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Wetting Solution and Electrical Double Layer Contributions to Bulk Electrical Conductivity of Sand–Clay Mixtures

机译:湿溶液和电双层对砂-粘土混合物体电导率的贡献

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8 August 2007. This study investigated the contributions of the wetting liquid and electrical double layers (EDLs) to the bulk electrical conductivity () of sand–clay mixtures. The conductivity is small at small water content due to few conductive pathways and low ionic mobility. The fully expanded state of the EDLs provided the largest in distilled water but not in salt solutions. At small water content, increases following a logarithmic function, but changes linearly at large water content after reaching a transitional large value. This conductivity increases with increasing electrical conductivity of the wetting solution (w) exponentially at small water content, but linearly at large water content. Existing bulk electrical conductivity models described the measured values well and resulted in stable values of the electrical formation factor (F) and dimensionless parameter. Due to considerable leach cations in the clay, the cations in the bulk solution exerted negligible influence on the surface conductivity (s). Although F is independent of w, the confounding effect of shrink–swell in the samples with changing w shows an apparent dependency of F on w. The surface mobility of the counterions decreased nonlinearly with increasing water-filled porosity (), and also with increasing w. The cementation exponent (m) decreased monotonically from –4.4 at = 0.22 to –94.1 at = 0.93 in the samples wetted with distilled water. With increasing w, m also increased. The value of m for three samples wetted with salt solutions of w = 0.878, 1.273, and 1.572 S m–1 ranged from 2.1 to 2.5 at = 0.22 and 4.1 to 5.3 at = 0.93.
机译:2007年8月8日。这项研究调查了润湿液体和双电层(EDL)对砂土混合物的整体电导率()的贡献。由于很少的导电途径和低的离子迁移率,所以在水含量少时,电导率很小。 EDL的完全膨胀状态在蒸馏水中提供了最大的浓度,但在盐溶液中却没有提供。在小水含量下,随对数函数增加,但在大水含量达到过渡大值后线性变化。当水含量低时,此电导率随润湿溶液(w)的电导率成指数增加,而当水含量大时则呈线性增长。现有的整体电导率模型很好地描述了测量值,并获得了稳定的电形成因数(F)和无量纲参数值。由于粘土中大量的浸出阳离子,本体溶液中的阳离子对表面电导率的影响可忽略不计。尽管F与w无关,但是随着w的变化,样品中的收缩-膨胀的混杂效应显示出F对w的明显依赖性。抗衡离子的表面迁移率随充水孔隙率()的增加以及w的增加而非线性降低。在用蒸馏水润湿的样品中,胶结指数(m)从–4.4 at = 0.22单调降低至–94.1 at = 0.93。随着w的增加,m也增加。三个用w = 0.878、1.273和1.572 S m-1的盐溶液润湿的样品的m值范围在2.1到2.5 at = 0.22和4.1到5.3 at 0.93。

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