Haworth S T, Rickaby D A, Linehan J H, Dawson C A
Biomedical Engineering Department, Marquette University, Milwaukee 53233, USA.
J Appl Physiol (1985). 1995 Aug;79(2):615-22. doi: 10.1152/jappl.1995.79.2.615.
The reported values for the pressure difference between lobar artery and subpleural arteriole and between subpleural venule and lobar vein as a fraction of the total arterial-to-venous pressure drop across the dog lung have varied considerably. We carried out the present study to provide an additional set of measurements and to determine whether it is likely that differences in venous pressure or transpulmonary pressure between studies might make a substantial contribution to variations between studies. We measured the lobar arterial pressure (Pa) to subpleural arteriole (22-60 microns diam) pressure (Pma) to subpleural venule (30-80 microns diam) pressure (Pmv) to lobar venous pressure (Pv) distribution over a range of alveolar pressures (PA; 2.5-13.1 mmHg) and venous pressures (0-24.2 mmHg) in isolated dog lung lobes using the micropuncture servo-null technique. On average, near functional residual capacity (PA = 3 mmHg) and venous pressure equal to PA, (Pa-Pma)/(Pma-Pmv)/(Pmv-Pv) was 37:30:33%. Under zone 3 conditions, there was a small positive correlation between the fractional Pa-to-Pma pressure difference and PA and Pv, but dependence of the Pmv-to-Pv fraction on PA and Pv was not consistent. The overall effects of PA and Pv on the fractional pressure drops were not sufficient to account for differences between previous studies. Under zone 2 conditions as the venous pressure was varied, the changes in Pmv were nearly equal to the changes in Pv, whereas Pma was relatively insensitive to Pv. Thus, the zone 2 results were consistent with a capillary location for the flow-limiting segment under zone 2 conditions.
据报道,叶动脉与胸膜下小动脉之间以及胸膜下小静脉与叶静脉之间的压差占犬肺总动静脉压差的比例差异很大。我们进行了本研究,以提供另一组测量数据,并确定研究之间静脉压或跨肺压的差异是否可能对研究之间的差异有重大影响。我们使用微穿刺伺服零位技术,在离体犬肺叶的一系列肺泡压(PA;2.5 - 13.1 mmHg)和静脉压(0 - 24.2 mmHg)范围内,测量了叶动脉压(Pa)至胸膜下小动脉(直径22 - 60微米)压(Pma)至胸膜下小静脉(直径30 - 80微米)压(Pmv)至叶静脉压(Pv)的分布。平均而言,在功能残气量附近(PA = 3 mmHg)且静脉压等于PA时,(Pa - Pma)/(Pma - Pmv)/(Pmv - Pv)为37:30:33%。在3区条件下,Pa至Pma压差分数与PA和Pv之间存在小的正相关,但Pmv至Pv分数对PA和Pv的依赖性不一致。PA和Pv对压差分数的总体影响不足以解释先前研究之间的差异。在2区条件下,随着静脉压的变化,Pmv的变化几乎与Pv的变化相等,而Pma对Pv相对不敏感。因此,2区的结果与2区条件下流量限制段位于毛细血管位置一致。