Frost RL, Kristof J, Paroz GN, Kloprogge JT
Centre for Instrumental and Developmental Chemistry, Queensland University of Technology, 2 George Street, Brisbane, Queensland, 4001, Australia
J Colloid Interface Sci. 1998 Dec 1;208(1):216-225. doi: 10.1006/jcis.1998.5780.
A low-defect kaolinite of 7.18-Å basal spacing was expanded upon intercalation with hydrazine. The 001 d-spacing was broad and the peak resolved into components at 10.28, 9.48, and 8.80 Å. It was found that the ordered kaolinite predominantly expanded to 9.48 Å with 31.2% and 10.28 Å with 38.0% of the total peak area. A high-defect kaolinite showed expansion by hydrazine in identical steps with d-spacings of 10.27, 9.53, and 8.75 Å. It is proposed that the intercalation of the kaolinite by hydrazine occurs according to the orientation of the hydrazine molecule and that water plays an integral part in the process of kaolinite expansion. For the hydrazine-intercalated kaolinite, hydroxyl stretching bands attributed to water are observed at 3413, 3469, and 3599 cm-1 for the low-defect kaolinite and at 3600 and 3555 cm-1 for the high-defect kaolinite. Upon the exposure of the low-defect hydrazine-intercalated kaolinite to air, an additional water band is observed at 3555 cm-1. Water bending modes are observed at 1578, 1598, 1612, 1627, 1650, and 1679 cm-1 for the hydrazine-intercalated low-defect kaolinite and at 1578, 1598, 1613, 1627, 1652, and 1678 cm-1 for the hydrazine-intercalated high-defect kaolinite. The intensities of these bands are a function of the exposure to air and measurement time. The 1650- and 1679 cm-1 bands increased in intensity as the intensity of the 1612 cm-1 band decreased. Even after exposure to air for 24 h, water remained in the kaolinite interlayer space and only after heating was the water removed. The 1578, 1598, and 1612 cm-1 bands as well as the 1627 cm-1 band are attributed to (a) free or non-hydrogen-bonded water held in the interlayer spaces of the kaolinite, (b) water in the hydration spheres of the hydrazine, and (c) adsorbed water on the kaolinite surface. In kaolinites additional bands at 1650 and 1679 cm-1 are attributed to water coordinated to the siloxane surface. Copyright 1998 Academic Press.
一种基面间距为7.18 Å的低缺陷高岭石在与肼插层时发生膨胀。其001 d间距变宽,峰在10.28、9.48和8.80 Å处分解为多个组分。发现有序高岭石主要膨胀至9.48 Å,占总峰面积的31.2%,以及10.28 Å,占总峰面积的38.0%。一种高缺陷高岭石在肼作用下以相同步骤膨胀,d间距为10.27、9.53和8.75 Å。有人提出,肼对高岭石的插层是根据肼分子的取向发生的,并且水在高岭石膨胀过程中起着不可或缺的作用。对于肼插层的高岭石,低缺陷高岭石在3413、3469和3599 cm-1处观察到归因于水的羟基伸缩带,高缺陷高岭石在3600和3555 cm-1处观察到。将低缺陷肼插层高岭石暴露于空气中后,在3555 cm-1处观察到一个额外的水带。对于肼插层的低缺陷高岭石,在1578、1598、1612、1627、1650和1679 cm-1处观察到水弯曲模式,对于肼插层的高缺陷高岭石,在1578、1598、1613、1627, 1652和1678 cm-1处观察到。这些带的强度是暴露于空气和测量时间的函数。随着1612 cm-1带的强度降低,1650和1679 cm-1带的强度增加。即使在暴露于空气24小时后,水仍保留在高岭石层间空间中,只有在加热后水才被去除。1578、1598和1612 cm-1带以及1627 cm-1带归因于:(a) 存在于高岭石层间空间中的游离或非氢键结合水,(b) 肼水合球中的水,以及(c) 高岭石表面吸附的水。在高岭石中,1650和1679 cm-1处的额外带归因于与硅氧烷表面配位的水。版权所有1998年学术出版社。