Steady-state response of normal subjects to inspiratory resistive load

Tidal volume (VT) is usually preserved when conscious humans are made to breathe against an inspiratory resistance. To identify the neural changes responsible for VT compensation we calculated the respiratory driving pressure waveform during steady-state unloaded and loaded breathing (delta R = 8.5 cmH2O X 1(-1) X s) in eight conscious normal subjects. Driving pressure (DP) was calculated according to the method of Younes et al. (J. Appl. Physiol. 51: 963-989, 1981), which provides the equivalent of occlusion pressure at functional residual capacity throughout the breath. VT during resistance breathing was 108% of unloaded VT, as opposed to a predicted value of 82% of control in the absence of neural compensation. Compensation was accomplished through three changes in the DP waveform: 1) peak amplitude increased (+/- 23%), 2) the duration of the rising phase increased (+42%); and 3) the rising phase became more concave to the time axis. There were no changes in the relative decay rate of inspiratory pressure during expiration, in the shape of the declining phase of DP, or in end-expiratory lung volume.     

Oxygen cost of resistive-loaded breathing in quadriplegia.

We hypothesized that, in quadriplegia, chest wall distortion would increase the energy cost of ventilation. To assess this, we measured the oxygen cost of breathing (VO2 resp) and changes in chest wall configuration during inspiratory resistive-loaded breathing tasks in five quadriplegic and five normal subjects. Each subject performed three breathing tasks that spanned a range of work rates (Wtot). Configurational changes of the abdomen and upper, lower, and transverse rib cage were assessed with magnetometers. We found that 1) in both groups, VO2resp increased linearly with Wtot over the range of tasks performed, 2) the mean slope of the regression line of VO2resp vs. Wtot was greater for quadriplegic than for normal subjects (3.7 +/- 0.8 vs. 2.0 +/- 0.7 ml O2/J, P less than 0.01), 3) efficiency of breathing (Wtot/VO2resp) was less for quadriplegic than for normal subjects (1.9 +/- 0.6 vs. 3.5 +/- 1.4%, P less than 0.001), 4) during inhalation, upper and lower rib cages behaved similarly in the two groups, but the quadriplegic subjects had a decrease in transverse rib cage and a much greater increase in abdomen than normal subjects, and 5) functional residual capacity decreased in normal but not in quadriplegic subjects during the breathing tasks. We conclude that the lesser efficiency of breathing in quadriplegia may be related to the elastic work of chest wall distortion, shorter mean operational diaphragm length, and possibly differences between normal and quadriplegic subjects in mechanical advantage of available inspiratory muscles.     

Respiratory responses to ventilatory loading following low cervical spinal cord injury

This study compared the respiratory responses to ventilatory loading in 8 normal subjects and 11 quadriplegic patients with low cervical spinal cord transection. Progressive hypercapnia was produced by rebreathing. Rebreathing trials were carried out with no added load and with inspiratory resistive loads of 5 and 16 cmH2O. l-1 X s. Measurements were made of ventilation and of diaphragmatic electromyographic activity. Base-line hypercapnic ventilatory responses were significantly lower than normal in the quadriplegic patients, but the effects of resistive loading on the ventilatory responses were comparable in the two groups. The change in peak moving-average diaphragmatic electrical activity (DI peak) for a given change in CO2 partial pressure (PCO2) and DI peak at PCO2 55 Torr increased significantly with resistive loading both in the normal subjects and the quadriplegic patients. In the normal subjects, but not in the quadriplegic patients, inspiratory duration increased progressively with increasing resistance. The increase in DI peak during ventilatory loading in the normal subjects was a consequence of inspiratory prolongation. In contrast, in the quadriplegic patients during breathing against the larger resistive load, there was a significant increase in the average rate of rise (DI peak divided by the time from onset to peak) of diaphragmatic activity. The change in DI rate of rise for a given change in PCO2 increased to 137 +/- 13% (SE), and the DI rate of rise at PCO2 55 Torr increased to 128 +/- 8% (SE) of control values. These results indicate that compensatory increases in diaphragmatic activation during ventilatory loading occur in quadriplegic patients in whom afferent feedback from rib cage receptors is disrupted.     

Mechanisms of respiratory elastic load compensation in anesthetized humans

In anesthetized humans the nature of tidal volume (VT) compensation during elastic loading (as reflected in the difference between passive and effective respiratory elastances (Ers) and (E*rs), respectively) has not been fully elucidated. We assessed the relative contribution of various mechanisms contributing to VT compensation during linear elastic loading in 10 young anesthetized adults free of cardiorespiratory disease. Ers averaged 22.0 cmH2O X 1(-1), representing 64% of E*rs. Most of E*rs (84%) was comprised of the active elastance (E'rs), reflecting the major role played by the addition of force-length properties of inspiratory muscles to the internal impedance, and chest wall distortion played in the defense of VT. Of the remaining 16% of E*rs, the difference between E*rs and isotime E*rs, representing the contribution of prolongation of inspiratory time (TI) via the Hering-Breuer reflex, amounted to only 9%. Finally, the remainder of E*rs, which reflects the difference between E*rs and E'rs in the absence of vagal modulation, and attributed to several factors [shape of driving pressure wave, duration of control TI, and magnitude of E'rs and intrinsic flow resistance plus external resistances (Zin, Rossi, Zocchi, and Milic-Emili. J. Appl. Physiol. 57: 271-277, 1984)], amounted to less than 7%.     

Response of normal subjects to inspiratory resistive unloading

The purpose of this study was to examine the role of the normal inspiratory resistive load in the regulation of respiratory motor output in resting conscious humans. We used a recently described device (J. Appl. Physiol. 62: 2491-2499, 1987) to make mouth pressure during inspiration positive and proportional to inspiratory flow, thus causing inspiratory resistive unloading (IRUL); the magnitude of IRUL (delta R = -3.0 cmH2O.1(-1).s) was set so as to unload most (approximately 86% of the normal inspiratory resistance. Six conscious normal humans were studied. Driving pressure (DP) was calculated according to the method of Younes et al. (J. Appl. Physiol. 51: 963-1001, 1981), which provides the equivalent of occlusion pressure at functional residual capacity throughout the breath. IRUL resulted in small but significant changes in minute ventilation (0.6 1/min) and in end-tidal CO2 concentration (-0.11%) with no significant change in tidal volume or respiratory frequency. There was a significant shortening of the duration (neural inspiratory time) of the rising phase of the DP waveform and the shape of the rising phase became more convex to the time axis. There was no change in the average rate of rise of DP or in the duration or shape of the declining phase. We conclude that 1) the normal inspiratory resistance is an important determinant of the duration and shape of the rising phase of DP and 2) the neural responses elicited by the normal inspiratory resistance are similar to those observed with added inspiratory resistive loads.     

Reflex compensation of spontaneous breathing when immersion changes diaphragm length

We measured tidal volume (VT), chest wall dimensions, end-tidal PCO2, and respiratory muscle electromyograms as seated subjects were immersed in water. We studied nine spontaneously breathing subjects; five were uninformed. Raising the water to xiphoid level pushed the abdomen in and expanded the rib cage at end expiration. This increased the diaphragm's operating length, giving it a contractile advantage, and shortened the inspiratory intercostals, giving them a contractile disadvantage. Peak inspiratory activities of both muscle groups decreased; inspiratory time (TI), respiratory frequency (f), and VT were unchanged. The experiments thus demonstrated operational length compensation during immersion and further showed that inspiratory muscle activation is not adjusted locally, according to changes in each muscle's length, but rather that the response is global. Xiphoid-to-shoulder immersion was less easily interpreted, since both rib cage and abdomen were compressed, lengthening both inspiratory muscles. Our subjects continued to maintain VT, f, and TI. Peak inspiratory activities of both muscles were further reduced. We do not attribute the change in inspiratory muscle activation to altered chemical drive or to voluntary response. Rather, the response appears to be a mechanoreceptive reflex that employs afferent information from the lungs or diaphragm to adjust all inspiratory muscle activities.     

Effect of SO2 on control of breathing in anesthetized cats

In seven anesthetized tracheotomized cats we studied the acute respiratory effects of SO2 inhalation at different steady-state levels of arterial CO2 tension (Paco2). During room air breathing, SO2 (0.05%) addition caused a progressive reduction in tidal volume (VT) and increases in both respiratory frequency (f) and pulmonary resistance (RL). Atropine sulfate abolished the bronchoconstriction response to SO2 and thus permitted the study of the influence of SO2 on VT and f in the absence of constricted airways. Despite marked reductions in the VT VS. PaCO2 relationships with SO2 exposure after atropine, the relationship between pulmonary ventilation (VE) and PaCO2 was not signifcantly altered. This was the case since SO2 caused solely a reduction in inspiratory duration (Ti), affecting neither the mean rate of rise of inspiratory activity (i.e., VT/Ti) nor the relationship between Ti and breath duration. Thus, airways irritation with SO2 produced rapid, shallow breathing characterized by a shortening of inspiratory and total respiratory cycle times with no change in the rate of development of inspiratory activity. The findings suggest an influence exclusively concerned with the timing of inspiration. Perhaps premature onset of inspiratory activity accounts for the observed effects.     

Effect of mechanical loading on displacements of chest wall during breathing in humans

Using a respiratory inductive plethysmograph (Respitrace) we studied thoracoabdominal movements in eight normal subjects during inspiratory resistive (Res) and elastic (El) loading. The magnitude of loads was chosen so as to produce a fall in inspiratory mouth pressure of 20 cmH2O. The contribution of rib cage (RC) to tidal volume (VT) increased significantly from 68% during quiet breathing (QB) to 74% during El and 78% during Res. VT and breathing frequency did not change significantly. During loading a phase lag was present on inspiration so that the abdomen led the rib cage. However, outward movement of the abdomen ceased in the latter part of inspiration, and the RC became the sole contributor to VT. These observations suggest greater recruitment of the inspiratory musculature of the RC than the diaphragm during loading, although changes in the mechanical properties of the chest wall may also have contributed. Indeed, an increase in abdominal end-expiratory and end-inspiratory pressures was observed in five out of six subjects, indicating abdominal muscle recruitment which may account for part of the reduction in abdominal excursion. Both Res and El increased the rate of emptying of the respiratory system during the ensuing unloaded expiration as a result of a reduction in rib cage expiratory-braking mechanisms. The time course of abdominal displacements during expiration was unaffected by loading.     

Airway anesthesia effects on hypercapnic breathing pattern in humans

Minute ventilation (VE) and breathing pattern during an abrupt increase in fractional CO2 were compared in 10 normal subjects before and after airway anesthesia. Subjects breathed 7% CO2-93% O2 for 5 min before and after inhaling aerosolized lidocaine. As a result of airway anesthesia, VE and tidal volume (VT) were greater during hypercapnia, but there was no effect on inspiratory time (TI). Therefore, airway anesthesia produced an increase in mean inspiratory flow (VT/TI) during hypercapnia. The increase in VT/TI was compatible with an increase in neuromuscular output. There was no effect of airway anesthesia on the inspiratory timing ratio or the shape and position of the curve relating VT and TI. We also compared airway resistance (Raw), thoracic gas volume, forced vital capacity, forced expired volume at 1s, and maximum midexpiratory flow rate before and after airway anesthesia. A small (0.18 cmH2O X l-1 X s) decrease in Raw occurred after airway anesthesia that did not correlate with the effect of airway anesthesia on VT/TI. We conclude that airway receptors accessible to airway anesthesia play a role in hypercapnic VE.     

Induction of periodic breathing during sleep causes upper airway obstruction in humans

To test the hypothesis that occlusive apneas result from sleep-induced periodic breathing in association with some degree of upper airway compromise, periodic breathing was induced during non-rapid-eye-movement (NREM) sleep by administering hypoxic gas mixtures with and without applied external inspiratory resistance (9 cmH2O X l-1 X s) in five normal male volunteers. In addition to standard polysomnography for sleep staging and respiratory pattern monitoring, esophageal pressure, tidal volume (VT), and airflow were measured via an esophageal catheter and pneumotachograph, respectively, with the latter attached to a tight-fitting face mask, allowing calculation of total pulmonary system resistance (Rp). During stage I/II NREM sleep minimal period breathing was evident in two of the subjects; however, in four subjects during hypoxia and/or relief from hypoxia, with and without added resistance, pronounced periodic breathing developed with waxing and waning of VT, sometimes with apneic phases. Resistive loading without hypoxia did not cause periodicity. At the nadir of periodic changes in VT, Rp was usually at its highest and there was a significant linear relationship between Rp and 1/VT, indicating the development of obstructive hypopneas. In one subject without added resistance and in the same subject and in another during resistive loading, upper airway obstruction at the nadir of the periodic fluctuations in VT was observed. We conclude that periodic breathing resulting in periodic diminution of upper airway muscle activity is associated with increased upper airway resistance that predisposes upper airways to collapse.     

Active and passive respiratory mechanics in anesthetized dogs

In six spontaneously breathing anesthetized dogs (pentobarbital sodium, 30 mg/kg) airflow, volume, and tracheal and esophageal pressures were measured. The active and passive mechanical properties of the total respiratory system, lung, and chest wall were calculated. The average passive values of respiratory system, lung, and chest wall elastances amounted to, respectively, 50.1, 32.3, and 17.7 cmH2O X l-1. Resistive pressure-vs.-flow relationships for the relaxed respiratory system, lung, and chest wall were also determined; a linear relationship was found for the former (the total passive intrinsic resistance averaged 4.1 cmH2O X l-1 X s), whereas power functions best described the others: the pulmonary pressure-flow relationship exhibited an upward concavity, which for the chest wall presented an upward convexity. The average active elastance and resistance of the respiratory system were, respectively, 64.0 cmH2O X l-1 and 5.4 cmH2O X l-1 X s. The greater active impedance reflects pressure losses due to force-length and force-velocity properties of the inspiratory muscles and those due to distortion of the respiratory system from its relaxed configuration.     

Partitioning of respiratory mechanics in halothane-anesthetized humans

In five spontaneously breathing anesthetized subjects [halothane approximately 1 minimal alveolar concentration (MAC), 70% N2O, 30% O2], flow, changes in lung volume, and esophageal and airway opening pressure were measured in order to partition the elastance (Ers) and flow resistance (Rrs) of the total respiratory system into the lung and chest wall components. Ers averaged (+/- SD) 23.0 +/- 4.9 cmH2O X l-1, while the corresponding values of pulmonary (EL) and chest wall (EW) elastance were 14.3 +/- 3.2 and 8.7 +/- 3.0 cmH2O X l-1, respectively. Intrinsic Rrs (upper airways excluded) averaged 2.3 +/- 0.2 cmH2O X l-1 X s, the corresponding values for pulmonary (RL) and chest wall (RW) flow resistance amounting to 0.8 +/- 0.4 and 1.5 +/- 0.5 cmH2O X l-1 X s, respectively. Ers increased relative to normal values in awake state, mainly reflecting increased EL. Rw was higher than previous estimates on awake seated subjects (approximately 1.0 cmH2O X l-1 X s). RL was relatively low, reflecting the fact that the subjects had received atropine (0.3-0.6 mg) and were breathing N2O. This is the first study in which both respiratory elastic and flow-resistive properties have been partitioned into lung and chest wall components in anesthetized humans.     

Respiratory mechanics during halothane anesthesia and anesthesia-paralysis in humans

In six spontaneously breathing anesthetized subjects [halothane approximately 1 maximum anesthetic concentration (MAC), 70% N2O-30% O2], we measured flow (V), volume (V), and tracheal pressure (Ptr). With airway occluded at end-inspiration tidal volume (VT), we measured Ptr when the subjects relaxed the respiratory muscles. Dividing relaxed Ptr by VT, total respiratory system elastance (Ers) was obtained. With the subject still relaxed, the occlusion was released to obtain the V-V relationship during the ensuing relaxed expiration. Under these conditions, the expiratory driving pressure is V X Ers, and thus the pressure-flow relationship of the system can be obtained. By subtracting the flow resistance of equipment, the intrinsic respiratory flow resistance (Rrs) is obtained. Similar measurements were repeated during anesthesia-paralysis (succinylcholine). Ers averaged 23.9 +/- 4 (+/- SD) during anesthesia and 21 +/- 1.8 cmH2O X 1(-1) during anesthesia-paralysis. The corresponding values of intrinsic Rrs were 1.6 +/- 0.7 and 1.9 +/- 0.9 cmH2O X 1(-1) X s, respectively. These results indicate that Ers increases substantially during anesthesia, whereas Rrs remains within the normal limits. Muscle paralysis has no significant effect on Ers and Rrs. We also provide the first measurements of inspiratory muscle activity and related negative work during spontaneous expiration in anesthetized humans. These show that 36-74% of the elastic energy stored during inspiration is wasted in terms of negative inspiratory muscle work.     

Effects of inspiratory resistive load on respiratory control in hypercapnia and exercise

Eight healthy young men underwent two separate steady-state incremental exercise runs within the aerobic range on a treadmill with alternating periods of breathing with no load (NL) and with an inspiratory resistive load (IRL) of approximately 12 cmH2O.1-1.s. End-tidal PCO2 was maintained constant throughout each run at the eucapnic or a constant hypercapnic level by adding 0-5% CO2 to the inspired O2. Hypercapnia caused a steepening, as well as upward shift, relative to the corresponding eucapnic ventilation-CO2 output (VE - VCO2) relationship in NL and IRL. Compared with NL, the VE - VCO2 slope was depressed by IRL, more so in hypercapnic [-19.0 +/- 3.4 (SE) %] than in eucapnic exercise (-6.0 +/- 2.0%), despite a similar increase in the slope of the occlusion pressure at 100 ms - VCO2 (P100 - VCO2) relationship under both conditions. The steady-state hypercapnic ventilatory response at rest was markedly depressed by IRL (-22.6 +/- 7.5%), with little increase in P100 response. For a given inspiratory load, breathing pattern responses to separate or combined hypercapnia and exercise were similar. During IRL, VE was achieved by a greater tidal volume (VT) and inspiratory duty cycle (TI/TT) along with a lower mean inspiratory flow (VT/TI). The increase in TI/TT was solely because of a prolongation of inspiratory time (TI) with little change in expiratory duration for any given VT. The ventilatory and breathing pattern responses to IRL during CO2 inhalation and exercise are in favor of conservation of respiratory work.(ABSTRACT TRUNCATED AT 250 WORDS)     

Ventilatory response to high-frequency airway oscillation in humans

To investigate respiratory control during high-frequency oscillation (HFO), ventilation was monitored in conscious humans by respiratory inductive plethysmography during application at the mouth of high-frequency pressure oscillations. Studies were conducted before and after airway and pharyngeal anesthesia. During HFO, breathing became slow and deep with an increase in tidal volume (VT) of 37% (P less than 0.01) and inspiratory duration (TI) of 34% (P less than 0.01). Timing ratio (TI/TT) increased 14% (P less than 0.05) and respiratory frequency (f) decreased 12% (P less than 0.01). Mean inspiratory flow (VT/TI) did not change during HFO. Following airway anesthesia, VT increased only 26% during HFO (P less than 0.01), whereas significant changes in TI, TI/TT, and f were not observed. Pharyngeal anesthesia failed to diminish the effect of HFO on TI, TT, or f, although the increase in VT was reduced. These results indicate that 1) HFO presented in this manner alters inspiratory timing without affecting the level of inspiratory activity, and 2) receptors in the larynx and/or lower airways may in part mediate the response.     

Respiratory abdominal muscle recruitment and chest wall motion in myotonic muscular dystrophy.

Abdominal muscles are selectively active in normal subjects during stress and may increase the potential energy for inspiration by reducing the end-expiratory lung volume (EELV). We hypothesized that a similar process would occur in subjects with myotonic muscular dystrophy (MMD), but would be less effective, because of to their weakness and altered chest wall mechanics. Fine-wire electromyography (EMG) of the transversus abdominis (TA), internal oblique (IO), external oblique, and rectus abdominis was recorded in 10 MMD and 10 control subjects. EMG activity, respiratory inductive plethysmography, and gastric pressure were recorded during static pressure measurement and at increasing levels of inspiratory resistance breathing. EELV was reduced and chest wall motion was synchronous only in controls. Although the TA and IO were selectively recruited in both groups, EMG activity of the MMD group was twice that of controls at the same inspiratory pressure. In MMD subjects with mildly reduced forced vital capacity, significant differences can be seen in abdominal muscle recruitment, wall motion, work of breathing, and ventilatory parameters.     

Inspiratory muscle forces and endurance in maximum resistive loading

The ability of the respiratory muscles to sustain ventilation against increasing inspiratory resistive loads was measured in 10 normal subjects. All subjects reached a maximum rating of perceived respiratory effort and at maximum resistance showed signs of respiratory failure (CO2 retention, O2 desaturation, and rib cage and abdominal paradox). The maximum resistance achieved varied widely (range 73-660 cmH2O X l-1 X s). The increase in O2 uptake (delta Vo2) associated with loading was linearly related to the integrated mouth pressure (IMP): delta Vo2 = 0.028 X IMP + 19 ml/min (r = 0.88, P less than 0.001). Maximum delta Vo2 was 142 ml/min +/- SD 68 ml/min. There were significant (P less than 0.05) relationships between the maximum voluntary inspiratory pressure against an occluded airway (MIP) and both maximum IMP (r = 0.80) and maximum delta Vo2 (r = 0.76). In five subjects, three imposed breathing patterns were used to examine the effect of different patterns of respiratory muscle force deployment. Increasing inspiratory duration (TI) from 1.5 to 3.0 and 6.0 s, at the same frequency of breathing (5.5 breaths/min) reduced peak inspiratory pressure and increased the maximum resistance tolerated (190, 269, and 366 cmH2O X l-1 X s, respectively) and maximum IMP (2043, 2473, and 2913 cmH2O X s X min-1, but the effect on maximum delta Vo2 was less consistent (166, 237, and 180 ml/min). The ventilatory endurance capacity and the maximum O2 uptake of the respiratory muscles are related to the strength of the inspiratory muscles, but are also modified through the pattern of force deployment.     

Lung and chest wall impedances in the dog: effects of frequency and tidal volume.

Dependences of the mechanical properties of the respiratory system on frequency (f) and tidal volume (VT) in the normal ranges of breathing are not clear. We measured, simultaneously and in vivo, resistance and elastance of the total respiratory system (Rrs and Ers), lungs (RL and EL), and chest wall (Rcw and Ecw) of five healthy anesthetized paralyzed dogs during sinusoidal volume oscillations at the trachea (50-300 ml, 0.2-2 Hz) delivered at a constant mean lung volume. Each dog showed the same f and VT dependences. The Ers and Ecw increased with increasing f to 1 Hz and decreased with increasing VT up to 200 ml. Although EL increased slightly with increasing f, it was independent of VT. The Rcw decreased from 0.2 to 2 Hz at all VT and decreased with increasing VT. Although the RL decreased from 0.2 to 0.6 Hz and was independent of VT, at higher f RL tended to increase with increasing f and VT (i.e., as peak flow increased). Finally, the f and VT dependences of Rrs were similar to those of Rcw below 0.6 Hz but mirrored RL at higher f. These data capture the competing influences of airflow nonlinearities vs. tissue nonlinearities on f and VT dependence of the lung, chest wall, and total respiratory system. More specifically, we conclude that 1) VT dependences in Ers and Rrs below 0.6 Hz are due to nonlinearities in chest wall properties, 2) above 0.6 Hz, the flow dependence of airways resistance dominates RL and Rrs, and 3) lung tissue behavior is linear in the normal range of breathing.     

Interrupter technique for measurement of respiratory mechanics in anesthetized cats

In six spontaneously breathing anesthetized cats (pentobarbital sodium, 35 mg/kg ip), airflow, changes in lung volume, and tracheal and esophageal pressures were measured. Airflow was interrupted by brief airway occlusions during relaxed expirations (elicited via the Breuer-Hering inflation reflex) and throughout spontaneous breaths. A plateau in tracheal pressure occurred throughout relaxed expirations and the latter part of spontaneous expirations indicating respiratory muscle relaxation. Measurement of tracheal pressure, immediately preceding airflow, and corresponding volume enabled determination of respiratory system elastance and flow resistance. These were partitioned into lung and chest wall components using esophageal pressure. Respiratory system elastance was constant over the tidal volume range, divided approximately equally between the lung and chest wall. While the passive pressure-flow relationship for the respiratory system was linear, those for the lung and chest wall were curvilinear. Volume dependence of chest wall flow resistance was demonstrated. During inspiratory interruptions, tracheal pressure increased progressively; initial tracheal pressure was estimated by backward extrapolation. Inspiratory flow resistance of the lung and total respiratory system were constant. Force-velocity properties of the contracting inspiratory muscles contributed little to overall active resistance.     

Breathing pattern and CO2 response in newborn rats before and during anesthesia

We have studied the breathing pattern (minute ventilation VE, tidal volume VT, and respiratory rate f) in newborn rats before and during barbiturate (20-30 mg/kg ip) or ketamine anesthesia (40-80 mg/kg ip). Animals were intact and prone in a flow plethysmograph in thermoneutral conditions. Before anesthesia, CO2 breathing (5 min in 5% and 5 min in 10% CO2 in O2) resulted in a substantial increase in VE (169 and 208%, respectively), which was maintained throughout the entire CO2 breathing period. This indicates that, despite the extremely large VE per kilogram at rest, in these small animals there is still a large reserve for a sustained increase in VE. During barbiturate, the resting VE dropped to 45% of control, due to a reduction in VT (83%) and f (59%). This latter result was due to a prolongation of the expiratory time (214%) with no significant changes in inspiratory time. CO2 response was also much depressed, to approximately 63% of the control. The late portion of the expiratory flow-volume curves, the slope of which represents the expiratory time constant of the system, was similar before and during anesthesia in approximately 50% of the animals, whereas it increased during anesthesia in the remaining animals. Although compliance of the respiratory system was generally unaltered, the increased impedance during anesthesia probably reflected an increased resistance. Qualitatively similar results were obtained during ketamine anesthesia. Therefore, as observed in adult mammals, anesthesia in newborn rats has a marked depressant effect on resting breathing pattern and CO2 response, occasionally accompanied by an increase in the expiratory impedance of the respiratory system.