{"title":"毛细管流动阻力与边缘层宽度和轴芯粘度的关系。","authors":"D Braasch","doi":"10.3233/bir-1984-23s125","DOIUrl":null,"url":null,"abstract":"<p><p>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).</p>","PeriodicalId":79205,"journal":{"name":"Biorheology. Supplement : the official journal of the International Society of Biorheology","volume":"1 ","pages":"135-43"},"PeriodicalIF":0.0000,"publicationDate":"1984-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.3233/bir-1984-23s125","citationCount":"1","resultStr":"{\"title\":\"Dependence of capillary flow resistance upon the width of the marginal layer and the viscosity of the axial core.\",\"authors\":\"D Braasch\",\"doi\":\"10.3233/bir-1984-23s125\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>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).</p>\",\"PeriodicalId\":79205,\"journal\":{\"name\":\"Biorheology. Supplement : the official journal of the International Society of Biorheology\",\"volume\":\"1 \",\"pages\":\"135-43\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1984-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.3233/bir-1984-23s125\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Biorheology. Supplement : the official journal of the International Society of Biorheology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.3233/bir-1984-23s125\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Biorheology. Supplement : the official journal of the International Society of Biorheology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.3233/bir-1984-23s125","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
摘要
毛细血管血流可以被认为是两个室室的流动a)低粘性细胞自由边缘层,周围b)高粘性轴向核心。如果两个隔室的流量分别根据泊泽维尔计算,则两个计算的相加允许将泊泽维尔定律适用于小毛细血管中的非牛顿血流。修正后的理论和实验数据的相关系数R2 = 0.99。(H = 0.3 - 0.7, tau W = 0.1 - 1.2 Pa,血液粘度5 - 20mpa X s,毛细血管内径0.3 mm)。通过将血液灌注毛细血管中电阻的剪切依赖变化与无细胞边缘层的发育联系起来,计算出边缘层的宽度。用弯曲玻璃纤维(φ = 10微米)测定芯的粘度。
Dependence of capillary flow resistance upon the width of the marginal layer and the viscosity of the axial core.
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).