
Severinchaus
,
J. W.
(
1965
).
Blood gas concentrations
.
In Handbook of Physiology, Section 3 : Respiration
, vol.
2
(ed.
W. O.
Fenn
and
H.
Rahn
), pp.
1475
1487
. Am. Physiol. Soc.,
Washington, D.C
.
Seymour
,
R. S.
(
1973
).
Physiological correlates of forced activity and burrowing in the spadefoot toad, Scaphiopur hammondii
.
Copeta
1
,
103
114
.
Simkiss
,
K.
(
1968
).
Calcium and carbonate metabolism in the frog (Rana temporaria) during respiratory acidosis
.
Am. J. Physiol
.
214
,
627
634
.
Stuart
,
L. C.
(
1951
).
The distributional implications of temperature tolerances and hemoglobin values ft in the toads Bufo marinus (Linnaeus) and Bufo bocourti Brocchi
.
Copeia
3
,
220
229
.
Sulze
,
W.
(
1942
).
Uber die physiologische Bedeuting des Kalkasackchenapparates der Amphibien
.
Arch. ges. Physiol
.
246
,
250
257
.
Toews
,
D. P.
,
Shelton
,
G.
&
Randall
,
D. J.
(
1971
).
Gas tensions in the lungs and major blood vessels of the urodele amphibian. Amphiuma tridactylum
.
J. exp. Biol
.
55
,
47
61
.
Toews
,
D.
&
Macintyre
,
D.
(
1978
).
Respiration and circulation in an apodan amphibian
.
Can. J. Zool
.
56
,
998
1004
.
Truchot
,
J. P.
(
1976
).
Carbon dioxide combining properties of the blood of the shore crab, Carcinus maenas (L.) : Carbon dioxide solubility coefficient and carbonic acid dissociation constants
.
J. exp. Biol
.
64
,
45
57
.
Van Slyke
,
D. D.
,
Sendroy
,
J. JR.
,
Hastings
,
A. B.
&
Neill
,
J. M.
(
1928
).
The solubility of carbon dioxide at 38 °C in water, salt solution, serum and blood cells
.
J. biol. Chem
.
78
,
765
799
.
Vaughan
,
G. A.
(
1976
).
.
B.Sc. thesis
,
,
.
Woodbury
,
J. W.
(
1974
).
Body acid-base state and its regulation
.
In Physiology and Biophysics
, vol.
2
(ed.
T. C.
Ruch
and
H. D.
Patton
).
:
W. B. Saunders Co
.
Ziegler
,
T. W.
,
Ludens
,
J. H.
&
Fanestil
,
D. D.
(
1974
).