Noise prediction for a turbulent jet using different hybrid methods

Abstract The acoustic field of a cold single stream jet at Mach number 0.9 and Reynolds number 3600 is determined via computational aeroacoustics (CAA) methods. The jet computation of the acoustical field is performed by two hybrid approaches using a large-eddy simulation (LES) for the flow field and various systems of equations for the acoustical field to construct a robust, efficient, and reliable LES/CAA solver. The acoustic equations are the Ffowcs Williams–Hawkings equation (FWH) in the frequency domain and the acoustic perturbation equations (APE). The pronounced impact of the data windowing and the radial and streamwise extension of the integration surface on the directivity of the FWH solution is discussed at length. The comparison with available experimental and numerical results at similar flow conditions based on the noise characteristics in the near field shows the solution of the APE system to match the results of the direct LES more accurately than the FWH approach. The APE solution is less susceptible to the size of the source term region than the FWH approach to the location of the source surface. In conjunction with the APE formulation the LES domain can be chosen smaller than for the FWH ansatz resulting in less computational cost for the jet flow. The dominant source term in the APE system for cold jet noise is shown to be the Lamb vector.

[1]  E. Krause,et al.  A comparison of second- and sixth-order methods for large-eddy simulations , 2002 .

[2]  Wolfgang Schröder,et al.  Reduced-order representation of turbulent jet flow and its noise source , 2007 .

[3]  Roland Ewert,et al.  Comparison of source term formulations for a hybrid CFD/CAA method , 2001 .

[4]  W. Schröder,et al.  Acoustic perturbation equations based on flow decomposition via source filtering , 2003 .

[5]  M.Y. Hussaini,et al.  Low-Dissipation and Low-Dispersion Runge-Kutta Schemes for Computational Acoustics , 1994 .

[6]  J. Freund Noise sources in a low-Reynolds-number turbulent jet at Mach 0.9 , 2001, Journal of Fluid Mechanics.

[7]  W. Schröder,et al.  On the simulation of trailing edge noise with a hybrid LES/APE method , 2004 .

[8]  Geert Brethouwer,et al.  A numerical investigation on the effect of the inflow conditions on the self-similar region of a round jet , 1998 .

[9]  A. Lyrintzis,et al.  3-D large eddy simulation for jet aeroacoustics , 2003 .

[10]  A. Lyrintzis,et al.  Coupling of Integral Acoustics Methods with LES for Jet Noise Prediction , 2004 .

[11]  C. Tam,et al.  Dispersion-relation-preserving finite difference schemes for computational acoustics , 1993 .

[12]  D. L. Hawkings,et al.  Sound generation by turbulence and surfaces in arbitrary motion , 1969, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[13]  J. S. Shang,et al.  High-Order Compact-Difference Schemes for Time-Dependent Maxwell Equations , 1999 .

[14]  P. Sagaut,et al.  Large-eddy simulation of a compressible flow in a three-dimensional open cavity at high Reynolds number , 2004, Journal of Fluid Mechanics.

[15]  P. Moin,et al.  A General Class of Commutative Filters for LES in Complex Geometries , 1998 .

[16]  Christophe Bailly,et al.  Decrease of the Effective Reynolds Number with Eddy-Viscosity Subgrid-Scale Modeling , 2005 .

[17]  William K. George,et al.  Velocity measurements in a high-Reynolds-number, momentum-conserving, axisymmetric, turbulent jet , 1994, Journal of Fluid Mechanics.

[18]  F. Farassat,et al.  Extension of Kirchhoff's formula to radiation from moving surfaces , 1988 .

[19]  Christophe Bailly,et al.  Effects of Inflow Conditions and Forcing on Subsonic Jet Flows and Noise. , 2005 .

[20]  Philippe R. Spalart,et al.  Towards the prediction of noise from jet engines , 2003 .

[21]  Christophe Bailly,et al.  Investigation of Subsonic Jet Noise Using LES: Mach and Reynolds Number Effects , 2004 .

[22]  David P. Lockard,et al.  AN EFFICIENT, TWO-DIMENSIONAL IMPLEMENTATION OF THE FFOWCS WILLIAMS AND HAWKINGS EQUATION , 2000 .

[23]  Dennis K. McLaughlin,et al.  Flow field and acoustic properties of a Mach number 0·9 jet at a low Reynolds number , 1980 .

[24]  M. Fisher,et al.  A MODELLING OF THE NOISE FROM SIMPLE COAXIAL JETS, PART I: WITH UNHEATED PRIMARY FLOW , 1998 .

[25]  K. Thompson Time-dependent boundary conditions for hyperbolic systems, II , 1990 .

[26]  P. Sagaut,et al.  Large-Eddy Simulations for Acoustics , 2007 .