From Charles to IC : X 3 from Finite Volume to Spectral ... · Channel flow test case Charles -...

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From Charles to IC : from Finite Volume to Spectral Difference LES J. Bodart , T. Lunet, R. Lamouroux, J. Gressier, G. Grondin, F. Grabner, DAEP/ISAE-SUPAERO 4th International Workshop on High-Order CFD Methods (ECCOMAS Congress). FORTH, Island of Crete, June 2016 X 3

Transcript of From Charles to IC : X 3 from Finite Volume to Spectral ... · Channel flow test case Charles -...

Page 1: From Charles to IC : X 3 from Finite Volume to Spectral ... · Channel flow test case Charles - Compressible NS LES unstructured • 2nd to 4th order/ skew-symmetric form of the

From Charles to IC : from Finite Volume to Spectral Difference LES

J. Bodart, T. Lunet, R. Lamouroux, J. Gressier, G. Grondin, F. Grabner,

DAEP/ISAE-SUPAERO

4th International Workshop on High-Order CFD Methods (ECCOMAS Congress).

FORTH, Island of Crete, June 2016

X 3

Page 2: From Charles to IC : X 3 from Finite Volume to Spectral ... · Channel flow test case Charles - Compressible NS LES unstructured • 2nd to 4th order/ skew-symmetric form of the

Past applications (FV solver Charles )I. Bermejo Moreno (2013) et al.

Hifire Scramjet(PSAAP program)

Uncertainty quantifications applied on scramjet unstart at Stanford

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Performance of the finite volume solver(2013) Pushing the strong scaling as far as we could...

2600 CV/cores

Scaling on Sequoia Supercomputer(Livermore National Lab):

up to 96K nodes = 1.5 million cores

as low as 450 CV/core

Good scaling up to 2600 CV/core

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Scalability limits FV vs SD

Spatially weighted projections for discontinuities treatment adapted to compact high-order schemes.

Monday, CS 930, 4.30pm

A fair performance comparison between HO and classical FV schemes for unstructured grids and complex

turbulent flows Tuesday, CS 500, 4.30pm

Page 5: From Charles to IC : X 3 from Finite Volume to Spectral ... · Channel flow test case Charles - Compressible NS LES unstructured • 2nd to 4th order/ skew-symmetric form of the

Channel flow test caseCharles - Compressible NS LES unstructured

• 2nd to 4th order/ skew-symmetric form of the advective term

• Left/Right states uses(n +1) points stencil

• Convective flux: Blending between fully centered and approximate Riemann

solver based on mesh quality (Structured mesh: >99% centered)

• Vreman model

Hybrid - Compressible NS DNS/LES structured

• Order 6 centered derivatives for diffusion and advection operators.

• Dynamic Smagorinsky LES model

• Disclaimer: not expert user

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faces

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Grid resolutionsType Resolution ID Number of d of ∆x ×x∆y × ∆z Solver

Struct. Fine MS1 256x96x128 14.5x0.7x14.5 FD6,FV2

Struct. Baseline MS2 192x96x96 19.3x0.7x19.3 FD6,FV2

Struct. Coarse MS3 128x96x64 29x0.7x29 FD6,FV2

Unstruct. Fine MU1 -x96x- 14.5x0.7x14.5 FV2

Unstruct. Baseline MU2 -x96x- 19.3x0.7x19.3 FV2

Unstruct. Coarse MU3 -x96x- 29x0.7x29 FV2

+ + +

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Unstructured grid(x/z direction)

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Unstructured grid(x/z direction)

1x1 Zoom

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Results (Velocity, FD, MS)

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Results (Velocity, FV, MS)

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Results (Velocity, FV, MU)

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Results (Reynolds stress, FD, MS)

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Results (Reynolds stress, FV, MS)

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Results (Reynolds stress, FV, MU)

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Results (Spectra-z, FV, MS) y =501+

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Results (Spectra-z, FV, MS) y =249+

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Results (Spectra-z, FV, MS) y =59+

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Results (Spectra-z, FV, MS), y =10+

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Results (Spectra-x, FV, MS) y+=501

Page 20: From Charles to IC : X 3 from Finite Volume to Spectral ... · Channel flow test case Charles - Compressible NS LES unstructured • 2nd to 4th order/ skew-symmetric form of the

Results (Spectra-x, FV, MS) y =249+

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Results (Spectra-x, FV, MS) y =59+

Page 22: From Charles to IC : X 3 from Finite Volume to Spectral ... · Channel flow test case Charles - Compressible NS LES unstructured • 2nd to 4th order/ skew-symmetric form of the

Results (Spectra-x, FV, MS) y =10+

Page 23: From Charles to IC : X 3 from Finite Volume to Spectral ... · Channel flow test case Charles - Compressible NS LES unstructured • 2nd to 4th order/ skew-symmetric form of the

Summary1. Fundamental test case for wall-bounded turbulent flows

2. Does not need to be driven by constant pressure gradient

3. Constant flow rate is much faster

4. Grid is not well suited to FV schemes

5. Maybe not challenging enough for LES with HO