scholarly journals Supercritical water: Local order and molecular dynamics

2004 ◽  
Vol 76 (1) ◽  
pp. 133-139 ◽  
Author(s):  
T. Tassaing ◽  
Y. Danten ◽  
M. Besnard

This paper is a study of the structure and dynamics of near-critical and supercritical water for thermodynamic states above the critical temperature in a wide range of density by infrared absorption and quasi-elastic neutron scattering. The evolution of the shape of the infrared profiles associated with the internal vibrational modes of water has been investigated. In supercritical water, at T = 380 °C and low pressure (density), in the range 25-50 bar (0.01-0.05 g·cm-3), only monomers are detected. A progressive increase of the pressure (density) from 50 to 250 bar (from 0.05 to 0.4 g·cm-3) leads to the appearance of dimers and trimers. In order to obtain information on the dynamics, we have performed incoherent quasi-elastic neutron-scattering experiments on light water for several thermodynamic states (200 < T < 400 °C and 184 < P < 400 bar) corresponding to densities ranging from 0.2 to 0.9 g·cm-3. The results have been analyzed using a jump diffusion model and the two parameters of this model, namely, τ0, the residence time and D, the translational diffusion coefficient, have been determined as a function of the density.

Author(s):  
Santhosh K. Matam ◽  
C. Richard A. Catlow ◽  
Ian P. Silverwood ◽  
Alexander J. O’Malley

AbstractMethanol dynamics in zeolite H-ZSM-5 (Si/Al of 25) with a methanol loading of ~ 30 molecules per unit cell has been studied at 298, 323, 348 and 373 K by incoherent quasi-elastic neutron scattering (QENS). The elastic incoherent structure factor (EISF) reveals that the majority of methanol is immobile, in the range between 70 and 80%, depending on the measurement temperature. At 298 K, ≈ 20% methanol is mobile on the instrumental timescale, exhibiting isotropic rotational dynamics with a rotational diffusion coefficient (DR) of 4.75 × 1010 s−1. Upon increasing the measurement temperature from 298 to 323 K, the nature of the methanol dynamics changes from rotational to translational diffusion dynamics. Similar translational diffusion rates are measured at 348 and 373 K, though with a larger mobile fraction as temperature increases. The translational diffusion is characterised as jump diffusion confined to a sphere with a radius close to that of a ZSM-5 channel. The diffusion coefficients may be calculated using either the Volino–Dianoux (VD) model of diffusion confined to a sphere, or the Chudley–Elliot (CE) jump diffusion model. The VD model gives rise to a self-diffusion co-efficient (Ds) of methanol in the range of 7.8–8.4 × 10–10 m2 s−1. The CE model gives a Ds of around 1.2 (± 0.1) × 10–9 m2 s−1 with a jump distance of 2.8 (either + 0.15 or − 0.1) Å and a residence time (τ) of ~ 10.8 (either + 0.1 or − 0.2) ps. A correlation between the present and earlier studies that report methanol dynamics in H-ZSM-5 with Si/Al of 36 is made, suggesting that with increasing Si/Al ratio, the mobile fraction of methanol increases while DR decreases.


1995 ◽  
Vol 73 (11-12) ◽  
pp. 687-696 ◽  
Author(s):  
Myer Bloom ◽  
Thomas M. Bayerl

After reviewing some of the basic measurements that characterize the study of physical properties of matter using neutron scattering and nuclear magnetic resonance (NMR), connections between information obtained in current research on fluid membranes using these two complementary techniques are explored in two major chapters. In the first, the type of information on the structure of fluid membranes obtained from coherent elastic neutron scattering is compared with that from NMR spectral characteristics. Then, the type of information obtained on dynamical properties from NMR relaxation (T1 and T2) measurements is compared with that from quasi-elastic neutron scattering. Examples of such connections are given with an emphasis on relationships between the time and distance scales intrinsic to neutron scattering and NMR.


1987 ◽  
Vol 55 (2) ◽  
pp. 183-201 ◽  
Author(s):  
W. Petry ◽  
G. Vogl ◽  
A. Heidemann ◽  
K.-H. Steinmetz

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