Effect of positive-pressure ventilatory frequency on regional pleural pressure

Regional lung ventilation is modulated by the spatiotemporal distribution of alveolar distending forces. During positive-pressure ventilation, regional transmission of airway pressure (Paw) to the pleural surface may vary with ventilatory frequency (f), thus changing interregional airflow distribution. Pendelluft phenomena may result owing to selective regional hyperventilation or phase differences in alveolar distension. To define the effects of f on regional alveolar distension during positive-pressure ventilation, we compared regional pleural pressure (Ppl) swings from expiration to inspiration (delta Ppl) and end-expiratory Ppl over the f range 0-150 min-1 in anesthetized, paralyzed, close-chested dogs with normal lungs. We inserted six pleural balloon catheters to analyze Ppl distribution along three orthogonal axes of the right hemithorax. Increases in regional Ppl were synchronously coupled with inspiratory increases in Paw regardless of f. However, at a constant tidal volume and percent inspiratory time, end-expiratory Paw and Ppl increased in all regions once a f threshold was reached (P less than 0.01). Supradiaphragmatic delta Ppl were less than in other regions (P less than 0.05), but thoracoabdominal binding abolished this difference by decreasing thoracoabdominal compliance. We conclude that the distribution of forces determining dynamic regional alveolar distension are temporally synchronous but spatially asymmetric during positive-pressure ventilation at f less than or equal to 150/min.     

Hemodynamic effects of resistive breathing

To examine the acute hemodynamic effects induced by large swings in intrathoracic pressure such as may be generated by obstructive lung disease, airway obstruction was simulated by means of two different fixed external alinear resistances and the results were compared with those for unobstructed breathing (C). Eight normal subjects breathed through external resistances during inspiration (I), expiration (E), or both (IE) at rest (Re) and exercise (Ex). The resistances were chosen to induce similar mouth pressure (Pm) swings at Re and Ex. Pleural pressures (Ppl) were found to correlate closely with Pm. During IE resistive breathing mean swings in Pm were -31 and +19 cmH2O at Re and -38 and +22 cmH2O at Ex, with a corresponding decrease in minute ventilation (-30 and -18%) and an increase in end-tidal PCO2 (+5.6 and +4.2 Torr); these were associated with an increase in heart rate (delta HR = 4 and 6 beats/min) and systolic systemic arterial pressure (delta Psas = 10 and 14 Torr at Re and Ex, respectively). O2 consumption and cardiac output did not change. The myocardial O2 consumption, estimated from the product HR X (Psas--Ppl), increased by 17 and 20% at Re and Ex, respectively. Changes in mechanics, gas exchange, and hemodynamics were less pronounced during I or E resistive loading. It is concluded that breathing through a tight external resistance during IE at Re and Ex increases the metabolic load on the myocardium.     

Pleural pressure increases during inspiration in the zone of apposition of diaphragm to rib cage

The zone of apposition of diaphragm to rib cage provides a theoretical mechanism that may, in part, contribute to rib cage expansion during inspiration. Increases in intra-abdominal pressure (Pab) that are generated by diaphragmatic contraction are indirectly applied to the inner rib cage wall in the zone of apposition. We explored this mechanism, with the expectation that pleural pressure in this zone (Pap) would increase during inspiration and that local transdiaphragmatic pressure in this zone (Pdiap) must be different from conventionally determined transdiaphragmatic pressure (Pdi) during inspiration. Direct measurements of Pap, as well as measurements of pleural pressure (Ppl) cephalad to the zone of apposition, were made during tidal inspiration, during phrenic stimulation, and during inspiratory efforts in anesthetized dogs. Pab and esophageal pressure (Pes) were measured simultaneously. By measuring Ppl's with cannulas placed through ribs, we found that Pap consistently increased during both maneuvers, whereas Ppl and Pes decreased. Whereas changes in Pdi of up to -19 cmH2O were measured, Pdiap never departed from zero by greater than -4.5 cmH2O. We conclude that there can be marked regional differences in Ppl and Pdi between the zone of apposition and regions cephalad to the zone. Our results support the concept of the zone of apposition as an anatomic region where Pab is transmitted to the interior surface of the lower rib cage.     

Pleural pressure between diaphragm and rib cage during inspiratory muscle activity

We measured the changes in pleural surface pressure (delta Ppl) in the area of apposition of the rib cage to the diaphragm (Aap) in anesthetized dogs during spontaneous breathing, inspiratory efforts after airway occlusion at functional residual capacity, and phrenic stimulation. Intact dogs were in supine or lateral posture; partially eviscerated dogs were in lateral posture. delta Ppl,ap often differed significantly from changes in abdominal pressure (delta Pab); sometimes they differed in sign (except during phrenic stimulation). Changes in transdiaphragmatic pressure in Aap (delta Pdi,ap) could be positive or negative and were less in eviscerated than in intact dogs. delta Pdi,ap could differ in sign among respiratory maneuvers and over different parts of Aap. Hence average delta Pdi,ap should be closer to zero than delta Pdi,ap at a given site. Since delta Ppl,ap = delta Prc,ap, where Prc,ap represents rib cage pressure in Aap, delta Pdi,ap = delta Pab - delta Prc,ap. Hence, considering that delta Pab and delta Prc depend on different factors, delta Pdi,ap may differ from zero. This pressure difference seems related to the interaction between two semisolid structures (contracted diaphragm and rib cage in Aap) constrained to the same shape and position.     

Changes in breathing pattern at loads near perceptual threshold at different work levels

Five subjects were tested to determine the threshold for detection of an added resistance to inspiration in three tests, one at rest and two with exercise (mild = 50 W; moderate = 100 W) on a cycle ergometer. Changes in the breathing pattern were examined at added resistances near the perceptual threshold. Added inspiratory resistances with a 50% probability of detection were very variable at rest; they decreased significantly from rest (250 Pa.l-1.s-1) to moderate exercise (98 Pa.l-1.s-1) in four subjects. It is suggested that physical exercise may cause discomfort even when workers wearing a respirator do not have any abnormal sensation during sedentary work. Breathing patterns were compared between resistance loaded and unloaded breathing during each test. Decreases in inspiratory peak flow and acceleration of flow early in inspiration were found in resistance loaded breathing in almost all tests and a tendency for tidal volume to decrease was found during moderate exercise only. The ratios of resistance loaded to unloaded breathing for inspiratory time (ti) and total time (tt) tended to be greater in the detected than in the undetected responses at rest and during mild exercise but not during moderate exercise. This would imply that further prolongation of ti and tt in the detected responses was attributable to conscious or subconscious aspects of the resistance leading responses: however, these adjustments in breathing, which reduce frequency, would be less likely to occur as the work rate increases.     

Pulsus paradoxus in asthmatic children.

Pulsus paradoxus is a useful physical sign in the assessment of the severity of asthma in adults. Whether this is also true for asthmatic children was determined by measuring respiratory fluctuations in systolic blood pressure during attacks of asthma in 24 children. A decrease in systolic pressure during inspiration exceeding 15 mm Hg was found only when the 1-second forced expiratory volume was less tha 60 percent of the predicted value. There was a highly significant (P smaller than 0.001) correlation between the degree of pulsus paradoxus and the severity of airway obstruction. In nonasthmatic children the systolic pressure was found to fluctuate by as much as 7 mm Hg during the respiratory cycle. It is concluded that, as in adults, the presence of pulsus paradoxus (larger than or equal to 15 mm Hg) in children indicates that their asthma is very severe.     

Effect of resistive loads on pattern of respiratory muscle recruitment during exercise.

In healthy subjects, we compared the effects of an expiratory (ERL) and an inspiratory (IRL) resistive load (6 cmH2O.l-1.s) with no added resistive load on the pattern of respiratory muscle recruitment during exercise. Fifteen male subjects performed three exercise tests at 40% of maximum O2 uptake: 1) with no-added-resistive load (control), 2) with ERL, and 3) with IRL. In all subjects, we measured breathing pattern and mouth occlusion pressure (P0.1) from the 3rd min of exercise, in 10 subjects O2 uptake (VO2), CO2 output (VCO2), and respiratory exchange ratio (R), and in 5 subjects we measured gastric (Pga), pleural (Ppl), and transdiaphragmatic (Pdi) pressures. Both ERL and IRL induced a high increase of P0.1 and a decrease of minute ventilation. ERL induced a prolongation of expiratory time with a reduction of inspiratory time (TI), mean expiratory flow, and ratio of inspiratory to total time of the respiratory cycle (TI/TT). IRL induced a prolongation of TI with a decrease of mean inspiratory flow and an increase of tidal volume and TI/TT. With ERL, in two subjects, Pga increased and Ppl decreased more during inspiration than during control suggesting that the diaphragm was the most active muscle. In one subject, the increases of Ppl and Pga were weak; thus Pdi increased very little. In the two other subjects, Ppl decreased more during inspiration but Pga also decreased, leading to a decrease of Pdi. This suggests a recruitment of abdominal muscles during expiration and of accessory and intercostal muscles during inspiration. With IRL, in all subjects, Ppl again decreased more, Pga began to decrease until 40% of TI and then increased.(ABSTRACT TRUNCATED AT 250 WORDS)     

Locus of hypoxic vasoconstriction in isolated ferret lungs

To determine whether hypoxic pulmonary vasoconstriction (HPV) occurs mainly in alveolar or extra-alveolar vessels in ferrets, we used two groups of isolated lungs perfused with autologous blood and a constant left atrial pressure (-5 Torr). In the first group, flow (Q) was held constant at 50, 100, and 150 ml.kg-1 X min-1, and changes in pulmonary arterial pressure (Ppa) were recorded as alveolar pressure (Palv) was lowered from 25 to 0 Torr during control [inspired partial pressure of O2 (PIO2) = 200 Torr] and hypoxic (PIO2 = 25 Torr) conditions. From these data, pressure-flow relationships were constructed at several levels of Palv. In the control state, lung inflation did not affect the slope of the pressure-flow relationships (delta Ppa/delta Q), but caused the extrapolated pressure-axis intercept (Ppa0), representing the mean backpressure to flow, to increase when Palv was greater than or equal to 5 Torr. Hypoxia increased delta Ppa/delta Q and Ppa0 at all levels of Palv. In contrast to its effects under control condition, lung inflation during hypoxia caused a progressive decrease in delta Ppa/delta Q, and did not alter Ppa0 until Palv was greater than or equal to 10 Torr. In the second group of experiments flow was maintained at 100 ml.kg-1 X min-1, and changes in lung blood volume (LBV) were recorded as Palv was varied between 20 and 0 Torr. In the control state, inflation increased LBV over the entire range of Palv. In the hypoxic state inflation decreased LBV until Palv reached 8 Torr; at Palv 8-20 Torr, inflation increased LBV.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effects of arterial pressure on lung capillary pressure and edema after microembolism

The effect of increased arterial pressure (Pa) on microvessel pressure (Pc) and edema following microvascular obstruction (100-micron glass spheres) was examined in the isolated ventilated dog lung lobe pump perfused with blood. Lobar vascular resistance (PVR) increased 2- to 10-fold following emboli when either Pa or flow was held constant. Microbead obstruction increased the ratio of precapillary to total PVR from 0.60 +/- 0.05 to 0.84 +/- 0.02 (SE) or to 0.75 +/- 0.06 (n = 6), as determined by the venous occlusion and the isogravimetric capillary pressure techniques, respectively. Isogravimetric Pc (5.0 +/- 0.7) did not differ from Pc obtained by venous occlusion (3.8 +/- 0.2 Torr, n = 6). After embolism, Pc in constant Pa decreased from 6.2 +/- 0.3 to 4.4 +/- 0.3 Torr (n = 16). In the constant-flow group, embolism doubled Pa while Pc increased only 40% (6.7 +/- 0.6 to 9.2 +/- 1.4 Torr, n = 6) with no greater edema formation than in the constant Pa groups. These data indicate poor transmission of Pa to filtering capillaries. Microembolism, even when accompanied by elevated Pa and increased flow velocity of anticoagulated blood of low leukocyte and platelet counts, caused little edema. Our results suggest that mechanical effects alone of lung microvascular obstruction cause minimal pulmonary edema.     

Effects of sleep-induced increases in upper airway resistance on ventilation

To determine the effects of the sleep-induced increases in upper airway resistance on ventilatory output, we studied five subjects who were habitual snorers but otherwise normal while awake (AW) and during non-rapid-eye-movement (NREM) sleep under the following conditions: 1) stage 2, low-resistance sleep (LRS); 2) stage 3-4, high-resistance sleep (HRS) (snoring); 3) with continuous positive airway pressure (CPAP); 4) CPAP + end-tidal CO2 partial pressure (PETCO2) mode isocapnic to LRS; and 5) CPAP + PETCO2 isocapnic to HRS. We measured ventilatory output via pneumotachograph in the nasal mask, PETCO2, esophageal pressure, inspiratory and expiratory resistance (RL,I and RL,E). Changes in PETCO2 were confirmed with PCO2 measurements in arterialized venous blood in all conditions in one subject. During wakefulness, pulmonary resistance (RL) remained constant throughout inspiration, whereas in stage 2 and especially in stage 3-4 NREM sleep, RL rose markedly throughout inspiration. Expired minute ventilation (VE) decreased by 12% in HRS, and PETCO2 increased in LRS (3.3 Torr) and HRS (4.9 Torr). CPAP decreased RL,I to AW levels and increased end-expiratory lung volume 0.25-0.93 liter. Tidal volume (VT) and mean inspiratory flow rate (VT/TI) increased significantly with CPAP. Inspiratory time (TI) shortened, and PETCO2 decreased 3.6 Torr but remained 1.3 Torr above AW. During CPAP (RL,I equal to AW), with PETCO2 returned to the level of LRS, VT/TI and VE were 83 and 52% higher than during LRS alone. Also on CPAP, with PETCO2 made equal to HRS, VT, VT/TI, and VE were 67, 112, and 67% higher than during HRS alone.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effects of unilateral hyperinflation on the interpulmonary distribution of pleural pressure.

Motivated by single lung transplantation, we studied the mechanics of the chest wall during single lung inflations in recumbent dogs and baboons and determined how pleural pressure (Ppl) is coupled between the hemithoraces. In one set of experiments, the distribution of Ppl was inferred from known volumes and elastic properties of each lung. In a second set of experiments, costal pleural liquid pressure (Pplcos) was measured with rib capsules. Both methods revealed that the increase in Ppl over the ipsilateral or inflated lung (delta Ppli) is greater than that over the contralateral or noninflated lung (delta Pplc). Mean d(delta Pplc)/d(delta Ppli) and its 95% confidence interval was 0.7 +/- 0.1 in dogs and 0.5 +/- 0.1 in baboons. In a third set of experiments in three dogs and three baboons, we prevented sternal displacement and exposed the abdominal diaphragm to atmospheric pressure during unilateral lung inflation. These interventions had no significant effect on Ppl coupling between the hemithoraces. We conclude that lungs of unequal size and mechanical properties need not be exposed to the same surface pressure, because thoracic midline structures and the lungs themselves resist displacement and deformation.     

Liquid-filled esophageal catheter for measuring pleural pressure in preterm neonates

The precise measurement of esophageal pressure (Pes) as a reflection of pleural pressure (Ppl) is crucial to the measurement of lung mechanics in the newborn. The fidelity of Pes as a measurement of Ppl is determined by the occlusion test in which, during respiratory efforts against an occlusion at the airway opening, changes in pressure (delta Pao) (Pao is assumed to be equal to alveolar pressure) are shown to be equal to changes in Pes (delta Pes). Eight intubated premature infants (640-3,700 g) with chest wall distortion were studied using a water-filled catheter system to measure Pes. During the occlusion test, all patients had a finite region of the esophagus where delta Pes equaled delta Pao, which corresponded to points in the esophagus above the cardia but below the carina. In conclusion, even in the presence of chest wall distortion, a liquid-filled catheter with the tip between the cardia and carina can provide an accurate measurement of Ppl, even in the very small premature infant with chest wall distortion.     

Respiratory load compensation in neuromuscular disorders

First-breath ventilatory responses to graded elastic (delta E) and resistive (delta R) loads from 10 people with spinal muscular atrophy (SMA), 15 people with Duchenne muscular dystrophy (DMD), and 80 able-bodied people were compared. The SMA and DMD groups produced equal tidal volume, respiratory frequency, inspiratory duration (TI), expiratory duration, mean inspiratory airflow, and duty cycle responses to both delta E and delta R. Thus SMA (primarily a motoneuron disorder) and DMD (primarily a muscle disorder) have the same net effect on loaded breathing responses. The SMA and DMD groups failed to duplicate the normal group's short expirations during delta E, long inspirations during delta R, and thus, extended duty cycles during both delta E and delta R. The deficit in load compensation therefore was due to impaired regulation of respiratory timing (reflecting neural mechanisms) but not airflow defense (reflecting mechanical and neural mechanisms). One-fifth of the normal but none of the SMA or DMD subjects actively generated an "optimal" TI response (defined theoretically as TI greater than 160% control during large delta R and TI less than 75% control during large delta E). This lack of optimal responses, which is the same abnormality exhibited by quadriplegic people, suggests that SMA and DMD also impair human ability to discriminate between large delta R and delta E. These findings support the hypothesis that neuromuscular disorders can lead to disturbances in respiratory perception.     

Partitioning of inspiratory pressure swings between diaphragm and intercostal/accessory muscles

We tested the hypothesis that the inspiratory pressure swings across the rib-cage pathway are the sum of transdiaphragmatic pressure (Pdi) and the pressures developed by the intercostal/accessory muscles (Pic). If correct, Pic can only contribute to lowering pleural pressure (Ppl), to the extent that it lowers abdominal pressure (Pab). To test this we measured Pab and Ppl during during Mueller maneuvers in which deltaPab = 0. Because there was no outward displacement of the rib cage, Pic must have contributed to deltaPpl, as did Pdi. Under these conditions the total pressure developed by the inspiratory muscles across the rib-cage pathway was less than Pdi + Pic. Therefore, we rejected the hypothesis. A plot of Pab vs. Ppl during relaxation allows partitioning of the diaphragmatic and intercostal/accessory muscle contributions to inspiratory pressure swings. The analysis indicates that the diaphragm can act both as a fixator, preventing transmission of Ppl to the abdomen and as an agonist. When abdominal muscles remain relaxed it only assumes the latter role to the extent that Pab increases.     

Effect of resistive loading on inspiratory work output in anesthetized cats

In five spontaneously breathing anesthetized cats, we determined the inspiratory elastic (Wel), resistive (Wres), and total (WI) mechanical work rates (power) during control and first loaded inspirations through graded linear resistances (delta R) by "Campbell diagrams" based on measurement of esophageal pressure. WI did not change with delta R's up to 0.31 cmH2O X ml-1 X s, the concomitant decrease in Wel being balanced by an increase in Wres. The stability of WI in the face of delta R's was due to the vagally mediated prolongation of inspiration and the intrinsic properties of the respiratory system and of the contracting inspiratory muscles. To assess the separate contributions of volume-related and flow-related intrinsic mechanisms to the stability of WI, we made model predictions of the immediate effects of delta R's on inspiratory mechanical work output based on measurements of inspiratory driving pressure waves and passive and active respiratory resistance and elastance on the same five cats. The results suggest that the intrinsic stability of WI in the face of delta R's is provided primarily by the active elastance.     

Ventilatory muscle recruitment in exercise with O2 in obstructed patients with mild hypoxemia

Respiratory muscle dysfunction limits exercise endurance in severe chronic airflow obstruction (CAO). To investigate whether inspiring O2 alters ventilatory muscle recruitment and improves exercise endurance, we recorded pleural (Ppl) and gastric (Pga) pressures while breathing air or 30% O2 during leg cycling in six patients with severe CAO, mild hypoxemia, and minimal arterial O2 desaturation with exercise. At rest, mean (+/- SD) transdiaphragmatic pressure (Pdi) was lower inspiring 30% O2 compared with air (23 +/- 4 vs. 26 +/- 7 cmH2O, P less than 0.05), but the pattern of Ppl and Pga contraction was identical while breathing either gas mixture. Maximal transdiaphragmatic pressure was similar breathing air or 30% O2 (84 +/- 30 vs. 77 +/- 30 cmH2O). During exercise, Pdi increased similarly while breathing air or 30% O2, but the latter was associated with a significant increase in peak inspiratory Pga and decreases in peak inspiratory Ppl and expiratory Pga. In five out of six patients, exercise endurance increased with O2 (671 +/- 365 vs. 362 +/- 227 s, P less than 0.05). We conclude that exercise with O2 alters ventilatory muscle recruitment and increases exercise endurance. During exercise inspiring O2, the diaphragm performs more ventilatory work which may prevent overloading the accessory muscles of respiration.     

Effect of inspiratory resistance and PEEP on 99mTc-DTPA clearance

Experiments were performed to determine the effect of markedly negative pleural pressure (Ppl) or positive end-expiratory pressure (PEEP) on the pulmonary clearance (k) of technetium-99m-labeled diethylenetriaminepentaacetic acid (99mTc-DTPA). A submicronic aerosol containing 99mTc-DTPA was insufflated into the lungs of anesthetized intubated sheep. In six experiments k was 0.44 +/- 0.46% (SD)/min during the initial 30 min and was unchanged during the subsequent 30-min interval [k = 0.21 +/- 12%/min] when there was markedly increased inspiratory resistance. A 3-mm-diam orifice in the inspiratory tubing created the resistance. It resulted on average in a 13-cmH2O decrease in inspiratory Ppl. In eight additional experiments sheep were exposed to 2, 10, and 15 cmH2O PEEP (20 min at each level). During 2 cmH2O PEEP k = 0.47 +/- 0.15%/min, and clearance increased slightly at 10 cmH2O PEEP [0.76 +/- 0.28%/min, P less than 0.01]. When PEEP was increased to 15 cmH2O a marked increase in clearance occurred [k = 1.95 +/- 1.08%/min, P less than 0.001]. The experiments demonstrate that markedly negative inspiratory pressures do not accelerate the clearance of 99mTc-DTPA from normal lungs. The effect of PEEP on k is nonlinear, with large effects being seen only with very large increases in PEEP.     

Effect of inspiratory resistive loading on control of ventilation during progressive exercise

Eight healthy volunteers performed gradational tests to exhaustion on a mechanically braked cycle ergometer, with and without the addition of an inspiratory resistive load. Mean slopes for linear ventilatory responses during loaded and unloaded exercise [change in minute ventilation per change in CO2 output (delta VE/delta VCO2)] measured below the anaerobic threshold were 24.1 +/- 1.3 (SE) = l/l of CO2 and 26.2 +/- 1.0 l/l of CO2, respectively (P greater than 0.10). During loaded exercise, decrements in VE, tidal volume, respiratory frequency, arterial O2 saturation, and increases in end-tidal CO2 tension were observed only when work loads exceeded 65% of the unloaded maximum. There was a significant correlation between the resting ventilatory response to hypercapnia delta VE/delta PCO2 and the ventilatory response to VCO2 during exercise (delta VE/delta VCO2; r = 0.88; P less than 0.05). The maximal inspiratory pressure generated during loading correlated with CO2 sensitivity at rest (r = 0.91; P less than 0.05) and with exercise ventilation (delta VE/delta VCO2; r = 0.83; P less than 0.05). Although resistive loading did not alter O2 uptake (VO2) or heart rate (HR) as a function of work load, maximal VO2, HR, and exercise tolerance were decreased to 90% of control values. We conclude that a modest inspiratory resistive load reduces maximum exercise capacity and that CO2 responsiveness may play a role in the control of breathing during exercise when airway resistance is artificially increased.     

Respiratory effect of the lower rib displacement produced by the diaphragm

The diaphragm acting alone causes a cranial displacement of the lower ribs and a caudal displacement of the upper ribs. The respiratory effect of the lower rib displacement, however, is uncertain. In the present study, two sets of experiments were performed in dogs to assess this effect. In the first, all the inspiratory intercostal muscles were severed, so that the diaphragm was the only muscle active during inspiration, and the normal inspiratory cranial displacement of the lower ribs was suppressed at regular intervals. In the second experiment, the animals were given a muscle relaxant to abolish respiratory muscle activity, and external, cranially oriented forces were applied to the lower rib pairs to simulate the action of the diaphragm on these ribs. The data showed that 1) holding the lower ribs stationary during spontaneous, isolated diaphragm contraction had no effect on the change in lung volume during unimpeded inspiration and no effect on the fall in pleural pressure (Ppl) during occluded breaths; 2) the procedure, however, caused an increase in the caudal displacement of the upper ribs; and 3) pulling the lower rib pairs cranially induced a cranial displacement of the upper ribs and a small fall in Ppl. These observations indicate that the force applied on the lower ribs by the diaphragm during spontaneous contraction, acting through the interdependence of the ribs, is transmitted to the upper ribs and has an inspiratory effect on the lung. However, this effect is very small compared to that of the descent of the dome.     

Within-breath electromyographic changes during loaded breathing in adult sheep

To investigate the changes in diaphragm electromyogram (EMG) during the course of severe loaded breathing, we subjected five conscious adult sheep to inspiratory flow resistive breathing (resistance greater than 150 cmH2O X l-1 X s) for up to 2-3 h and studied the total EMG power per breath (iEMG) and the EMG power per unit time after dividing the duration of EMG activity within each breath into three equal parts (iEMG1, iEMG2, and iEMG3). Both total breath iEMG and transdiaphragmatic pressure (Pdi) increased, remained at a high level for a certain period of time, and then started to fall. A change in the pattern of iEMG within a breath was observed during loaded breathing. The increase in total-breath iEMG was associated mostly with an increase in iEMG3, or the last part of the EMG power within each inspiration. Similarly, the decrease in total breath iEMG was primarily due to a decrease in iEMG3. We conclude that, in sheep subjected to severe IFR loads for prolonged periods the marked increase in total-breath iEMG at the beginning of loaded breathing and the marked decrease in this iEMG at the time of decrease in Pdi are largely due to changes in iEMG that occur during the latter third of each breath. We speculate that during loaded breathing the recruitment pattern of diaphragmatic muscle fibers changes during the course of an inspiratory effort.