论文标题
哺乳动物肺的水和热交换
Water and heat exchanges in mammalian lungs
论文作者
论文摘要
哺乳动物呼吸系统的次要功能是在灵感中,将空气加热到体温并在达到肺泡之前用水饱和。依靠数学模型,我们考虑了所有陆地哺乳动物(涵盖六个体重的数量级,$ m $),并专注于肺对此空调的唯一贡献。结果凸显了小型哺乳动物和大型哺乳动物以及休息与努力之间的显着差异,这些差异在肺中的热量和水交换的空间分布以及航空公司管腔中发生的传质状态。有趣的是,结果表明,哺乳动物的肺似乎是正当的,以最大程度的努力完全调节空气:为此目的,动员了肺的支气管区域的所有世代。对于质量高于一定阈值的哺乳动物(剩余的$ \ simeq 5 $ kg和$ \ simeq 50 $ g在最大努力下),似乎这种蒸发速率的最大价值缩放为$ m^{ - 1/8} $,在静止和$ m^{ - 1/16} $左右的努力和最大努力(在40米)左右的时间里(在50米)(在50米上)由于不同现象之间的微妙耦合,在启发过程中从肺部从肺部提取的水/热返回了支气管粘膜。最后的结果意味着,高于这些阈值,通过通风量表从肺部从肺部提取的水量和热量,例如通风速率(即,在静止和最大努力下为$ m^{3/4} $,$ m^{3/4} $)。最后,值得一提的是,即使在最大努力(4-6 \%)中,这些金额似乎仍然有限,但与相关的全球数量相比,这些数量似乎仍然有限,但与相关的全球数量相比并不可忽略。
A secondary function of the mammals' respiratory system is during inspiration to heat the air to body temperature and to saturate it with water before it reaches the alveoli. Relying on a mathematical model, we comprehensively analyze this function, considering all the terrestrial mammals (spanning six orders of magnitude of the body mass, $M$) and focusing on the sole contribution of the lungs to this air conditioning. The results highlight significant differences between the small and the large mammals, as well as between rest and effort, regarding the spatial distribution of heat and water exchanges in the lungs, and in terms of regime of mass transfer taking place in the lumen of the airways. Interestingly, the results show that the mammalian lungs appear to be designed just right to fully condition the air at maximal effort: all generations of the bronchial region of the lungs are mobilized for this purpose. For mammals with a mass above a certain threshold ($\simeq 5$ kg at rest and $\simeq 50$ g at maximal effort), it appears that the maximal value of this evaporation rate scales as $M^{-1/8}$ at rest and $M^{-1/16}$ at maximal effort and that around 40\% (at rest) or 50\% (at maximal effort) of the water/heat extracted from the lungs during inspiration is returned to the bronchial mucosa during expiration, independently of the mass, due to a subtle coupling between different phenomena. This last result implies that, above these thresholds, the amounts of water and heat extracted from the lungs by the ventilation scale with the mass such as the ventilation rate (i.e. as $M^{3/4}$ at rest and $M^{7/8}$ at maximal effort). Finally, it is worth mentioning that these amounts appear to remain limited, but not negligible when compared to relevant global quantities, even at maximal effort (4-6\%).