Mink S, Ziesmann M, Wood L D
J Appl Physiol Respir Environ Exerc Physiol. 1979 Sep;47(3):490-502. doi: 10.1152/jappl.1979.47.3.490.
We used the retrograde-catheter technique to investigate the effect of a helium-oxygen gas mixture (HeO2) on resistance to maximum expiratory flow (Vmax) in airways subsegments between alveoli and the equal pressure point (EPP), and between EPP and the flow-limiting segment (FLS). FLS were found at the same site in main-stem bronchi on both air and HeO2 in most dogs studied. Static elastic recoil pressure (Pel = 7 +/- 1 cmH2O) and the lateral pressure at FLS (Ptm' = 11 +/- cmH2O) were not different on the two gases, and delta Vmax averaged 33 +/- 12%. EPP were located on HeO2 in segmental bronchi (7 +/- 2 mm ID), and EPP on air were always located more downstream. There was no density dependence of resistance between alveoli and EPP on HeO2, and delta Vmax was due to the marked density dependence of the pressure losses of convective acceleration in the short airway segment between EPP HeO2 and FLS. Assuming that FLS is the "choke point," these findings are consistent with wave-speed theory of flow limitation modified to account for viscous pressure losses in peripheral airways. These results and conclusions question previous interpretations of delta Vmax as an index of peripheral airways obstruction, and demonstrate the utility of wave-speed theory in explaining complicated mechanisms of expiratory flow limitation.
我们采用逆行导管技术,研究氦氧混合气(HeO₂)对肺泡与等压点(EPP)之间以及EPP与气流受限段(FLS)之间气道亚段最大呼气流量(Vmax)阻力的影响。在大多数研究的犬中,主支气管的FLS在空气和HeO₂条件下位于同一位置。两种气体条件下的静态弹性回缩压力(Pel = 7 ± 1 cmH₂O)和FLS处的侧压力(Ptm' = 11 ± cmH₂O)无差异,Vmax平均变化33 ± 12%。在段支气管(内径7 ± 2 mm)中,EPP位于HeO₂条件下,而在空气条件下EPP总是位于更下游的位置。在HeO₂条件下,肺泡与EPP之间的阻力不存在密度依赖性,Vmax的变化是由于EPP与HeO₂和FLS之间短气道段中对流加速压力损失的显著密度依赖性。假设FLS是“阻塞点”,这些发现与经修正以考虑外周气道粘性压力损失的气流受限波速理论一致。这些结果和结论对之前将Vmax变化解释为外周气道阻塞指标的观点提出了质疑,并证明了波速理论在解释呼气气流受限复杂机制方面的实用性。