Louis B, Isabey D
Institut National de la Santé et de la Recherche Médicale Unité 296, Centre Hospitalo-Universitaire Henri Mondor, Créteil, France.
J Appl Physiol (1985). 1993 Jan;74(1):116-25. doi: 10.1152/jappl.1993.74.1.116.
Measurement of input respiratory impedance is carried out by superimposing forced oscillations on spontaneous breathing. The latter thus acts as a quasi-steady unidirectional flow component, with effects on the measured impedance that are habitually neglected (linearity assumption). We examined the validity of that assumption in the case of a turbulent steady flow. We tested the validity of a fluid dynamics criterion previously proposed in water channel experiments for gas flow in a tube. This criterion states that oscillatory and continuous turbulent flow may or may not interact if the Stokes boundary layer (ls) is embedded within the viscous sublayer (lv), i.e., if lS+ = lS/lv < or = 10, implying Re7/8 < or = (100 alpha/square root of 2), for a fully developed hydraulically smooth turbulent flow in a tube (where alpha is Womersley parameter and Re is Reynolds number of the steady-flow component). Experiments were performed in long rigid circular and semicircular tubes by superimposing two independent well-defined flows: 1) laminar oscillatory flow obeying the linear transmission line model (frequency = 1.5-250 Hz, i.e., alpha = 6-80) and 2) fully developed turbulent flow characterized by Blasius resistance formula (Re = 3,000-16,000). Confirming the validity of the criterion above, we found that the real and the imaginary parts of the long-tube impedance did not differ from those measured in the absence of a steady-flow component, provided lS+ < or = 10. On the contrary, the real parts measured with and without the continuous component differed greatly as soon as lS+ > 10, both for circular and semicircular tubes and for outward as well as inward steady flows. We concluded that the proposed criterion is pertinent for predicting appropriate oscillation frequency for a given rate of spontaneous flow, such that oscillatory and turbulent flows do not interact. Application of the forced oscillation measurement technique during spontaneous breathing requires use of a range of oscillatory frequencies higher than the frequency range classically used during apnea.
通过在自主呼吸上叠加强迫振荡来进行输入呼吸阻抗的测量。自主呼吸因此充当准稳态单向流分量,其对测量阻抗的影响通常被忽略(线性假设)。我们研究了在湍流稳定流情况下该假设的有效性。我们测试了先前在水槽实验中针对管内气流提出的流体动力学标准的有效性。该标准指出,如果斯托克斯边界层(ls)嵌入粘性底层(lv)内,即如果lS+ = lS/lv < 或 = 10,则振荡湍流和连续湍流可能相互作用,也可能不相互作用,这意味着对于管内充分发展的水力光滑湍流(其中α是沃默斯利参数,Re是稳定流分量的雷诺数),Re7/8 < 或 = (100α/√2)。通过叠加两种独立的明确界定的流在长刚性圆形和半圆形管中进行实验:1)遵循线性传输线模型的层流振荡流(频率 = 1.5 - 250 Hz,即α = 6 - 80)和2)由布拉修斯阻力公式表征的充分发展的湍流(Re = 3000 - 16000)。证实上述标准的有效性后,我们发现,只要lS+ < 或 = 10,则长管阻抗的实部和虚部与在没有稳定流分量时测量的结果没有差异。相反,一旦lS+ > 10,对于圆形和半圆形管以及向外和向内的稳定流,有和没有连续分量时测量的实部差异很大。我们得出结论,所提出的标准对于预测给定自主流速下的合适振荡频率是相关的,使得振荡流和湍流不相互作用。在自主呼吸期间应用强迫振荡测量技术需要使用比呼吸暂停期间经典使用的频率范围更高的一系列振荡频率。