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肺间质-淋巴系统模型。

A model of the lung interstitial-lymphatic system.

作者信息

Drake R E, Laine G A, Allen S J, Katz J, Gabel J C

机构信息

Center for Microvascular and Lymphatic Studies, University of Texas Medical School, Houston 77030.

出版信息

Microvasc Res. 1987 Jul;34(1):96-107. doi: 10.1016/0026-2862(87)90082-3.

DOI:10.1016/0026-2862(87)90082-3
PMID:3657607
Abstract

Our model of the pulmonary interstitial-lymphatic system is based on the assumption that the lung interstitial space can be divided into two compartments. The first compartment (C1) contains the terminal lymph vessels. Increases in the fluid pressure within this compartment, along with increased pressure generated by lymph vessel pumping, cause the lymph flow rate to increase. The lymph vessels run through the second compartment (C2) which we believe represents the perivascular spaces. Increases in the fluid volume of C2 cause the lymph vessels to dilate and this causes lymph vessel resistance to decrease. Normally the lymph flow rate equals the microvascular filtration rate so that lung fluid volume is constant. According to our model, increases in filtration rate cause fluid to collect in C1 and C2. The resulting increase in fluid pressure in C1, increased lymph vessel pumping, and the decrease in lymph vessel resistance in C2 cause lymph flow to increase. Eventually, the lymph flow rises to equal the filtration rate and lung fluid volume becomes constant again. The results of simulations with our model indicate that decreases in lymph vessel resistance are essential for lymph flow to increase substantially as edema develops.

摘要

我们的肺间质 - 淋巴系统模型基于这样一种假设,即肺间质空间可分为两个腔室。第一个腔室(C1)包含终末淋巴管。该腔室内流体压力的增加,以及淋巴管泵血产生的压力增加,会导致淋巴流速增加。淋巴管贯穿第二个腔室(C2),我们认为它代表血管周围间隙。C2中液体量的增加会导致淋巴管扩张,进而使淋巴管阻力降低。正常情况下,淋巴流速等于微血管滤过率,因此肺液体积保持恒定。根据我们的模型,滤过率增加会导致液体在C1和C2中积聚。C1中由此产生的流体压力增加、淋巴管泵血增加以及C2中淋巴管阻力降低,会导致淋巴流量增加。最终,淋巴流量上升至等于滤过率,肺液体积再次保持恒定。我们模型的模拟结果表明,随着水肿的发展,淋巴管阻力降低对于淋巴流量大幅增加至关重要。

相似文献

1
A model of the lung interstitial-lymphatic system.肺间质-淋巴系统模型。
Microvasc Res. 1987 Jul;34(1):96-107. doi: 10.1016/0026-2862(87)90082-3.
2
Active lymphatic pumping and sheep lung lymph flow.活跃的淋巴泵作用与绵羊肺淋巴液流动
J Appl Physiol (1985). 1991 Jul;71(1):99-103. doi: 10.1152/jappl.1991.71.1.99.
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[Relation between lymph flow and pressure in the interstitium and the degree of hydration of the lungs].[肺间质中淋巴液流动与压力及肺水合程度之间的关系]
Fiziol Zh SSSR Im I M Sechenova. 1985 Sep;71(9):1124-30.
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A mathematical model of flow through the terminal lymphatics.通过终末淋巴管的血流数学模型。
Med Eng Phys. 1995 Mar;17(2):134-40. doi: 10.1016/1350-4533(95)91885-k.
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Dynamics of subatmospheric pressure in the pulmonary interstitial fluid.肺间质液中负压的动态变化
Ciba Found Symp. 1976(38):77-100. doi: 10.1002/9780470720202.ch6.
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Mechanics of lung fluid balance.肺液体平衡的力学原理。
Crit Rev Biomed Eng. 1986;13(3):171-200.
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Network Scale Modeling of Lymph Transport and Its Effective Pumping Parameters.淋巴运输的网络规模建模及其有效泵浦参数
PLoS One. 2016 Feb 4;11(2):e0148384. doi: 10.1371/journal.pone.0148384. eCollection 2016.
8
Lymph flow characteristics and microvascular exchange: an analog computer simulation.
Lymphology. 1982 Dec;15(4):156-62.
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Pulmonary interstitial resistance.肺间质阻力
Ann Biomed Eng. 1987;15(2):173-82. doi: 10.1007/BF02364052.
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