1993
DOI: 10.1103/physreve.47.388
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Global thermodynamic behavior of fluid mixtures in the critical region

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Cited by 70 publications
(53 citation statements)
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“…20 Subsequently, in the one-component limit A iso → A = (T c /r c P c )A ∼ and we can write: Since the critical parameters T c (ζ), η c (ζ), and P c (ζ) are functions of the field variable ζ while the experimental data for these parameters are available only as functions of the mole fraction x, in order to apply the isomorphic viscosity EoS to the mixtures, the variable x have to be converted into the variable ζ by using Eq. (41).…”
Section: The Isomorphism Principle Of Critical Phenomenamentioning
confidence: 99%
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“…20 Subsequently, in the one-component limit A iso → A = (T c /r c P c )A ∼ and we can write: Since the critical parameters T c (ζ), η c (ζ), and P c (ζ) are functions of the field variable ζ while the experimental data for these parameters are available only as functions of the mole fraction x, in order to apply the isomorphic viscosity EoS to the mixtures, the variable x have to be converted into the variable ζ by using Eq. (41).…”
Section: The Isomorphism Principle Of Critical Phenomenamentioning
confidence: 99%
“…Since along the critical line ζ = x, the quantities T c (ζ), ρ c (ζ), and P c (ζ) can be defined as: In practice, the critical temperature and pressure are characterized by a polynomial form as: 20 Behnejad where M 1 and M 2 are molecular weights of the corresponding components.…”
Section: Applicationsmentioning
confidence: 99%
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