SGH-P730 schematics

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It is this feature that provides the information needed for extrapolating the isotherm to much higher compressions. The eXp-6 potential has been characterized as an effective pair-potential because it includes in a phenomenological fashion the effects of the many-body interactions While retaining the convenient features of a two-body function. For this reason it is of interest to compare the present results to those for a purely two-body potential. 2), with the two-body potential of Aziz and Chen 24 (HFD-C, their designation) Which they obtained by fitting to second virial coefficients, gas phase transport data and to Hartree-Fock atom-atom calculations at small interatomic separations.

And A. C. Mitchell. J. Chem. Phys. 73. 6137. 1980. M. Van Thiel, M. J. Shaner, and E. Salinas, Lawrence Livermore National Laboratory Report UCRL 50108, Vols. 1-3. Rev. 1. 1977. S. P. Marsh. LASL Shock Data. (Berkeley: University of California Press. 1980). L. V. AI'tsbuler, A. A. Bakanova. I. P. Dudoladov. E. A. Dynin. R. F. Trunin. and B. A. Chekin. J. Appl. Mech. Tech. Phys. 22. 145. 1981. V. Y. Klimenko and A. N. Dremin, in Detonatsiya. Chernogolovka. edited by O. N. Breusov et al. (Akad. Nauk.

5) 36 M. 28 r )2] [ - ( ~-1 , r 5. 7) attenuates the long-range multipole terms at small r. The factor rm is the position of the attractive minimum of p(r). The SG potential has been found to reproduce both the melting properties and the static compression data of liquid H2 and D2 at 75-300 K to 2 GPa. However, it becomes less suitable to explain the high pressure static and the dynamic data. 8) + constant, The first term is due to the kinetic energies of translation and rotation; the second term, within the bracket, represents the free energy of a vibrating molecule with frequency hv/k = 6340 K and 4395 K for H2 and D2' respectively.

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