Abstract:In 11 isolated dog lung lobes, we studied the size distribution of recruited alveolar volumes that become available for gas exchange during inflation from the collapsed state. Three catheters were wedged into 2-mm-diameter airways at total lung capacity. Small-amplitude pseudorandom pressure oscillations between 1 and 47 Hz were led into the catheters, and the input impedances of the regions subtended by the catheters were continuously recorded using a wave tube technique during inflation from -5 cm H(2)O tran… Show more
“…This phenomenon is expected, for example, in acute lung injury. Indeed, Suki et al 24 measured Z L continuously during slow inflation of a collapsed lung to show that recruitment occurs in discrete cascades of airway openings. The present analysis, however, is the first to consider how recruitment occurring during the actual measurement of Z L might affect what is measured.…”
Mechanical lung function is frequently assessed in terms of lung resistance (R (L)), lung elastance (E (L)), and airway resistance (R (aw)). These quantities are determined by measuring input impedance at various oscillation frequencies, and allow lung tissue resistance (R (t)) to be estimated as the difference between R (L) and R (aw). These various parameters change in characteristic ways in the presence of lung pathology. In particular, the ratio R (t)/E (L) (known as hysteresivity, (eta) has been shown both experimentally and in numerical simulations to increase when regional heterogeneities in mechanical function develop throughout the lung. In this study, we performed an analytical investigation of a two-compartment lung model and showed that while heterogeneity always leads to an increase in E (L), eta will increase only initially. When heterogeneity becomes extreme, eta stops increasing and starts to decrease. However, there are no experimental reports of eta decreasing under conditions in which heterogeneity would be expected to exist. We speculate that this is because liquid bridges invariably form across airway lumen that narrow to a certain point, thereby preventing them from achieving arbitrarily small non-zero radii. We also show that recruitment of closed lung units during lung inflation may lead to variables responses in both eta and E (L).
“…This phenomenon is expected, for example, in acute lung injury. Indeed, Suki et al 24 measured Z L continuously during slow inflation of a collapsed lung to show that recruitment occurs in discrete cascades of airway openings. The present analysis, however, is the first to consider how recruitment occurring during the actual measurement of Z L might affect what is measured.…”
Mechanical lung function is frequently assessed in terms of lung resistance (R (L)), lung elastance (E (L)), and airway resistance (R (aw)). These quantities are determined by measuring input impedance at various oscillation frequencies, and allow lung tissue resistance (R (t)) to be estimated as the difference between R (L) and R (aw). These various parameters change in characteristic ways in the presence of lung pathology. In particular, the ratio R (t)/E (L) (known as hysteresivity, (eta) has been shown both experimentally and in numerical simulations to increase when regional heterogeneities in mechanical function develop throughout the lung. In this study, we performed an analytical investigation of a two-compartment lung model and showed that while heterogeneity always leads to an increase in E (L), eta will increase only initially. When heterogeneity becomes extreme, eta stops increasing and starts to decrease. However, there are no experimental reports of eta decreasing under conditions in which heterogeneity would be expected to exist. We speculate that this is because liquid bridges invariably form across airway lumen that narrow to a certain point, thereby preventing them from achieving arbitrarily small non-zero radii. We also show that recruitment of closed lung units during lung inflation may lead to variables responses in both eta and E (L).
“…The distribution of the recruited ∆Vs has been predicted to be a power law with an exponent of 2 [21] and has recently been measured indirectly [6]. Our data reflect a direct assessment of the distribution of alveolar recruited ∆Vs.…”
supporting
confidence: 66%
“…The distribution of these ∆Vs, which correspond to avalanches reaching the alveoli, should follow a power law [6,33].…”
Section: Lung Recruitment and The P−v Relationshipmentioning
“…A slow forced expiration to RV followed by chest strapping is known to reduce lung volume below that of voluntary effort (Douglas et al 1981), demonstrating that RV is not necessarily an anatomical limitation of the lungs. Alveoli commonly reach their closing volumes during full expiration and immersion (Bondi et al 1976), collapse harmlessly, and then reopen with a deep inspiration (Salmon et al 1981;Suki et al 2000). A degree of tracheal compression can occur in some individuals under negative pressure owing to invagination of the trachealis muscle spanning the posterior wall (Lindholm and Nyrén 2005).…”
The world record for a sled-assisted human breath-hold dive has surpassed 200 m. Lung compression during descent draws blood from the peripheral circulation into the thorax causing engorgement of pulmonary vessels that might impose a physiological limitation due to capillary stress failure. A computer model was developed to investigate cardiopulmonary interactions during immersion, apnea, and compression to elucidate hemodynamic responses and estimate vascular stresses in deep human breath-hold diving. The model simulates active and passive cardiovascular adjustments involving blood volumes, flows, and pressures during apnea at diving depths up to 200 m. Redistribution of blood volume from peripheral to central compartments increases with depth. Pulmonary capillary transmural pressures in the model exceed 50 mm Hg at record depth, producing stresses in the range known to cause alveolar capillary damage in animals. Capillary pressures are partially attenuated by blood redistribution to compliant extra-pulmonary vascular compartments. The capillary pressure differential is due mainly to a large drop in alveolar air pressure from outward elastic chest wall recoil. Autonomic diving reflexes are shown to influence systemic blood pressures, but have relatively little effect on pulmonary vascular pressures. Increases in pulmonary capillary stresses are gradual beyond record depth.
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