粘土中水的层间吸附热力学。I.-Sodium蛭石

H van Olphen
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引用次数: 136

摘要

测定了水蒸汽和高电荷密度蛭石钠在25℃下的吸附-解吸等温线。50°C。在粘土水化的不同阶段获得了x射线图。用量热法测定了干燥粘土和部分水化样品的浸没热。水的吸附似乎分两个不同的步骤进行,与晶格插入一个和两个单分子水层相对应。等温线的形状可以看作是两条朗缪尔型等温线的叠加。观察到的滞后归因于吸附过程的延迟,这是由于水在单位层之间的初始外围渗透期间晶体中弹性应力的发展造成的。在假设脱附等温线代表平衡值的前提下,确定了吸附过程的热力学常数。量热数据表明,在每一层水的形成过程中,每摩尔水的积分吸附热是恒定的,第一层每摩尔水的吸附热大约是第二层的两倍。量热数据与两个温度下的等温线测得的热量之间的一致性在第一阶段是合理的,在第二阶段是良好的。吸附的积分熵相对于液态水的熵是负的。由于系统被视为一个单组分系统(吸附质),计算的积分熵包括由于单位层的分离和层间阳离子位置的变化而导致的固体熵变化。根据等温线,可以计算出单位层相互作用的净功作为单位层距离的函数,并由此推导出挤出水层所需的压力。该网络由水化能本身减去静电势能和范德华单位层引力组成。从吸引能的估计,估计水化能大大小于离子水化能在散装溶液。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Thermodynamics of interlayer adsorption of water in clays. I.—Sodium vermiculite

Adsorption-desorption isotherms for water vapor and a high charge density sodium vermiculite were determined at 25°C. and at 50°C. X-ray patterns were obtained at various stages of hydration of the clay. Heats of immersion were determined calorimetrically for the dry clay and for partially hydrated samples. The adsorption of water appears to take place in two distinct steps corresponding with the intercalation of the lattice with one and with two monomolecular layers of water. The shape of the isotherms can be seen as the superposition of two Langmuir-type isotherms. The observed hysteresis is attributed to a retardation of the adsorption process owing to the development of elastic stresses in the crystallites during the initial peripheral penetration of water between the unit layers. On the assumption that the desorption isotherm represents equilibrium values, the thermodynamic constants for the sorption process were determined.

The calorimetric data suggest that the integral heats of sorption per mole of water are constant during the formation of each layer of water, the heat of sorption for the first layer per mole of water being about twice that for the second layer. Agreement between the calorimetric data and the heats determined from the isotherms at two temperatures is reasonable for the first stage, and good for the second.

The integral entropy of sorption is negative with respect to the entropy of liquid water. Since the system was treated as a one-component system (the adsorbate), the computed integral entropy includes entropy changes in the solid due to the parting of the unit layers and changes in the positions of the interlayer cations.

From the isotherms the net work of unit layer interaction can be computed as a function of unit layer distance, from which the pressures required to squeeze out the water layers are derived. The net work consists of the hydration energy proper minus the potential energy of electrostatic and van der Waals unit layer attraction. From an estimate of the attraction energy, the hydration energy is estimated to be considerably smaller than ion hydration energy in bulk solution.

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