Pipich Vitaliy, Kohlbrecher Joachim, Schwahn Dietmar
Jülich Centre for Neutron Science (JCNS) at Heinz Maier-Leibnitz-Zentrum (MLZ), Forschungszentrum Jülich GmbH, Garching D-85747, Germany.
Laboratory for Neutron Scattering, Paul-Scherrer Institute, Villigen CH-5232 PSI, Switzerland.
J Phys Chem B. 2024 May 23;128(20):5072-5082. doi: 10.1021/acs.jpcb.4c01422. Epub 2024 May 15.
The phase behavior of the liquid CD below and above the critical point was investigated using small-angle neutron scattering (SANS) in temperature and pressure ranges from 10 to 45 °C and 20 to 126 bar, respectively. The scattering of thermal fluctuations of the molecular density was determined and thus the gas-liquid and Widom lines. At the same time, we observed additional scattering of droplets of more densely packed CD molecules above the gas-liquid line and in the supercritical fluid regime from just below the critical point for all temperatures at about Δ = 10 bar above the Widom line. This line is interpreted as the Frenkel line. These results are consistent with our previous studies on CO and thus indicate a universal phase behavior for monomolecular liquids below and above the critical point. The interpretation of the Frenkel line as the lower limit of a polymorphic phase transition is in contrast to the usual interpretation as the limit of a dynamic process. The correlation lengths (ξ) of the thermal density fluctuations at the critical point and at the Widom line are determined between 20 and 35 Å and thus in the range of the droplet radius between 60 and 80 Å. These long-range fluctuations appear to suppress the formation of droplets, which can only form at about 10 bar above the critical point and the Widom line when ξ becomes smaller than 10 Å.
分别在温度范围为10至45°C和压力范围为20至126巴的条件下,使用小角中子散射(SANS)研究了临界点以下和以上液体CD的相行为。确定了分子密度热涨落的散射,从而确定了气液线和维德曼线。同时,我们观察到在气液线以上以及在超临界流体区域中,对于所有温度,在高于维德曼线约Δ = 10巴处,存在更密集堆积的CD分子液滴的额外散射。这条线被解释为弗伦克尔线。这些结果与我们之前对CO的研究一致,因此表明了单分子液体在临界点以下和以上的普遍相行为。将弗伦克尔线解释为多晶型相变的下限,这与通常将其解释为动态过程的极限形成对比。确定了临界点和维德曼线处热密度涨落的关联长度(ξ)在20至35 Å之间,因此处于液滴半径在60至80 Å的范围内。这些长程涨落似乎抑制了液滴的形成,液滴只能在高于临界点和维德曼线约10巴处形成,此时ξ小于10 Å。