非对称肺顺应性模型中的呼吸动力学评估

S. Yun, Ho-jin Lee, Yong-Hun Lee, Jong Cook Park
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The lung model was mechanically ventilated, and the airway internal diameter (ID) was changed from 3 to 8 mm in 1-mm increments. Results The mean ± standard deviation ratio of volumes distributed to each lung (VL1/VL2) in airway ID 3, 4, 5, 6, 7, and 8 were in order, 0.10 ± 0.05, 0.11 ± 0.03, 0.12 ± 0.02, 0.12 ± 0.02, 0.12 ± 0.02, and 0.12 ± 0.02 in the C15 group; 1.05 ± 0.16, 1.01 ± 0.09, 1.00 ± 0.07, 0.97 ± 0.09, 0.96 ± 0.06, and 0.97 ± 0.08 in the C60 group; and 1.46 ± 0.18, 3.06 ± 0.41, 3.72 ± 0.37, 3.78 ± 0.47, 3.77 ± 0.45, and 3.78 ± 0.60 in the C120 group. The positive end-expiratory pressure (PEEP) of lung1 was significantly increased at airway ID 3 mm (1.65 cmH2O) in the C15 group; at ID 3, 4, and 5 mm (2.21, 1.06, and 0.95 cmH2O) in the C60 group; and ID 3, 4, and 5 mm (2.92, 1.84, and 1.41 cmH2O) in the C120 group, compared to ID 8 mm (P < 0.05). 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引用次数: 2

摘要

背景:单侧肺恶性膨胀发生于不对称顺应性肺,可导致生命不稳定。本研究旨在探讨不对称顺应性肺模型在机械通气过程中呼吸动力学和气道直径对潮气量分布的影响。方法设计三组肺模型,分别模拟对称顺应性和非对称顺应性肺模型。肺模型由两个试验肺组成,肺1和肺2。C15、C60、C120组肺1的静态顺应性分别为15、60、120 ml/cmH2O。同时,将lung2的静态顺应性固定在60 ml/cmH2O。在模型气管上方(近端测量)和下方(远端测量)测量呼吸变量。肺模型机械通气,气道内径(ID)以1 mm的增量从3 ~ 8 mm改变。结果气道ID 3、4、5、6、7、8各肺分配容积(VL1/VL2)的平均值±标准差比依次为:C15组为0.10±0.05、0.11±0.03、0.12±0.02、0.12±0.02、0.12±0.02、0.12±0.02;C60组为1.05±0.16、1.01±0.09、1.00±0.07、0.97±0.09、0.96±0.06、0.97±0.08;C120组为1.46±0.18、3.06±0.41、3.72±0.37、3.78±0.47、3.77±0.45、3.78±0.60。C15组在气道ID 3 mm (1.65 cmH2O)时肺1呼气末正压(PEEP)显著升高;在ID 3、4和5 mm(2.21、1.06和0.95 cmH2O)时,C60组;C120组与ID 8 mm组相比,ID 3、4、5 mm(2.92、1.84、1.41 cmH2O)差异有统计学意义(P < 0.05)。结论C15、C120组潮气量向双肺分布不均匀,与肺顺应性呈正相关。C120组在气道内径等于或小于4 mm时,潮气量分布不均匀得到改善,但PEEP明显升高。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Evaluation of Respiratory Dynamics in an Asymmetric Lung Compliance Model
Background Unilateral lung hyperinflation develops in lungs with asymmetric compliance, which can lead to vital instability. The aim of this study was to investigate the respiratory dynamics and the effect of airway diameter on the distribution of tidal volume during mechanical ventilation in a lung model with asymmetric compliance. Methods Three groups of lung models were designed to simulate lungs with a symmetric and asymmetric compliance. The lung model was composed of two test lungs, lung1 and lung2. The static compliance of lung1 in C15, C60, and C120 groups was manipulated to be 15, 60, and 120 ml/cmH2O, respectively. Meanwhile, the static compliance of lung2 was fixed at 60 ml/cmH2O. Respiratory variables were measured above (proximal measurement) and below (distal measurement) the model trachea. The lung model was mechanically ventilated, and the airway internal diameter (ID) was changed from 3 to 8 mm in 1-mm increments. Results The mean ± standard deviation ratio of volumes distributed to each lung (VL1/VL2) in airway ID 3, 4, 5, 6, 7, and 8 were in order, 0.10 ± 0.05, 0.11 ± 0.03, 0.12 ± 0.02, 0.12 ± 0.02, 0.12 ± 0.02, and 0.12 ± 0.02 in the C15 group; 1.05 ± 0.16, 1.01 ± 0.09, 1.00 ± 0.07, 0.97 ± 0.09, 0.96 ± 0.06, and 0.97 ± 0.08 in the C60 group; and 1.46 ± 0.18, 3.06 ± 0.41, 3.72 ± 0.37, 3.78 ± 0.47, 3.77 ± 0.45, and 3.78 ± 0.60 in the C120 group. The positive end-expiratory pressure (PEEP) of lung1 was significantly increased at airway ID 3 mm (1.65 cmH2O) in the C15 group; at ID 3, 4, and 5 mm (2.21, 1.06, and 0.95 cmH2O) in the C60 group; and ID 3, 4, and 5 mm (2.92, 1.84, and 1.41 cmH2O) in the C120 group, compared to ID 8 mm (P < 0.05). Conclusions In the C15 and C120 groups, the tidal volume was unevenly distributed to both lungs in a positive relationship with lung compliance. In the C120 group, the uneven distribution of tidal volume was improved when the airway ID was equal to or less than 4 mm, but a significant increase of PEEP was observed.
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