颗粒状膨润土混合物微观结构可视化及传质参数测量

M. Nazir, A. Matsuno, Takeshi Saito, K. Kawamoto, T. Sakaki
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引用次数: 1

摘要

膨润土通常被认为是放射性废物处理工程屏障系统(EBS)的关键组成部分之一。对膨润土的力学、热、水力特性进行深入研究,以保证膨润土的安放质量,控制EBS的性能。研究了干密度和相对湿度对颗粒状膨润土混合物(GBM)微观结构和质量输运特性的影响。所测试的GBM样品是通过筛选和分级日本膨润土(商品名:OK膨润土,Kunimine Industries, Japan)制备的。在干密度控制条件下,风干的GBM样品(相对湿度60%,重量含水量6.38%)以六种不同的干密度(1.25至1.75 g/cm)进行包装。湿度控制条件下的样品在干密度为1.45 g/cm的条件下制备,在RH 90%的条件下保存(0 ~ 12周)。微聚焦x射线计算机断层扫描(MFXCT)扫描设备用于可视化包装测试样品的微观结构。对于每个测试样品,测量了气体扩散系数(Dp/Do)、空气渗透性(ka)、导热系数(λ)和体积热容(C)的质量传递参数。结果表明,干密度对GBM CT亮度值影响较大;CT亮度直方图较好地捕捉了密度的内部分布,随着干密度的增大,CT亮度更加均匀化。测得Dp/Do和ka。主要受干密度控制。另一方面,热性能如λ和C都受干密度和相对湿度的控制。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Visualization of microstructure and measurement of mass transport parameters for granulated bentonite mixtures
Bentonite is often considered as one of the key components of the Engineered Barrier System (EBS) for the radioactive waste disposal; mechanical, thermal, and hydraulic behaviors of bentonite should be thoroughly studied to ensure the emplaced the quality and to control the performance of EBS. This study examined the effects of dry density and relative humidity (RH) on microstructure and mass transport characteristics of Granulated Bentonite Mixtures (GBM). The tested GBM samples were prepared by sieving and grading Japanese bentonite (trade name: OK Bentonite, Kunimine Industries, Japan). For dry density-controlled conditions, air-dried GBM samples (RH 60%, water content of 6.38% by weight) were packed at six different dry densities ranging from 1.25 to 1.75 g/cm. The samples for humidity-controlled conditions were prepared at the dry density of 1.45 g/cm and stored at RH 90% (0 to 12 weeks). A microfocus X-ray computerized tomography (MFXCT) scanning apparatus was used to visualize the microstructures of packed tested samples. For each tested sample, the mass transport parameters of gas diffusivity (Dp/Do), air permeability (ka), thermal conductivity (λ), and volumetric heat capacity (C) were measured. The results indicated that dry density greatly affected the CT brightness values of GBM; the histogram of CT brightness well captured the internal distribution of density and the CT brightness homogenized more with increasing in dry density. The measured Dp/Do and ka. were mainly controlled by the dry density. On the other hand, the thermal properties such as λ and C were governed both dry density and RH.
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