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Scientific and Technical Aerospace Reports Volume 39 April 6, 2001

Scientific and Technical Aerospace Reports Volume 39 April 6, 2001

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<strong>2001</strong>0022648 Stanford Univ., Center for Turbulence Research, Stanford, CA USA<br />

A New Method for Accurate Treatment of Flow Equations in Cylindrical Coordinates Using Series Expansions<br />

Constantinescu, G.S., Stanford Univ., USA; Lele, S. K., Stanford Univ., USA; Annual Research Briefs - 2000: Center for Turbulence<br />

Research; December 2000, pp. 199-210; In English; See also <strong>2001</strong>0022631<br />

Contract(s)/Grant(s): NAG2-1373; No Copyright; Avail: CASI; A03, Hardcopy; A03, Microfiche<br />

The motivation of this work is the ongoing effort at the Center for Turbulence Research (CTR) to use large eddy simulation<br />

(LES) techniques to calculate the noise radiated by jet engines. The focus on engine exhaust noise reduction is motivated by the<br />

fact that a significant reduction has been achieved over the last decade on the other main sources of acoustic emissions of jet<br />

engines, such as the fan <strong>and</strong> turbomachinery noise, which gives increased priority to jet noise. to be able to propose methods to<br />

reduce the jet noise based on results of numerical simulations, one first has to be able to accurately predict the spatio-temporal<br />

distribution of the noise sources in the jet. Though a great deal of underst<strong>and</strong>ing of the fundamental turbulence mechanisms in<br />

high-speed jets was obtained from direct numerical simulations (DNS) at low Reynolds numbers, LES seems to be the only realistic<br />

available tool to obtain the necessary near-field information that is required to estimate the acoustic radiation of the turbulent<br />

compressible engine exhaust jets. The quality of jet-noise predictions is determined by the accuracy of the numerical method that<br />

has to capture the wide range of pressure fluctuations associated with the turbulence in the jet <strong>and</strong> with the resulting radiated noise,<br />

<strong>and</strong> by the boundary condition treatment <strong>and</strong> the quality of the mesh. Higher Reynolds numbers <strong>and</strong> coarser grids put in turn a<br />

higher burden on the robustness <strong>and</strong> accuracy of the numerical method used in this kind of jet LES simulations. As these calculations<br />

are often done in cylindrical coordinates, one of the most important requirements for the numerical method is to provide a<br />

flow solution that is not contaminated by numerical artifacts. The coordinate singularity is known to be a source of such artifacts.<br />

In the present work we use 6th order Pade schemes in the non-periodic directions to discretize the full compressible flow equations.<br />

It turns out that the quality of jet-noise predictions using these schemes is especially sensitive to the type of equation treatment<br />

at the singularity axis. The objective of this work is to develop a generally applicable numerical method for treating the singularities<br />

present at the polar axis, which is particularly suitable for highly accurate finite-differences schemes (e.g., Pade schemes) on<br />

non-staggered grids. The main idea is to reinterpret the regularity conditions developed in the context of pseudo-spectral methods.<br />

A set of exact equations at the singularity axis is derived using the appropriate series expansions for the variables in the original<br />

set of equations. The present treatment of the equations preserves the same level of accuracy as for the interior scheme. We also<br />

want to point out the wider utility of the method, proposed here in the context of compressible flow equations, as its extension<br />

for incompressible flows or for any other set of equations that are solved on a non-staggered mesh in cylindrical coordinates with<br />

finite-differences schemes of various level of accuracy is straightforward. The robustness <strong>and</strong> accuracy of the proposed technique<br />

is assessed by comparing results from simulations of laminar forced-jets <strong>and</strong> turbulent compressible jets using LES with similar<br />

calculations in which the equations are solved in Cartesian coordinates at the polar axis, or in which the singularity is removed<br />

by employing a staggered mesh in the radial direction without a mesh point at r = 0.<br />

Author<br />

Large Eddy Simulation; Numerical Analysis; Series Expansion; Cylindrical Coordinates<br />

<strong>2001</strong>0022649 Stanford Univ., Center for Turbulence Research, Stanford, CA USA<br />

An Evaluation of a Conservative Fourth Order DNS Code in Turbulent Channel Flow<br />

Gullbr<strong>and</strong>, Jessica, Stanford Univ., USA; Annual Research Briefs - 2000: Center for Turbulence Research; December 2000, pp.<br />

211-218; In English; See also <strong>2001</strong>0022631; No Copyright; Avail: CASI; A02, Hardcopy; A03, Microfiche<br />

Direct numerical simulation (DNS) <strong>and</strong> large eddy simulation (LES) of turbulent flows require a numerical method that is<br />

able to capture a wide range of turbulent length scales. In DNS, all the turbulent length <strong>and</strong> time scales are resolved. In LES, the<br />

large energy carrying length scales of turbulence are resolved <strong>and</strong> the small structures are modeled. The separation of large <strong>and</strong><br />

small scales is done using a filtering procedure that is applied to the Navier-Stokes equations. The effect of the small scale turbulence<br />

on the resolved scales is modeled using a subgrid scale (SGS) model. Widely used SGS models are the scale similarity models<br />

by Bardina et al. <strong>and</strong> Liu et al <strong>and</strong> the eddy viscosity based dynamic Smagorinsky model proposed by Germano et al.. In general,<br />

scale similarity models do not dissipate enough energy, <strong>and</strong> eddy viscosity models do not carry enough stress. SGS models tend<br />

to over- <strong>and</strong> underpredict velocity fluctuations. SGS models typically use information from the smallest resolved length scales<br />

to model the stresses of the unresolved scales. Therefore, it is of great importance that these resolved length scales are captured<br />

accurately. This requires that the numerical error of the scheme is sufficiently small. One approach is to use high order finite difference<br />

schemes. However, high order schemes require that the differentiation <strong>and</strong> filtering operations commute. This is generally<br />

not the case in inhomogeneous flow fields where the required smallest resolved length scales vary throughout the flow field. For<br />

this situation, the filter width varies introducing commutation errors of O(del(exp 2)) where del represents the filter width. High<br />

order finite difference schemes with good conservation properties <strong>and</strong> three-dimensional commutative filters have been developed<br />

by Morinishi et al., Vasilyev et al. <strong>and</strong> Vasilyev. These discretization schemes can conserve energy, which ensures a stable<br />

59

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