Turbulence and Fluent

Transcription

1 Turbulence and Fluent

2 Turbulence Modeling

3 What is Turbulence? We do not really know 3D, unsteady, irregular motion in which transported quantities fluctuate in time and space. Turbulent eddies (spatial structures). Diffusive (mixing). Self-sustaining if a mean shear exist. Entrainment. Energy cascade. Energy is added at the large eddies. Energy is dissipated at the small eddies.

4 Turbulent Flows Smaller Structures Larger Structures

5 Computational Approaches DNS (Direct Numerical Simulation) Solves the Navier-Stokes (N-S) equations. No turbulence modeling required. Not practical for industrial flows (requires Low Re and simple geometries). LES (Large Eddy Simulation) Solves a filtered version of the N-S equations. Less expensive than DNS, but still too expensive for most applications. RANS (Reynolds-Averaged N-S) Solve the ensemble-averaged N-S equations. All turbulence is modeled. The most widely used approach for calculating industrial flows. There is not yet a single turbulence model that can reliably predict all turbulent flows found in industrial applications with sufficient accuracy.

6 Computational Approaches(2) LES, DNS RANS

7 RANS Modeling Reynolds decomposition: The Reynolds-averaged momentum equations are as follows: where is called the Reynolds stresses. The Reynolds stresses must be modeled to close the equations. j ij j i j i k i k i x R x U x x p x U U t U + + = + µ ρ j i ij u u R = ρ ( ) ( ) ( ) t x u t x U t x u i i i,,, r r r + = Turbulent fluctuation Mean u' i U i u i time u

8 The Closure Problem Reynolds equations does not contain enough equations to solve for all the uknown variables. Thus, the Reynolds stresses must be modeled. Eddy-Viscosity Models (EVM): Modeling approaches Boussinesq hypothesis: Reynolds stresses are modeled using an eddy (or turbulent) viscosity µ t. Assumes Isotropic turbulence. R ij = ρu u i j Ui µ = t x j U + x i j 2 U µ t 3 x k k 2 δij ρkδ ij 3 Reynolds-Stress Models (RSM): solves transport equations for all individual Reynolds stresses. Require modeling for many terms in the Reynolds stress equations. Does NOT assume isotropic turbulence.

9 Modeling the Eddy Viscosity Basic approach made through dimensional arguments Units of ν t = µ t /ρ are [m 2 /s] Typically one needs 2 out of the 3 scales: velocity - length - time Commonly used scales is the turbulent kinetic energy [L 2 /T 2 ] is the turbulence dissipation rate [L 2 /T 3 ] is the specific dissipation rate [1/T] Models classified in terms of number of transport equations solved, zero-equation models one-equation models two-equation models

10 Spalart-Allmaras A one-equation RANS model A low-cost model solving an equation for the modified eddy viscosity ν ~ Eddy-viscosity is obtained from µ = t ρ ~ ν f v1, f v1 ~ 3 ( ν / ν ) 3 3 ( ~ ν / ν ) + C v1 Mainly for aerodynamic/turbo-machinery applications with mild separation (supersonic/transonic flows over airfoils, boundary-layer flows, etc).

11 Standard k-ε (SKE) Transport equations for k and ε: where D Dt D Dt C ( ρk) ( ρε ) = x A two-equation RANS model j = x j µ + µ t k σ k x + G µ t ε µ + + C σ ε x j ε G k ρc The most widely-used engineering turbulence model for industrial applications Robust Performs poorly for flows with strong separation, large streamline curvature, and large pressure gradient. j k e1 ρε k ε 2 2 ε k µ = σ ε 0.09, Cε1 = 1.44, Cε 2 = 1.92, σ k = 1.0, = 1.3

12 Realizable k-ε (RKE) Realizable k-ε (RKE) Positivity of normal stresses Schwarz inequality for Reynolds shear-stresses Good performance for flows with axisymmetric jets. RNG k-ε (RNG) Constants in the k-ε equations are derived using the Renormalization Group theory. RNG s sub-models include: Differential viscosity model to account for low-re effects Analytically derived algebraic formula for turbulent Prandtl/Schmidt number Swirl modification Performs better than SKE for more complex shear flows, and flows with high strain rates, swirl, and separation.

13 k-ω models + + = + + = = j t j j i ij j k t j j i ij t x x f x U k Dt D x k x k f x U Dt Dk k ω σ µ µ ω ρ β τ ω α ω ρ σ µ µ ω ρ β τ ρ ω ρ α µ ω β β 2 * * * τ ε ω 1 k specific dissipation rate: ω Two-equation RANS models Fluent supports the standard k-ω model by Wilcox (1998), and Menter s SST k- ω model (1994). k-ω models are inherently low-re models: Can be integrated to the wall without using any damping functions Accurate and robust for a wide range of boundary layer flows with pressure gradient Most widely adopted in the aerospace and turbo-machinery communities. Several sub-models/options of k-ω : compressibility effects, transitional flows and shear-flow corrections.

14 Reynolds-Stress Model (RSM) t x ( ) ( ) T ρu iu j + ρ U k u iu j = Pij + Fij + Dij + Φij εij Stress-production Rotation-production k Turbulent diffusion Dissipation Pressure strain Modeling required for these terms Attempts to address the deficiencies of the EVM. Anisotropy, history effects of Reynolds stresses. RSM requires more modeling (the pressure-strain is most critical and difficult one among them). More expensive and harder to converge. Most suitable for complex 3-D flows with strong streamline curvature, swirl and rotation.

15 Near Wall Modeling

16 The Structure of Near-Wall Flows The structure of turbulent boundary layers in the near-wall region:

17 Near-Wall Modeling Wall Functions Wall Integration Accurate near-wall modeling is important to correctly predict frictional drag, pressure drop, separation, heat transfer etc.

18 Near-Wall Modeling Options Wall functions provide boundary conditions for momentum, energy, species and turbulent quantities. The Standard and Non-equilibrium Wall Functions (SWF and NWF) use the law of the wall. Enhanced Wall Treatment Combines the use of blended law-of-the wall and a two-layer zonal model. Suitable for low-re flows or flows with complex near-wall phenomena. Turbulence models are modified for the inner layer. Generally requires a fine near-wall mesh capable of resolving the viscous sub-layer (more than 10 cells within the inner layer) outer layer inner layer

19 Placement of The First Grid Point For standard or non-equilibrium wall functions, each wall-adjacent + cell s centroid should be located within: y p For the enhanced wall treatment (EWT), each wall-adjacent cell s centroid should be located: + Within the viscous sublayer, y p 1, for the two-layer zonal model: + Preferably within for the blended wall function y p How to estimate the size of wall-adjacent cells before creating the grid: + + y y u / ν y y ν u, u τ ρ = U c / 2 p p τ p p / w / e f The skin friction coefficient can be estimated from empirical correlations: τ τ

20 Near-Wall Modeling: Recommended Strategy Use SWF or NWF in high Re applications (Re > 10 6 ) where you cannot afford to resolve the viscous sub-layer. Use NWF for mildly separating, reattaching, or impinging flows. You may consider using EWT if: Near wall characteristics are important. The physics and near-wall mesh of the case is such that y + is likely to vary significantly over a wide portion of the wall region. Try to make the mesh either coarse or fine enough to avoid placing the wall-adjacent cells in the buffer layer (y + = 5 ~ 30).

21 Enhanced Wall Treatment Fully-Developed Channel Flow (Re t = 590) For fixed pressure drop cross periodic boundaries, different nearwall mesh resolutions yielded different volume flux as follows y + = 1 y + = 4 y + = 8 y + = 16 Std. Wall fn EWT The enhanced near-wall treatment gives a much smaller variation for different near-wall mesh resolutions compared to the variations found using standard wall functions.

22 Inlet/Outlet Conditions Boundary conditions for k, ε, wand/or u u i j must be specified. Direct or indirect specification of turbulence parameters: Explicitly input k, ε, w, or u u i j This method allows for profile definition. Turbulence intensity and length scale For boundary layer flows: l 0.4d 99 For flows downstream of grid: l opening size Turbulence intensity and hydraulic diameter Internal flows Turbulence intensity and turbulent viscosity ratio For external flows: 1 < m t /m < 10

23 Choosing Models

24 Is the Flow Turbulent? External Flows Rex Re D ,000 Internal Flows Re Dh 2,300 along a surface around an obstacle where Re L ρul µ L = x, D, D h, etc. Other factors such as free-stream turbulence, surface conditions, and disturbances may cause earlier transition to turbulent flow. Natural Convection 8 10 Ra where Ra 3 gβ TL ρ µα

25 Turbulence Models in Fluent Increase in Computational Cost Per Iteration Zero-Equation Models One-Equation Models Spalart-Allmaras Two-Equation Models Standard k-ε RNG k-ε Realizable k-ε Standard k-ω SST k-ω V2F Model Reynolds-Stress Model Detached Eddy Simulation Large-Eddy Simulation Direct Numerical Simulation RANS models Available in FLUENT Auxiliary Models Buoyancy effects Compressibility effects Low Re effects Pressure gradient effects Near-wall options Standard wall functions Non-equilibrium wall functions Enhanced wall treatment Customization Turbulent viscosity Source terms Turbulence transport equations

26 GUI for Turbulence Models Define Models Viscous... Inviscid, Laminar, or Turbulent Turbulence Model options Near Wall Treatments Additional Turbulence options

27 RANS Turbulence Model Behavior and Usage Model Spalart- Allmaras Standard k-ε RNG k-ε Realizable k-ε Standard k-ω SST k-ω RSM Behavior and Usage Economical for large meshes Performs poorly for 3D flows, free shear flows, flows with strong separation Suitable for mildy complex (quasi-2d) flows (turbo, wings, fuselages, missilies) Robust, but performs poorly for complex flows Suitable for initial conditions, fast design screening and parametric studies Suitable for complex shear flows involving rapid strain, moderate swirl, vortices, locally transitional flows (e.g. b.l. Separation, massive separation, vortex shedding) Similar benefits and applications as the RNG model Possibly more accurate and easier to converge Superior for wall-bounded, free shear, and low-re flows Suitable for complex b.l flows (e.g. external aero, turbomachinery, vortex shedding) Can predict transition (usually predict to early transition, though) Similar benefits as SKO, less sensitive to outer disturbances Suitable for wall bounded flows, less suited for free shear flows The most physically sound RANS model (handels anisotrophy) Computationally expensive and harder to converge Suitable for complex 3D flows with strong streamline curvature, strong swirl (e.g. Curved duct, swirl combustors, cyclones)

28 Examples

29 Heat Transfer Behind a 2D Backstep Heat transfer predictions along the bottom Measured by Vogel and Eaton (1980) SKE, RNG, and RKE models are employed with standard wall functions.

30 Factors affecting accuracy The accuracy of turbulent flow predictions can be affected by user decisions involving Turbulence model Boundary conditions Grid resolution and near wall modeling Grid quality

31 Impact of Turbulence Model k-ε Results

32 Impact of Boundary Conditions Run X-Velocity B.C. Thermal B.C. 1 Profile Uniform 2 Uniform Uniform Turbulence B.C. Profile Intensity & Hydraulic Diameter 3 Profile Uniform k=1, ε=1

33 Impact of Grid Quality Structured Tri w b/l Quad Pave Tri

34 Impact of Near Wall Modeling y+ values must be appropriate for selected near wall treatment Realizable k-ε with SWF

35 Stream Function Contours for 180 Degree Bend Spalart-Allmaras Standard k-ε RNG k-ε RSM

36 Rotating Flow in a Cyclone 0.1 m Highly swirling flows (W max = 1.8 U in ) High-order discretization on 40,000 cell hexahedral mesh Computed using a family of k-ε models (SKE, RNG, RKE), k-ω models (Wilcox, SST) and RSM models 0.97 m 0.12 m U in = 20 m/s 0.2 m

37 Cyclone Velocity Profiles