Sakhawoth Yasine, Michot Laurent, Levitz Pierre, Rollet Anne-Laure, Sirieix-Plenet Juliette, Merino Daniel Hermida, Malikova Natalie
Laboratory of Physical Chemistry of Electrolytes and Interfacial Nanosystems (PHENIX), Sorbonne Université, CNRS , 75005 Paris , France.
ESRF (The European Synchrotron Radiation Facility) , 71 Avenue des Martyrs , 38000 Grenoble France.
Langmuir. 2019 Aug 20;35(33):10937-10946. doi: 10.1021/acs.langmuir.9b00939. Epub 2019 Aug 8.
We study the aggregation of charged plate-like colloids, Na-montmorillonite clays, in the presence of ionenes, oppositely charged polymer chains. The choice of the charged polymer allows tuning its linear charge density to match/mismatch the average charge separation on the clay surfaces. We assess the nanoscale structure of the aggregates formed by small-angle X-ray and neutron scattering. The nanoscale features of the formed clay aggregates are dominated by the presence of a stacking peak, giving clear evidence for the formation of clay tactoids, that is, a face-to-face aggregation geometry of the clay platelets. The chain charge density of ionenes influences not only the stacking repeat distance within the clay tactoids but also the extent of stacking and abundance of the tactoids. We may distinguish two regimes as a function of clay and ionene polymer charge densities ( and , respectively). The first regime applies to > and ≈ , that is, for highly and "matching" charged chains. Under these conditions, the intercalated chains lie in a flat conformation within the tactoids, irrespective of the ionic strength (within the range studied, i.e., up to 0.05 M NaBr). For weakly charged chains, < , undulation of the ionene chains within the tactoid is seen. The degree of undulation increases with ionic strength due to the decreasing persistence length of the ionene chains. The extent of stacking (5-10 platelets per tactoid) is a general feature of all the systems, and its origin remains unknown. The system corresponding to the closest match in charge separations on the clay surface and on the polymer chain ( ≈ ) features the highest abundance of tactoids. This coincides with the highest macroscopic density as deduced from simple visual inspection of sediment volumes. This leads to the open question regarding the link between the density at the nanoscale and the macroscopic density and sedimentation behavior of the aggregate.
我们研究了在离子烯(带相反电荷的聚合物链)存在下,带电荷的片状胶体钠蒙脱石粘土的聚集情况。选择带电荷的聚合物可以调节其线性电荷密度,以匹配/不匹配粘土表面的平均电荷间距。我们通过小角X射线和中子散射评估所形成聚集体的纳米级结构。所形成的粘土聚集体的纳米级特征主要由一个堆叠峰主导,这为粘土准晶体的形成提供了明确证据,即粘土片层的面对面聚集几何结构。离子烯的链电荷密度不仅影响粘土准晶体内的堆叠重复距离,还影响堆叠程度和准晶体的丰度。根据粘土和离子烯聚合物的电荷密度(分别为 和 ),我们可以区分两种情况。第一种情况适用于 > 且 ≈ ,即对于高电荷且“匹配”的链。在这些条件下,插入的链在准晶体内呈扁平构象,与离子强度无关(在所研究的范围内,即高达0.05 M NaBr)。对于弱电荷链, < ,可以看到离子烯链在准晶体内发生波动。由于离子烯链的持久长度减小,波动程度随离子强度增加。堆叠程度(每个准晶体5 - 10个片层)是所有系统的一个普遍特征,其起源仍然未知。粘土表面和聚合物链上电荷间距最接近匹配( ≈ )的系统具有最高的准晶体丰度。这与通过简单观察沉积物体积推断出的最高宏观密度相吻合。这就引出了一个关于纳米级密度与聚集体宏观密度和沉降行为之间联系的开放性问题。