Theory of Viscosity of Concentrated Suspensions

Theory of Viscosity of Concentrated Suspensions
复制标题

DOI:
10.1038/155364b0
复制
发表时间:
1945-03
期刊:
影响因子:
64.8
通讯作者:
V. Vand
V. Vand
中科院分区:
综合性期刊1区
文献类型:
--
作者:
V. Vand

文献摘要

被引文献

相似文献

对于刚性球体的无限稀释悬浮液,爱因斯坦在严格的理论基础上推导出公式η = η0(1 +kc),…(1)式中η为悬浮液粘度,η为纯溶剂粘度,顺式为体积浓度,k= 2.5为常数。(1)也适用于非球形粒子,其因素是它们的形状、刚性和布朗运动的函数。对于伸长的刚性颗粒,k> 2·5。
FOR infinitely diluted suspensions of rigid spheres, Einstein1derived on a rigorously theoretical basis the formula η = η0(1 +kc),... (1) where η is the viscosity of the suspension, η0is the viscosity of the pure solvent,cis the concentration by volume andk= 2·5 is a constant. It has been shown that (1) is also valid for non-spherical particles, the factorkbeing a function of their shape, rigidity and Brownian movement. For elongated rigid particles,k> 2·5.