Hudetz A G, Conger K A, Halsey J H, Pal M, Dohan O, Kovach A G
J Cereb Blood Flow Metab. 1987 Jun;7(3):342-55. doi: 10.1038/jcbfm.1987.72.
The objective of the present work was a theoretical evaluation of pial arterial pressures in normotensive rats and spontaneously hypertensive rats based on the geometry and topography of the pial arterial system as well as on various topological models of the vascular trees. Pial branches of the middle cerebral artery in the diameter range of 30-320 microns were selectively visualized by corrosion compound, and the diameter and length of vascular segments were measured. The vessels were classified into branching orders by the methods of Horsfield and Strahler. The steady-state pressure distribution in the pial arterial system was calculated assuming that the flow at the bifurcations was partitioned in proportion to a given power of the diameters of the daughter branches (diameter exponent). The maximum number of vascular segments along the longest branch varied between 16 and 33. The mean branching ratio was 4.14 +/- 0.23 (SD). The mean diameter of vessels classified into Strahler orders 1-5 were: 50 +/- 12, 71 +/- 19, 106 +/- 22, 168 +/- 22, and 191 +/- 7 microns, respectively. The calculated pressure drop in the pial trees of normotensive rats was approximately twice as large in proximal orders 3 and 4 than in distal orders 1 and 2. The mean pressure in arteries of order 1 ranged from 54.4 to 58.4 mm Hg in the normotensive rat (input pressure: 83 mm Hg), and from 77.2 to 89.0 mm Hg in the spontaneously hypertensive rat (input pressure: 110 mm Hg). The coefficient of variation of terminal pressures in vessels of order 1 increased linearly with the mean pressure drop in the system. The coefficient of variation in terminal pressure had a minimum as a function of the diameter exponent in case of each pial tree. At its minimum, it was higher in all spontaneously hypertensive rats (10.1-22.9%) than in any normotensive rats (6.0-8.5%). The corresponding diameter exponents were in most cases lower in the spontaneously hypertensive rat (1.3-2.5) than in the normotensive rat (2.5-3.0). Topologically consistent models of the pial arterial network predicted significantly less variation in intravascular pressures than was obtained by direct calculations. More idealized models suggested the dependence of coefficient of variation in terminal pressure on the total number of vascular segments contained by the tree. All models predicted the existence of the minimum of coefficient of variation in terminal pressure in function of the diameter exponent.(ABSTRACT TRUNCATED AT 400 WORDS)
本研究的目的是基于软脑膜动脉系统的几何形状和拓扑结构以及血管树的各种拓扑模型,对正常血压大鼠和自发性高血压大鼠的软脑膜动脉压进行理论评估。通过腐蚀铸型法选择性地显示直径范围为30 - 320微米的大脑中动脉软脑膜分支,并测量血管段的直径和长度。采用霍斯菲尔德和斯特拉勒的方法将血管分类为分支等级。假设分支处的血流按子分支直径的给定幂次(直径指数)成比例分配,计算软脑膜动脉系统中的稳态压力分布。最长分支上的血管段最大数量在16至33之间变化。平均分支比为4.14±0.23(标准差)。分类为斯特拉勒1 - 5级的血管平均直径分别为:50±12、71±19、106±22、168±22和191±7微米。正常血压大鼠软脑膜树中计算出的近端3级和4级压力降大约是远端1级和2级的两倍。正常血压大鼠(输入压力:83毫米汞柱)中1级动脉的平均压力范围为54.4至58.4毫米汞柱,自发性高血压大鼠(输入压力:110毫米汞柱)中为77.2至89.0毫米汞柱。1级血管中终末压力的变异系数随系统中的平均压力降线性增加。在每个软脑膜树中,终末压力变异系数作为直径指数的函数有一个最小值。在最小值时,所有自发性高血压大鼠(10.1 - 22.9%)的该系数均高于任何正常血压大鼠(6.0 - 8.5%)。相应的直径指数在大多数情况下,自发性高血压大鼠(1.3 - 2.5)低于正常血压大鼠(2.5 - 3.0)。软脑膜动脉网络的拓扑一致模型预测的血管内压力变化明显小于直接计算得到的结果。更理想化的模型表明终末压力变异系数与树中包含的血管段总数有关。所有模型都预测终末压力变异系数作为直径指数的函数存在最小值。(摘要截断于400字)