Lai-Fook Stephen J, Lai Yih-Loong
Center for Biomedical Engineering, Wenner-Gren Research Laboratory, University of Kentucky-Lexington, Lexington, KY 40506-0070, USA.
J Appl Physiol (1985). 2005 Jun;98(6):2204-18. doi: 10.1152/japplphysiol.00869.2004. Epub 2005 Jan 27.
We developed a method for measuring airway resistance (R(aw)) in mice that does not require a measurement of airway flow. An analysis of R(aw) induced by alveolar gas compression showed the following relationship for an animal breathing spontaneously in a closed box: R(aw) = A(bt)V(b)/[V(t) (V(e) + 0.5V(t))]. Here A(bt) is the area under the box pressure-time curve during inspiration or expiration, V(b) is box volume, V(t) is tidal volume, and V(e) is functional residual capacity (FRC). In anesthetized and conscious unrestrained mice, from experiments with both room temperature box air and body temperature humidified box air, the contributions of gas compression to the box pressure amplitude were 15 and 31% of those due to the temperature-humidity difference between box and alveolar gas. We corrected the measured A(bt) and V(t) for temperature-humidity and gas compression effects, respectively, using a sinusoidal analysis. In anesthetized mice, R(aw) averaged 4.3 cmH(2)O.ml(-1).s, fourfold greater than pulmonary resistance measured by conventional methods. In conscious mice with an assumed FRC equal to that measured in the anesthetized mice, the corrected R(aw) at room temperature averaged 1.9 cmH(2)O.ml(-1).s. In both conscious mice and anesthetized mice, exposure to aerosolized methacholine with room temperature box air significantly increased R(aw) by around eightfold. Here we assumed that in the conscious mice both V(t) and FRC remained constant. In both conscious and anesthetized mice, body temperature humidified box air reduced the methacholine-induced increase in R(aw) observed at room temperature. The method using the increase in A(bt) with bronchoconstriction provides a conservative estimate for the increase in R(aw) in conscious mice.
我们开发了一种测量小鼠气道阻力(R(aw))的方法,该方法无需测量气道流量。对肺泡气体压缩诱导的R(aw)进行分析,得出了动物在密闭箱中自主呼吸时的如下关系:R(aw) = A(bt)V(b)/[V(t) (V(e) + 0.5V(t))]。其中,A(bt)是吸气或呼气过程中箱内压力-时间曲线下的面积,V(b)是箱体积,V(t)是潮气量,V(e)是功能残气量(FRC)。在麻醉和清醒自由活动的小鼠中,通过室温箱内空气和体温加湿箱内空气的实验发现,气体压缩对箱内压力幅度的贡献分别为箱内与肺泡气体温度-湿度差异所导致贡献的15%和31%。我们分别使用正弦分析对测量得到的A(bt)和V(t)进行温度-湿度和气体压缩效应的校正。在麻醉小鼠中,R(aw)平均为4.3 cmH₂O·ml⁻¹·s,比传统方法测量的肺阻力大四倍。在假设功能残气量与麻醉小鼠测量值相等的清醒小鼠中,室温下校正后的R(aw)平均为1.9 cmH₂O·ml⁻¹·s。在清醒小鼠和麻醉小鼠中,用室温箱内空气雾化吸入乙酰甲胆碱均使R(aw)显著增加约八倍。这里我们假设清醒小鼠的V(t)和FRC均保持恒定。在清醒和麻醉小鼠中,体温加湿箱内空气均减少了室温下观察到的乙酰甲胆碱诱导的R(aw)增加。使用支气管收缩时A(bt)的增加来计算的方法为清醒小鼠中R(aw)的增加提供了一个保守估计。