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肺膨胀对肺泡上皮溶质和水转运特性的影响。

Effects of lung inflation on alveolar epithelial solute and water transport properties.

作者信息

Kim K J, Crandall E D

出版信息

J Appl Physiol Respir Environ Exerc Physiol. 1982 Jun;52(6):1498-505. doi: 10.1152/jappl.1982.52.6.1498.

Abstract

Paired hollow bullfrog lungs (Rana catesbeiana) were used to study the effects of lung inflation on alveolar epithelial transport of water and hydrophilic solutes. Frogs were double pithed and the lungs were removed after bronchial placement of a Lucite plug. Three openings in the plug accommodated the insertion of two agar-Ringer bridges (for electrical potential measurement and passage of direct current) and the injection and removal of alveolar bathing fluid. Ringer solution containing a tracer quantity of radioactive solute was instilled into the lung sacs (5 ml or 50 ml) and the lungs were suspended in baths of Ringer solution containng appropriate cold solutes (5 mM). Permeability properties of each solute (and water) were determined from the rate of radiotracer concentration change in the bath. The spontaneous potential difference, tissue resistance, and solute permeability properties determined in these experiments showed no significant differences between the 5- and 50-ml lungs. Assuming homogeneous, cylindrical water-filled pores to be present in the tissue, the equivalent pore radii estimated from the rates of solute and water fluxes were 1.1 (for 5-ml lungs) and 0.9 nm (for 50-ml lungs). After overinflation of the lung (to greater than 80 ml), experiments at 50 ml yielded a pore radius of 3.4 nm. These data suggest that passive alveolar epithelial transport properties do not change with degrees of lung inflation normally encountered in vivo but that overinflation can lead to increased leakiness of the barrier.

摘要

使用成对的牛蛙空心肺(牛蛙)来研究肺膨胀对肺泡上皮水和亲水性溶质转运的影响。将青蛙双毁髓,在支气管放置一个有机玻璃塞后取出肺。塞子上的三个开口用于插入两个琼脂 - 林格桥(用于测量电势和通过直流电)以及注入和排出肺泡灌洗液。将含有微量放射性溶质示踪剂的林格溶液注入肺囊(5毫升或50毫升),然后将肺悬浮在含有适当冷溶质(5毫摩尔)的林格溶液浴中。根据浴中放射性示踪剂浓度变化率确定每种溶质(和水)的渗透性。在这些实验中测定的自发电位差、组织电阻和溶质渗透性在5毫升和50毫升的肺之间没有显著差异。假设组织中存在均匀的圆柱形充水孔隙,根据溶质和水流速估计的等效孔隙半径分别为1.1纳米(对于5毫升的肺)和0.9纳米(对于50毫升的肺)。在肺过度膨胀(至大于80毫升)后,50毫升时的实验得到的孔隙半径为3.4纳米。这些数据表明,被动肺泡上皮转运特性在体内通常遇到的肺膨胀程度下不会改变,但过度膨胀会导致屏障的渗漏增加。

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