The reduction of pollution and noise emissions of modern aero engines represents a key concept to meet the requirements of the future air traffic. This requires an improvement in the understanding of combustion noise and its sources, as well as the development of accurate predictive tools. This is the major goal of the current study where the LOTAN network solver and a hybrid CFD/CAA approach are applied on a generic premixed and pressurized combustor to evaluate their capabilities for combustion noise predictions. LOTAN solves the linearized Euler equations (LEE) whereas the hybrid approach consists of RANS mean flow and frequency-domain simulations based on linearized Navier-Stokes equations (LNSE). Both solvers are fed in turn by three different combustion noise source terms which are obtained from the application of a statistical noise model on the RANS simulations and a postprocessing of an incompressible and compressible LES. In this way the influence of the source model and acoustic solver is identified. The numerical results are compared with experimental data. In general good agreement with the experiment is found for both the LOTAN and LNSE solvers. The LES source models deliver better results than the statistical noise model with respect to the amplitude and shape of the heat release spectrum. Beyond this it is demonstrated that the phase relation of the source term does not affect the noise spectrum. Finally, a second simulation based on the inhomogeneous Helmholtz equation indicates the minor importance of the aerodynamic mean flow on the broadband noise spectrum.
NomenclatureA Area, m 2 c Speed of sound, m/s c p , c v Specific isobaric and isochoric heat capacities, J/(kgK) δ f Flame thickness in network model, m f Frequency, Hz F Fourier transformation, 1/Hz h 0 f ,k Enthalpy of formation of k-th species, J/(kgK) η Dynamic viscosity, kg/(m s) H u Lower heating value, J/kg i Imaginary unit k Wave-number, 1/m κ Isentropic exponent l Length, m λ Thermal conductivity, W/(m K) M Mach numbeṙ m Mass flow rate, kg/s n Surface normal p Pressure, N/m 2 φ Arbitrary field quantity * Address all correspondence to this author. GTP-16-1249, Ullrich, page 2 P ± Complex pressure amplitude, N/m 2 q V Volumetric heat release, W/m 3 Q Integral spectrum of fluctuating heat release, W/Hz ρ Density, kg/m 3 s Specific entropy, J/(kgK) s V Volume source, 1/s S V Integral spectrum of the fluctuating volume source, 1/s t Time, s T Temperature, K u Velocity vector, m/s ω Circular frequency, 1/s x Position vector, m Z Reduced (non dimensional) impedance
IntroductionIn the near future the air traffic is expected to increase significantly which makes a further reduction of aircraft noise indispensable. This must address all aircraft components, but particularly the engine, in order to meet strict political requirements such as the ACARE 1 goal prescribing a noise reduction of 50% by 2020. Combustion noise is becoming increasingly important as a major noise source in aircraft. This is partially because advances in the design of a...