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Fluid hydrogen

Various equations of state have been developed to treat association ia supercritical fluids. Two of the most often used are the statistical association fluid theory (SAET) (60,61) and the lattice fluid hydrogen bonding model (LEHB) (62). These models iaclude parameters that describe the enthalpy and entropy of association. The most detailed description of association ia supercritical water has been obtained usiag molecular dynamics and Monte Carlo computer simulations (63), but this requires much larger amounts of computer time (64—66). [Pg.225]

Wang, Q. Johnson, J. K. Broughton, J. Q., Thermodynamic properties and phase equilibrium of fluid hydrogen from path integral simulations, Mol. Phys. 1996, 89, 1105-1119... [Pg.32]

P. G. Jessop, Y. Hsiao, T. Ikariya, R. Noyori, Homogeneous Catalysis in Supercritical Fluids Hydrogenation of Supercritical Carbon Dioxide to Formic Acid, Alkyl Formates, and Formamides ,J. Am Chem Soc 1996,118, 344-355. [Pg.25]

Heterogeneously catalyzed hydrogenation reactions can be run in batch, semibatch, or continous reactors. Our catalytic studies, which were carried out in liquid, near-critical, or supercritical C02 and/or propane mixtures, were run continuously in oil-heated (200 °C, 20.0 MPa) or electrically heated flow reactors (400 °C, 40.0 MPa) using supported precious-metal fixed-bed catalysts. The laboratory-scale apparatus for catalytic reactions in supercritical fluids is shown in Figure 14.2. This laboratory-scale apparatus can perform in situ countercurrent extraction prior to the hydrogenation step in order to purify the raw materials employed in our experiments. Typically, the following reaction conditions were used in our supercritical fluid hydrogenation experiments catalyst volume, 2-30 mL total pressure, 2.5-20.0 MPa reactor temperature, 40-190 °C carbon dioxide flow, 50-200 L/h ... [Pg.230]

The forces leading to microstructure formation in complex fluids are relatively few Excluded-volume, van der Waals, and electrostatic forces are the main ones. In some fluids, hydrogen bonding, hydrophobic, or various solvation forces are also important. Simplified theories can account for the effects of these forces on fluid structure and, to some extent, on relaxation rates. [Pg.96]

K. Delaney, C. Pierleoni and D.M. Ceperley (2006) Quantum Monte Carlo Simulation of the High-Pressure Molecular-Atomic Transition in Fluid Hydrogen. cond-mat/0603750, submitted to Phys. Rev. Letts.,... [Pg.684]

Jessop, P.G. Hsiao, Y. Ikariya, T. Noyori, R. Homogeneous catalysis in supercritical fluids hydrogenation of supercritical carbon dioxide to formic acid, alkyl formates, and formamides. J. Am. Chem. Soc. 1996, 118 (2), 344-55. [Pg.1346]

It has recently become more widely appreciated that the presence of rotational diffusional anisotropy in proteins and other macromolecules can have a significant affect on the interpretation of NMR relaxation data in terms of molecular motion. Andrec et al. used a Bayesian statistical method for the detection and quantification of rotational diffusion anisotropy from NMR relaxation data. Sturz and Dolle examined the reorientational motion of toluene in neat liquid by using relaxation measurements. The relaxation rates were analyzed by rotational diffusion models. Chen et al measured self-diffusion coefficients for fluid hydrogen and fluid deuterium at pressures up to 200 MPa and in the temperature range 171-372 K by the spin echo method. The diffusion coefficients D were described by the rough sphere (RHS) model invoking the rotation translational coupling parameter A = 1. [Pg.210]

According to our approach, known in the literature as the LFHB (lattice fluid hydrogen bonding) approach, the system partition function can be factored into a physical and a chemical or hydrogen bonding term ... [Pg.16]

This volume begins with a chapter on modem cluster methods in equilibrium statistical mechanics and shows how topological reduction can be used to renormalize bonds. A general discussion of renormalization methods is given and the formalism is applied to the study of polar gases, ionic solutions, perturbation theory of fluids, hydrogen-bonded fluids, and integral equations. [Pg.248]

Takishima, S., O Neill, M. L. and Johnston, K. P. (1997) Solubility of Block Copolymer Surfactants in Compressed C02 Using a Lattice Fluid Hydrogen Bonding Model, Ind. Eng. Chem.Res. 36,2821-2833. [Pg.225]

Weir et al. (1996) measured the electrical conductivity of their hydrogen sample in situ using electrodes inserted through the walls of the cell, flush with the fluid hydrogen-sapphire interface. The conductivity rises continuously over five orders of magnitude with pressure increasing from... [Pg.107]

Mbar to 1.8 Mbar. When we compare the conductivity versus density curves of hydrogen with those obtained for rubidium and cesium at comparable temperatures in Fig. 3.22, it is clear that all three elements undergo a density-induced transition to a highly conducting state (o-(O) 2000 fl cm ). But the density at which this occurs for fluid hydrogen is about 100 times that required for rubidium and cesium. [Pg.108]


See other pages where Fluid hydrogen is mentioned: [Pg.1957]    [Pg.1960]    [Pg.554]    [Pg.46]    [Pg.554]    [Pg.799]    [Pg.237]    [Pg.239]    [Pg.152]    [Pg.13]    [Pg.649]    [Pg.490]    [Pg.2059]    [Pg.71]    [Pg.46]    [Pg.216]    [Pg.93]    [Pg.838]    [Pg.89]    [Pg.93]    [Pg.239]    [Pg.1957]    [Pg.1960]    [Pg.264]    [Pg.919]    [Pg.92]    [Pg.213]    [Pg.324]    [Pg.1543]    [Pg.2033]    [Pg.107]    [Pg.109]   
See also in sourсe #XX -- [ Pg.133 , Pg.135 ]




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