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Density Profile Decomposition

Yoshimura et al. [23] measured the V-P curve of ice firstly using the in situ high-pressure and low-temperature synchrotron X-ray diffraction and Raman spectroscopy. Numerical match of calculations to measurements of ice-VIII V-P curves [23] in Fig. 34.2b gives rise to the equation of state V/Vq — P with Vo = 1-06 cm /kg. Numerical simultaneous reproduction of both the V/Vq — P and the djdxo — P profiles means that the latter decomposes the former with high reliability [31]. [Pg.692]

MD results show the general trend of pressure-induced 0 H shortening and H-O lengthening. An extrapolation of the MD-derived polynomial expressions leads to the proton symmetrization occurring at 58.6 GPa with the 0-0 distance of 0.221 nm, which is in good accordance with measurements of 59 GPa and 0.220 nm [10]. Therefore, it is confirmed that the proton symmetrization arises from the pressure-induced asymmetric segmental relaxation. [Pg.694]


The isotropic pair potential 4>s r) does not depend on any orientations. Hence it is possible to apply a conventional perturbative decomposition as proposed for instance by Weeks et.al (WCA) [15] or Barker et.al (BH) [16]. Now the isotropic part (11) can be integrated without any effort along the orientations Wi and W2. That way the considerations arrive at the mean field term which only depends on the particle density profile, Fs[p] s nM],... [Pg.103]

SAFETY PROFILE Human poison by unspecified route. Human systemic effects by ingestion nerve or sheath structural changes, extra-ocular muscle changes, sweating, and other effects. Flammable in the form of dust when exposed to heat or flame. Violent reaction with F2. When heated to decomposition it emits toxic fumes of Tl. Used as a rodenticide and fungicide, and in lenses and prisms, in high-density liquids, See also THALLIUM COMPOUNDS and POWDERED METALS. [Pg.1327]

Abstract Recent advances in molecular modeling provide significant insight into electrolyte electrochemical and transport properties. The first part of the chapter discusses applications of quantum chemistry methods to determine electrolyte oxidative stability and oxidation-induced decomposition reactions. A link between the oxidation stability of model electrolyte clusters and the kinetics of oxidation reactions is established and compared with the results of linear sweep voltammetry measurements. The second part of the chapter focuses on applying molecular dynamics (MD) simulations and density functional theory to predict the structural and transport properties of liquid electrolytes and solid elecfiolyte interphase (SEI) model compounds the free energy profiles for Uthium desolvation from electrolytes and the behavior of electrolytes at charged electrodes and the electrolyte-SEl interface. [Pg.371]

A typical sequence of pressure profiles for the initiation of nitromethane is shown in Figure 3.6. The shock travels into the explosive shock heating occurs and results in chemical decomposition. Explosion occurs at the rear boundary, and a detonation develops with the C-J pressure and velocity characteristic of the explosive at the shocked pressure and density. Because these pressures and velocities are often much larger than the explosive normal maximum C-J performance, these detonations in the shocked explosive are called super detonations. The detonation wave overtakes the shock wave and then decays to the normal density C-J pressure and velocity. An animation of the shock initiation of nitromethane is on the CD-ROM in the /MOVIE/NM.MVE directory and in the PowerPoint HOMO.PPT in the /CLASS.PPT/CHAPT3 directory. [Pg.155]

We now have a set of equations which allow us to solve for the temperature profile through a laminate using known values of heat capacity, density, thermal conductivity and the heats of decomposition and combustion of the resin and pyrolysis products respectively. However it remains to establish a proper model for the movement of gas formed within the laminate to the surface and into the headspace above the laminate, a problem which is concerned with the hydrodynamics of the molten laminate. To do this we use an expression of the form of equation 14.11, proposed by Staggs et al. [8] ... [Pg.346]


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Density profiles

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