Fluid dynamics during initial aeration of mature fetal lung and effect of temperature

Physiology of the alveolar surface network

The alveolar surface network (ASN) is the totally fluid intraacinar conformation of the alveolar surface liquid (ASL) continuum circulating, both in series and in parallel, through ultrathin (to <7 nm) molecular conduits formed by appositions of unit bubbles of alveolar gas. The ASN is the analogue of foam in vitro. Appositions of unit bubble films, namely foam films, include (a) bubble-to-bubble at the alveolar entrance, across alveolar ducts, and at pores of Kohn ('classical foam films'); (b) bubble-to-epithelial cell surface ('cell-surface foam film'); and (c) bubble-to-open surface liquid layer of the terminal conducting airways ('surface foam film'). These appositions of monolayer bubble films create (a) 'macrochannels' ('pressure points', 'reservoirs') that modulate ASL transfers, volume and flow throughout the acinus and between acinar surface and both the interstitium and the terminal conducting airways surfaces, and (b) 'microchannels' along the broadest surfaces of the appositions. 'Microchannels', which are expectedly bilayer, serve several functions, including (a) virtually frictionless orientation of unit bubbles and ASL to fill the acinar air space; (b) virtually unrestricted diffusion of respiratory gases; (c) architectural support ('infrastructure') against the 'mass' and 'recoil' force of the interstitium; and (d) provision of 'gate' and 'bridge' dynamics that further modulate and direct ASL circulation. The physiological and anatomical boundary between acinar ASN and the bubble-free open liquid surfaces of the conducting airways is marked by the surface foam film. The ASN operates as outlined above in all regions of the lung, at all lung volumes, beginning at the onset of air-breathing at birth and continuing throughout life. Reports of its discovery (Pulmonary Physiology of the Fetus, Newborn and Child (1975) 116; Pediatr. Res. 12 (1978) 1070) and subsequent confirmatory research including the adult lung are summarized in this review by progressive development of each function. These functions, which are normal for a relatively dry foam such as the ASN (where gas:liquid volume ratio is >99:1) cannot be duplicated by the conventional theories and models of an open 'alveolar lining layer'. The unfortunate research technologies upon which these theories and models have been formulated have, indeed, obfuscated recognition of the ASN in vivo. They are also presented and critiqued in this review.

The alveolar surface network: a new anatomy and its physiological significance

It is generally held that the terminal lung unit (TLU) is an agglomeration of alveoli that opens into the branching air spaces of respiratory bronchioles, alveolar ducts, and alveolar sacs and that these structures are covered by a continuous thin liquid layer bearing a monomolecular film of surfactants at the open gas-liquid interface. The inherent structural and functional instability given TLUs by a broad liquid surface layer of this nature has been mitigated by the discovery that the TLU surface is in fact an agglomeration of bubbles, a foam (the alveolar surface network) that fills the TLU space and forms ultrathin foam films that 1) impart infrastructural stability to sustain aeration, 2) modulate circulation of surface liquid, both in series and in parallel, throughout the TLU and between TLUs and the liquid surface of conducting airways, 3) modulate surface liquid volume and exchange with interstitial liquid, and 4) sustain gas transfer between conducting airways and pulmonary capillaries throughout the respiratory cycle. The experimental evidence, from discovery to the present, is addressed in this report. Lungs were examined in thorax by stereomicroscopy immediately from the in vivo state at volumes ranging from functional residual capacity to maximal volume (Vmax). Lungs were then excised; bubble topography of all anterior and anterolateral surfaces was reaffirmed and also confirmed for all posterior and posterolateral surfaces. The following additional criteria verify the ubiquitous presence of normal intraalveolar bubbles. 1) Bubbles are absent in conducting airways. 2) Bubbles are stable and stationary in TLUs but can be moved individually by gentle microprobe pressure. 3) Adjoining bubbles move into the external medium through subpleural microincisions; there is no free gas, and vacated spaces are rendered airless. Adjacent bubbles may shift position in situ, while more distal bubbles remain stationary. 4) The position and movement of "large" bubbles identifies them as intraductal bubbles. 5) Transection of the lung reveals analogous bubble occurrence and history in central lung regions. 6) Bubbles become fixed in place and change shape when the lung is dried in air; the original shape and movement are restored when the lung is rewet. 7) All exteriorized bubbles are stable with lamellar (film) surface tension near zero. 8) Intact lungs prepared and processed by the new double-embedding technique reveal the intact TLU bubbles and bubble films. Lungs were also monitored directly by stereomicroscopy to establish their presence, transformations, and apparent function from birth through adulthood, as summarized in the following section.

ANATOMY

Intraalveolar bubbles and bubble films (the unit structures of the alveolar surface network) have been found in all mammalian species examined to date, including lambs, kids, and rabbit pups and adult mice, rats, rabbits, cats, and pigs. Rabbits were used for the definitive studies. 1) A unit bubble occupies each alveolus and branching airway of the TLU; unit bubbles in clusters correspond with alveolar clusters. 2) The appositions of unit bubble lamellae (films) form a network of liquid channels within the TLUs. The appositions are bubble to bubble (near alveolar entrances, at pores of Kohn, and between ductal bubbles), bubble to epithelial cell surface, and bubble to surface liquid of conducting airways. They rapidly form stable Newtonian black foam films (approximately 7 nm thick) under hydrodynamic conditions expected in vivo. 3) Lamellae of the foam films and bubbles tend to exclude bulk liquid and thus maintain near-zero surface tension. At the same time, the foam film formations--abetted by the constant but small retractive force of tissue recoil--stabilize unit bubble position within the network. 4) Unit bubble mobility in response to applied force increases as liquid accumulates within the network (e.g. (ABSTRACT TRUNCATED)

Intraalveolar bubbles and bubble films: II. Formation in vivo through adulthood

BACKGROUND

Intraalveolar bubbles and bubble films have been shown to be part of the normal alveolar architecture in vivo from birth through the first 2 days of extrauterine life of rabbit pups (Scarpelli et al., 1996a. Anat. Rec. 244:344-357). The intraluminal boundary between air-way free gas and alveolar bubbles at the level of respiratory bronchioles is established within 1 hour after birth. We now examine the lung through the rest of development, namely, 2 weeks, 1, 2, and 3 months, and adulthood.

METHODS

In quick succession in anesthetized spontaneously breathing rabbits, the abdominal aorta was transected and trachea was occluded either after an end-tidal exhalation at functional residual capacity (FRC) or after volume expansion in vivo by a single inflation from FRC to 20 or 25 cm H2O pressure (V20, V25). Immediately the thorax was opened and lungs were examined (anterior, anterolateral) through a dissecting stereomicroscope while still in the chest, unperturbed (pleural surface temperature 34 degrees C). Heart and lungs were then removed en bloc and re-examined (anterior, lateral, posterior) to confirm that architecture had not changed (22-27 degrees C). After these immediate examinations, lungs were entered into one of the protocols enumerated in Results.

RESULTS

Immediate examination revealed bubbles in all aerated subpleural and deep ("central") alveoli from apex to base at all ages and temperatures. Bubbles were confirmed from two views (top and tangential) and from their individual mobility in response to gentle microprobe pressure. A "common bubble" (> 30 microns to approximately 120 microns inside diameter at FRC) appeared to occupy a single alveolus, sometimes arranged in clusters and collectively accounting for approximately 84% of the total bubble population. Few "large bubbles" appeared to be intraductal. We concluded that "small bubbles" (< or = 30 microns; approximately 16% of the total population) were contracted common bubbles. The free gas-bubble film boundary of the airways was at the level of respiratory bronchioles. Subsequent protocols: (1) Common bubbles moved out of adjoining tissue following subpleural incision. Adjacent bubbles either moved into vacated spaces or into the outside liquid medium. Large bubble(s) followed common bubbles out of the tissue. Small bubbles were less mobile and distal common bubbles did not move. The sequence of bubble movement at V25 was the same. Isolated bubbles had normal surfactant content and surface tension according to "Pattle's stability ratio." Transection revealed analogous conditions in central alveoli. (2) Bubble size increased during inflation from FRC to V25. Airless spaces were aerated with bubbles during inflation. (3) The bubble surface was compressed during deflation to 81% of maximal volume (Vmax) and below, including deflation to minimal volume (Vmin). (4) Bubble/alveolar shape changed from spherical-oval to polygonal when the pleural surface dried at FRC and V25. The original shape was restored when the surface was re-wet. Dry tissue showed but did not emit bubbles when cut; re-wet tissue did. (5) Lung liquid content and volume-pressure were normal at FRC. (6) As expected, conventionally fixed, dehydrated, and embedded sections showed no bubbles.

CONCLUSIONS

Bubbles and bubble films are fundamental to normal architecture of aerated alveoli at all lung volumes from birth through adulthood. As infrastructure, they sustain aeration and resist deformation. With ductal films, they may be expected to form an alveolar surface liquid (foam film) network (Scarpelli, 1988. Surfactants and the Lining of the Lung) that modulates liquid balance principally at Plateau borders. They expand and contract respectively during inflation and deflation, maintaining their closed film integrity. Films are compressed to "film collapse" in situ during deflation from volumes well above FRC to Vmin. At these volumes, intact films sustain aeration; some may disperse into t

Intraalveolar bubbles and bubble films. I. formation and development during the first 48 hours of extrauterine life in rabbits

BACKGROUND

Aeration of mature lungs at birth depends on formation of intraalveolar bubbles and bubble films (Scarpelli 1978. Pediatr. Res., 12:1070-1076). Bubbles establish immediately structural stability and pulmonary gas exchange. Given that air spaces are cleared in minutes of fetal liquid (the initial substrate for bubble formation), in formation possible beyond this period? If so, is this related to early development of pulmonary function and structure?

METHODS

Mature, spontaneously breathing rabbit pups at 1-10 min and 1, 3, 8, 24, and 48 h after vaginal birth were anesthetized, trachea was occluded at "resting volume" (approximately functional residual capacity), and lungs were rapidly exposed to preserve in vivo intrapulmonary status. The entire lung was examined by stereomicroscopy. Other determinations included resting volume, lung wet weight, volume-pressure curves, histological sections, lung dry weight, tissue hydroxyproline (OH-Pro), and lavage phospholipids (PL). Bubble mobility in situ was tested. Bubbles were released into bathing liquid by incision of peripheral units and monitored over time.

RESULTS

Pup activity and gross appearance of the lungs, together with septal thinning, secondary septal development, clearance of intraluminal liquid, increasing tissue OH-Pro, and PL distribution indicated normal postnatal development. Each aerated unit examined at resting volume (all lobes, all ages) contained intraalveolar bubbles. Transition to free gas exclusively in conducting airways and bubbles/bubble films in peripheral gas exchange units occurred within 1 h. Bubbles appeared to be exclusively within alveoli at 4 h and thereafter. Bubbles persisted and new bubbles were formed during subsequent inflation to maximal volume and deflation to atmospheric pressure (P0). Volume of intact lungs at P0 was maintained by the counterforce of rigid bubble films against tissue retraction. When bubbles were released either at resting volume or at P0, the bubble-free loci became airless. Constant size and stability of released bubbles support preferential incorporation of surfactants into bubble films and constant "near-zero surface tension" (Scarpelli 1978. Pediatr. Res., 12:1070-1076).

CONCLUSIONS

We show the ubiquitous presence of intraalveolar bubbles and bubble films in vivo throughout the first 48 h of postnatal life. Bubble film rigidity sustains aeration and prevents collapse, while low surface tension of the films facilitate liquid removal from the air spaces. Bubbles in situ are stable and, within apparent limits, mobile; after birth they are quickly restricted to the alveolar spaces, leaving airways bubble free.

The effects of reversing distending pressure sequences in the neonatal piglet

We studied different sequences of lung inflation in ventilated newborn piglets with normal lungs in order to determine the effects of sequence, magnitude and duration of distending pressure on pulmonary function, and/or hemodynamics. End-expiratory pressure was varied using a continuous negative extrathoracic pressure (CNEP) device. Three groups of ventilated piglets with normal lungs were exposed to 2 cmH2O increments of CNEP from -2 to -12 cmH2O, and to decrements from -12 to -2 cmH2O, or to only -6 cmH2O. Lung inflation sequence, magnitude of inflation pressure, and duration of inflation had significant effects on end-expiratory lung volume and lung compliance at numerically equivalent pressure levels. End-expiratory lung volume and lung compliance varied (at four and five of six inflation pressures studied) by as much as 68% and 104%, respectively. Hemodynamic effects of the lung inflation sequence were more variable; those found to be different at numerically equivalent pressure levels were associated with changes in lung compliance and ventilation. Differences in pulmonary mechanics can best be explained by the effects of lung inflation on alveolar recruitment versus overinflation.