Braasch D
Biorheology Suppl. 1984;1:135-43. doi: 10.3233/bir-1984-23s125.
Capillary blood flow may be considered as the flow of two compartments a.) the low viscous cell free marginal layer, surrounding b.) the higher viscous axial core. If the flow of both compartments is calculated separately according to Poiseuille, the addition of the two calculations allows to adapt Poiseuille's law to the non-Newtonian blood flow in small capillaries. The modified law correlates theoretical and experimental data with R2 = 0.99. (H = 0.3 - 0.7, tau W = 0.1 - 1.2 Pa, blood viscosity 5 to 20 mPa X s, capillary I.D. 0.3 mm). The width of the marginal was calculated by relating the shear dependent change in electrical resistance in blood perfused capillaries to the development of a cell free marginal layer. The viscosity of the core was determined with a bended glass fibre (phi = 10 microns).
a.) 低粘性的无细胞边缘层,围绕着b.) 高粘性的轴向核心。如果根据泊肃叶定律分别计算两个腔室的血流,将这两个计算结果相加就能使泊肃叶定律适用于小毛细血管中的非牛顿血流。修正后的定律将理论数据和实验数据关联起来,相关系数R2 = 0.99。(H = 0.3 - 0.7,τW = 0.1 - 1.2帕斯卡,血液粘度5至20毫帕斯卡·秒,毛细血管内径0.3毫米)。边缘层的宽度通过将血液灌注毛细血管中与剪切相关的电阻变化与无细胞边缘层的形成相关联来计算。核心层的粘度用弯曲玻璃纤维(φ = 10微米)测定。