Federspiel W J
Department of Biomedical Engineering, Boston University, Massachusetts 02215.
Microvasc Res. 1990 Nov;40(3):394-411. doi: 10.1016/0026-2862(90)90035-p.
Most techniques for making quantitative measurements of flow within single microvessels rely on tracers which are injected upstream of the microvessel and monitored noninvasively (e.g., optical densitometry) at selected sites along the microvessel. This study examines theoretically the measurement of average flow velocity (v) within individual microvessels from tracer flow data at monitoring sites. Starting with a fundamental convection-diffusion equation, the theory considers tracers which can distribute across both plasma and red cell phases. An integral analysis indicates that v = delta zeta/delta tau, where delta zeta is the distance between monitoring sites, and delta tau is the tracer transit or "residence" time needed to traverse that distance. The residence time which arises explicitly requires measurement of the flow-weighted average tracer concentration at each monitoring site. Because noninvasive tracer measurements provide indices of the unweighted average tracer concentration, a velocity measurement error, delta(zeta), arises, delta(zeta) is quantified in relation to the axial location of the measurement site, the velocity profile, the tracer Peclet number, and the radial distribution of tracer at the vessel inlet. delta(zeta) does not vanish when tracer enters a microvessel with a radially uniform concentration profile, but does vanish past a critical distance, Lc, from the microvessel entrance. The critical distance can be estimated using Lc/d = 0.05(vd)/D (d. vessel diameter; v, average flow velocity; D, tracer diffusivity). Accordingly, tracer data can be used to quantify flow velocity within a microvessel provided the microvessel length allows for monitoring tracer flow beyond the estimated Lc value. This study serves as a necessary precursor to analyses of plasma-phase tracers used to measure microvascular plasma flow.
大多数用于对单个微血管内的血流进行定量测量的技术都依赖于示踪剂,这些示踪剂被注入微血管的上游,并在沿微血管的选定部位进行非侵入性监测(例如,光密度测定法)。本研究从理论上探讨了根据监测部位的示踪剂流动数据来测量单个微血管内的平均流速(v)。该理论从一个基本的对流扩散方程出发,考虑了能够在血浆和红细胞相中分布的示踪剂。积分分析表明,v = Δζ/Δτ,其中Δζ是监测部位之间的距离,而Δτ是示踪剂穿过该距离所需的传输或“停留”时间。明确出现的停留时间需要测量每个监测部位的流量加权平均示踪剂浓度。由于非侵入性示踪剂测量提供的是未加权平均示踪剂浓度的指标,因此会产生速度测量误差Δ(ζ),Δ(ζ)是根据测量部位的轴向位置、速度分布、示踪剂佩克莱数以及血管入口处示踪剂的径向分布来量化的。当示踪剂以径向均匀的浓度分布进入微血管时,Δ(ζ)不会消失,但在距微血管入口超过临界距离Lc时会消失。临界距离可以用Lc/d = 0.05(vd)/D来估计(d为血管直径;v为平均流速;D为示踪剂扩散率)。因此,只要微血管长度允许在估计的Lc值之外监测示踪剂流动,示踪剂数据就可用于量化微血管内的流速。本研究是用于测量微血管血浆流动的血浆相示踪剂分析的必要前提。