Fujii S, Richtering W
Institute for Physical Chemistry, RWTH Aachen University, Landoltweg 2, 52056, Aachen, Germany.
Eur Phys J E Soft Matter. 2006 Feb;19(2):139-48. doi: 10.1140/epje/e2006-00015-6. Epub 2006 Jan 31.
We studied viscoelastic properties and scaling behavior of multilamellar vesicles (MLVs) confined between two parallel plates as a function of the shear rate and sample thickness (gap size between parallel plates). The rheological properties are classified into two regimes; the shear-thinning regime at high shear rates and the shear-thickening regime at low shear rates. In the former, the MLV radius results from the mechanical balance between the effective surface tension sigma(eff) and viscous stress force. The MLV radius is independent of the gap size. sigmaeff estimated by van der Linden model is 2.1+/-0.15x10(-4) Nm-1 corresponding to the same value obtained by SANS measurement. Power law exponents for the steady state viscosity and yield stress against pre-shear rate ([see text], [see text]) well agree with prediction based on the layering of membranes. Therefore, viscoelastic properties in this regime could be modeled by assuming that the dynamics of MLVs are driven by layering of MLV polydomains, which could be accompanied by the viscous dissipation, i.e., the stress relaxation on the MLV, induced by continuous sequence of yields of MLVs. The flow curve is empirically explained by the assumption of a relaxation time for the MLV shape. In the latter, however, scaling laws observed in the shear-thinning regime break down. The MLV radius increases when the gap size is reduced below the threshold value and MLV is no longer formed at very small gap sizes. Different dynamics from the shear-thinning regime seem to dominate the viscoelasticity.
我们研究了限制在两个平行板之间的多层囊泡(MLV)的粘弹性性质和标度行为,该行为是剪切速率和样品厚度(平行板之间的间隙尺寸)的函数。流变性质分为两种状态;高剪切速率下的剪切变稀状态和低剪切速率下的剪切增稠状态。在前一种状态下,MLV半径由有效表面张力σeff和粘性应力之间的力学平衡决定。MLV半径与间隙尺寸无关。通过范德林登模型估计的σeff为2.1±0.15×10⁻⁴ Nm⁻¹,与小角中子散射测量得到的相同值相对应。稳态粘度和屈服应力相对于预剪切速率的幂律指数([见正文],[见正文])与基于膜分层的预测非常吻合。因此,该状态下的粘弹性性质可以通过假设MLV的动力学由MLV多畴的分层驱动来建模,这可能伴随着粘性耗散,即MLV上的应力松弛,由MLV的连续屈服序列引起。流动曲线可以通过假设MLV形状的弛豫时间来进行经验解释。然而,在后一种状态下,在剪切变稀状态下观察到的标度律失效。当间隙尺寸减小到阈值以下时,MLV半径增大,并且在非常小的间隙尺寸下不再形成MLV。与剪切变稀状态不同的动力学似乎主导了粘弹性。