1996
DOI: 10.1088/0953-4075/29/19/014
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The isotropic temperature-dependent potential describing the binary interactions in gaseous and

Abstract: The parameters of the temperature-dependent isotropic potentials of binary - and - interactions are obtained from the experimentally measured second virial coefficient B and viscosity of these gases. The parameters of the ground state (equilibrium distance and the potential depth well at , together with the repulsive parameter n and the temperature dependence ) are defined and can be used to calculate any potential-dependent property of the two gases. The measured viscosities of the - and - mixtures… Show more

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Cited by 10 publications
(4 citation statements)
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“…12 It was introduced in order to speed up the calculations for heavy molecules ͑UF 6 , 23 WF 6 , 23,24 MoF 6 23,24 ͒ and mixtures of different globular molecules. 31 It permits us to obviate some theoretical difficulties bound to the calculation of the viscosity of the considered globular gas as a mixture of different vibrationally excited states.…”
Section: Isotropic Temperature-dependentmentioning
confidence: 99%
“…12 It was introduced in order to speed up the calculations for heavy molecules ͑UF 6 , 23 WF 6 , 23,24 MoF 6 23,24 ͒ and mixtures of different globular molecules. 31 It permits us to obviate some theoretical difficulties bound to the calculation of the viscosity of the considered globular gas as a mixture of different vibrationally excited states.…”
Section: Isotropic Temperature-dependentmentioning
confidence: 99%
“…The model and procedure of obtaining potential parameters are described in detail elsewhere (see for example Zarkova 1996, Zarkova andPirgov 1995). We used in the calculations of B and η a four-parameter (n − 6) Lennard-Jones potential with temperature-dependent equilibrium distance r (eff) m and potential-well depth ε (eff) V…”
Section: General Considerationmentioning
confidence: 99%
“…As expected, such a potential is applicable only for the calculation of properties of the same type. Progress was achieved recently in developing more complicated models for simultaneous fits of the transport and equilibrium data for SF 6 (Boushehri et al 1987, Aziz et al 1991, Zarkova 1996, CF 4 (Boushehri et al 1987, Stefanov 1992, Zarkova 1996, UF 6 (Zarkova and Pirgov 1995), WF 6 and MoF 6 (Zarkova and Pirgov 1996) and CCl 4 (Zarkova et al 1997).…”
Section: Introductionmentioning
confidence: 99%
“…The binary interactions are described by means of an effective isotropic potential with temperature-dependent parameters (Zarkova 1996). This model has already been applied with success for pure heavy globular gases (CF 4 and SF 6 , Zarkova 1996; UF 6 , Zarkova and Pirgov 1995;WF 6 and MoF 6 , Zarkova and Pirgov 1996). Recently, the investigation of the collision-induced light scattering (CILS) spectra of CF 4 -CF 4 and SF 6 -SF 6 (Meinander 1993) has shown that no available isotropic potentials can simultaneously reproduce the viscosity, the second virial coefficient and the spectroscopic data.…”
Section: Introductionmentioning
confidence: 99%