CFD Simulations AC1-01

Aero-acoustic cavity

Application Challenge 1-01 © copyright ERCOFTAC 2004

Overview of CFD Simulations

To date [2,3,4], various CFD codes have accurately predicted the more dominant narrow-band tones, and with limited success broad-band tones using 2D meshes, particularly in the case with doors deployed at 90o. Further investigation for 3D effects may improve this situation and this is being investigated. The results for 2D and 3D meshes using STAR-CD v3.1 and v3.15 will be made available to the project.

Simulation Case

Solution strategy

STAR-CD employs the following solution parameters;

- Conservation of mass, momentum and energy by solving the Navier-Stokes equations using the SIMPLE/PISO algorithm for compressible flow.

- Use of second-order spatial discretisation MARS scheme, (unstructured TVD), and optionally first-order (Euler implicit) or second-order (Crank-Nicholson) temporal discretisation.

- Turbulence represented optionally by eddy-viscosity, Reynolds-stress transport or large-eddy simulation.

The calculations are performed in transient mode for a limited time span, sufficiently long to capture several limit-cycled periods (see also Figure 3), but starting from a steady state solution which may be converged (see also Figure 4) or for which the residuals have been minimized to ensure a representative starting solution. © ERCOFTAC 2004 Computational Domain

Measurements taken off the centreline during the experimental study indicate that the 3D effects are not significant. Hence the case can be modelled as 'quasi-3D'. This allows the predictions of the fundamental flow physics to be evaluated for effects of grid and time-step dependency, turbulence model, order of temporal discretisation and other numerical settings.

The case can and will also be run 3D during the QNET project. © ERCOFTAC 2004 Boundary Conditions

The boundary conditions faithfully represent the test conditions listed in section 2.2. The upstream and top boundaries (Figure 2) are defined as inlets at M=0.85. The surfaces of the cavity, upstream and downstream are treated as rigid and non-slip. The downstream boundary is treated as a fixed pressure boundary and deemed to be far enough away to make any boundary reflection issues negligible. Symmetry planes are applied in the third dimension. © ERCOFTAC 2004 Application of Physical Models

For the calculations already completed, some results for which are reported below, a standard k-ε turbulence model with wall-functions was employed. The near-wall y+ values were approximately 20-100, reducing below that lower limit for a very small number of near-wall cells. © ERCOFTAC 2004 Numerical Accuracy

Mesh density and time-step size studies already undertaken for this calculation indicate the suitability of the calculation methodology for predicting the inherent flow and acoustic characteristics. These are discussed in more detail in Section 3.2.6 and Section 4. Figure 2 illustrates flow domain and typical coarse and fine mesh resolution for this geometry. Further studies will also be subject to similar sensitivity checks.

Figure 2: Coarse mesh (left) and fine mesh (right) © ERCOFTAC 2004 CFD Results

Sample results are presented below.

Figure 3. Residual histories for converged steady-state run

Figure 4: Sample of CFD transient pressure trace (total 0.2 seconds)

Figure 3 illustrates a typical steady-state residual history. The solution from such a calculation, used as the starting (time zero) solution for a transient calculation, produces a transient pressure history at the measurement points typified by Figure 4.

The combined steady state and transient calculation take in the order of one to two days on a single processor machine (workstation or high performance PC processor) © ERCOFTAC 2004 References

[2] Henderson J., Babcock K. and Richards B. E., “Subsonic and transonic transitional cavity flows”, AIAA-2000-1966, June 2000, 6th AIAA/CEAS Aeroacoustics Conference and Exhibit.

[3] Shieh C. M. and Morris P. J., “Parallel computational aeroacoustic simulation of turbulent subsonic cavity flow”, AIAA-2000-1914, June 2000, 6th AIAA/CEAS Aeroacoustics Conference and Exhibit.

[4] Mendonça, F., Allen, R., de Charentenay, J., Lewis, M., “Towards Understanding LES and DES for Industrial Aeroacoustics Predictions”, International workshop on ‘LES for Acoustics’, DLR Göttingen, Germany, 7-8th October 2002, © copyright ERCOFTAC 2004

Contributors: Fred Mendonca; Richard Allen - Computational Dynamics Ltd

Site Design and Implementation: Atkins and UniS

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