Zhao Chuanzhuang, Yuan Guangcui, Han Charles C
State Key Laboratory of Polymer Physics and Chemistry, Joint Laboratory of Polymer Science and Materials, Beijing National Laboratory for Molecular Sciences, Institute of Chemistry, Chinese Academy of Science, Beijing 100190, China.
Soft Matter. 2014 Nov 28;10(44):8905-12. doi: 10.1039/c4sm01798f.
Gelation and glass transition in a mixed suspension of polystyrene (PS) microsphere and poly(N-isopropylacrylamide) (PNIPAM) microgel were studied as a function of the total colloid volume fraction and mixing ratio of these two components. The PNIPAM microgel, which is adsorbable on the PS microsphere surface, can induce bridging or stabilizing effect between microspheres depending on whether the volume fraction of microgel (ΦMG) is smaller or larger than the saturated adsorption concentration (ΦMG) for a given volume fraction of the microsphere (ΦMS). ΦMG is in a linear relationship with ΦMS, and the value of ΦMG/ΦMG can be taken as an approximate measure of surface coverage. A state diagram of gelation and glass transition is constructed with the short-ranged attractive interaction, resulting from the well-defined bridging bonding. Keeping ΦMG/ΦMG = 0.20 and increasing ΦMS from 0.25 to 0.55, the mixed suspension transforms from a bridging gel into an attractive glass; moreover, while keeping ΦMS = 0.45 and increasing ΦMG/Φ*MG from 0.20 to 1.2, the mixed suspension changes from a bridging gel into an attractive glass, and then to a repulsive glass. The bridging effect and the cage effect can be distinguished by the yielding behaviors in rheological measurements. In the nonlinear dynamic rheological experiments, one-step yielding, corresponding to the disconnecting of bridge network, is observed in the bridging gel, and one-step yielding, corresponding to the breaking of cage, is observed in the repulsive glass. However, a two-step yielding behavior is found in the bridging-induced attractive glass, which is attributed to the bridging effect of microgels and the caging effect of the dense environment.
研究了聚苯乙烯(PS)微球与聚(N-异丙基丙烯酰胺)(PNIPAM)微凝胶混合悬浮液中的凝胶化和玻璃化转变,考察了其作为这两种组分的总胶体体积分数和混合比例的函数关系。可吸附在PS微球表面的PNIPAM微凝胶,根据微凝胶的体积分数(ΦMG)对于给定微球体积分数(ΦMS)是小于还是大于饱和吸附浓度(ΦMG),可在微球之间诱导桥连或稳定作用。ΦMG与ΦMS呈线性关系,ΦMG/ΦMG的值可作为表面覆盖率的近似度量。利用明确的桥连键合产生的短程吸引相互作用,构建了凝胶化和玻璃化转变的状态图。保持ΦMG/ΦMG = 0.20并将ΦMS从0.25增加到0.55,混合悬浮液从桥连凝胶转变为吸引性玻璃;此外,保持ΦMS = 0.45并将ΦMG/Φ*MG从0.20增加到1.2时,混合悬浮液从桥连凝胶变为吸引性玻璃,然后变为排斥性玻璃。桥连效应和笼效应可通过流变测量中的屈服行为来区分。在非线性动态流变实验中,在桥连凝胶中观察到对应于桥连网络断开的一步屈服,在排斥性玻璃中观察到对应于笼破裂的一步屈服。然而,在桥连诱导的吸引性玻璃中发现了两步屈服行为,这归因于微凝胶的桥连效应和致密环境的笼效应。