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液体输注的物理和生理模型。

Model for the physics and physiology of fluid administration.

作者信息

Philip J H

机构信息

Department of Anesthesia, Brigham and Women's Hospital, Boston, MA.

出版信息

J Clin Monit. 1989 Apr;5(2):123-34. doi: 10.1007/BF01617887.

DOI:10.1007/BF01617887
PMID:2656923
Abstract

This article describes a model designed to provide an understanding of fluid flow in intravenous systems and human subjects. Experiments were developed which demonstrate that the model can represent common clinical situations. The model depicts physical devices as ideal resistors, pressure sources, and flow sources. The patient's venous system is depicted as a combination of ordinary and Starling resistors. For flows between 0 and 300 ml/hr, both physical devices and patients are adequately represented by a straight line representing the pressure-flow relationship (PFR): pressure = opening pressure + flow X resistance, where the slope is the resistance to fluid flow and the intercept is the opening pressure. The PFR for a normal vein is characterized by a flat slope (vein resistance = 22 +/- 20 mm Hg/L/hr, mean +/- SD) and a low intercept (opening pressure = 15 +/- 8 mm Hg). The PFR for a partially obstructed vein has a resistance equal to that of an unobstructed vein and an opening pressure elevated approximately equal to the pressure obstructing the vein. For perivascular tissue, the PFR has a steep slope (tissue resistance = 1,125 +/- 1,376 mm Hg/L/hr), while tissue opening pressure depends on the amount of fluid infused. At the onset of fluid extravasation (infiltration), tissue pressure usually is lower than venous pressure (8 +/- 8 versus 15 +/- 8 mm Hg), until fluid fills the distensible tissue compartment. In clinical practice, when infiltration or obstruction occurs, flow decreases and the clinician adjusts the roller clamp until correct flow resumes; no problem is obvious. The combined model for the intravenous tubing and venous systems explains the behavior of current clinical infusion devices.

摘要

本文描述了一个旨在理解静脉系统和人体受试者中流体流动的模型。开展了相关实验,结果表明该模型能够代表常见的临床情况。该模型将物理装置描述为理想的电阻器、压力源和流量源。患者的静脉系统被描述为普通电阻器和斯塔林电阻器的组合。对于0至300毫升/小时的流量,物理装置和患者都可以通过一条代表压力-流量关系(PFR)的直线得到充分体现:压力 = 开启压力 + 流量×阻力,其中斜率为流体流动阻力,截距为开启压力。正常静脉的PFR特征是斜率平缓(静脉阻力 = 22±20毫米汞柱/升/小时,平均值±标准差)且截距较低(开启压力 = 15±8毫米汞柱)。部分阻塞静脉的PFR阻力与未阻塞静脉相同,开启压力升高幅度大致等于阻塞静脉的压力。对于血管周围组织,PFR斜率陡峭(组织阻力 = 1125±1376毫米汞柱/升/小时),而组织开启压力取决于输注的液体量。在液体外渗(浸润)开始时,组织压力通常低于静脉压力(8±8对15±8毫米汞柱),直到液体充满可扩张的组织腔室。在临床实践中,当发生浸润或阻塞时,流量会降低,临床医生会调整滚轮夹,直到恢复正确的流量;此时问题并不明显。静脉输液管和静脉系统的组合模型解释了当前临床输液装置的行为。

相似文献

1
Model for the physics and physiology of fluid administration.液体输注的物理和生理模型。
J Clin Monit. 1989 Apr;5(2):123-34. doi: 10.1007/BF01617887.
2
Is the i.v. obstructed or infiltrated? A simple clinical test.静脉输液是受阻还是渗漏了?一项简单的临床检查。
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3
Resistance to fluid flow in veins.静脉中流体流动的阻力。
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6
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7
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8
Detection of intravenous fluid extravasation using resistance measurements.通过电阻测量检测静脉输液外渗
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9
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引用本文的文献

1
Sensing Technologies for Extravasation Detection: A Review.渗出检测传感技术:综述。
ACS Sens. 2023 Mar 24;8(3):1017-1032. doi: 10.1021/acssensors.2c02602. Epub 2023 Mar 13.
2
Detection of intravenous fluid extravasation using resistance measurements.通过电阻测量检测静脉输液外渗
J Clin Monit. 1996 Jul;12(4):325-30. doi: 10.1007/BF02221754.
3
An analysis of the effect of venous resistance on the performance of gravity-fed intravenous infusion systems.静脉阻力对重力式静脉输液系统性能影响的分析

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