Relationship between hypercapnic and hypoxic stimuli of respiration during muscular activity]

Pulmonary ventilation (V) and alveolar gas composition (PACO2, PAO2) were studied in 12 healthy men who performed gradual muscular work under conditions of controlled hypercapnia, hypoxia, hyperoxia or their combinations. The respiratory response was estimated by absolute values of ventilation at the given PACO2 value and by its rise by 1 mm Hg of increased PACO2 (delta V/delta PACO2) under rest and under transitional and steady-state exercise. The exercise on-switch was accompanied by displacement to the top and an increased slope of the response curve (delta V/delta PACO2) not related to the work load. These changes suggest multiplicative interaction of the neurogenic and hypercapnic drives in the load switch-on. During steady-state exercise an important role of the hypoxic drive was revealed: hypoxemia induced a shift of the delta V/delta PACO2 response curve to a higher level, especially with the great work load. Thus the positive interaction between the hypercapnic and hypoxic respiratory drive augments with muscular exercise.     

Estimates of mean alveolar PCO2 during steady-state exercise in man: a theoretical study.

The partial pressure of carbon dioxide in arterial blood is an important operator in the control of breathing, by actions on peripheral and central chemoreceptors. In experiments on man we must often assume that lung alveolar PCO2 equals arterial PCO2 and obtain estimates of the former derived from measurements in expired gas sampled at the mouth. This paper explores the potential errors of such estimates, which are magnified during exercise. We used a published model of the cardiopulmonary system to simulate various levels of exercise up to 300 W. We tested three methods of estimating mean alveolar PCO2 (PACO2) against the true value derived from a time average of the within-breath oscillation in steady-state exercise. We used both sinusoidal and square-wave ventilatory flow wave forms. Over the range 33-133 W end-tidal PCO2 (P(et)CO2) overestimated PACO2 progressively with increasing workload, by about 4 mmHg at 133 W with normal respiratory rate for that load. PCO2 by a graphical approximation technique (PgCO2; "graphical method") underestimated PACO2 by 1-2 mmHg. PCO2 from an experimentally obtained empirical equation (PnjCO2; "empirical method") overestimated PACO2 by 0.5-1.0 mmHg. Graphical and empirical methods were insensitive to alterations in cardiac output or respiratory rate. End-tidal PCO2 was markedly affected by respiratory rate during exercise, the overestimate of PACO2 increasing if respiratory rate was slowed. An increase in anatomical dead space with exercise tends to decrease the error in P(et)CO2 and increase the error in the graphical method. Changes in the proportion of each breath taken up by inspiration make no important difference, and changes in functional residual capacity, while important in principle, are too small to have any major effect on the estimates. Changes in overall alveolar ventilation which alter steady-state PACO2 over a range of 30-50 mmHg have no important effect. At heavy work loads (200-300 W), P(et)CO2 grossly overestimates by 6-9 mmHg. The graphical method progressively underestimates, by about 5 mmHg at 300 W. A simulated CO2 response (the relation between ventilation and increasing PCO2) performed at 100 W suggests that a response slope close to the true one can be obtained by using any of the three methods. The graphical method gave results closest to the true absolute values. Either graphical or empirical methods should be satisfactory for detecting experimentally produced changes in PACO2 during steady-state exercise, to make comparisons between different steady-state exercise loads, and to assess CO2 response in exercise.(ABSTRACT TRUNCATED AT 400 WORDS)     

Heart rates and gas exchange in the Amazonian Manatee (Trichechus inunguis) in relation to diving

Unrestrained Amazonian manatees (Trichechus inunguis) maintained a constant heart rate during diving and exhibited a slight tachycardia during breathing. 'Forcing' the manatees to dive caused a marked bradycardia. They exhibited a more pronounced tachycardia during breathing after 'forced' dives and hyperventilated during recovery dives. Manatees are capable of dives exceeding 10 min duration without having to resport to anaerobic metabolism, and even after 10 min dives recover within 3-4 short dives. The ability of manatees to make long dives, in spite of relatively poor O2 stores, is due to their low metabolic rate, while the rapid recovery is aided by their high CO2 stores which minimizes CO2 storage in the body. In manatees the changes in alveolar O2 and CO2 pressure (PAO2 and PACO2) in relation to dive time are slower and more variable than in other marine mammals. The lower rate of change is probably due to the manatees' reduced metabolic rate, while the greater variability is due to their breathing pattern, in which both ventilation and body gas stores influence alveolar gases.     

Effects of upper or lower airway anesthesia on hypercapnic ventilation in humans

To evaluate the contribution of vagal airway receptors to ventilatory control during hypercapnia, we studied 11 normal humans. Airway receptor block was induced by inhaling an aerosol of lidocaine; a preferential upper oropharyngeal block was also induced in a subgroup by gargling a solution of the anesthetic. Inhalation of lidocaine aerosol adequate to increase cough threshold, as measured by citric acid, did not change the ventilatory response to CO2, ratio of the change in minute ventilation to change in alveolar PCO2 (delta VI/delta PACO2), compared with saline control. Breathing pattern at mean CO2-stimulated ventilation of 25 l/min showed significantly decreased respiratory frequency, increased tidal volume, and prolonged inspiratory time compared with saline. Resting breathing pattern also showed significantly increased tidal volume and inspiratory time. In nine of the same subjects gargling a lidocaine solution adequate to extinguish gag response without altering cough threshold did not change delta VI/delta PACO2 or ventilatory pattern during CO2-stimulated or resting ventilation compared with saline. These results suggest that lower but not upper oropharyngeal vagal airway receptors modulate breathing pattern during hypercapnic as well as resting ventilation but do not affect delta VI/delta PACO2.     

Step changes in end-tidal CO2: methods and implications.

A dynamic end-tidal forcing technique for producing step changes in end-tidal CO2 with end-tidal O2 held constant independent of the ventilation response or the mixed venous return is introduced for characterizing the human ventilation response to end-tidal CO2 step changes for both normoxic (PAO2 = 125 Torr) and hypoxic (PAO2 = 60 Torr) conditions. The ventilation response approaches a steady state within 5 min. In normoxia, the on-transient is faster than the off-transient, presumably reflecting the action of cerebral blood flow. The hypoxic step response is faster than the normoxic response presumably reflecting the increased contribution from the carotid body. The delay in the ventilation response after the change in end-tidal CO2 is less in hypoxia than in normoxia and reflects the action of a transport delay and that of a virtual delay. These delays are interpreted with respect to the high-frequency phase shift data for the same subject, generated using sinusoidal end-tidal forcing. The methods of others for experiments utilizing step changes in inspired CO2 are considered with respect to our methods.     

A comparison of indirect methods for continuous estimation of arterial PCO2 in men

Four different measures (PETCO2, PACO2, PADCO2, and PJCO2) for indirectly estimating arterial PCO2 (PaCO2) from respired gas at the mouth have been investigated. PETCO2 was the end-tidal PCO2. PACO2 was calculated using a reconstruction of the alveolar oscillation of PCO2 obtained from the end-tidal "plateau" in PCO2. PADCO2 was calculated as for PACO2 except that the effects of dead space were incorporated. PJCO2 was calculated from an empirical relationship involving PETCO2 and tidal volume. Six subjects were studied at rest and during cycle ergometry at 50 and 100 W while breathing a variety of gas mixtures. Arterial samples were drawn for determination of true PaCO2. The differences for each method between estimated and true PaCO2 at rest and at 50 and 100 W were as follows: PETCO2, -1.35 +/- 2.64, 1.67 +/- 2.31, and 2.67 +/- 2.02 (SD) Torr; PaCO2, -2.15 +/- 2.73, -0.80 +/- 2.18, and -0.35 +/- 2.31 (SD) Torr; PADCO2, -1.55 +/- 2.54, 0.25 +/- 2.16, and 0.63 +/- 2.26 (SD) Torr; and PJCO2, -1.41 +/- 2.30, 0.12 +/- 1.79, and 0.08 +/- 1.96 (SD) Torr. It is concluded that, at rest, all methods significantly underestimate true PaCO2 and during exercise PETCO2 significantly overestimates PaCO2, but no bias was detected for any of the other methods.     

A visual aid for teaching ventilation-perfusion relationships

To help students understand the concept of the ventilation-perfusion ratio (VA/Q) and the effects that VA/Q mismatching has on pulmonary gas exchange, a "sliding rectangles" visual aid was developed to teach VA/Q relationships. Adjacent rectangles representing "ventilation" and "perfusion" are slid past one another so that portions of the ventilation and perfusion rectangles are not touching, illustrating the concepts of dead-space ventilation (VD) and shunt flow (QS). The portion of the ventilation bar representing VD is further subdivided into anatomical and alveolar VD and used to show the effects of alveolar dead space on the PO2 (PAO2) and PCO2 of alveolar air (PACO2); movement away from the "ideal" point). Similarly, the portion of the perfusion bar representing QS is used to define anatomical and physiological shunts and the effect of shunts on the PO2 (PaO2) and PCO2 of arterial blood (PaCO2). The genesis of the PAO2-PaO2 (A-a) PO2 difference as well as the effects of VA/Q mismatching and diffusion abnormalities can all be discussed with this visual aid. This approach has greatly assisted some students in mastering this traditionally difficult area of respiratory physiology.     

Reduced oxygen diffusion across the shell of Gray gull (Larus modestus) eggs

Gray gulls, Larus modestus, nest 1500 m above sea level in northern Chile's Atacama Desert, one of the driest in the world. Their eggshell gas permeability, one third of that found in other Larus species, is an adaptation that reduces water loss, but at the expense of oxygen diffusion into the air cell with resultant hypoxia and reduced metabolic rate. This contrasts with characteristics found in birds nesting at very high altitudes where oxygen diffusion across the egg shell is maximized at the expense of water conservation. The oxygen consumption (MO2) of Larus modestus is 66% that of Larus argentatus; the oxygen conductance (GO2) is equivalent to 48% of that obtained in 5 other bird species. The oxygen partial pressure (PAO2) in the air chamber of Larus modestus (84 Torr) is lower than that of 10 other bird species whose average (PAO2) is 106 Torr. The CO2 partial pressure (PACO2) in the air chamber of Larus modestus is 68 Torr, a higher value than that found in 9 other bird species whose average (PACO2) is 39 Torr.     

Slow respiratory stimulant effect of hyperoxia in chemodenervated decerebrate cats.

A direct stimulating action of oxygen on the CO2 respiratory control system was determined from steady-state and dynamic observations in unanesthetized decerebrate cats. In peripheral nerve-intact animals, inhalation of oxygen (1 atm) produced a small but significant shift to the left as well as a decrease in slope in the steady-state VT vs. log PACO2 relationship. Carotid sinus neurotomy more than doubled the shift, to the extent that the mean PACO2 apneic point was lowered by 6.5 mmHg. Neither vagotomy nor chronic ablation of the area postrema had any detectable influence on the stimulating effect of oxygen on CO2 responsiveness. The arterial-alveolar PCO2 difference, prior to and following carotid chemo-denervation, remained unchanged or was increased by a negligible amount during oxygen inhalation. The oxygen threshold for respiratory stimulation, obtained isocapnically, occurred between 115 and 200 mmHg; VT then increased exponentially tending to level off as PAO2 approached 1 atm. The dynamic response to sudden presentation of oxygen after carotid chemodenervation consisted of a monotonic rise in VT, starting after 20-30 s with a t 1/2 of about 75 s.     

Control of depth and frequency of breathing during baroreceptor stimulation in cats.

In 10 tracheotomized anesthetized cats during steady-state inhalation of various concentrations of CO2 and O2, the acute respiratory response to baroreceptor stimulation produced by transient inflation of a balloon placed in the descending aorta was studied. The latter induced a sudden rise in mean arterial pressure, ranging from 62 to 95 mmHg. At all PACO2 levels above 30 mmHg, elevation in arterial pressure was accompanied by an immediate drop in tidal volume (VT) and prolongation of the durations of inspiration (Ti) and total breath (Ttot). Breaths obtained during baroreceptor stimulation fell along the same VT vs. Ti and VT vs. Ttot relationships obtained in the normotensive state, suggesting that the lung volume-related vagal control of Ti and Ttot is unaffected by changes in arterial pressure. Since, for a given change in arterial pressure, a constant reduction in VT was obtained at all PACO2 levels above 30 mmHg, it can be concluded that the interaction between PACO2 and arterial pressure is additive. In three cats, at PACO2 levels below 30 mmHg, aortic obstruction resulted in brief periods of apnea. Following apnea, the control of Ti and Ttot was transiently offset, describing hysteresis pathways on the VT vs. Ti and VT vs. Ttot relationships.     

Ventilatory control during exercise with increased external dead space

Effects of increased external dead space (VD) on ventilatory control in steady-state exercise were determined in three healthy adults. The subjects performed cycle ergometer exercise on six occasions, each with a different VD (range: 0.1--1.0 liter); work rate was incremented every 5 min by 15--20 W. Minute ventilation (VE), CO2 output (VCO2), and mean alveolar PCO2 (PACO2) were measured in the steady state. Without VD, the VE-VCO2 relationship was linear, having a small positive VE intercept, and PACO2 was constant, independent of VCO2. Increased VD was associated with an upward shift of the VE-VCO2 relationship, and an elevated PACO2, again independent of VCO2. At each work rate, the increases in VE accompanying increased VD were no greater than could be expected from a conventional CO2 inhalation study. It is concluded that increasing external dead space does not impair the ability of the human respiratory system to regulate PACO2 during exercise except for resetting the regulated PCO2 level.     

Validation of a maskless CO2-response test for sleep and infant studies

The Hazinski method is an indirect, noninvasive, and maskless CO2-response test useful in infants or during sleep. It measures the classic CO2-response slope (i.e., delta VI/delta PCO2) divided by resting ventilation Sr = (VI'--VI')/(VI'.delta PCO2) between low (')- and high (')-inspired CO2 as the fractional increase of alveolar ventilation per Torr rise of PCO2. In steady states when CO2 excretion (VCO2') = VCO2', Hazinski CO2-response slope (Sr) may be computed from the alveolar exchange equation as Sr = (PACO2'--PICO2')/(PACO2'--PICO2') where PICO2 is inspired PCO2. To avoid use of a mask or mouthpiece, the subject breathes from a hood in which CO2 is mixed with inspired air and a transcutaneous CO2 electrode is used to estimate alveolar PCO2 (PACO2). To test the validity of this method, we compared the slopes measured simultaneously by the Hazinski and standard steady-state methods using a pneumotachograph, mask, and end-tidal, arterial, and four transcutaneous PCO2 samples in 15-min steady-state challenges at PICO2 23.5 +/- 4.5 and 37 +/- 4.1 Torr. Sr was computed using PACO2 and arterial PCO2 (PaCO2) as well as with the four skin PCO2 (PSCO2) values. After correction for apparatus dead space, the standard method was normalized to resting VI = 1, and its CO2 slope was designated directly measured normalized CO2 slope (Sx), permitting error to be calculated as Sr/Sx.(ABSTRACT TRUNCATED AT 250 WORDS)     

Human respiration at rest in rapid compression and at high pressures and gas densities

Ventilation (V), end-tidal PCO2 (PACO2), and CO2 elimination rate were measured in men at rest breathing CO2-free gas over the pressure range 1-50 ATA and the gas density range 0.4-25 g/l, during slow and rapid compressions, at stable elevated ambient pressures and during slow decompressions in several phases of Predictive Studies III-1971 and Predictive Studies IV-1975. Inspired O2 was at or near natural O2 levels during compressions and at stable high pressures; it was 0.5 ATA during decompressions. Rapid compressions to high pressures did not impair respiratory homeostasis. Progressive increase in pulmonary gas flow resistance due to elevation of ambient pressure and inspired gas density to the He-O2 equivalent of 5,000 feet of seawater was not observed to progressively decrease resting V, or to progressively increase resting PACO2. Rather, a complex pattern of change in PACO2 was seen. As both ambient pressure and pulmonary gas flow resistance were progressively raised, PACO2 at first increased, went through a maximum, and then declined towards values near the 1 ATA level. It is suggested that this pattern of PACO2 change results from interaction on ventilation of 1) increase in pulmonary resistance due to elevation of gas density with 2) increase in respiratory drive postulated as due to generalized CNS excitation associated with exposure to high hydrostatic pressure. There may be a similar interaction between increased gas flow resistance and increase in respiratory drive related to nitrogen partial pressure and the narcosis resulting therefrom.     

Local regulation of pulmonary blood flow and ventilation-perfusion ratios in the coatimundi.

Small catheters (ca. 3 mm diam at tip) were wedged in subsegmental bronchi in anesthetized coatimundi (Nasua nasua) during spontaneous breathing. Mixed expired gases of a group of lobules were sampled continuously without contamination from neighboring units, and local tidal volume, frequency, carbon dioxide production, and oxygen consumption were measured, as well as mixed venous PO2 and PCO2. Local ventilation-perfusion ratio, alveolar PO2, PCO2, and blood flow were calculated. There was a 22% reduction (range 15-38) in local perfusion (as percent of flow at PAO2 100 mmHg) per 10 mmHg fall in local alveolar oxygen tension over the PAO2 range 150-36 mmHg. Local hypercapnia had little effect on local flow. Local tidal volume (ca. 1% of total tidal volume) was unaffected by changes in alveolar gas tensions. The contribution of vasoconstriction or vasodilatation, as a negative feedback system, to the stability of local PAO2 was greatest close to the physiologic range (65-85 mmHg) falloderate efficiency.     

Ventilatory interaction between hypoxia and [H+] at chemoreceptors of man.

By measuring ventilation during isocapnic progressive hypoxia, peripheral chemoreceptor sensitivity to acute hypoxia (deltaV40) was measured in five normal young men under four sets of conditions: 1) at sea level at the subject's resting PCO2, 2) at sea level with PCO2 5 Torr above resting PCO2, 3) after 24 h at a simulated altitude of 4,267 m (PB = 447 Torr) at the subject's resting PCO2 measured during acute hyperoxia, and 4) after 24 h at high altitude, with PCO2 elevated to the subject's sea-level resting PCO2. With this experimental design, we were able to systematically vary the PCO2 and [H+] at the peripheral and central chemoreceptors of man. When mean pHa was decreased from 7.424 to 7.377 without significant change in PACO2, the mean deltaV40 increased from 18.0 to 55.9 1/min. Conversely, when mean PACO2 was altered between 33.8 and 41.6 Torr with pHa held relatively constant, the mean deltaV40 did not change. This suggests that it is the H+ and not CO2 which interacts with hypoxia in stimulating the ventilation of man. An additional finding was that the intrinsic sensitivity of the peripheral chemoreceptors to acute hypoxia did not change during 24 h of acclimatization to high altitude.     

Temporal effects in the estimation of pulmonary diffusing capacity

Steady state estimates of the pulmonary diffusing capacity for carbon monoxide (DLCO) require measurement of the uptake and the average alveolar partial pressure of carbon monoxide (PACO). The expired alveolar sample obtained by different experimental methods and/or breathing patterns rarely represents the actual PACO. It is widely accepted that nonuniform distribution of ventilation, diffusion and perfusion causes discrepancies in the measurement of diffusing capacity. tan additional source of error in choosing PACO arises in the sampling time chosen by the experimental method. A theoretical study of a ramp-with-pause and a square breathing pattern demonstrates that the sample-time error exists even in the homogeneous lung. The study shows for the homogeneous lung that the correct fractional concentration of alveolar carbon monoxide (FAV) occurs at a time (TAV), one-half of a breathing period after the effective inspiration time (TI) for the two very different breathing patterns. TI is well-defined in relation to any breathing pattern which can be approximated by ramps and pauses. If TAV and the sample time chosen by the experimental method are known, then the measured DLCO can be corrected to the actual diffusing capacity (DL). The theory agrees with experimental results and computer simulations of inhomogeneous lungs from the literature. This agreement suggests that the theory for the homogeneous lung is also relevant to the inhomogeneous lung.     

Contribution of continuing gas exchange to phase III exhaled PCO2 and PO2 profiles

Changes in PCO2 and PO2 during expiration have been ascribed to simultaneous gas exchange, but other factors such as ventilation-perfusion inhomogeneity in combination with sequential emptying may also contribute. An experimental and model approach was used to study the relationship between gas exchange and changes in expired PCO2 and PO2 in anesthetized dogs during prolonged high tidal volume expirations. Changes in PCO2 and PO2 were quantified by taking the area bounded by the sloping exhalation curve and a line drawn horizontally from a point where the Fowler dead space plus 250 ml had been expired. This procedure is similar to using the slope of the exhalation curve but it circumvents problems caused by nonlinearity of the PCO2 and PO2 curves. The gas exchange components of the CO2 and O2 areas were calculated using a single-alveolus lung model whose input parameters were measured in connection with each prolonged expiration. The relationship between changes in experimental CO2 areas caused by sudden reductions in mixed venous PCO2 (produced by right atrial infusions of NaOH) and those calculated by the model was also studied. In seven dogs, calculated CO2 and O2 areas were 13% higher and 25% lower than the respective experimental areas, but interindividual variations were large. Changes in experimental CO2 areas caused by step changes in mixed venous PCO2 were almost identical to changes in the calculated areas. We conclude that the changes in PCO2 and PO2 during expiration cannot be explained solely by gas exchange. However, the single-alveolus lung model accurately predicts changes in the CO2 exhalation curve caused by alterations in the alveolar CO2 flow.     

Effect of waveforms of inspired gas tension on the respiratory oscillations of carotid body discharge

The responses of carotid body chemoreceptor discharge to repeated ramps (20- to 60-s forcing cycle durations) of inspired gas tensions were studied in spontaneously breathing and in artificially ventilated pentobarbitone-anesthetized cats. In all animals the mean intensity of chemoreceptor discharge followed the frequency of the forcing cycle, and superimposed on this were oscillations at the frequency of ventilation (breath-by-breath oscillations). The amplitude of the breath-by-breath oscillations in discharge was often large, and it waxed and waned with the forcing cycle. It was greatest when the mean level of discharge was falling and smallest near the peak of mean discharge. No qualitative differences were observed between PO2-alone forcing in constant normocapnia and PCO2-alone forcing in constant hypoxia. The variation in the amplitudes of breath-by-breath oscillations was shown to be due primarily to variations in the amplitudes of the downslope component of the discharge oscillation. Variations in the upslope component of individual oscillations were small. The factors responsible for the breath-by-breath oscillations are discussed, and it is concluded that the shape of the waveform of arterial gas tensions that stimulate the peripheral chemoreceptors departs markedly from that of a line joining end-tidal gas tensions. This causes breath-by-breath oscillations of discharge to be very large after an "off" stimulus. Reflex studies involving the forcing of respiratory gases should therefore include consideration of these effects.     

Gas exchange in healthy rabbits during high-frequency oscillatory ventilation

We examined the effects of oscillatory frequency (f), tidal volume (VT), and mean airway pressure (Paw) on respiratory gas exchange during high-frequency oscillatory ventilation of healthy anesthetized rabbits. Frequencies from 3 to 30 Hz, VT from 0.4 to 2.0 ml/kg body wt (approximately 20-100% of dead space volume), and Paw from 5 to 20 cmH2O were studied. As expected, both arterial partial pressure of O2 and CO2 (PaO2 and PaCO2, respectively) were found to be related to f and VT. Changing Paw had little effect on blood gas tensions. Similar values of PaO2 and PaCO2 were obtained at many different combinations of f and VT. These relationships collapsed onto a single curve when blood gas tensions were plotted as functions of f multiplied by the square of VT (f. VT2). Simultaneous tracheal and alveolar gas samples showed that the gradient for PO2 and PCO2 increased as f. VT2 decreased, indicating alveolar hypoventilation. However, venous admixture also increased as f. VT2 decreased, suggesting that ventilation-perfusion inequality must also have increased.     

Evidence for minimal oxygen heterogeneity in the healthy human pulmonary acinus

It has been suggested that the human pulmonary acinus operates at submaximal efficiency at rest due to substantial spatial heterogeneity in the oxygen partial pressure (Po(2)) in alveolar air within the acinus. Indirect measurements of alveolar air Po(2) could theoretically mask significant heterogeneity if intra-acinar perfusion is well matched to Po(2). To investigate the extent of intra-acinar heterogeneity, we developed a computational model with anatomically based structure and biophysically based equations for gas exchange. This model yields a quantitative prediction of the intra-acinar O(2) distribution that cannot be measured directly. Temporal and spatial variations in Po(2) in the intra-acinar air and blood are predicted with the model. The model, representative of a single average acinus, has an asymmetric multibranching respiratory airways geometry coupled to a symmetric branching conducting airways geometry. Advective and diffusive O(2) transport through the airways and gas exchange into the capillary blood are incorporated. The gas exchange component of the model includes diffusion across the alveolar air-blood membrane and O(2)-hemoglobin binding. Contrary to previous modeling studies, simulations show that the acinus functions extremely effectively at rest, with only a small degree of intra-acinar Po(2) heterogeneity. All regions of the model acinus, including the peripheral generations, maintain a Po(2) >100 mmHg. Heterogeneity increases slightly when the acinus is stressed by exercise. However, even during exercise the acinus retains a reasonably homogeneous gas phase.