Sturm Robert, Hofmann W
Brunnleitenweg 41, A-5061 Elsbethen, Salzburg, Austria.
Bull Math Biol. 2007 Jan;69(1):395-415. doi: 10.1007/s11538-006-9143-3. Epub 2006 Sep 14.
Bronchial clearance of deposited particles was simulated using a stochastic model of the tracheobronchial tree. The clearance model introduced in this study considers (1) a continuous decrease of the mucus thickness from the trachea to the terminal bronchioles according to a linear or an exponential function, (2) the possibility of mucus discontinuities, which are mainly found in intermediate and distal airways of the tracheobronchial compartment, (3) mucus production in proximal airways, (4) a slow bronchial clearance phase due to the capture of a defined particle fraction f (s) in the periciliary sol phase, and (5) an eventual delay of the mucociliary transport at carinal ridges of airway bifurcations. Based on the concept of mucus volume conservation in single bifurcations, a reduction of the thickness of the mucus blanket from proximal to distal airways causes a significant increase of the mucus velocities in small ciliated airways compared to other stochastic modeling predictions assuming a constant thickness of the mucus layer throughout the conducting airways. This effect is further enhanced by the consideration of mucus discontinuities. In contrast, the ability of bronchial airways to produce a certain volume of mucus has a decreasing effect on the mucus velocities. In all generated clearance velocity models, mucociliary clearance is completely terminated within 24 h after exposure, consistent with the experimental evidence. Implementation of a slow bronchial clearance phase predicts a long-term retention fraction, which is fully cleared from the lung after several weeks. For 1-microm MMAD particles, 24-h retention varies between 0.42 and 0.52, in line with the suggestions of the ICRP. Mucus delay at carinal ridges only affects short-term clearance by increasing the retained particle fraction at a given time, while long-term retention is not influenced.
使用气管支气管树的随机模型模拟沉积颗粒的支气管清除。本研究中引入的清除模型考虑了:(1) 从气管到终末细支气管的黏液厚度根据线性或指数函数持续减小;(2) 黏液连续性中断的可能性,这主要见于气管支气管段的中间和远端气道;(3) 近端气道的黏液分泌;(4) 由于在纤毛周围溶胶相中捕获一定比例的特定颗粒f(s)而导致的缓慢支气管清除阶段;(5) 在气道分叉的隆突处最终出现的黏液纤毛运输延迟。基于单个分叉处黏液体积守恒的概念,与假设整个传导气道黏液层厚度恒定的其他随机模型预测相比,从近端气道到远端气道黏液毯厚度的减小会导致小纤毛气道中黏液速度显著增加。考虑黏液连续性中断会进一步增强这种效应。相比之下,支气管气道产生一定量黏液的能力对黏液速度有降低作用。在所有生成的清除速度模型中,黏液纤毛清除在暴露后24小时内完全终止,这与实验证据一致。实施缓慢支气管清除阶段可预测长期滞留分数,该分数在数周后从肺部完全清除。对于1微米的质量中值空气动力学直径(MMAD)颗粒,24小时滞留率在0.42至0.52之间,符合国际辐射防护委员会(ICRP)的建议。隆突处的黏液延迟仅通过增加给定时间的滞留颗粒分数来影响短期清除,而对长期滞留没有影响。