论文标题

颗粒聚集在干胶体二氧化硅层结构上的作用

Role of particle aggregation on the structure of dried colloidal silica layers

论文作者

Lesaine, Arnaud, Bonamy, Daniel, Rountree, Cindy, Gauthier, Georges, Impéror-Clerc, Marianne, Lazarus, Veronique

论文摘要

胶体干燥的过程在包括光子学或生物技术在内的众多ELD中让位于粒子自组装。然而,在干胶体层中驱动NAL颗粒排列的机制和条件仍然难以捉摸。在这里,我们研究了干燥速率如何在四个二氧化硅纳米球悬浮液中选择厚干层的纳米结构。取决于粒度和分散性,要么是无定形排列,结晶排列或速率依赖性的无定形至晶状过渡,发生在干燥表面。在两个最多分散的悬浮液中观察到无定形的排列,而当分散性较低时发生结晶度。在后一种情况下,违反直觉,更高的干燥速率有利于颗粒的排序。为了补充这些测量值并库存层的大量特性,进行了对层孔隙率的测试。对于本文研究的所有悬浮液,更快的干燥均可使干燥层密集。晶体表面布置意味着大容量分数($ \ sim $ 0.65),而可以在低(降至$ \ sim $ 0.53)或高($ \ sim $ 0.65)体积分数的层中观察到无定形布置。最后,我们通过有针对性的其他实验和SAXS测量来证明,层的填料结构主要是由聚集体的形成及其随后的填料驱动的,而不是由布朗尼屈光度和对流之间的竞争驱动。这强调了,除了peclet数字外,第二个无量纲比率应考虑到蒸发时间尺度上的聚集。

The process of colloidal drying gives way to particle self-assembly in numerous elds including photonics or biotechnology. Yet, the mechanisms and conditions driving the nal particle arrangement in dry colloidal layers remain elusive. Here, we examine how the drying rate selects the nanostructure of thick dried layers in four dierent suspensions of silica nanospheres. Depending on particle size and dispersity, either an amorphous arrangement, a crystalline arrangement, or a rate-dependent amorphous-to-crystalline transition occurs at the drying surface. Amorphous arrangements are observed in the two most polydisperse suspensions while crystallinity occurs when dispersity is lower. Counter-intuitively in the latter case, a higher drying rate favors ordering of the particles. To complement these measurements and to take stock of the bulk properties of the layer, tests on the layer porosity were undertaken. For all suspensions studied herein, faster drying yields denser dry layers. Crystalline surface arrangement implies large bulk volume fraction ($\sim$ 0.65) whereas amorphous arrangements can be observed in layers with either low (down to $\sim$ 0.53) or high ($\sim$ 0.65) volume fraction. Lastly, we demonstrate via targeted additional experiments and SAXS measurements, that the packing structure of the layers is mainly driven by the formation of aggregates and their subsequent packing, and not by the competition between Brownian diusion and convection. This highlights that a second dimensionless ratio in addition to the Peclet number should be taken into account, namely the aggregation over evaporation timescale.

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