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Colloid deposition onto a solid surface under low-flow conditions in parallel-plate geometry.

机译:胶体在平行板几何形状的低流量条件下沉积到固体表面上。

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The attachment, detachment, and deposition of colloids, 0.33-μm in diameter, at a glass surface of a narrow parallel-plate channel were experimentally investigated. Colloids were suspended in synthetic groundwater, similar to a natural groundwater at the Nevada Test Site. Experiments were conducted at pH 8, ionic strengths of 0.003, 0.025, and 0.05 M and flow rates between 0 and 0.16 ml/hr (average velocities between 0 and 2.8 × 10−3 cm/s). A video microscopic setup and image processing routines were developed to in situ enumerate attached, detached, and deposited colloids, and to track previously occupied locations at the surface. The setup utilized dark field microscopy to visualize colloids with sufficient resolution (0.5 μm) and provided a relatively large field of view (330 x 245 μm) to increase statistical accuracy of extracted data. A “moving window” approach was employed to establish connectivity between successive images captured every 90-s.; Within the range of flow rates employed, colloid deposition at 0.003 M was negligible. At 0.025 M, colloid attachment and detachment exhibited two successive regions with time: an initial nonlinear region and a linear region. At 0.05 M, colloid attachment exhibited similar behavior with time, while the detachment process was persistently linear. Colloid deposition fluxes reached a constant = 0 for no-flow condition, >0 for flow and 0.025 M, and 0 for flow and 0.05 M. The final colloid attachment, and detachment fluxes increased linearly with flow rate and almost exponentially with ionic strength.; Analysis of results suggested that colloid attachment and detachment processes were controlled by continuous activation and deactivation of sites at the glass surface. Results were interpreted based on a two-sites model, in which two types of sites were identified: Sites I, formed during the preconditioning of the glass surface with particle-free solution; and Sites II, formed during the experiments. The concentration of Sites I increased linearly with preconditioning times >17 hours, and with ionic strength. Tracking of previously occupied sites indicated that no attachment occurred later at these sites. Analysis suggested that the deactivation of these sites, which was attributed to glass dissolution, was not caused by, but associated with detached colloids.
机译:实验研究了直径为0.33μm的胶体在狭窄的平行平板通道的玻璃表面上的附着,分离和沉积。胶体悬浮在合成地下水中,类似于内华达州试验场的天然地下水。实验是在pH 8,离子强度为0.003、0.025和0.05 M / italic以及流速为0至0.16 ml / hr(平均速度为0至2.8×10 −3 cm / s)。开发了视频显微镜设置和图像处理例程,以就地枚举附着,分离和沉积的胶体,并跟踪先前在表面上占据的位置。该设置利用暗场显微镜以足够的分辨率(0.5μm)可视化胶体,并提供相对较大的视野(330 x 245μm),以提高提取数据的统计准确性。采用“移动窗口”方法在每90秒捕获的连续图像之间建立连接。在所使用的流速范围内,在0.003 M 处的胶体沉积可以忽略不计。在0.025 M 时,胶体的附着和分离随时间表现出两个连续的区域:一个初始的非线性区域和一个线性区域。在0.05 M 时,胶体附着随时间表现出相似的行为,而分离过程则持续呈线性。胶体沉积通量在无流量条件下达到常数= 0,在流量下> 0,在0.025 M ,在流量下<0,在0.05 M 。最终的胶体附着和分离通量随流速线性增加,而与离子强度成指数关系。结果分析表明,胶体的附着和脱离过程是由玻璃表面部位的连续活化和失活控制的。结果基于两个位点的模型进行解释,其中识别出两种类型的位点:在无颗粒溶液预处理玻璃表面期间形成的 Site I ;和 Sites II ,是在实验过程中形成的。 Sites I 的浓度随着预处理时间> 17小时和离子强度的增加而线性增加。跟踪先前占用的站点表明以后在这些站点上没有附件发生。分析表明,这些位点的失活归因于玻璃溶解,不是由胶体脱落引起的,而是与胶体脱离有关。

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