González Sánchez Fátima, Jurányi Fanni, Gimmi Thomas, Van Loon Luc, Unruh Tobias, Diamond Larryn W
Laboratory for Waste Management, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
J Chem Phys. 2008 Nov 7;129(17):174706. doi: 10.1063/1.3000638.
The water diffusion in four different, highly compacted clays [montmorillonite in the Na- and Ca-forms, illite in the Na- and Ca-forms, kaolinite, and pyrophyllite (bulk dry density rho(b)=1.85+/-0.05 gcm(3))] was studied at the atomic level by means of quasielastic neutron scattering. The experiments were performed on two time-of-flight spectrometers and at three different energy resolutions [FOCUS at SINQ, PSI (3.65 and 5.75 A), and TOFTOF at FRM II (10 A)] for reliable data analysis and at temperatures between 27 and 95 degrees C. Two different jump diffusion models were used to describe the translational motion. Both models describe the data equally well and give the following ranking of diffusion coefficients: Na-montmorillonite<or=Ca-montmorillonite<Ca-illite<Na-illite<water<or=pyrophyllite<or=kaolinite. Uncharged clays had slightly larger diffusion coefficients than that of bulk water due to their hydrophobic surfaces. The time between jumps, tau(t), follows the sequence: Ca-montmorillonite>or=Na-montmorillonite>Ca-illite>Na-illite>or=kaolinite>pyrophyllite>or=water, in both jump diffusion models. For clays with a permanent layer charge (montmorillonite and illite) a reduction in the water content by a factor of 2 resulted in a decrease in the self-diffusion coefficients and an increase in the time between jumps as compared to the full saturation. The uncharged clay kaolinite exhibited no change in the water mobility between the two hydration states. The rotational relaxation time of water was affected by the charged clay surfaces, especially in the case of montmorillonite; the uncharged clays presented a waterlike behavior. The activation energies for translational diffusion were calculated from the Arrhenius law, which adequately describes the systems in the studied temperature range. Na- and Ca-montmorillonite (approximately 11-12 kJmol), Na-illite (approximately 13 kJmol), kaolinite and pyrophyllite (approximately 14 kJmol), and Ca-illite (approximately 15 kJmol) all had lower activation energies than bulk water (approximately 17 kJmol in this study). This may originate from the reduced number and strength of the H-bonds between water and the clay surfaces, or ions, as compared to those in bulk water. Our comparative study suggests that the compensating cations in swelling clays have only a minor effect on the water diffusion rates at these high densities, whereas these cations influence the water motion in non-swelling clays.
通过准弹性中子散射在原子水平上研究了四种不同的高度压实粘土(钠型和钙型蒙脱石、钠型和钙型伊利石、高岭土和叶蜡石,堆积干密度ρ(b)=1.85±0.05 g/cm³)中的水扩散。实验在两台飞行时间光谱仪上进行,并且在三种不同的能量分辨率下(瑞士保罗谢勒研究所SINQ的FOCUS,3.65 Å和5.75 Å;德国慕尼黑工业大学FRM II的TOFTOF,10 Å)进行,以进行可靠的数据分析,实验温度范围为27至95摄氏度。使用两种不同的跳跃扩散模型来描述平移运动。两种模型对数据的描述同样良好,并给出了以下扩散系数排名:钠蒙脱石≤钙蒙脱石<钙伊利石<钠伊利石<水≤叶蜡石≤高岭土。由于其疏水表面,不带电荷的粘土的扩散系数略大于本体水的扩散系数。在两种跳跃扩散模型中,跳跃之间的时间τ(t)遵循以下顺序:钙蒙脱石≥钠蒙脱石>钙伊利石>钠伊利石≥高岭土>叶蜡石≥水。对于具有永久层电荷的粘土(蒙脱石和伊利石),与完全饱和相比,含水量降低2倍会导致自扩散系数降低,跳跃之间的时间增加。不带电荷的粘土高岭土在两种水合状态之间的水迁移率没有变化。水的旋转弛豫时间受带电荷的粘土表面影响,特别是在蒙脱石的情况下;不带电荷的粘土表现出类似水的行为。根据阿仑尼乌斯定律计算平移扩散的活化能,该定律在研究的温度范围内充分描述了这些系统。钠型和钙型蒙脱石(约11 - 12 kJ/mol)、钠型伊利石(约13 kJ/mol)、高岭土和叶蜡石(约14 kJ/mol)以及钙型伊利石(约15 kJ/mol)的活化能均低于本体水(本研究中约17 kJ/mol)。这可能源于与本体水中相比,水与粘土表面或离子之间氢键的数量和强度减少。我们的比较研究表明,在这些高密度下,膨胀粘土中的补偿阳离子对水扩散速率的影响较小,而这些阳离子会影响非膨胀粘土中的水运动。