Engineering. Spring Department of Fluid Mechanics, Budapest University of Technology and Economics. Large-Eddy Simulation in Mechanical
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1 Outline Geurts Book Department of Fluid Mechanics, Budapest University of Technology and Economics Spring 2013
2 Outline Outline Geurts Book 1 Geurts Book
3 Origin This lecture is strongly based on the book: Outline Geurts Book Bernard J. Geurts : Elements of Direct and Simulation books/072/index.html
4 Part I Second Lecture
5 The idea Reduced flow description Low-pass filtering (in wave number space), with characteristic length of non-linear terms Closure problems Important to consider the ratio /η. As /η O(1), LES converge to DNS. /η is the main parameter of the LES. It characterise the resolution/quality of various results of the simulation.
6 The governing Incompressible, isochoric fluid ρ = const. Constant viscosity ν = const. Continuity equation: i u i = 0 (1) t u i + u j j u i = p i ρ + ν j j u i (2) Let us assume that ρ = 1 so we can skip it from the.
7 Transformation properties of the Galilean invariance etc.
8 Notation of the filtering Let us define an operator L which reduces the spatial scales of the flow-field: L : ϕ ϕ 1D example (ϕ(x, t) or e.g. u(x, t)): ϕ = L(ϕ)(x, t) = x+ /2 x /2 ϕ(ξ, t) dξ (3) 2) = l/16 Two filtering is shown: 1) = l/4,
9 Preliminary comment on filter width We are interested in a quantitative variable q of a specific flow (for example flow around cylinder, channel flow). The filtered flow-field can be used also for the evaluation. Depending on the interesting quantity (drag coefficient, turbulence level), the accuracy of the estimation q err will clearly depend on the applied filter length i.e. how many details of the flow we keep. For some quantity the very smoothed signal ( is big) gives already a good prediction (q err is small), for other quantities fines scales are also responsible and only filtering at smaller scales can be applied.
10 Notation of the filtering In 3D a generic homogeneous filter can be defined: ϕ (x, t) = L(ϕ)(x, t) = + G (x x)ϕ(x, t) dx = G ϕ (4) This a convolution filter (multiplied by something shifted over)! No temporal filtering is carried out! Causality: future does not influence the past Temporal averaging would lead us to RANS Normalization of the kernel: + G (x ) dx = 1 (5)
11 Commutation of the filter This type of filtering is a linear integral operator. The above defined homogeneous convolution filter commutes both with temporal and spatial derivation: t f = t f ; i f = i f (6)
12 Commuting of the mom. eq. Because of the commutation property: (ρ = 1 and everything is rearranged to the LHS) t u i + j ( u i u j ) + i p ν j j u i = 0 (7) If we want to see the same terms on LHS as in the orig. NS. we have to add the required term j ( u i u j ) and subtract the one available j ( u i u j ) on both side of the equation: t u i + j ( u i u j ) + i p ν j j u i = j τ ij (8) where: τ ij def = u i u j u i u j (9)
13 SGS tensor τ ij is called the SubGrid Scale stress tensor. It is responsible for the effect of the unresolved (removed by the filter) scales. Its actual effect is j τ ij which needs to be led. It is called historically sub grid scale, since the filtering was originally (but not very logically) related to the numerical grid size (h).
14 SGS tensor as a commutator Let us define the product operator: Π(u i, u j ) def = u i u j (10) The SGS stress can be written using this as a commutator: τ ij = u i u j u i u j = = L(Π(u i, u j )) Π(L(u i ), L(u i )) = = [L, Π](u i, u j ) (11) where [a, b] def = ab ba is the commutator symbol for spaces where addition and multiplication are defined. It measures the strength of not commuting.
15 Identities of the commutator operator Wikipedia section 1 [A, A] = 0 2 [A, B] = [B, A], anti-commutativity 3 [A, [B, C]] + [B, [C, A]] + [C, [A, B]] = 0, Jacobi identity 4 [A, BC] = [A, B]C + B[A, C], Leibnitz rule Example for Leibnitz rule: A B C def = d x ( ) = ( ) def = f ( ) def = g( ) (12) I.e.: (fg) = f g + fg
16 Non-uniform filtering In convolution filtering the filter width ( ) is constant. Practically the mesh size is changing (e.g.: see channel in wall normal direction)! 1D example (ϕ(x, t) or e.g. u(x, t)): ϕ = L(ϕ)(x, t) = x+ +(x) x (x) g(x, ξ) ϕ(ξ, t) dξ (13) (x) where (x) = + + is the spatially varying filter width.
17 Commutation error at non-uniform filtering i ϕ i ϕ because of the varying filter width. This can be written more formally: L( i ϕ) i L(ϕ) = [L, i ](ϕ) 0 (14)
18 Non-uniformly filtered set of Continuity The continuity equation: j u j = [L, j ](u j ) (15) i.e. the filtered flow-field is not any more divergence free (solenoidal). Variation of the filter width is related to local mass production or destruction.
19 Non-uniformly filtered set of Momentum The momentum equation: t u i + j ( u i u j ) + i p ν j j u i = j ([L, Π](u i, u j )) ([L, j ](p) ν[l, jj ](u i ) + [L, j ](Π(u i, u j )) (16) The RHS is much more complicated now. The new terms even destroy the conservation property of the original. Flow structures travelling in the direction of filter width change experience a scale reduction or occurrence simply by the change in the filter.
20 Non-uniformly filtered set of Momentum E.g. a vortex arriving to a region of higher filter width will be smoothed corresponding to local kinetic energy reduction, which is against conservation. The effect can be quantified by material derivative of the filter width: u j j
21 Summary We arrive at the LES-template : NS( U ) = R(U, U ) (17) where R is the residual because of the filtering. R(U, U) = 0, since in this case L = Id identity operator, and DNS should be recovered. In the ling exercise R(U, U ) M( U ), i.e. the residual has to be approximated using the filtered flow-field.
22 How to develop the? How to separate between large and small scales? Spatial filtering, smoothing using a kernel function ϕ (x j, t) def = G (r i ; x j ) ϕ(x j r i, t)dr i (18) V
23 kernel G is the filtering kernel with a typical size of. G has a compact support (its definition set where the value is non-zero is closed) in its first variable To be the filtered value of a constant itself it has to be true: G (r i ; x j )dr i = 1 (19) V If G (r i ; x j ) is homogeneous in its second variable and isotropic in its first variable than G ( r i ) is a function of only one variable
24 kernel Examples
25 Physical space Fluctuation: ϕ def = ϕ ϕ (20) ϕ 0, a difference compared to Reynolds averaging
26 Spectral space Recall: the cutting wavenumber (κ c ), below which ling is needed
27 If using the previously defined (homogeneous, isotropic) filter Averaging and the derivatives commute (exchangeable) i u i = 0 (21) t u i + u j j u i = 1 ρ p + ν j j u i j τ ij (22) 3D (because turbulence is 3D) unsteady (because the large eddies are unsteady)
28 Sub Grid Scale stress τ ij is called Sub-Grid Scale stress SGS from the times when filtering was directly associated to the grid τ ij def = u i u j u i u j (23) It represents the effect of the filtered scales It is in a form of a stress tensor Should be dissipative to represent the dissipation on the filtered small scale
29 Same as in RANS τ ij 1 3 τ kkδ ij = 2ν t s ij (24) Relatively a better approach (compared to the application for RANS) since the small scales are more universal Dissipative if ν t > 0.
30 Smagorinsky ν t = (C s ) 2 S (25) S def = 2s ij s ij (26) C s Smagorinsky constant to be determined using spectral theory of turbulence using validations on real flow computations to be prescribed determine the computational cost (if too small) determine the accuracy (if too big) resolving 80% of the energy is a good compromise
31 Scale Similarity Let us assume that the cuted small scales are similar to the kept large scales! A logical : τ ij def = u i u j u i u j (27) The unfiltered quantities are led by the filtered ones. Properties It is not dissipative enough It gives feasible shear stresses (from experience) Logical to combine with Smag.!
32 Dynamic approach The idea is the same as in the scale similarity The theory is more complicated Any can be made dynamic Dynamic Smagorinsky is widely used (combining the two advantages)
33 Periodicity Periodicity is used to infinite long domain The length of periodicity is given by the length scales of turbulence
34 Inlet Much more difficult than in RANS Turbulent structures should be represented Vortices should be synthesized Separate precursor simulation to provide real turbulence
35 Wall y + 1 (28) x + 50 (29) z (30)
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