2005
DOI: 10.1115/1.1852491
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Validation of a 3D RANS Solver With a State Equation of Thermally Perfect and Calorically Imperfect Gas on a Multi-Stage Low-Pressure Steam Turbine Flow

Abstract: A state equation of thermally perfect and calorically imperfect gas is implemented in a 3D RANS solver for turbomachinery flow applications. The specific heats are assumed as linear functions of temperature. The model is validated on a five-stage low-pressure steam turbine. The computational results exhibit the process of expansion in the turbine. The computed and measured distributions of flow parameters in axial gaps downstream of subsequent turbine stages are found to agree reasonably well. It is also shown… Show more

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Cited by 13 publications
(14 citation statements)
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“…The initial data for modeling regenerative extractions and labyrinth seal flows were determined earlier in [14] using a one-dimensional approach. They are included in Table 1 …”
Section: Computational Resultsmentioning
confidence: 99%
“…The initial data for modeling regenerative extractions and labyrinth seal flows were determined earlier in [14] using a one-dimensional approach. They are included in Table 1 …”
Section: Computational Resultsmentioning
confidence: 99%
“…Flow computations are made with the help of a code IPMFlow [5,6], which draws on the following mathematical models: Reynolds (Favre) averaging of Navier-Stokes equations, SST turbulence model of Menter, implicit quasi-monotonous high-order ENO scheme. The results of computations obtained from the code IPMFlow provide flow details and global characteristics of turbine blading systems [7,8].…”
Section: Methods For Solving 3d Flowmentioning
confidence: 99%
“…The results of these studies were, as a rule, in more than good agreement with the measurement data recorded on both model turbines and real turbosets in operation in Polish power plants. It is noteworthy that this good agreement referred not only to overall turbine performance parameters such as efficiency, mass flow rate, etc, but also to local distributions of flow parameters such as pressures, velocities and flow angles [7][8]. As far as unsteady vortex interactions are concerned, direct code validation was not performed due to the lack of relevant reference data.…”
Section: Fig 1 Turbine Stage Geometrymentioning
confidence: 99%
“…The rotor wake (8), this time located on the left-hand side of the each figure, is accompanied by a number of additional vortices in its lower part, a possible effect of the rotor passage vortex breakdown. The lower part of the passage vortex (5), which in plane z/c = 0.9 was a single structure, now has a form of a vortex pair, t/T = 3/8 ÷ 4/8.…”
Section: Fig 12 Passage Vortex Formation In the Les Rotor In Steadymentioning
confidence: 99%