Distributions of lung ventilation and perfusion in prone and supine humans exposed to hypergravity.

When normal subjects are exposed to hypergravity [5 times normal gravity (5 G)] there is an impaired arterial oxygenation that is less severe in the prone compared with supine posture. We hypothesized that under these conditions the heterogeneities of ventilation and/or perfusion distributions would be less prominent when subjects were prone compared with supine. Expirograms from a combined rebreathing-single breath washout maneuver (Rohdin M, Sundblad P, and Linnarsson D. J Appl Physiol 96: 1470-1477, 2004) were analyzed for vital capacity (VC), phase III slope, and phase IV amplitude, to analyze heterogeneities in ventilation (Ar) and perfusion [CO(2)-to-Ar ratio (CO(2)/Ar)] distribution, respectively. During hypergravity, VC decreased more in the supine than in the prone position (ANOVA, P = 0.02). Phase III slope was more positive for Ar (P = 0.003) and more negative for CO(2)/Ar (P = 0.007) in the supine compared with prone posture at 5 G, in agreement with the notion of a more severe hypergravity-induced ventilation-perfusion mismatch in supine posture. Phase IV amplitude became lower in the supine than in the prone posture for both Ar (P = 0.02) and CO(2)/Ar (P = 0.004) during hypergravity as a result of the more reduced VC in the supine posture. We speculate that results of VC and phase IV amplitude are due to the differences in heart-lung interaction and diaphragm position between postures: a stable position of the heart and diaphragm in prone hypergravity, in contrast to supine in which the weight of the heart and a cephalad shift of the diaphragm compress lung tissue.     

Effects of gravity and blood volume shifts on cardiogenic oscillations in respired gas.

During the cardiac cycle, cardiogenic oscillations of expired gas (x) concentrations (COS([x])) are generated. At the same time, there are heart-synchronous cardiogenic oscillations of airway flow (COS(flow)), where inflow occurs during systole. We hypothesized that both phenomena, although primarily generated by the heartbeat, would react differently to the cephalad blood shift caused by inflation of an anti-gravity (anti-G) suit and to changes in gravity. Twelve seated subjects performed a rebreathing-breath-holding-expiration maneuver with a gas mixture containing O2 and He at normal (1 G) and moderately increased gravity (2 G); an anti-G suit was inflated to 85 mmHg in each condition. When the anti-G suit was inflated, COS(flow) amplitude increased (P = 0.0028) at 1 G to 186% of the control value without inflation (1-G control) and at 2 G to 203% of the control value without inflation (2-G control). In contrast, the amplitude of COS of the concentration of the blood-soluble gas O2 (COS([O2/He])), an index of the differences in pulmonary perfusion between lung units, declined to 75% of the 1-G control value and to 74% of the 2-G control value (P = 0.0030). There were no significant changes in COS(flow) or COS([O2/He]) amplitudes with gravity. We conclude that the heart-synchronous mechanical agitation of the lungs, as expressed by COS(flow), is highly dependent on peripheral-to-central blood shifts. In contrast, COS([blood-soluble gas]) appears relatively independent of this mechanical agitation and seems to be determined mainly by differences in intrapulmonary perfusion.     

Differential changes of lung diffusing capacity and tissue volume in hypergravity.

In normal gravity, lung diffusing capacity (DL(CO)) and lung tissue volume (LTV; including pulmonary capillary blood volume) change in concert, for example, during shifts between upright and supine. Accordingly, DL(CO) and LTV might be expected to decrease together in sitting subjects in hypergravity due to peripheral pooling of blood and reduced central blood volume. Nine sitting subjects in a human centrifuge were exposed to one, two, and three times increased gravity in the head-to-feet direction (G(z+)) and rebreathed a gas containing trace amounts of acetylene and carbon monoxide. DL(CO) was 25.2 +/- 2.6, 20.0 +/- 2.1, and 16.7 +/- 1.7 ml. min(-1). mbar(-1) (means +/- SE) at 1, 2, and 3 G(z+), respectively (ANOVA P < 0.001). Corresponding values for LTV increased from 541 +/- 34 to 677 +/- 43, and 756 +/- 71 ml (P < 0.001) at 2 and 3 G(z+). Results are compatible with sequestration of blood in the dependent part of the pulmonary circulation just as in the systemic counterpart. DL(CO,) which under normoxic conditions is mainly determined by its membrane component, decreased despite an increased pulmonary capillary blood volume, most likely as a consequence of a less homogenous distribution of alveolar volume with respect to pulmonary capillary blood volume.     

Ventilation-perfusion matching in long-term microgravity.

We studied the ventilation-perfusion matching pattern in normal gravity (1 G) and short- and long-duration microgravity (microG) using the cardiogenic oscillations in the sulfur hexaflouride (SF(6)) and CO(2) concentration signals during the phase III portion of vital capacity single-breath washout experiments. The signal power of the cardiogenic concentration variations was assessed by spectral analysis, and the phase angle between the oscillations of the two simultaneously expired gases was obtained through cross-correlation. For CO(2), a significant reduction of cardiogenic power was observed in microG, with respect to 1 G, but the reduction was smaller and more variable in the case of SF(6). A shift from an in-phase condition in 1 G to an out-of-phase condition was found for both short- and long-duration microG. We conclude that, although the distribution of ventilation and perfusion becomes more homogeneous in microG, significant inhomogeneities persist and that areas of high perfusion become associated with areas of relatively lower ventilation. In addition, these modifications seem to remain constant during long-term exposure to microG.     

Chronic centrifugation (hypergravity) disrupts the circadian system of the rat.

The present study was conducted to evaluate the response of rat deep body temperature (DBT) and gross locomotor activity (LMA) circadian rhythms to acute hypergravity onset and adaptation to chronic (14 day) hypergravity exposure over three gravity intensities (1.25, 1.5, and 2 G). Centrifugation of unanesthetized naive animals resulted in a dramatic acute decrease in DBT (-1.45, -2.40, and -3.09 degrees C for the 1.25, 1.5, and 2.0 G groups, respectively). LMA was suppressed for the duration of centrifugation (vs. control period); the percent decrease for each group on days 12-14, respectively, was 1.0 G, -15.2%, P = not significant; 1.25 G, -26.9%, P < 0.02; 1.5 G, -44.5%, P < 0.01; and 2.0 G, -63.1%, P < 0.002. The time required for DBT and LMA circadian rhythmic adaptation and stabilization to hypergravity onset increased from 1.25 to 2.0 G in all circadian metrics except daily means. Periodicity analysis detected the phenomenon of circadian rhythm splitting, which has not been reported previously in response to chronic hypergravity exposure. Our analysis documents the disruptive and dose-dependent effects of hypergravity on circadian rhythmicity and the time course of adaptation to 14-day chronic centrifugation exposure.     

Effects of the inhibitors on glutamate uptake by nerve terminals after exposure of rats to centrifuge-induced hypergravity

L-[14C]glutamate uptake process by nerve terminals has been investigated using glutamate analogs (nontransportable and transportable inhibitors of glutamate transporters) as tools. The effects of L-threo-beta-benzyloxyaspartate (DL-TBOA) and L-threo-beta-hydroxyaspartate (L-TBHA) on uptake of L-[14C] glutamate have been evaluated after exposure of rats to centrifuge-induced hypergravity. Both glutamate analogs potently inhibited L-[14C] glutamate uptake in dose-dependent manner. The IC50 values for DL-TBOA (nontransportable analog) calculated on the basis of curves of non-linear regression kinetic analysis was 18 +/- 2 micromoles and 11 +/- 2 micromoles (P < or = 0.05) before and after exposure to artificial gravity, respectively. Inhibition caused by 10 micromoles DL-TBOA was significantly increased from 38.0 +/- 3.8% in control group to 51.0 +/- 4.1% in animals, exposed to hypergravity (P < or = 0.05). L-TBHA, transportable analog, exhibited similar inhibitory characteristics.     

Effects of hypergravity on mammary metabolic function: gravity acts as a continuum.

Mammary metabolic activity in pregnant rats is significantly increased in response to spaceflight. To determine whether changes in mammary metabolism are related to gravity load, we exposed pregnant rats to hypergravity and measured mammary metabolic activity. From days 11-20 of gestation (G), animals were centrifuged (20 rpm; 1.5, 1.75, or 2.0 x gravity) or were maintained at 1 G. On G20, five rats from each group were removed from the centrifuge and euthanized. The remaining dams (n = 5/treatment) were housed at 1 G until parturition. After 2 h of nursing by the pups, the postpartum dams were euthanized (G22). Glucose oxidation to CO2 and incorporation into lipids was measured. Mammary glands from dams euthanized on G20 revealed a strong negative correlation between metabolic rate and increased G load. Approximately 98% of the variation in glucose oxidation and 94% of the variation in glucose incorporation into lipids can be accounted for by differences in G load. Differences in metabolic activity disappeared in the postpartum dams. When we combined previous data from the microgravity with hypergravity environments and plotted the ratio of mammary metabolic rate vs. G load, there was a significant exponential relationship (r2 = 0.99). These data demonstrate a remarkable continuum of response across the microgravity and hypergravity environments and support the concept that gravitational load influences mammary tissue metabolism.     

Body mass change during altered gravity: spaceflight, centrifugation, and return to 1 G

To assess the effect of gravity on growth, immature rats (130-200 g) were studied during chronic altered gravity exposure and while transitioning between gravity fields. Body mass gain of rats (n = 12) exposed to 14 days of microgravity (spaceflight) was evaluated and compared to mass gain of 1 G controls. Spaceflight did not affect mass gain. Six rats exposed to 1 G following spaceflight, when compared to controls, experienced a significant (0 < 0.05) post-flight mass loss over 48 h of 13 g. Over subsequent days, however, this loss was compensated for, and no difference from 1 G controls was noted after 5 days. Exposure to hypergravity (2 G) for 16 days was evaluated [(n = 6/group): Centrifuge (C); On Center Control (OCC); Centrifuge Control (CC)]. Body mass of centrifuged and OCC rats was reduced within 24 h, with OCCs regaining control mass within 13 days. The mass difference (44 g) in centrifuged animals persisted, however, with no subsequent difference in rate of mass gain between centrifuged animals and controls over Days 3-16 (3.7 +/- 0.1 vs. 3.9 +/- 0.1 g/day, respectively). Transitioning from 2 G to 1 G resulted in a mass increase within 48 hours for centrifuged animals. Over Days 3-16 at 1 G, the rate of gain for centrifuged animals continued to increase (3.1 +/- 0.1 g/day compared to 2.1 +/- 0.1 g/day for controls); differences from control, however, were still noted on Day 16. Transitioning to an increase in a gravity field causes acute losses in body mass. In hypergravity, the acute reduction in body mass persists but the rate of mass gain is normal. Animals returning to 1 G, after acute changes, adjust to attain control mass.     

Inter- and intraregional ventilation inhomogeneity in hypergravity and after pressurization of an anti-G suit.

This study assessed the effects of increased gravity in the head-to-foot direction (+G(z)) and anti-G suit (AGS) pressurization on functional residual capacity (FRC), the volume of trapped gas (V(TG)), and ventilation distribution by using inert- gas washout. Normalized phase III slope (Sn(III)) analysis was used to determine the effects on inter- and intraregional ventilation inhomogeneity. Twelve men performed multiple-breath washouts of SF(6) and He in a human centrifuge at +1 to +3 G(z) wearing an AGS pressurized to 0, 6, or 12 kPa. Hypergravity produced moderately increased FRC, V(TG), and overall and inter- and intraregional inhomogeneities. In normogravity, AGS pressurization resulted in reduced FRC and increased V(TG), overall, and inter- and intraregional inhomogeneities. Inflation of the AGS to 12 kPa at +3 G(z) reduced FRC markedly and caused marked gas trapping and intraregional inhomogeneity, whereas interregional inhomogeneity decreased. In conclusion, increased +G(z) impairs ventilation distribution not only between widely separated lung regions, but also within small lung units. Pressurizing an AGS in hypergravity causes extensive gas trapping accompanied by reduced interregional inhomogeneity and, apparently, results in greater intraregional inhomogeneity.     

Development of CO2 sensitivity: effects of gestational age, postnatal age, and sleep state

To determine the independent effects of sleep state, gestational age, and postnatal age on eucapnic ventilation and steady-state CO2 sensitivity, nine premature (146 +/- 3 days) and eight full-term (168 +/- 2 days) monkeys, Macaca nemestrina, from accurately timed conceptions were studied serially over the first 3 wk of life. Minute volume (VE)/kg,tidal volume (VT)/kg, and respiratory frequency were quantitated during rapid-eye-movement sleep (REM) and nonrapid-eye-movement sleep (NREM)in room air and when animals were breathing varied concentrations of cO2 in 21% O2. Eucapnic VE/kg and CO2 sensitivity [(deltaVE/kg)/delta PaCO2] increased progressively with advancing postnatal age during NREM sleep in grouped term and premature animals. CO2 sensitivity was not significantly different between REM and NREM sleep except in full-term animals at the highest postconceptual age studied (189 +/- 2 days) when [(delta VE/kg)/delta PaCO2] was lower in REM sleep than in NREM sleep (209 +/- 54 vs. 301 +/- 71 ml.min-1.kg-1.Torr-1; P less than 0.05, paired-t test). Gestational age had no measurable effect on eucapnic ventilation or CO2 sensitivity. These results support the hypothesis that REM sleep-induced depression of CO2 sensitivity develops in the neonatal monkey with advancing postconceptual age.     

Effects of gravity on lung diffusing capacity and cardiac output in prone and supine humans.

Both in normal subjects exposed to hypergravity and in patients with acute respiratory distress syndrome, there are increased hydrostatic pressure gradients down the lung. Also, both conditions show an impaired arterial oxygenation, which is less severe in the prone than in the supine posture. The aim of this study was to use hypergravity to further investigate the mechanisms behind the differences in arterial oxygenation between the prone and the supine posture. Ten healthy subjects were studied in a human centrifuge while exposed to 1 and 5 times normal gravity (1 G, 5 G) in the anterioposterior (supine) and posterioanterior (prone) direction. They performed one rebreathing maneuver after approximately 5 min at each G level and posture. Lung diffusing capacity decreased in hypergravity compared with 1 G (ANOVA, P = 0.002); it decreased by 46% in the supine posture compared with 25% in the prone (P = 0.01 for supine vs. prone). At the same time, functional residual capacity decreased by 33 and 23%, respectively (P < 0.001 for supine vs. prone), and cardiac output by 40 and 31% (P = 0.007 for supine vs. prone), despite an increase in heart rate of 16 and 28% (P < 0.001 for supine vs. prone), respectively. The finding of a more impaired diffusing capacity in the supine posture compared with the prone at 5 G supports our previous observations of more severe arterial hypoxemia in the supine posture during hypergravity. A reduced pulmonary-capillary blood flow and a reduced estimated alveolar volume can explain most of the reduction in diffusing capacity when supine.     

Depression of ventilatory responses after daily, cyclic hypercapnic hypoxia in piglets.

Ventilatory responses (VRs) were measured via a sealed face mask and pneumotachograph in 30 unsedated, mixed-breed miniature piglets at 12.6 +/- 2.3 days of age (day 1) and then repeated after seven daily 24-min exposures to 10% O(2)-6% CO(2) [hypercapnic hypoxia (HH)]. Arterial blood was sampled at baseline, after 10 min of exposure, and after 10 min of recovery. VRs included hypoxia (10% O(2) in N(2)), hypercapnia (6% CO(2) in air), and HH (10% O(2)-6% CO(2)-balance N(2)). Treatment groups (n = 10 each) were exposed to 24 min of HH from day 2 to 8 as sustained HH (24 min of HH and then 24 min of air) or cyclic HH (4 min of HH alternating with 4 min of air). Day 1 and 9 data were compared in treatment and control groups. After cyclic HH, respiratory responses to CO(2) were reduced during hypercapnia and during HH (P < 0.001 vs. control for minute ventilation in both). In both treatment groups, time to peak minute ventilation was delayed in hypoxia (P = 0.02, ANOVA), and response amplitude was increased (P < 0.001 and P = 0.003, sustained and cyclic HH, respectively, vs. control). Respiratory pattern was also altered during the VRs and among treatment groups. Stimulus presentation characteristics exert effects on VRs that are independent of those elicited by daily HH.     

Induction of oscillatory ventilation pattern using dynamic modulation of heart rate through a pacemaker

For disease states characterized by oscillatory ventilation, an ideal dynamic therapy would apply a counteracting oscillation in ventilation. Modulating respiratory gas transport through the circulation might allow this. We explore the ability of repetitive alternations in heart rate, using a cardiac pacemaker, to elicit oscillations in respiratory variables and discuss the potential for therapeutic exploitation. By incorporating acute cardiac output manipulations into an integrated mathematical model, we observed that a rise in cardiac output should yield a gradual rise in end-tidal CO2 and, subsequently, ventilation. An alternating pattern of cardiac output might, therefore, create oscillations in CO2 and ventilation. We studied the effect of repeated alternations in heart rate of 30 beats/min with periodicity of 60 s, on cardiac output, respiratory gases, and ventilation in 22 subjects with implanted cardiac pacemakers and stable breathing patterns. End-tidal CO2 and ventilation developed consistent oscillations with a period of 60 s during the heart rate alternations, with mean peak-to-trough relative excursions of 8.4 +/- 5.0% (P < 0.0001) and 24.4 +/- 18.8% (P < 0.0001), respectively. Furthermore, we verified the mathematical prediction that the amplitude of these oscillations would depend on those in cardiac output (r = 0.59, P = 0.001). Repetitive alternations in heart rate can elicit reproducible oscillations in end-tidal CO2 and ventilation. The size of this effect depends on the magnitude of the cardiac output response. Harnessed and timed appropriately, this cardiorespiratory mechanism might be exploited to create an active dynamic responsive pacing algorithm to counteract spontaneous respiratory oscillations, such as those causing apneic breathing disorders.     

Dynamics of the ventilatory response to central hypoxia in cats

The dynamics of the effect of central hypoxia on ventilation were investigated by the technique of artificial perfusion of the brain stem in alpha-chloralose-urethan-anesthetized cats. A two-channel roller pump and a four-way valve allowed switching the gas exchanger into and out of the extracorporeal circuit which controlled the brain stem perfusion. When isocapnic hypoxia (arterial PO2 range 18-59 Torr) was limited to the brain stem, a decline in ventilation was consistently found. In 12 cats 47 steps into and 48 steps out of central hypoxia were made. The ventilatory response was fitted using least squares with a model that consisted of a latency followed by a single-exponential function. The latencies for the steps into and out of hypoxia were not significantly different (P = 0.14) and were 32.3 +/- 4.0 and 25.1 +/- 3.6 (SE) s, respectively. The time constant for the steps into hypoxia (149.7 +/- 8.5 s) was significantly longer (P = 0.0002) than for the steps out of hypoxia (105.5 +/- 10.1 s). The time constants for the increase and decrease in ventilation after step changes in the central arterial PCO2 found in a previous study (J. Appl. Physiol. 66: 2168-2172, 1989) were not significantly different (P greater than 0.2) from the corresponding time constants in this study (for 7 cats common to both studies). Theories of the mechanisms behind hypoxic ventilatory decline need to account for the long latency, the similarity between the time constants for the ventilatory response to O2 and CO2, and the differences between the time constants for increasing and decreasing ventilation.     

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.     

A respiratory sensory reflex in response to CO2 inhibits breathing in preterm infants.

Traditionally, the increase in ventilation occurring after approximately 4 s of CO2 inhalation in preterm infants has been attributed to an action at the peripheral chemoreceptors. However, on a few occasions, we have observed a short apnea (2-3 s) in response to 3-5% CO2 in these infants. To test the hypothesis that this apnea reflects a respiratory sensory reflex to CO2, we gave nine preterm infants [birth wt 1.5 +/- 0.1 (SE) kg, gestational age 31 +/- 1 wk] 7-8% CO2 while they breathed 21% O2. To study the dose-response relationship, we also gave 2, 4, 6, and 8% CO2 to another group of seven preterm infants (birth wt 1.5 +/- 0.1 kg, gestational age 31 +/- 1 wk). In the first group of infants, minute ventilation during 21% O2 breathing (0.232 +/- 0.022 l.min-1.kg-1) decreased after CO2 administration (0.140 +/- 0.022, P < 0.01) and increased with CO2 removal (0.380 +/- 0.054, P < 0.05). This decrease in ventilation was related to an apnea (12 +/- 2.6 s) occurring 7.7 +/- 0.8 s after the beginning of CO2 inhalation. There was no significant change in tidal volume. In the second group of infants, minute ventilation increased during administration of 2, 4, and 6% CO2 but decreased during 8% CO2 because of the presence of an apnea. These findings suggest that inhalation of a high concentration of CO2 (> 6%) inhibits breathing through a respiratory sensory reflex, as described in adult cats (H. A. Boushey and P. S. Richardson. J. Physiol. Lond. 228: 181-191, 1973).(ABSTRACT TRUNCATED AT 250 WORDS)     

Ventilation-perfusion distribution and shunt fraction during one-lung ventilation: effect of different inhaled oxygen levels

Ventilation with higher fraction of inspired oxygen (F(I)O2) is one of the commonly-chosen strategies executed for treatment of hypoxemia during one lung ventilation (OLV) for thoracic surgery. In this study, we investigated the effect of F(I)O2 on pulmonary ventilation-perfusion (VA/Q) distribution during OLV. Six pigs, weighing 27 to 34 kg, were selected for this study. Following by a steady-state period, randomized administrations of F(I)O2 with 0.4, 0.6 and 1.0 were performed for 30 minutes at the right lateral decubitus position during OLV, while hemodynamic data and lung mechanics were simultaneously monitored. The VA/Q distributions of the lung(s) were assessed by the multiple inert gas elimination technique (MIGET). PaO2 at F(I)O2 of 100% was significantly reduced in OLV compared with two-lung ventilation (TLV) (522 +/- 104 vs. 653 +/- 21 mmHg; P < 0.001) at right lateral decubitus position. MIGET algorithms demonstrated a wider VA/Q distribution during OLV at F(I)O2 of 40%, as compared with distribution during TLV at F(I)O2 of 100%, but a bimodal perfusion distribution shifted to lower VA/Q component during OLV at F(I)O2 of 100%. There was an increase of pulmonary shunting in OLV, as compared with TLV at F(I)O2 of 100% (1.94 +/- 2.2% vs. 9.5 +/- 9.7%; P < 0.01). In addition, OLV caused a significant increase in the dispersion of perfusion at F(I)O2 of 100% (0.62 +/- 0.20 vs. 0.44 +/- 0.23; P < 0.01), but ventilation showed no denoting changes (1.06 +/- 0.20 vs. 0.98 +/- 0.35; P > 0.01). During OLV with right lateral decubitus position, there were no significant changes in the pulmonary shunt, the dispersion of perfusion and ventilation at different F(I)O2. OLV resulted in an increase in pulmonary shunting and heterogeneity compared with TLV. Furthermore, the PaO2 decreased during OLV regardless of the postural changes. At different F(I)O2, there were no significant changes in the pulmonary shunt, the dispersion of perfusion and ventilation during OLV with right lateral decubitus posture.     

Pulmonary gas exchange during exercise in highly trained cyclists with arterial hypoxemia.

The causes of exercise-induced hypoxemia (EIH) remain unclear. We studied the mechanisms of EIH in highly trained cyclists. Five subjects had no significant change from resting arterial PO(2) (Pa(O(2)); 92.1 +/- 2.6 Torr) during maximal exercise (C), and seven subjects (E) had a >10-Torr reduction in Pa(O(2)) (81.7 +/- 4.5 Torr). Later, they were studied at rest and during various exercise intensities by using the multiple inert gas elimination technique in normoxia and hypoxia (13.2% O(2)). During normoxia at 90% peak O(2) consumption, Pa(O(2)) was lower in E compared with C (87 +/- 4 vs. 97 +/- 6 Torr, P < 0.001) and alveolar-to-arterial O(2) tension difference (A-aDO(2)) was greater (33 +/- 4 vs. 23 +/- 1 Torr, P < 0. 001). Diffusion limitation accounted for 23 (E) and 13 Torr (C) of the A-aDO(2) (P < 0.01). There were no significant differences between groups in arterial PCO(2) (Pa(CO(2))) or ventilation-perfusion (VA/Q) inequality as measured by the log SD of the perfusion distribution (logSD(Q)). Stepwise multiple linear regression revealed that lung O(2) diffusing capacity (DL(O(2))), logSD(Q), and Pa(CO(2)) each accounted for approximately 30% of the variance in Pa(O(2)) (r = 0.95, P < 0.001). These data suggest that EIH has a multifactorial etiology related to DL(O(2)), VA/Q inequality, and ventilation.     

大气CO2浓度升高对绿豆叶片光合作用及叶绿素荧光参数的影响

利用FACE系统在大田条件下通过盆栽试验研究了大气CO2浓度升高[CO2浓度平均为(550+60) μmol·mo1-1]对绿豆叶片光合生理和叶绿素荧光参数的影响.结果表明:与对照[ CO2浓度平均为(389+40) μmol·mol-1左右]相比,大气CO2浓度升高使花荚期绿豆叶片净光合速率(Pn)和胞间CO2浓度(Ci)分别升高11.7％和9.8％,气孔导度(Gs)和蒸腾速率(Tr)分别下降32.0％和24.6％,水分利用效率(WUE)提高83.5％;在蕾期,CO2浓度升高对绿豆叶片叶绿素初始荧光(Fo)、最大荧光(Fm)、可变荧光(Fv)、Fv/Fm和Fv/Fo没有显著影响;在鼓粒期,CO2浓度升高使绿豆叶片Fo增加19.1％,Fm和Fv分别下降9.0％和14.3％,Fv/Fo和Fv/Fm分别下降25.8％和6.2％.表明大气CO2浓度升高可能使绿豆生长后期光系统Ⅱ反应中心结构受到破坏,叶片的光合能力下降.     

Effect of elastic loading on ventilatory pattern during progressive exercise

Ventilatory responses to progressive exercise, with and without an inspiratory elastic load (14.0 cmH2O/l), were measured in eight healthy subjects. Mean values for unloaded ventilatory responses were 24.41 +/- 1.35 (SE) l/l CO2 and 22.17 +/- 1.07 l/l O2 and for loaded responses were 24.15 +/- 1.93 l/l CO2 and 20.41 +/- 1.66 l/l O2 (P greater than 0.10, loaded vs. unloaded). At levels of exercise up to 80% of maximum O2 consumption (VO2max), minute ventilation (VE) during inspiratory elastic loading was associated with smaller tidal volume (mean change = 0.74 +/- 0.06 ml; P less than 0.05) and higher breathing frequency (mean increase = 10.2 +/- 0.98 breaths/min; P less than 0.05). At levels of exercise greater than 80% of VO2max and at exhaustion, VE was decreased significantly by the elastic load (P less than 0.05). Increases in respiratory rate at these levels of exercise were inadequate to maintain VE at control levels. The reduction in VE at exhaustion was accompanied by significant decreases in O2 consumption and CO2 production. The changes in ventilatory pattern during extrinsic elastic loading support the notion that, in patients with fibrotic lung disease, mechanical factors may play a role in determining ventilatory pattern.