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The application of multiscale quasi 4D CT to the study of SrCrO4 distributions and the development of porous networks in epoxy-based primer coatings

机译:多尺度拟4D CT技术在研究SrCrO4分布和环氧树脂基底漆中多孔网络发展中的应用

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摘要

Transport paths for inhibitor release within a model strontium chromate (SrCrO4) inhibited/epoxy primer have been studied using a combination of tomography techniques. It has been found that the SrCrO4 particles form independent clusters within the model primer. The clusters have a range of fractal dimensions with the largest clusters (a few hundred microns in size) having a fractal dimension of 2.36. Leaching of the SrCrO4 from the primer appears to be initially through direct dissolution of particles in contact with the electrolyte but changes to diffusion through void pathways created by dissolution of the SrCrO4 phase. No evidence was found for the diffusion of chromate ions through the epoxy. Transport through such clusters does not follow Fickian diffusion, which has traditionally been employed to describe inhibitor release dynamics. Release kinetics typically follow a tm behaviour where t is time and m is an index which would be 0.5 for Fickian diffusion. Thus the overall release with time will evolve, being initially the result of direct dissolution, then at intermediate times, be dominated by transport through the fractal network and at the final stage go to zero since all the strontium chromate will be dissolved from the cluster connected to the surface. Clusters not connected to the surface remain undissolved and form additional reservoirs for further release in when local damage occurs in their vicinity. This new model of inhibitor transport creates new strategies for the development of self-healing properties for coatings.
机译:已结合层析成像技术研究了在铬酸锶(SrCrO4)抑制/环氧底漆中释放抑制剂的传输路径。已经发现,SrCrO4颗粒在模型引物内形成独立的簇。团簇具有一定的分形维数范围,最大的团簇(大小为几百微米)的分形维数为2.36。从底漆中渗出SrCrO4最初似乎是通过直接溶解与电解质接触的颗粒而实现的,但后来通过由SrCrO4相溶解而产生的空隙途径转变为扩散。没有发现铬酸盐离子通过环氧树脂扩散的证据。通过此类簇的运输不遵循菲克扩散,传统上已采用菲克扩散来描述抑制剂释放动力学。释放动力学通常遵循tm行为,其中t为时间,m为Fickian扩散指数,其值为0.5。因此,随着时间的流逝,总释放量会逐渐增加,最初是直接溶解的结果,然后是中间时间,主要通过分形网络的传输来控制,最后阶段归零,因为所有铬酸锶将从连接的簇中溶解。到表面。未连接到表面的簇保持溶解状态,并形成额外的储层,以便在附近发生局部破坏时进一步释放。这种抑制剂转移的新模型为开发涂料的自愈性能创造了新的策略。

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