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2011
DOI: 10.1134/s2070048211060032
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Nonstationary nonisothermal flow of gas mix in offshore gas pipelines

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Cited by 2 publications
(3 citation statements)
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“…One of rather general mathematical models of the above-mentioned processes is the VBVK (Vasil'ev-Boldyrev-Voevodin-Kanibolotsky) model published in 1978 in [5], and up to now this model is often in use [6,7,8]. Our mathematical model developed in [1,3] mainly differs from the VBVK model in the description of thermodynamic processes, while in both models the presentations of continuity equation (mass conservation), equation of motion (or momentum equation), and energy equation (law of conservation of energy) coincide with an accuracy of up to symbols:…”
Section: General Modelmentioning
confidence: 99%
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“…One of rather general mathematical models of the above-mentioned processes is the VBVK (Vasil'ev-Boldyrev-Voevodin-Kanibolotsky) model published in 1978 in [5], and up to now this model is often in use [6,7,8]. Our mathematical model developed in [1,3] mainly differs from the VBVK model in the description of thermodynamic processes, while in both models the presentations of continuity equation (mass conservation), equation of motion (or momentum equation), and energy equation (law of conservation of energy) coincide with an accuracy of up to symbols:…”
Section: General Modelmentioning
confidence: 99%
“…By now, a vast number of such analytical forms has been proposed, but the most known ones are the Redlich-Kwong, Soave, Peng-Robinson, Benedict-Webb-Rubin equations of state [7,11,13]. In our works [1,3] as well as in [4,7] the two-parameter Redlich-Kwong equation of state is used, for this equation is considered one of the best which works in a wide range of variations of p, ρ and T, including hyperpressure range. For a gas mixture it can be written as [13]: In the second approach, caloric equation is written in terms of internal energy ε(T,V), and the balance equation of internal energy Eq.…”
Section: Modeling Of Thermodynamic Processesmentioning
confidence: 99%
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