2009
DOI: 10.1088/1742-6596/180/1/012035
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Massively parallel LES of azimuthal thermo-acoustic instabilities in annular gas turbines

Abstract: Massively parallel LES of azimuthal thermo-acoustic instabilities in annular gas turbines Abstract. Most of the energy produced worldwide comes from the combustion of fossil fuels. In the context of global climate changes and dramatically decreasing resources, there is a critical need for optimizing the process of burning, especially in the field of gas turbines. Unfortunately, new designs for efficient combustion are prone to destructive thermo-acoustic instabilities. Large Eddy Simulation (LES) is a promisin… Show more

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Cited by 27 publications
(36 citation statements)
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“…The flow rate fluctuations control the flame response and the heat release perturbation. Further analysis [38,40] show that all burners react in the same way to this flow rate fluctuation: the azimuthal instability coincides with a mode which is driven by the azimuthal shape of the annular chamber but it is also connected to purely longitudinal oscillations in each sector. The flow rate oscillations in each burner induces an unsteady reaction rate which then feeds the azimuthal mode.…”
Section: T Tmeanmentioning
confidence: 93%
“…The flow rate fluctuations control the flame response and the heat release perturbation. Further analysis [38,40] show that all burners react in the same way to this flow rate fluctuation: the azimuthal instability coincides with a mode which is driven by the azimuthal shape of the annular chamber but it is also connected to purely longitudinal oscillations in each sector. The flow rate oscillations in each burner induces an unsteady reaction rate which then feeds the azimuthal mode.…”
Section: T Tmeanmentioning
confidence: 93%
“…In the field of simulation, most models [7][8][9][10][11] assume adiabatic flows. For premixed flames, the famous BML (Bray Moss Libby) approach, for example, which is the workhorse of many theories for turbulent premixed flames [12,13] assumes that a single variable (the progress variable c ) is sufficient to describe the flow: this is true only when the flow is adiabatic.…”
Section: Introductionmentioning
confidence: 99%
“…AVBP is a parallel CFD code that solves the laminar and turbulent compressible Navier-Stokes equations in two and three space dimensions on unstructured and hybrid grids. Originally devoted to the computation of reactive flows in combustors (see for example Wolf et al [25] and Boileau et al [3]), AVBP has also been extensively validated in the case of pure aerodynamics by Prière et al [20] and Mendez and Nicoud [13].…”
Section: Numerical Set-upmentioning
confidence: 99%