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.     

Effect of mean airway pressure on gas exchange during high-frequency oscillatory ventilation

We studied the effect of mean airway pressure (Paw) on gas exchange during high-frequency oscillatory ventilation in 14 adult rabbits before and after pulmonary saline lavage. Sinusoidal volume changes were delivered through a tracheostomy at 16 Hz, a tidal volume of 1 or 2 ml/kg, and inspired O2 fraction of 0.5. Arterial PO2 and PCO2 (PaO2, PaCO2), lung volume change, and venous admixture were measured at Paw from 5 to 25 cmH2O after either deflation from total lung capacity or inflation from relaxation volume (Vr). The rabbits were lavaged with saline until PaO2 was less than 70 Torr, and all measurements were repeated. Lung volume change was measured in a pressure plethysmograph. Raising Paw from 5 to 25 cmH2O increased lung volume by 48-50 ml above Vr in both healthy and lavaged rabbits. Before lavage, PaO2 was relatively insensitive to changes in Paw, but after lavage PaO2 increased with Paw from 42.8 +/- 7.8 to 137.3 +/- 18.3 (SE) Torr (P less than 0.001). PaCO2 was insensitive to Paw change before and after lavage. At each Paw after lavage, lung volume was larger, venous admixture smaller, and PaO2 higher after deflation from total lung capacity than after inflation from Vr. This study shows that the effect of increased Paw on PaO2 is mediated through an increase in lung volume. In saline-lavaged lungs, equal distending pressures do not necessarily imply equal lung volumes and thus do not imply equal PaO2.     

Chemical and mechanical determinants of apnea during high-frequency ventilation

The factors responsible for the apnea observed during high-frequency ventilation (HFV) were evaluated in 14 pentobarbital sodium-anesthetized cats. A multiple logistic regression analysis provided an estimate of the probability of apnea during HFV as a function of four respiratory variables: mean airway pressure (Paw), tidal volume (VT), frequency, and arterial PCO2 (PaCO2). When mean Paw was 2 cmH2O, PaCO2, VT, and their interaction contributed significantly to the probability of apnea during HFV. At a low value of PaCO2 (25 Torr), the probability of apnea had a minimum value of 0.19 and gradually increased toward 1.0 as VT increased from 0.5 to 7 ml/kg. At higher levels of PaCO2 (30 and 35 Torr) the probability of apnea was zero in the low range of VT but sharply approached 1.0 above a VT of approximately 2.0 ml/kg. However, when Paw was increased to 6 cmH2O, only PaCO2 was an important determinant of apnea. In this case, the probability of apnea was 0.51 when PaCO2 was 25 Torr but decreased to 0.22 when PaCO2 was raised to 25 Torr. At neither Paw was the probability of apnea dependent on frequency. These results suggest that chemoreceptor inputs, in addition to both static and dynamic lung mechanoreceptor afferents, are responsible for determining the output of the central respiratory centers during HFV.     

Inspiratory-to-expiratory time ratio and alveolar ventilation during high-frequency ventilation in dogs

It has been suggested that the increase in inspiratory flow rate caused by a decrease in the inspiratory-to-expiratory time ratio (I:E) at a constant tidal volume (VT) could increase the efficiency of ventilation in high-frequency ventilation (HFV). To test this hypothesis, we studied the effect of changing I:E from 1:1 to 1:4 on steady-state alveolar ventilation (VA) at a given VT and frequency (f) and at a constant mean lung volume (VL). In nine anesthetized, paralyzed, supine dogs, HFV was performed at 3, 6, and 9 Hz with a ventilator that delivered constant inspiratory and expiratory flow rates. Mean airway pressure was adjusted so that VL was maintained at a level equivalent to that of resting FRC. At each f and one of the I:E chosen at random, VT was adjusted to obtain a eucapnic steady state [arterial pressure of CO2 (PaCO2) = 37 +/- 3 Torr]. After 10 min of each HFV, PaCO2, arterial pressure of O2 (PaO2), and CO2 production (VCO2) were measured, and I:E was changed before repeating the run with the same f and VT. VA was calculated from the ratio of VCO2 and PaCO2. We found that the change of I:E from 1:1 to 1:4 had no significant effects on PaCO2, PaO2, and VA at any of the frequencies studied. We conclude, therefore, that the mechanism or mechanisms responsible for gas transport during HFV must be insensitive to the changes in inspiratory and expiratory flow rates over the VT-f range covered in our experiments.     

Frequency and amplitude effects during high-frequency vibration ventilation in dogs

High-frequency external body vibration, combined with constant gas flow at the tracheal carina, was previously shown to be an effective method of ventilation in normal dogs. The effects of frequency (f) and amplitude of the vibration were investigated in the present study. Eleven anesthetized and paralyzed dogs were placed on a vibrating table (4-32 Hz). O2 was delivered near the tracheal carina at 0.51.kg-1.min-1, while mean airway pressure was kept at 2.4 +/- 0.9 cmH2O. Table vertical displacement (D) and acceleration (a), esophageal (Pes), and tracheal (Ptr) peak-to-peak pressures, and tidal volume (VT) were measured as estimates of the input amplitude applied to the animal. Steady-state arterial PCO2 (PaCO2) and arterial PO2 (PaO2) values were used to monitor overall gas exchange. Typically, eucapnia was achieved with f greater than 16 Hz, D = 1 mm, a = 1 G, Pes = Ptr = 4 +/- 2 cmH2O, and VT less than 2 ml. Inverse exponential relationships were found between PaCO2 and f, a, Pes, and Ptr (exponents: -0.69, -0.38, -0.48, and -0.54, respectively); PaCO2 decreased linearly with increased displacement or VT at a fixed frequency (17 +/- 1 Hz). PaO2 was independent of both f and D (393 +/- 78 Torr, mean +/- SD). These data demonstrate the very small VT, Ptr, and Pes associated with vibration ventilation. It is clear, however, that mechanisms other then those described for conventional ventilation and high-frequency ventilation must be evoked to explain our data. One such possible mechanism is forcing of flow oscillation between lung regions (i.e., forced pendelluft).     

Ventilatory response to fatiguing and nonfatiguing resistive loads in awake sheep

To study the changes in ventilation induced by inspiratory flow-resistive (IFR) loads, we applied moderate and severe IFR loads in chronically instrumented and awake sheep. We measured inspired minute ventilation (VI), ventilatory pattern [inspiratory time (TI), expiratory time (TE), respiratory cycle time (TT), tidal volume (VT), mean inspiratory flow (VT/TI), and respiratory duty cycle (TI/TT)], transdiaphragmatic pressure (Pdi), functional residual capacity (FRC), blood gas tensions, and recorded diaphragmatic electromyogram. With both moderate and severe loads, Pdi, TI, and TI/TT increased, TE, TT, VT, VT/TI, and VI decreased, and hypercapnia ensued. FRC did not change significantly with moderate loads but decreased by 30-40% with severe loads. With severe loads, arterial PCO2 (PaCO2) stabilized at approximately 60 Torr within 10-15 min and rose further to levels exceeding 80 Torr when Pdi dropped. This was associated with a lengthening in TE and a decrease in breathing frequency, VI, and TI/TT. We conclude that 1) timing and volume responses to IFR loads are not sufficient to prevent alveolar hypoventilation, 2) with severe loads the considerable increase in Pdi, TI/TT, and PaCO2 may reduce respiratory muscle endurance, and 3) the changes in ventilation associated with neuromuscular fatigue occur after the drop in Pdi. We believe that these ventilatory changes are dictated by the mechanical capability of the respiratory muscles or induced by a decrease in central neural output to these muscles or both.     

Interactions between lung stretch and PaCO2 in modulating ventilatory activity in dogs

The effects of changes in airway pressure (Paw) and arterial PCO2 (PaCO2) on ventilatory activity were studied in anesthetized thoracotomized dogs in which both lungs were ventilated separately. Pulmonary artery occlusion on one side and contralateral vagotomy allowed the reflex effects on ventilation of changes in Paw and PaCO2 to be elicited independently of each other. Ventilatory activity was assessed from integrated efferent phrenic activity, analyzed with respect to burst amplitude (Phr), burst frequency (f), and inspiratory TI) and expiratory duration (TE). While Phr increased linearly with PaCO2, it was independent of Paw. Both PaCO2 and Paw affected f in a complex nonadditive way; this response was entirely mediated by effects on TE, TI being unaffected by either stimulus. The analog of ventilation, estimated as Phr x f, increased linearly with PaCO2 and decreased linearly with Paw, but the effects of both stimuli appeared to be additive. It is concluded that the apparently simple effect of Paw and PaCO2 on ventilation results from more complex effects these stimuli exert on its components.     

Ventilatory responses to lung inflation and arterial CO2 in halothane-anesthetized dogs

Hypercapnia attenuates the effects of static airway pressure (Paw) on phrenic burst frequency (f) and the expiratory duration (TE) in chloralose-urethan-anesthetized dogs. Surgical removal of the carotid bodies abolishes this interaction. Since halothane anesthesia in hyperoxia greatly impairs peripheral chemoreflexes, experiments were conducted to determine whether hypercapnia would attenuate the effects of Paw on f and TE in halothane-anesthetized dogs (approximately 1.5 minimum alveolar concentration). Integrated activity of the phrenic nerve was monitored as a function of Paw (2-12 cmH2O) in a vascularly isolated left lung at varied levels of arterial PCO2 (PaCO2; 38-80 Torr) controlled by inspired gas concentrations ventilating the denervated but perfused right lung. Halothane was administered only to the right lung. The results were as follows: 1) integrated phrenic amplitude increased with PaCO2 but was unaffected by Paw; 2) f decreased as Paw increased but was not affected by PaCO2; 3) the inspiratory duration (TI) increased as PaCO2 increased but was unaffected by Paw; 4) TE increased as Paw increased but was unaffected by PaCO2; and 5) there was no phrenic response to intravenous sodium cyanide (50-100 micrograms/kg). Thus, unlike chloralose-urethan-anesthetized dogs, hypercapnia does not attenuate the effect of lung inflation on f or TE in halothane-anesthetized dogs. Furthermore, hypercapnia increases TI during halothane anesthesia, an effect found after carotid denervation but not found in intact chloralose-urethan-anesthetized dogs. It is suggested that these differences between chloralose-urethan- and halothane-anesthetized dogs may be due to functional carotid chemoreceptor denervation by halothane.     

The role of peripheral chemoreceptor activity on the respiratory responses to hypoxia and hypercapnia in anaesthetised rabbits with induced hypothyroidism

The purpose of this study was to investigate the role of peripheral chemoreceptor activity on the hypoxic and hypercapnic ventilatory drives in rabbits with induced hypothyroidism. Experiments were carried out in control and hypothyroid rabbits. Hypothyroidism was induced by an administration of an iodide-blocker, methimazole in food (75 mg/100 g food) for ten weeks. At the end of the tenth week, triiodothyronine (T3) and thyroxine (T4) levels significantly decreased (P<0.001) while thyroid stimulating hormone (TSH) increased (P<0.001). Tidal volume (VT), respiratory frequency (f/min), ventilation minute volume (VE) and systemic arterial blood pressure (BP) were recorded during the breathing of the normoxic, hypoxic (8% O2-92% N2) and hypercapnic (6% CO2-Air) gas mixtures, in the anaesthetised rabbits of both groups. At the end of each experimental phase, PaO2, PaCO2, and pHa were measured. The same experimental procedure was repeated after peripheral chemoreceptor denervation in both groups. VT significantly decreased in some of the rabbits with hypothyroidism during the breathing of the hypoxic gas mixture (nonresponsive subgroup) (P<0.05). After chemodenervation, a decrease in VT was observed in this nonresponsive subgroup during normoxia (P<0.05). The percent decrease in VT in nonresponsive subgroup of hypothyroid rabbits after chemodenervation was lower than that of the chemodenervated control animals (P<0.01). When these rabbits with hypothyroidism were allowed to breath the hypercapnic gas mixtures, increases in VT and VE were not significant. In conclusion, although there is a decrease in peripheral chemoreceptor activity in hypothyroidism, it does not seem to be the only cause of decrease in ventilatory drive during hypoxia and hypercapnia.     

High-frequency oscillations via the pleural surface: an alternative mode of ventilation?

We applied high-frequency oscillatory ventilation (HFOV) of low amplitude to the pleural surface of the isolated rat lung (IPL) perfused at 10 ml X min-1 with Krebs bicarbonate containing 4.5% albumin (hematocrit 34%). Lung volume was held constant by a continuous positive airways pressure (CPAP) of 5 cmH2O. Varying CPAP from 2 to 15 cmH2O did not affect O2 uptake. Tidal volume (VT) was estimated with an impedance pneumograph, and it bore a direct linear relationship to the amplitude of both the loudspeaker input signal and the pressure change in the chamber up to 30 Hz; VT was inversely proportional to the frequency (f). However, at a constant loudspeaker input of 10 V, minute expired ventilation (VE) remained constant (mean 104 ml X min-1) as f increased from 5 to 30 Hz. Hemoglobin saturation increased by more than 80% during HFOV of 5-40 Hz and amplitude of 10 V, the maximum O2 uptake being 14.6 ml O2 per 100 ml perfusate. Whereas dead space was approximately 335 microliters, a VT of less than 40 microliters could effect normal O2 uptake, suggesting that bulk flow is playing only a minor role in gas exchange. HFOV for 60 min (CPAP 5 cmH2O) did not affect the amount of alveolar surfactant compared with conventional ventilation at the same mean airway pressure. We conclude that normal O2 uptake can be maintained by applying HFOV to the pleural surface of the IPL held at constant volume.     

Combination of constant-flow and continuous positive-pressure ventilation in canine pulmonary edema

Constant-flow ventilation (CFV) maintains alveolar ventilation without tidal excursion in dogs with normal lungs, but this ventilatory mode requires high CFV and bronchoscopic guidance for effective subcarinal placement of two inflow catheters. We designed a circuit that combines CFV with continuous positive-pressure ventilation (CPPV; CFV-CPPV), which negates the need for bronchoscopic positioning of CFV cannula, and tested this system in seven dogs having oleic acid-induced pulmonary edema. Addition of positive end-expiratory pressure (PEEP, 10 cmH2O) reduced venous admixture from 44 +/- 17 to 10.4 +/- 5.4% and kept arterial CO2 tension (PaCO2) normal. With the innovative CFV-CPPV circuit at the same PEEP and respiratory rate (RR), we were able to reduce tidal volume (VT) from 437 +/- 28 to 184 +/- 18 ml (P less than 0.001) and elastic end-inspiratory pressures (PEI) from 25.6 +/- 4.6 to 17.7 +/- 2.8 cmH2O (P less than 0.001) without adverse effects on cardiac output or pulmonary exchange of O2 or CO2; indeed, PaCO2 remained at 35 +/- 4 Torr even though CFV was delivered above the carina and at lower (1.6 l.kg-1.min-1) flows than usually required to maintain eucapnia during CFV alone. At the same PEEP and RR, reduction of VT in the CPPV mode without CFV resulted in CO2 retention (PaCO2 59 +/- 8 Torr). We conclude that CFV-CPPV allows CFV to effectively mix alveolar and dead spaces by a small bulk flow bypassing the zone of increased resistance to gas mixing, thereby allowing reduction of the CFV rate, VT, and PEI for adequate gas exchange.     

Effects of acute hyperbaric oxygenation on respiratory control in cats

We studied ventilatory responsiveness to hypoxia and hypercapnia in anesthetized cats before and after exposure to 5 atmospheres absolute O2 for 90-135 min. The acute hyperbaric oxygenation (HBO) was terminated at the onset of slow labored breathing. Tracheal airflow, inspiratory (TI) and expiratory (TE) times, inspiratory tidal volume (VT), end-tidal PO2 and PCO2, and arterial blood pressure were recorded simultaneously before and after HBO. Steady-state ventilation (VI at three arterial PO2 (PaO2) levels of approximately 99, 67, and 47 Torr at a maintained arterial PCO2 (PaCO2, 28 Torr) was measured for the hypoxic response. Ventilation at three steady-state PaCO2 levels of approximately 27, 36, and 46 Torr during hyperoxia (PaO2 450 Torr) gave a hypercapnic response. Both chemical stimuli significantly stimulated VT, breathing frequency, and VI before and after HBO. VT, TI, and TE at a given stimulus were significantly greater after HBO without a significant change in VT/TI. The breathing pattern, however, was abnormal after HBO, often showing inspiratory apneusis. Bilateral vagotomy diminished apneusis and further prolonged TI and TE and increased VT. Thus a part of the respiratory effects of HBO is due to pulmonary mechanoreflex changes.     

舒利迭无创通气对慢性阻塞性肺疾病合并呼吸衰竭患者肺功能及动脉血 气分析的影响

目的:探讨舒利迭联合无创通气对慢性阻塞性肺疾病(COPD)合并呼吸衰竭患者肺功能和动脉血气的影响。方法:选取2013年5月-2015年5月在我院接受治疗的COPD合并呼吸衰竭患者92例,根据治疗方法不同,将患者分为研究组和对照组。对照组患者给予控制感染、化痰、平喘等常规治疗,研究组在此基础上给予舒利迭无创通气治疗。采用血气分析仪检测两组患者治疗前后二氧化碳分压(PaCO_2)、血氧分压(PaO_2)及酸碱度(pH)等动脉血气指标。应用肺功能检测仪检测患者用力肺活量(FVC)、呼气高峰流量(PEFR)以及1 s用力呼气容积(FEV1)等肺功能指标。结果:治疗前,两组患者PaCO_2,PaO_2,pH,FVC,PEFR及FEV1比较,差异均无统计学意义(P0.05);治疗后,两组患者PaCO_2较治疗前明显下降,而PaO_2与pH明显上升,差异具有统计学意义(P0.05);治疗后,研究组PaCO_2低于对照组,而PaO_2与pH高于对照组,差异具有统计学意义(P0.05);治疗后,两组患者FVC,PEFR及FEV1明显上升,且研究组高于对照组,差异均具有统计学意义(P0.05)。结论:舒利迭联合无创通气对COPD合并呼吸衰竭患者肺功能及动脉血气具有明显的改善作用,值得临床推广及应用。     

Effect of tracheal bias flow on gas exchange during high-frequency chest percussion

High-frequency chest percussion (HFP) with constant fresh gas flow (VBF) at the tracheal carina is a variant of high-frequency ventilation (HFV) previously shown to be effective with extremely low tracheal oscillatory volumes (approximately 0.1 ml/kg). We studied the effects of VBF on gas exchange during HFP. In eight anesthetized and paralyzed dogs we measured arterial and alveolar partial pressures of CO2 (PaCO2) and O2 (PaO2) during total body vibration at a frequency of 30 Hz, amplitude of 0.17 +/- 0.019 cm, and tidal volume of 1.56 +/- 0.58 ml. VBF was incrementally varied from 0.1 to 1.2 l.kg-1.min-1. At low flows (0.1-0.4 l.kg-1.min-1), gas exchange was strongly dependent on flow rate but became essentially flow independent with higher VBF (i.e., hyperbolic pattern). At VBF greater than 0.4 l.kg-1.min-1, hyperventilatory blood gas levels were consistently sustained (i.e., PaCO2 less than 20 Torr, PaO2 greater than 90 Torr). The resistance to CO2 transport of the airways was 1.785 +/- 0.657 l-1.kg.min and was independent of VBF. The alveolar-arterial difference of O2 was also independent of the flow. In four of five additional dogs studied as a control group, where constant flow of O2 was used without oscillations, the pattern of PaCO2 vs. VBF was also hyperbolic but at substantially higher levels of PaCO2. It is concluded that, in the range of VBF used, intraairway gas exchange was limited by the 30-Hz vibration. The fresh gas flow was important only to maintain near atmospheric conditions at the tracheal carina.     

Effect of lung inflation on regional lung expansion in supine and prone rabbits

At functional residual capacity, lung expansion is more uniform in the prone position than in the supine position. We examined the effect of positive airway pressure (Paw) on this position-dependent difference in lung expansion. In supine and prone rabbits postmortem, we measured alveolar size through dependent and nondependent pleural windows via videomicroscopy at Paw of 0 (functional residual capacity), 7, and 15 cmH2O. After the chest was opened, alveolar size was measured in the isolated lung at several transpulmonary pressures (Ptp) on lung deflation. Alveolar mean linear intercept (Lm) was measured from the video images taken in situ. This was compared with those measured in the isolated lung to determine Ptp in situ. In the supine position, the vertical Ptp gradient increased from 0.52 cmH2O/cm at 0 cmH2O Paw to 0.90 cmH2O/cm at 15 cmH2O Paw, while the vertical gradient in Lm decreased from 2.17 to 0.80 microns/cm. In the prone position, the vertical Ptp gradient increased from 0.06 cmH2O/cm at 0 cmH2O Paw to 0.35 cmH2O/cm at 15 cmH2O Paw, but there was no change in the vertical Lm gradient. In anesthetized paralyzed rabbits in supine and prone positions, we measured pleural liquid pressure directly at 0, 7, and 15 cmH2O Paw with dependent and nondependent rib capsules. Vertical Ptp gradients measured with rib capsules were similar to those estimated from the alveolar size measurements. Lung inflation during mechanical ventilation may reduce the vertical nonuniformities in lung expansion observed in the supine position, thereby improving gas exchange and the distribution of ventilation.     

Effect of hilar nerve denervation on breathing and arterial PCO2 during CO2 inhalation

We determined the effects of denervating the hilar branches (HND) of the vagus nerves on breathing and arterial PCO2 (PaCO2) in awake ponies during eupnea and when inspired PCO2 (PICO2) was increased to 14, 28, and 42 Torr. In five carotid chemoreceptor-intact ponies, breathing frequency (f) was less, whereas tidal volume (VT), inspiratory time (TI), and ratio of TI to total cycle time (TT) were greater 2-4 wk after HND than before HND. HND per se did not significantly affect PaCO2 at any level of PICO2, and the minute ventilation (VE)-PaCO2 response curve was not significantly altered by HND. Finally, the attenuation of a thermal tachypnea by elevated PICO2 was not altered by HND. Accordingly, in carotid chemoreceptor-intact ponies, the only HND effect on breathing was the change in pattern classically observed with attenuated lung volume feedback. There was no evidence suggestive of a PCO2-H+ sensory mechanism influencing VE, f, VT, or PaCO2. In ponies that had the carotid chemoreceptors denervated (CBD) 3 yr earlier, HND also decreased f, increased VT, TI, and TT, but did not alter the slope of the VE-PaCO2 response curve. However, at all levels of elevated PICO2, the arterial hypercapnia that had persistently been attenuated, since CBD was restored to normal by HND. The data suggest that during CO2 inhalation in CBD ponies a hilar-innervated mechanism influences PaCO2 by reducing physiological dead space to increase alveolar ventilation.     

Physiological dead space during high-frequency ventilation in dogs

Tidal volumes used in high-frequency ventilation (HFV) may be smaller than anatomic dead space, but since gas exchange does take place, physiological dead space (VD) must be smaller than tidal volume (VT). We quantified changes in VD in three dogs at constant alveolar ventilation using the Bohr equation as VT was varied from 3 to 15 ml/kg and frequency (f) from 0.2 to 8 Hz, ranges that include normal as well as HFV. We found that VD was relatively constant at tidal volumes associated with normal ventilation (7-15 ml/kg) but fell sharply as VT was reduced further to tidal volumes associated with HFV (less than 7 ml/kg). The frequency required to maintain constant alveolar ventilation increased slowly as tidal volume was decreased from 15 to 7 ml/kg but rose sharply with attendant rapid increases in minute ventilation as tidal volumes were decreased to less than 7 ml/kg. At tidal volumes less than 7 ml/kg, the data deviated substantially from the conventional alveolar ventilation equation [f(VT - VD) = constant] but fit well a model derived previously for HFV. This model predicts that gas exchange with volumes smaller than dead space should vary approximately as the product of f and VT2.     

Exercise performance following a carbohydrate load in chronic airflow obstruction

We evaluated the effects of a large (920 cal) liquid carbohydrate (CHO) load on the maximum exercise capacity of 18 patients with chronic airflow obstruction [forced expiratory volume at at 1 s (FEV1) = 1.27 +/- 0.48 liters; FEV1/forced vital capacity = 0.41 +/- 0.11]. Patients underwent duplicate incremental cycle ergometer exercise tests to a symptom-limited maximum following CHO and a liquid placebo in single-blind fashion. Expired gas measurements were obtained during each power output. In 12 patients arterial blood gases were measured, and in six patients venous blood was obtained for measurement of glucose, electrolytes, and osmolality. With CHO, the maximum power output decreased from 86 +/- 30 to 76 +/- 31 W (P less than 0.001), whereas the ventilation at exhaustion was nearly identical (47.6 +/- 13.2 and 46.8 +/- 12.5 l/min). Arterial partial pressure of CO2 (PaCO2) at exhaustion decreased (P less than 0.025), arterial partial pressure of O2 (PaO2) increased (P less than 0.01), and the ventilatory equivalent for CO2 (VE/VCO2) increased (P less than 0.005) with CHO. At equivalent power outputs, CHO resulted in significant increases in VE (P less than 0.001) and VCO2 (P less than 0.001); PaCO2 was unchanged, whereas PaO2 increased (P less than 0.01). CHO increased the serum glucose at rest and during exercise. No changes in serum osmolality or electrolytes occurred during exercise following CHO. After CHO loading, the majority of patients appeared to reach their limiting level of ventilation at a lower power output. In contrast, there was no significant difference in the mean maximum power output with CHO in six normal control subjects.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Physiological dead space and effective parabronchial ventilation in ducks

Gas exchange in avian lungs is described by a cross-current model that has several differences from the alevolar model of mammalian gas exchange [e.g., end-expired PCO2 greater than arterial PCO2 (PaCO2)]. Consequently the methods available for estimating effective ventilation and physiological dead space (VDphys) in alveolar lungs are not suitable for an analysis of gas exchange in birds. We tested a method for measuring VDphys in birds that is functionally equivalent to the conventional alveolar VDphys. A cross-current O2-CO2 diagram was used to define the ideal expired point (PEi) and VDphys was calculated as from the equation, VDphys = [(PEiCO2--PECO2)/PEiCO2]. VT, where VT is tidal volume. In seven Pekin ducks VDphys was 13.8 ml greater than anatomic dead space and measured changes in the instrument dead space volume. VDphys also reflected changes in ventilation-perfusion inequality induced by temporary unilateral pulmonary arterial occlusion. Bohr dead space, calculated by substituting end-expired PCO2 for PEiCO2, was insensitive to such inhomogeneity. Enghoff dead space, calculated by substituting PaCO2 for PEiCO2, is theoretically incorrect for cross-current gas exchange and was often less than anatomic dead space. We conclude that VDphys is a useful index of avian gas exchange and propose a standard definition for effective parabronchial ventilation (VP) analogous to alveolar ventilation (i.e., VP = VE--VDphys, where VE is total ventilation).