Large Eddy Simulation of Trailing Edge Acoustic Emissions ...

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Large Eddy simulation of Trailing Edge Acoustic Emissions of an Airfoil Jinlong Wu William Devenport Eric Paterson Rui Sun Heng Xiao

Transcript of Large Eddy Simulation of Trailing Edge Acoustic Emissions ...

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Large Eddy simulation of Trailing Edge Acoustic Emissions of an Airfoil

Jinlong Wu!William Devenport!Eric Paterson!Rui Sun!Heng Xiao!

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Main Topics

❖ Computational Aeroacoustics (CAA)!

!

❖ The role of Large Eddy Simulation (LES) in CAA!

!

❖ Results and Discussion

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General Acoustic Problem

Source Receiver

∂2 p∂t 2

− c02∇2p = 0

Acoustic Wave Equation

Assumptions

medium at rest

irrotational flow

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wave propagation

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Aeroacoustic Problem

http://www.cascadetechnologies.com/wp-content/uploads/crackle.pnghttp://www.totalsimulation.co.uk/wp/aeroacoustic-modelling-openfoam

http://flowgallery.stanford.edu/research.html

http://www.engineering.com/

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Computational Aeroacoustic(CAA)

❖ Methods with high fidelity:!

❖ Direct simulation (DNS/LES)!

❖ LES + Integral methods

airfoil

fully nonlinear domain

linear domain

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Acoustic Analogy

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∂2ρ∂t 2

− c02∇2ρ = ∂2

∂xi ∂x jTij

∂2 p∂t 2

− c02∇2p = 0

Acoustic Wave EquationLighthill’s Equation

Tij = ρuiu j + (p − c02ρ)δ ij −τ ij

momentum flux entropy production viscous stress

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Acoustic Analogy

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p(x!,t) ≅

xix j4π x! 3

c02

∂2

∂t 2Tij⎡⎣ ⎤⎦te dV (y

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V∫ space integration

surface integration

Simplifications can be made if Mach number is

small (Acoustic Compactness)

−x j

4π x! 2

c0

∂∂t

pni[ ]te dSS∫

p(x!,t) ≅ −

x j4π x! 2

c0

∂∂t

pni dSS∫

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Problem Description

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U = 40m / s

NACA0012

0.1524m

Re ≈ 400,000

Ma ≈ 0.115

❖ The Mach number is around 0.1, which indicates that the space integral can be neglected.!

❖ The unsteady pressure around the airfoil needs to be obtained before acoustic calculation.

trip wires is mounted at x/c=0.127

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Large Eddy Simulation (LES)

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❖ The role of LES is to provide unsteady pressure information around the airfoil.!

❖ Two main prerequisites of LES are required:!

❖ The design of a high-quality and affordable mesh, especially in the near wall region;!

❖ The generation of turbulent boundary layer in numerical simulation.

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Wall Resolved Cost

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W.Wolf & S.Lele, 2012

wall resolved54,000,000 grid points!

Re=408,000Δx+ ≈ 50Δz+ ≈ 20y+ ≈ 0.5

❖ This state-of-the-art simulation focuses on the influence of space integral in acoustic prediction.!

❖ For the engineering application, such cost is too high to be feasible currently.!

❖ What if we only put high resolution mesh in the near wall region and use relatively coarse mesh out of the region of interest?

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Aspect Ratio

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❖ It turns out that if the aspect ratio is too high, the information communication is unbalanced along different directions and leads to the pressure convergence problem.

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Pressure Convergence

❖ It is shown that the convergence problem can be solved if the highest aspect ratio of mesh is reduced.!

❖ It also indicates that the mesh design will influence not only the quality of LES result, but also the time cost.

original mesh new mesh

mesh 5.5 M 6 M

aspect ratio ~150 ~75

pressure iterations for each time step ~1000 ~10

total time cost estimation ~180 days ~5 days

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Mean Flow Information

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❖ It seems that the mean flow information around the airfoil is captured in the present simulation.

-Cp

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Boundary Layer Development

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❖ It is shown that an obvious offset of boundary layer development between our result and benchmark.

Cf

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Boundary Layer Development

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❖ The offset of boundary layer development is even more obvious near the trailing edge, which is the exact region of interest in our work.!

❖ It indicates that the numerical tripping needs to be adjusted.

Displacement thickness Momentum thickness

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Friction Coefficient

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Old tripping New tripping

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Reynolds Stress

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Rxy Rxy

Ryy Ryy

Old tripping New tripping

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Conclusions❖ Unsteady flow information can be obtained by LES, which

can be used for the further acoustic calculation.!

❖ Mesh design will influence not only the quality of LES result, but also the convergence and time cost consequently.!

❖ Numerical tripping will directly influence the development of boundary layer, which is the region of interest for CAA. !

❖ Since that the turbulent boundary layer exits for many engineering applications, finding a suitable numerical tripping is important for obtaining a reliable acoustic result.

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Thank you!

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