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Frequency-dependent streaming potential of Ottawa sand

机译:取决于频率的渥太华砂流潜力

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The scientific literature is almost devoid of frequency-dependent electrokinetic measurements on geological materials. An apparatus that allows the measurement of the streaming potential coupling coefficient of unconsolidated and disaggregated materials such as sands, gravels, and soils has been designed, constructed, and tested. The apparatus, which uses an electromagnetic drive, operates in the range 1 Hz to 1 kHz and has a 25.4 mm diameter sample chamber for samples up to 150 mm long. We have made streaming potential coupling coefficient measurements on samples of Ottawa sand as a function of frequency. The results have been analyzed using critically and variably damped second-order vibrational mechanics models as well as the theoretical models of Packard for capillary tubes and Pride for porous media. The best fit was provided by an underdamped second-order model with a damping factor of 0.8561 (R = 0.993). Transition frequencies were derived from the two vibrational models and the Pride model either by fitting the model to the data or directly from the model, giving 230, 273, and 256.58 Hz, respectively. These values are in good agreement with the transition frequency expected for a sand with an independently obtained effective pore radius of 6.76 x th~(-5) m from laser diffraction grain size measurements. The Packard model also agrees extremely well with the experimental data (R~2 = 0.987) directly providing a value of the equivalent capillary radius of 6.75 x 10~(-5) m that coincides within experimental errors with the independently obtained effective pore radius measurements.
机译:科学文献几乎没有对地质材料进行频率相关的电动测量。已经设计,构造和测试了一种设备,该设备可以测量未固结和分解的物料(例如沙子,砾石和土壤)的流动电位耦合系数。该设备使用电磁驱动器,工作频率范围为1 Hz至1 kHz,并具有25.4 mm直径的样品室,可容纳150 mm长的样品。我们已经对渥太华砂样品的流电势耦合系数进行了测量,作为频率的函数。使用临界和可变阻尼的二阶振动力学模型以及毛细管的Packard和多孔介质的Pride的理论模型对结果进行了分析。阻尼系数为0.8561(R = 0.993)的欠阻尼二阶模型提供了最佳拟合。通过将模型拟合到数据或直接从模型中分别从两个振动模型和Pride模型获得过渡频率,分别给出230、273和256.58 Hz。这些值与通过激光衍射粒度测量独立获得的有效孔径为6.76 x th〜(-5)m的砂子的预期转变频率非常吻合。 Packard模型也与实验数据非常吻合(R〜2 = 0.987),直接提供了等效毛细管半径的值6.75 x 10〜(-5)m,与独立获得的有效孔径半径测量值在实验误差范围内一致。

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