Scarpelli E M, Mautone A J, DeFouw D O, Clutario B C
Perinatology Center, Cornell University College of Medicine, New York, New York, USA.
Anat Rec. 1996 Oct;246(2):245-70. doi: 10.1002/(SICI)1097-0185(199610)246:2<245::AID-AR12>3.0.CO;2-O.
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.
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.
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.
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
肺泡内气泡和气泡膜已被证明是出生后至兔幼崽宫外生活的头2天内体内正常肺泡结构的一部分(斯卡佩利等人,1996a。《解剖学记录》244:344 - 357)。呼吸性细支气管水平气道游离气体与肺泡气泡之间的腔内边界在出生后1小时内形成。我们现在研究肺在其余发育阶段,即2周、1、2和3个月以及成年期的情况。
在麻醉的自主呼吸兔中,快速连续地在功能残气量(FRC)呼气末或通过从FRC单次充气至20或25 cm H₂O压力(V20、V25)进行体内容量扩张后,切断腹主动脉并阻塞气管。立即打开胸腔,在仍处于胸腔内且未受干扰(胸膜表面温度34摄氏度)的情况下,通过解剖立体显微镜检查肺(前部、前外侧)。然后将心脏和肺整体取出并再次检查(前部、外侧、后部)以确认结构未改变(22 - 27摄氏度)。在这些即时检查之后,将肺纳入结果中列举的方案之一。
即时检查显示,在所有年龄和温度下,从肺尖到肺底的所有充气胸膜下和深部(“中央”)肺泡中均有气泡。从两个视角(顶部和切线方向)以及它们对轻微微探针压力的个体移动性确认了气泡。一个“普通气泡”(在FRC时内径> 30微米至约120微米)似乎占据单个肺泡,有时成簇排列,总共约占气泡总数的84%。很少有“大气泡”似乎位于导管内。我们得出结论,“小气泡”(≤ 30微米;约占总数的16%)是收缩的普通气泡。气道的游离气体 - 气泡膜边界位于呼吸性细支气管水平。后续方案:(1)胸膜下切开后,普通气泡从相邻组织中移出。相邻气泡要么移入腾出的空间,要么移入外部液体介质。大气泡跟随普通气泡移出组织。小气泡移动性较小,远端普通气泡不移动。在V25时气泡移动顺序相同。根据“帕特尔稳定比”,孤立气泡具有正常的表面活性剂含量和表面张力。横切显示中央肺泡有类似情况。(2)从FRC充气至V25期间气泡大小增加。充气期间无气空间被气泡充气。(3)放气至最大体积(Vmax)的81%及以下时,包括放气至最小体积(Vmin),气泡表面被压缩。(4)当胸膜表面在FRC和V25时干燥时,气泡/肺泡形状从球形 - 椭圆形变为多边形。表面重新湿润时恢复原始形状。干燥组织切割时可见但不产生气泡;重新湿润的组织则产生气泡。(5)在FRC时肺液体含量和容量 - 压力正常。(6)如预期的那样,常规固定、脱水和包埋的切片未显示气泡。
从出生到成年,气泡和气泡膜是充气肺泡正常结构的基础。作为基础设施,它们维持通气并抵抗变形。借助导管膜,它们可能形成一个肺泡表面液体(泡沫膜)网络(斯卡佩利,1988。《表面活性剂与肺内衬》),主要在高原边界调节液体平衡。它们在充气和放气期间分别扩张和收缩,保持其封闭膜的完整性。从远高于FRC的体积放气至Vmin期间,膜在原位被压缩至“膜塌陷”。在这些体积下,完整的膜维持通气;一些可能分散成……