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)     

Effects of altered CSF [H+] on ventilatory responses to exercise in the awake goat

We investigated the effects of selective large changes in the acid-base environment of medullary chemoreceptors on the control of exercise hyperpnea in unanesthetized goats. Four intact and two carotid body-denervated goats underwent cisternal perfusion with mock cerebrospinal fluid (CSF) of markedly varying [HCO-3] (CSF [H+] = 21-95 neq/l; pH 7.68-7.02) until a new steady state of alveolar hypo- or hyperventilation was reached [arterial PCO2 (PaCO2) = 31-54 Torr]. Perfusion continued as the goats completed two levels of steady-state treadmill walking [2 to 4-fold increase in CO2 production (VCO2)]. With normal acid-base status in CSF, goats usually hyperventilated slightly from rest through exercise (-3 Torr PaCO2, rest to VCO2 = 1.1 l/min). Changing CSF perfusate [H+] changed the level of resting PaCO2 (+6 and -4 Torr), but with few exceptions, the regulation of PaCO2 during exercise (delta PaCO2/delta VCO2) remained similar regardless of the new ventilatory steady state imposed by changing CSF [H+]. Thus the gain (slope) of the ventilatory response to exercise (ratio of change in alveolar ventilation to change in VCO2) must have increased approximately 15% with decreased resting PaCO2 (acidic CSF) and decreased approximately 9% with increased resting PaCO2 (alkaline CSF). A similar effect of CSF [H+] on resting PaCO2 and on delta PaCO2/VCO2 during exercise also occurred in two carotid body-denervated goats. Our results show that alteration of the gain of the ventilatory response to exercise occurs on acute alterations in resting PaCO2 set point (via changing CSF [H+]) and that the primary stimuli to exercise hyperpnea can operate independently of central or peripheral chemoreception.     

Control of exercise hyperpnea during hypercapnia in humans

Previous studies have yielded conflicting results on the ventilatory response to CO2 during muscular exercise. To obviate possible experimental errors contributing to such variability, we have examined the CO2-exercise interaction in terms of the ventilatory response to exercise under conditions of controlled hypercapnia. Eight healthy male volunteers underwent a sequence of 5-min incremental treadmill exercise runs from rest up to a maximum CO2 output (VCO2) of approximately 1.5 l . min-1 in four successive steps. The arterial PCO2 (PaCO2) at rest was stabilized at the control level or up to 14 Torr above control by adding 0-6% CO2 to the inspired air. Arterial isocapnia (SD = 1.2 Torr) throughout each exercise run was maintained by continual adjustment of the inspired PCO2. At all PaCO2 levels the response in total ventilation (VE) was linearly related to exercise VCO2. Hypercapnia resulted in corresponding increases in both the slope (S) and zero intercept (V0) of the VE-VCO2 curve; these being directly proportional to the rise in PaCO2 (means +/- SE: delta S/ delta PaCO2, 2.73 +/- 0.28 Torr-1; delta V0/ delta PaCO2, 1.67 +/- 0.18 l . min-1 . Torr-1). Thus the ventilatory response to concomitant hypercapnia and exercise was characterized by a synergistic (additive plus multiplicative) effect, suggesting a positive interaction between these stimuli. The increased exercise sensitivity in hypercapnia is qualitatively consistent with the hypothesis that VE is controlled to minimize the conflicting challenges due to chemical drive and the mechanical work of breathing (Poon, C. S. In: Modelling and Control of Breathing, New York: Elsevier, 1983, p. 189-196).     

Carotid body excision significantly changes ventilatory control in awake rats

We determined the effects of carotid body excision (CBX) on eupneic ventilation and the ventilatory responses to acute hypoxia, hyperoxia, and chronic hypoxia in unanesthetized rats. Arterial PCO2 (PaCO2) and calculated minute alveolar ventilation to minute metabolic CO2 production (VA/VCO2) ratio were used to determine the ventilatory responses. The effects of CBX and sham operation were compared with intact controls (PaCO2 = 40.0 +/- 0.1 Torr, mean +/- 95% confidence limits, and VA/VCO2 = 21.6 +/- 0.1). CBX rats showed 1) chronic hypoventilation with respiratory acidosis, which was maintained for at least 75 days after surgery (PaCO2 = 48.4 +/- 1.1 Torr and VA/VCO2 = 17.9 +/- 0.4), 2) hyperventilation in response to acute hyperoxia vs. hypoventilation in intact rats, 3) an attenuated increase in VA/VCO2 in acute hypoxemia (arterial PO2 approximately equal to 49 Torr), which was 31% of the 8.7 +/- 0.3 increase in VA/VCO2 observed in control rats, 4) no ventilatory acclimatization between 1 and 24 h hypoxia, whereas intact rats had a further 7.5 +/- 1.5 increase in VA/VCO2, 5) a decreased PaCO2 upon acute restoration of normoxia after 24 h hypoxia in contrast to an increased PaCO2 in controls. We conclude that in rats carotid body chemoreceptors are essential to maintain normal eupneic ventilation and to the process of ventilatory acclimatization to chronic hypoxia.     

Mechanistic basis for the gas exchange threshold in Thoroughbred horses.

The exercising Thoroughbred horse (TB) is capable of exceptional cardiopulmonary performance. However, because the ventilatory equivalent for O2 (VE/VO2) does not increase above the gas exchange threshold (Tge), hypercapnia and hypoxemia accompany intense exercise in the TB compared with humans, in whom VE/VO2 increases during supra-Tge work, which both removes the CO2 produced by the HCO buffering of lactic acid and prevents arterial partial pressure of CO2 (PaCO2) from rising. We used breath-by-breath techniques to analyze the relationship between CO2 output (VCO2) and VO2 [V-slope lactate threshold (LT) estimation] during an incremental test to fatigue (7 to approximately 15 m/s; 1 m x s(-1) x min(-1)) in six TB. Peak blood lactate increased to 29.2 +/- 1.9 mM/l. However, as neither VE/VO2 nor VE/VCO2 increased, PaCO2 increased to 56.6 +/- 2.3 Torr at peak VO2 (VO2 max). Despite the presence of a relative hypoventilation (i.e., no increase in VE/VO2 or VE/VCO2), a distinct Tge was evidenced at 62.6 +/- 2.7% VO2 max. Tge occurred at a significantly higher (P < 0.05) percentage of VO2 max than the lactate (45.1 +/- 5.0%) or pH (47.4 +/- 6.6%) but not the bicarbonate (65.3 +/- 6.6%) threshold. In addition, PaCO2 was elevated significantly only at a workload > Tge. Thus, in marked contrast to healthy humans, pronounced V-slope (increase VCO2/VO2) behavior occurs in TB concomitant with elevated PaCO2 and without evidence of a ventilatory threshold.     

Effect of withdrawal of respiratory CO2 oscillations on respiratory control at rest

We examined the effect of sudden withdrawal of respiratory oscillations of arterial PCO2 (CO2 oscillations) at resting metabolic rate on the control of respiration in 11 anesthetized paralyzed vagotomized dogs in normoxic normocapnia. A double-lumen endotracheal tube was inserted so that the left and right lungs were ventilated independently. By alternately ventilating each lung, we could completely abolish CO2 oscillations without affecting the mean blood gas levels (withdrawal of CO2 oscillations). The CO2 oscillation was calculated from arterial pH oscillation measured by a rapidly responding intra-arterial pH electrode. Respiratory center output was monitored by use of a moving time average of the phrenic neurogram. A 3-min period of withdrawal of CO2 oscillations was bracketed by two control periods (simultaneous ventilation of lungs for 3 min) to avoid the confounding effect of the baseline drift in the respiratory center output. The amplitude of the CO2 oscillations in the control was 2.33 +/- 0.89 (SD) Torr. When the difference in the mean level of arterial PCO2 between the control and withdrawal of CO2 oscillations was minimized (-0.09 +/- 0.54 Torr; P greater than 0.25), we found negligible change in the minute phrenic activity during withdrawal of CO2 oscillations (-0.02 +/- 6.11% of the control, P greater than 0.98, n = 49; 99% confidence interval -2.36 to 2.32%). Thus we conclude that the maintenance of normal respiration at rest is not critically dependent on a phasic afferent input to the respiratory center arising from respiratory CO2 oscillations.     

Ventilation by external high-frequency oscillation in cats

Eight anesthetized tracheostomized cats were placed in an 8.2-liter airtight chamber with the trachea connected to the exterior. Thirty-two combinations of high-frequency oscillations (HFO) (0.5-30 Hz; 25-100 ml) were delivered for 10 min each in random order into the chamber. Arterial blood gas tensions during oscillation were compared with control measurements made after 10 min of spontaneous breathing without oscillation when the mean arterial PCO2 (PaCO2) was 30.1 Torr. Ventilation due to spontaneous breathing (Vs) and oscillation (Vo) were derived from the chamber pressure trace and a pneumotachograph, respectively. As the oscillation frequency increased, oscillated tidal volume (Vo) decreased from a mean of 39 (0.5 Hz) to 3.3 ml (30 Hz) when 100 ml was delivered to the chamber. From 6-25 Hz, apnea occurred with Vo less than estimated respiratory dead space (VD); the minimum effective Vo/VD ratio was 0.37 +/- 0.05. Although Vo was maximal at 10 Hz at each oscillation volume, the lowest PaCO2 occurred at 2-6 Hz, and arterial PO2 rose as expected during hypocapnia. Above 10 Hz, PaCO2 was determined by Vo and was independent of frequency, whereas at lower frequencies, PaCO2 was related to Vo; below 6 Hz, PaCO2 varied inversely with the calculated alveolar ventilation. As oscillations became more effective, both PaCO2 and Vs fell progressively and were highly correlated; apnea occurred when PaCO2 was reduced by a mean of 4.5 Torr. Mean chamber pressure remained near zero up to 15 Hz, indicating functional residual capacity did not change. We conclude that externally applied HFO can readily maintain gas exchange in vivo, with Vo less than VD at frequencies over 2 Hz.     

Blood-gas equilibration of CO2 and O2 in lungs of awake dogs during prolonged rebreathing

To reinvestigate the blood-gas CO2 equilibrium in lungs, rebreathing experiments were performed in five unanesthetized dogs prepared with a chronic tracheostomy and an exteriorized carotid loop. The rebreathing bag was initially filled with a gas mixture containing 6-8% CO2, 12, 21, or 39% O2, and 1% He in N2. During 4-6 min of rebreathing PO2 in the bag was kept constant by a controlled supply of O2 while PCO2 rose steadily from approximately 40 to 75 Torr. Spot samples of arterial blood were taken from the carotid loop; their PCO2 and PO2 were measured by electrodes and compared with the simultaneous values of end-tidal gas read from a mass spectrometer record. The mean end-tidal-to-arterial PO2 differences averaging 16, 4, and 0 Torr with bag PO2 about 260, 130, and 75 Torr, respectively, were in accordance with a venous admixture of about 1%. No substantial PCO2 differences between arterial blood and end-tidal gas (PaCO2 - PE'CO2) were found. The mean PaCO2 - PE'CO2 of 266 measurements in 70 rebreathing periods was -0.4 +/- 1.4 (SD) Torr. There was no correlation between PaCO2 - PE'CO2 and the level of arterial PCO2 or PO2. The mean PaCO2 - PE'CO2 became +0.1 Torr when the blood transit time from lungs to carotid artery (estimated at 6 s) and the rate of rise of bag PCO2 (4.5 Torr/min) were taken into account. These experimental results do not confirm the presence of significant PCO2 differences between arterial blood and alveolar gas in rebreathing equilibrium.     

Effect of high-intensity exercise on the VE-VCO2 relationship

The intrinsic relationship between ventilation (VE) and carbon dioxide output (VCO2) is described by the modified alveolar ventilation equation VE = VCO2 k/PaCO2(1-VD/VT) where PaCO2 is the partial pressure of CO2 in the arterial blood and VD/VT is the dead space fraction of the tidal volume. Previous investigators have reported that high-intensity exercise uncouples VE from VCO2; however, they did not measure the PaCO2 and VD/VT components of the overall relationship. In an attempt to provide a more complete analysis of the effects of high-intensity exercise on the VE-VCO2 relationship, we undertook an investigation where five subjects volunteered to perform three steady-state tests (SS1, SS2, SS3) at 60 W. One week after SS1 each subject was required to perform repeated 1-min bouts of exercise corresponding to a work rate of approximately 140% of maximal oxygen uptake (VO2max). Two and 24 h later the subjects performed SS2 and SS3, respectively. This exercise intervention caused PaCO2 during SS2 and SS3 to be regulated (P less than 0.01) approximately 4 Torr below the control (SS1) value of 38.8 Torr. Additionally, significant alterations were noted for VCO2 with corresponding values of 1.15 (SS1), 1.10 (SS2), and 1.04 (SS3) l/min. No changes were noted in either VD/VT or VE. In summary, it seems reasonable to suggest that the disproportionate increase in VE with respect to VCO2 noted in earlier work does not reflect an uncoupling. Rather the slope of the VE-VCO2 relationship is increased in a predictable manner as described by the modified alveolar ventilation equation.     

Ventilatory control during exercise with increased respiratory dead space in goats

Our objectives were to determine 1) the effects of increased respiratory dead space (VD) on the ventilatory response to exercise and 2) whether changes in the ventilatory response are due to changes in chemoreceptor feedback (rest to exercise) vs. changes in the feedforward exercise stimulus. Steady-state ventilation (VI) and arterial blood gas responses to mild or moderate hyperoxic exercise in goats were compared with and without increased VD. Responses were compared using a simple mathematical model with the following assumptions: 1) steady state, 2) linear CO2 chemoreceptor feedback, 3) linear feedforward exercise stimulus proportional to CO2 production (VCO2) and characterized by an exercise gain (Gex), and 4) additive exercise stimulus and CO2 feedback producing the system gain (Gsys = delta VI/delta VCO2). Model predictions at constant Gex [assuming VD-to-tidal volume (VT) ratio independent of VCO2] are that increased VD/VT will 1) increase arterial PCO2 (PaCO2) and VI at rest and 2) increase Gsys via changes in chemoreceptor feedback due to a small increase in the PaCO2 vs. VCO2 slope. Experimental results indicate that increased VD increased VD/VT, PaCO2, and VI at rest and increased Gsys during exercise. However, measurable changes in the PaCO2 vs. VCO2 slope occurred only at high VD/VT or running speeds. Gex was estimated at each VD for each goat by using the model in conjunction with experimental measurements. With 0.2 liter VD, Gex increased 40% (P less than 0.01); with 0.6 liter VD, Gex increased 110% between 0 and 2.4 km/h and 5% grade (P less than 0.01) but not between 2.4 and 4.8 km/h. Thus, Gex is increased by VD through a limited range. In goats, increases in Gsys with increased VD result from increases in both Gex and CO2 chemoreceptor feedback. These results are consistent with other experimental treatments that increase the exercise ventilatory response, maintaining constant relative PaCO2 regulation, and suggest that a common mechanism linked to resting ventilatory drive modulates Gex.     

Arterial-alveolar CO2 equilibration in exercising dogs during prolonged rebreathing

Arterial-alveolar equilibration of CO2 during exercise was studied by normoxic CO2 rebreathing in six dogs prepared with a chronic tracheostomy and exteriorized carotid loop and trained to run on a treadmill. In 153 simultaneous measurements of PCO2 in arterial blood (PaCO2) and end-tidal gas (PE'CO2) obtained in 46 rebreathing periods at three levels of mild-to-moderate steady-state exercise, the mean PCO2 difference (PaCO2-PE'CO2) was -1.0 +/- 1.0 (SD) Torr and was not related to O2 uptake or to the level of PaCO2 (30-68 Torr). The small negative PaCO2-PE'CO2 is attributed to the lung-to-carotid artery transit time delay which must be taken into account when both PaCO2 and PE'CO2 are continuously rising during rebreathing (average rate 0.22 Torr/s). Assuming that blood-gas equilibrium for CO2 was complete, a lung-to-carotid artery circulation time of 4.6 s accounts for the observed uncorrected PaCO2-PE'CO2 of -1.0 Torr. The results are interpreted to indicate that in rebreathing equilibrium PCO2 in arterial blood and alveolar gas are essentially identical. This conclusion is at variance with previous studies in exercising humans during rebreathing but is in full agreement with our recent findings in resting dogs.     

Ventilatory and PaCO2 responses to voluntary and electrically induced leg exercise

We studied the role of central command mediation of exercise hyperpnea by comparing the ventilatory and arterial CO2 partial pressure (PaCO2) responses to voluntary (ExV) and electrically induced (ExE) muscle contractions in normal, awake human subjects. We hypothesized that if central command signals are critical to a normal ventilatory response, then ExE should cause a slower ventilatory response resulting in hypercapnia at the onset of exercise. ExE was induced through surface electrodes placed over the quadriceps and hamstring muscles. ExE and ExV produced leg extension (40/min) against a spring load that increased CO2 production (VCO2) 100-1,000 ml/min above resting level. PaCO2 and arterial pH during work transitions and in the steady state did not differ significantly from rest (P greater than 0.05) or between ExE and ExV. The temporal pattern of ventilation, tidal volume, breathing frequency, and inspired and expired times, and the ventilation-VCO2 relationship were similar between ExE and ExV. We conclude that since central command was reduced and/or eliminated by ExE, central command is not requisite for the precise matching of alveolar ventilation to increases in VCO2 during low-intensity muscle contractions.     

Temperature-induced changes in blood acid-base status: Donnan rCl and red cell volume.

The Donnan ratio for chloride ion (rCl) was determined for human red cells in plasma utilizing 36Cl. The effect of altered PCO2 and pH on rCl was followed in two ways. CO2 partial pressure was varied (1-1.5% CO2 in O2; pH range 7.1-7.9) at 37.5 degrees C (isothermal); PCO2 and pH were also changed by altering temperature (range 5-45 degrees C) at constant CO2 content (temperature induced). At pH 7.4 and 37.5 degrees C, rCl was 0.631 +/- 0.0269 (SE, N = 5); isothermal drcl/dpH = -0.306 +/- 0.0234. When measured under conditions of variable temperature at constant CO2 content (pH range 7.3-7.9), drcl/dpH = .018 +/- 0.0232, significantly different from isothermal response (P less than 0.001). Hematocrit (H) changes with pH for conditions of initial H(7.4) of 0.45, under these conditions were also determined: isothermal dH/dpH = -0.031 +/- 0.0019; temperature induced, -0.004 +/- 0.0009. Temperature change alone at constant carbon dioxide content produces no significant change in distribution of chloride ions or water between erythrocyte and plasma compartments.     

Ventilatory changes during exercise and arterial PCO2 oscillations in chronic airway obstruction patients

Ventilatory kinetics during exercise (30 W for 6 min) were studied in 3 asthmatics, 14 patients with chronic airway obstruction (11 with bronchial or type B disease, 3 with emphysematous or type A disease), and in 5 normal age-matched controls. The measure of ventilatory increase during early exercise, alpha 1-3%, was calculated as (avg minute ventilation over 1st-3rd min of exercise--resting minute ventilation)/(avg minute ventilation over 4th-6th min of exercise--resting minute ventilation) X 100. Arterial pH, PO2, and PCO2 (PaCO2) were measured in vitro at rest and within 20 s of termination of exercise. Respiratory PaCO2 oscillations had previously been monitored at rest in the patients (indirectly as in vivo arterial pH, using a fast-response pH electrode) and quantified by upslope (delta PaCO2/delta t). alpha 1-3% was normal in asthmatics (whose respiratory oscillations as a group showed least attenuation) and in type A patients (whose respiratory oscillations as a group were most attenuated). In type B patients reduction in alpha 1-3% correlated with attenuation of delta PaCO2/delta t (r = 0.75; P less than 0.01). There was no significant correlation between delta PaCO2/delta t and change of in vitro PaCO2 from rest to the immediate postexercise period. These findings are consistent with the hypothesis that attenuation of delta PaCO2/delta t slows ventilatory kinetics during exercise in type B but not type A patients. Intact respiratory oscillations are not necessary for CO2 homeostasis after the first few minutes of exercise.     

Respiratory effects of the Jarvik-7 artificial heart

In five anesthetized patients with a Jarvik-7 artificial heart, pulmonary volume displacements generated by cardiogenic oscillations were measured using an indirect spirometric method. Consequences on gas exchange were also evaluated during a 15-min period of apnea by use of a tracheal insufflation of pure O2 at a constant flow rate of 20 l/min. The Jarvik-7 artificial heart generated a mean pulmonary volume displacement of 105 +/- 29 (SD) ml/heart beat. After 15 min of apnea, arterial PCO2 (PaCO2) significantly increased from 29 +/- 5 to 47 +/- 6 (SD) Torr. PaCO2 increased by 0.8 Torr/min from the 5th to the 15th min of apnea. Mean arterial PO2, mean pulmonary shunt, mean O2 consumption, and mean metabolic production of CO2 did not change significantly during the apnea period. Because cardiac output was kept constant during the study, O2 transport was adequately maintained throughout the apnea period. In patient 1, where the period of apnea was continued for 60 min, PaCO2 progressively increased until the 45th min and then remained stable at 61 Torr during the last 15 min of apnea. This "plateau" corresponded to an alveolar ventilation of 3,907 ml/min, representing 69% of the alveolar ventilation calculated during conventional mechanical ventilation. In conclusion, the Jarvik-7 artificial heart provides a potent respiratory support through the cardiogenic oscillations it generates.     

Carotid chemoreceptor discharge during epinephrine infusion in anesthetized cats.

It is known that during exercise there is an increase in plasma epinephrine. The purpose of the present investigation was to determine whether stimulation of carotid chemoreceptors by epinephrine is a direct effect or secondary to epinephrine-induced increases in arterial plasma [K+] and whole body CO2 production (VCO2). Chemoreceptor discharge was recorded from single fiber preparations of the carotid sinus nerves in anesthetized cats ventilated to a constant arterial PCO2 (PaCO2). Infusion of epinephrine (1 microgram.kg-1 x min-1) caused arterial [K+] to increase from a mean of 2.7 to 3.8 mM. VCO2 increased so that ventilation had to be increased by 60% to maintain PaCO2 constant. Mean chemoreceptor discharge increased by 50%, but this was no greater than would be predicted on the basis of the increases in arterial [K+] and VCO2. In a further group of experiments epinephrine was infused at 0.1 microgram.kg-1 x min-1 and produced no significant increase in chemoreceptor firing. These experiments provide no evidence for epinephrine having a direct effect on the carotid chemoreceptor.     

Model implications of gas exchange dynamics on blood gases in incremental exercise

In humans, arterial PCO2 (PaCO2) has been demonstrated to be regulated at or near resting levels in the steady state of moderate exercise (i.e., for work rates not associated with a sustained lactic acidosis). To determine how PaCO2 might be expected to behave under the nonsteady-state conditions of incremental exercise testing, the influence of the dynamic characteristics of the primary variables that determine PaCO2 was explored by means of computer modeling. We constructed a dynamic model that utilized previously reported experimental estimates for the kinetic response parameters of ventilation (VE) and CO2 output (VCO2). In response to incremental work rate forcings, the model yielded an increase in PaCO2, which reflected the disparity between the VE and VCO2 time constants; this hypercapnic condition was maintained despite VE and VCO2 both increasing linearly with respect to the input work rate profile. The degree of hypercapnia increased with the rate of the incremental forcing, reaching 9 Torr for a 50-W/min forcing. In conclusion, therefore, sustained increases in PaCO2 during nonsteady-state incremental exercise should be interpreted with caution, because this is the predicted response even in subjects with normal ventilatory control and lung function.     

Human whole-blood O2 affinity: effect of CO2

The proton Bohr factor (phi H = alpha log PO2/alpha pH), the carbamate Bohr factor (phi C = alpha log PO2/alpha log PCO2), the total Bohr factor (phi HC = d log PO2/dpH[base excess) and the CO2 buffer factor (d log PCO2/dpH) were determined in the blood of 12 healthy donors over the whole O2 saturation (SO2) range. All three Bohr factors proved to be dependent on SO2, although to a lesser extent than reported in some of the recent literature. At SO2 = 50% and 37 degrees C, we found phi H = -0.428 +/- 0.010 (SE), phi C = 0.054 +/- 0.006, and phi HC = -0.488 +/- 0.007. The values obtained for phi H, phi C, and d log PCO2/dpH were used to calculate phi HC. Calculated and measured values of phi HC proved to be in good agreement. In an additional series of 12 specimens of human blood we determined the influence of PCO2 on phi H and the influence of pH on phi C. At SO2 = 50%, phi H varied from -0.49 +/- 0.009 at PCO2 = 15 Torr to -0.31 +/- 0.010 at PCO2 = 105 Torr and phi C from 0.157 +/- 0.015 at pH = 7.80 to 0.006 +/- 0.009 at pH = 7.00. When on the basis of these data a second-order term is taken into account, a still slightly better agreement between measured and calculated values of phi HC can be attained.     

Effects of mean airway pressure on gas transport during high-frequency ventilation in dogs

In 10 anesthetized, paralyzed, supine dogs, arterial blood gases and CO2 production (VCO2) were measured after 10-min runs of high-frequency ventilation (HFV) at three levels of mean airway pressure (Paw) (0, 5, and 10 cmH2O). HFV was delivered at frequencies (f) of 3, 6, and 9 Hz with a ventilator that generated known tidal volumes (VT) independent of respiratory system impedance. At each f, VT was adjusted at Paw of 0 cmH2O to obtain a eucapnia. As Paw was increased to 5 and 10 cmH2O, arterial PCO2 (PaCO2) increased and arterial PO2 (PaO2) decreased monotonically and significantly. The effect of Paw on PaCO2 and PaO2 was the same at 3, 6, and 9 Hz. Alveolar ventilation (VA), calculated from VCO2 and PaCO2, significantly decreased by 22.7 +/- 2.6 and 40.1 +/- 2.6% after Paw was increased to 5 and 10 cmH2O, respectively. By taking into account the changes in anatomic dead space (VD) with lung volume, VA at different levels of Paw fits the gas transport relationship for HFV derived previously: VA = 0.13 (VT/VD)1.2 VTf (J. Appl. Physiol. 60: 1025-1030, 1986). We conclude that increasing Paw and lung volume significantly decreases gas transport during HFV and that this effect is due to the concomitant increase of the volume of conducting airways.     

Measurement of pH to quantify urease activity.

The rate of change of pH caused by the hydrolysis of urea was measured for urease solutions of 18 different concentrations. Concentrations were converted into an activity, A (measured in IU/cm3), by using a titrimetric method to assay the urease sample. For activities in the range 0.6-38 IU/cm3, A was related to the initial rate of change of pH, (dpH/dt)0, (measured in s-1) by the empirical relationship: A = 549(dpH/dt)0-1423(dpH/dt)2(0). Values of (dpH/dt)0 were sensitive to changes in the urease activity of about 0.6 IU/cm3.