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Rheological properties of water swellable microgel polymerized in a confined space

机译:在密闭空间中聚合的水溶胀性微凝胶的流变特性

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The rheological properties of a water swellable microgel polymerized in an inversed micelle, confined space, were studied. The chemical component of the microgel was poly(dimethylacrylamide-co-2-acrylamide-2-methyl-1-propanesulfonic acid) crosslinked with methylenebis-acrylamide. The flow curves of the microgel aqueous dispersion containing sodium chloride (3 mmol/L) were analyzed using the Herschel-Bulkley equation. Since the overlap concentration (c*) of the microgel was precisely agreed with 1/[eta], the microgel particle is likely to be dispersed as an impenetrable particle in the dilute regime according to the Einstein's law. The microgel aqueous dispersion showed the viseoelastic-liquid like behavior in a higher concentration above c*. There was a critical concentration that the apparent yield stress appeared. The effective volume fraction occupied by the microgel particle was 0.7 at the critical concentration. To investigate the mechanical properties of such a concentrated sample, steady state compliance (J(e0)) of the microgel dispersion was evaluated by the creep recovery measurement. The relationship between J(e0)(-1) and the concentration in semi-dilute regime was according to a scaling law. Moreover, the microgel dispersion behaved as if a bulkgel when its concentration was sufficient high. It is considered that the discrete microgel particles would be close packed, resulting deformed and deswollen the particles, and it seemed that the discrete gel networks were stuck each other as if the microgel dispersion turned to a continuous gel. (c) 2005 Elsevier B.V All rights reserved.
机译:研究了在反胶束,密闭空间中聚合的水溶胀性微凝胶的流变特性。所述微凝胶的化学成分是与亚甲基双丙烯酰胺交联的聚(二甲基丙烯酰胺-co-2-丙烯酰胺-2-甲基-1-丙烷磺酸)。使用Herschel-Bulkley方程分析了含氯化钠(3 mmol / L)的微凝胶水分散液的流动曲线。由于微凝胶的重叠浓度(c *)精确地等于1 /η,因此根据爱因斯坦定律,微凝胶颗粒可能在稀薄状态下作为不可渗透的颗粒而分散。该微凝胶水分散体在高于c *的较高浓度下显示出类固弹-液体行为。在一个临界浓度下,出现了明显的屈服应力。在临界浓度下,微凝胶颗粒占据的有效体积分数为0.7。为了研究这种浓缩样品的机械性能,通过蠕变回复率测量评估了微凝胶分散液的稳态顺应性(J(e0))。 J(e0)(-1)与半稀释状态下的浓度之间的关系根据比例定律。此外,当其浓度足够高时,微凝胶分散体表现得像块状凝胶。认为离散的微凝胶颗粒将紧密堆积,导致颗粒变形和溶胀,并且似乎离散的凝胶网络彼此粘附,就像微凝胶分散体变成连续的凝胶一样。 (c)2005 Elsevier B.V保留所有权利。

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