Zhou Zhi, Hollingsworth Javoris V, Hong Song, Cheng He, 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 Sciences , Beijing 100190, China.
Langmuir. 2014 May 27;30(20):5739-46. doi: 10.1021/la500866d. Epub 2014 May 13.
Rheological measurements are utilized to examine the yielding behavior of a polystyrene (PS) core and poly(N-isopropylacrylamide) (PNIPAM) shell microgel system with varying shell/core ratio. For a shell/core ratio of 0.15 at high concentrations, the suspensions show a typical hard sphere (HS) yielding response where the loss modulus (G″) exhibits a single peak due to cage breaking. As a result of tighter cages and less cage distortion prior to yielding, the peak location of G″ decreases with volume fraction. For a shell/core ratio of 1.10, which behaves like a soft jammed glass at high concentration, the suspensions exhibit a one-step yielding behavior similar to that of HS glass. However, the location of the peak in G″ increases with volume fraction, demonstrating the important role of particle deformation in the breakage of cages. For an intermediate shell/core ratio of 0.34, the system displays a two-step yielding behavior, as observed in previous reports for attractive glasses. By increasing the volume fraction, the strain of the first peak increases while the second one decreases. In addition, as the effective volume fraction increases to 112%, the two peaks merge into one broad peak. It is demonstrated that the first peak of G″ is due to deformation of the shell, and the second peak of G″ is attributed to cage breaking as a result of the cores colliding with each other. Combining these results, a yielding state diagram from typical HS to soft jammed glass is demonstrated.
利用流变学测量来研究具有不同壳/核比的聚苯乙烯(PS)核和聚(N-异丙基丙烯酰胺)(PNIPAM)壳微凝胶体系的屈服行为。对于高浓度下壳/核比为0.15的情况,悬浮液表现出典型的硬球(HS)屈服响应,其中损耗模量(G″)由于笼状结构破坏而呈现单峰。由于屈服前笼状结构更紧密且笼状结构变形更小,G″的峰值位置随体积分数降低。对于壳/核比为1.10的情况,其在高浓度下表现得像软堵塞玻璃,悬浮液呈现出与HS玻璃类似的一步屈服行为。然而,G″中峰值的位置随体积分数增加,这表明颗粒变形在笼状结构破坏中起重要作用。对于中间壳/核比为0.34的情况,该体系表现出两步屈服行为,如先前关于吸引性玻璃的报道中所观察到的。通过增加体积分数,第一个峰值的应变增加而第二个峰值的应变减小。此外,当有效体积分数增加到112%时,两个峰值合并为一个宽峰。结果表明,G″的第一个峰值是由于壳的变形,而G″的第二个峰值归因于核相互碰撞导致的笼状结构破坏。综合这些结果,展示了从典型HS到软堵塞玻璃的屈服状态图。