Combustion Noise 2009
DOI: 10.1007/978-3-642-02038-4_8
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Investigations Regarding the Simulation of Wall Noise Interaction and Noise Propagation in Swirled Combustion Chamber Flows

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Cited by 6 publications
(5 citation statements)
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“…The combustion also generates unsteady shear leading to vorticity perturbations [19], which also convect and generate pressure perturbations as they accelerate through the turbine nozzle guide vanes. Hence, at the combustor exit the interaction of the vortical and entropic perturbations with the mean streamwise velocity gradient results in energy transfer to an acoustic mode [19,20]. Acceleration of entropy and vorticity waves in the choked nozzle results in generation of pressure waves that propagate upstream (from where they can be reflected from the flame zone and/or the upstream geometry altering the downstream propagating waves) and downstream from the turbine stage as indirect combustion noise [12,17,18].…”
Section: Motivation: Gas Turbine Combustion Noise Sourcesmentioning
confidence: 99%
“…The combustion also generates unsteady shear leading to vorticity perturbations [19], which also convect and generate pressure perturbations as they accelerate through the turbine nozzle guide vanes. Hence, at the combustor exit the interaction of the vortical and entropic perturbations with the mean streamwise velocity gradient results in energy transfer to an acoustic mode [19,20]. Acceleration of entropy and vorticity waves in the choked nozzle results in generation of pressure waves that propagate upstream (from where they can be reflected from the flame zone and/or the upstream geometry altering the downstream propagating waves) and downstream from the turbine stage as indirect combustion noise [12,17,18].…”
Section: Motivation: Gas Turbine Combustion Noise Sourcesmentioning
confidence: 99%
“…In fact, most of the equations used for CAA modeling can be rearranged in order to include heat release in the acoustic source terms, e.g. in [18,19,20] (see also equation 5).I ti sh owever commonly avoided because the reaction rates of the species, which are principally required to evaluate the heat release rate, are not known (see section 2.3). In this case, as the solution of mass equations for each species may be computationally too expensive,modeling of reaction kinetics in most applications of combustion simulation is forced to use simplifiedorreduced chemistry [21], for example, in frame work of at abulation procedure with the ILDM (Intrinsic Low Dimensional Manifold)o rthe FGM (Flamelet Generated Manifold)approach [22].…”
Section: Introductionmentioning
confidence: 98%
“…Due to its simplicity,L ighthill'sa nalogy as well as its modifications are widely used for combustion noise problem in the last decade [3,9,10,11,12,13]. Recently,o ther more sophisticated methods, such as the Phillips' analogy [14], the Linearized Euler-Equations (LEE) [ 5] and the APE (Acoustic Perturbation Equations)system [15], have been successfully applied for the prediction of combustion noise [16,17,18], which are derivedf rom the governing equations for afl owing fluid as well. The Phillips' analogy is represented by awaveequation for the logarithmic pressure.…”
Section: Introductionmentioning
confidence: 99%
“…Pressure perturbations generated by fluctuation in heat release rate from the turbulent flame constitute the 'direct' acoustic noise. The 'indirect' noise is generated due to the acceleration of entropy and vorticity waves through the turbine blade rows [5][6][7]. Recent studies have shown that the indirect noise due to vorticity gives a negligible contribution to the total noise generated in the aircraft [3].…”
Section: Introductionmentioning
confidence: 99%