Xia Yongde, Dosseh Gilberte, Morineau Denis, Alba-Simionesco Christiane
Laboratoire de Chimie Physique, UMR CNRS 8000, Université de Paris Sud, Bâtiment 349, 91405 Orsay Cedex, France.
J Phys Chem B. 2006 Oct 5;110(39):19735-44. doi: 10.1021/jp063393i.
We used differential scanning calorimetry, neutron scattering, and proton NMR to investigate the phase behavior, the structure, and the dynamics of benzene confined in a series of cylindrical mesoporous materials MCM-41 and SBA-15 with pore diameters, d, between 2.4 and 14 nm. With this multitechnique approach, it was possible to determine the structure and, for the first time to our knowledge, the density of confined benzene as a function of temperature and pore size. Under standard cooling rates, benzene partially crystallizes in SBA-15 matrixes (4.7 <or= d <or= 14 nm) but not in MCM-41 (2.4 <or= d <or= 3.5 nm). Structure factors of the confined phases were recorded at different temperatures and compare to those of the bulk. The confined liquid has the same structure as the bulk above the bulk melting point. In SBA-15, the confined crystals are defective and have the same structure as the bulk. In MCM-41, the liquid undergoes a glass transition at low temperature regardless of the cooling rate or the thermal history of the sample. The density as a function of temperature was measured by neutron scattering contrast matching, and the glass transition temperatures were determined from the density versus temperature curves. The pore size dependence of T(g) does not show any evidence of finite size effects. A temperature versus pore diameter phase diagram of confined benzene is proposed combining liquid, supercooled liquid, crystal states, and glassy states. NMR relaxation time measurements showed that the dynamics of the confined liquids are slower than those of the bulk above its melting point. In the partially crystallized samples, the liquid and the crystal have the same relaxation times. The activation energies of reorientation motions in the confined phases, determined from spin lattice relaxation times, are smaller than the bulk ones.
我们使用差示扫描量热法、中子散射和质子核磁共振来研究限制在一系列孔径d在2.4至14纳米之间的圆柱形介孔材料MCM - 41和SBA - 15中的苯的相行为、结构和动力学。通过这种多技术方法,能够确定结构,并且据我们所知,首次确定了受限苯的密度作为温度和孔径的函数。在标准冷却速率下,苯在SBA - 15基质(4.7≤d≤14纳米)中部分结晶,但在MCM - 41(2.4≤d≤3.5纳米)中不结晶。在不同温度下记录受限相的结构因子,并与本体的结构因子进行比较。受限液体在本体熔点以上具有与本体相同的结构。在SBA - 15中,受限晶体是有缺陷的,并且具有与本体相同的结构。在MCM - 41中,无论冷却速率或样品的热历史如何,液体在低温下都会发生玻璃化转变。通过中子散射对比匹配测量密度作为温度的函数,并从密度与温度曲线确定玻璃化转变温度。T(g)对孔径的依赖性没有显示出任何有限尺寸效应的证据。结合液体、过冷液体、晶体状态和玻璃态,提出了受限苯的温度与孔径相图。核磁共振弛豫时间测量表明,受限液体的动力学比其熔点以上本体液体的动力学慢。在部分结晶的样品中,液体和晶体具有相同的弛豫时间。由自旋晶格弛豫时间确定的受限相中重取向运动的活化能小于本体中的活化能。