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THESE de DOCTORAT - cerfacs

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2.2 Direct Computation of noise through Large Eddy Simulation 25<br />

From this <strong>de</strong>finition it is possible to write the system of equations that govern LES for nonreacting<br />

flows. It yields [74]<br />

Mass<br />

∂ ¯ρ<br />

∂t + ∂ ( ) ¯ρũj = 0 (2.10)<br />

∂x j<br />

Momentum<br />

∂ ¯ρũ i<br />

∂t<br />

+ ∂<br />

∂x j<br />

( ¯ρũi ũ j<br />

) +<br />

∂ ¯p<br />

∂x i<br />

=<br />

∂ [<br />

¯τij − ¯ρ ( )]<br />

ũ i u j − ũ i ũ j<br />

∂x j<br />

(2.11)<br />

Chemical species<br />

∂ ¯ρỸ k<br />

∂t<br />

+ ∂ ( )<br />

¯ρũ j Ỹ<br />

∂x k = ∂ [<br />

)]<br />

V<br />

j ∂x k,j Y k − ¯ρ<br />

(ũj Y k − ũ j Ỹ k + ¯˙ω k (2.12)<br />

j<br />

Enthalpy<br />

∂ ¯ρ˜h s<br />

∂t<br />

[<br />

∂<br />

( )<br />

¯ρũ j˜hs = Dp<br />

∂x j Dt + ∂ λ ∂T<br />

) ] ∂u j<br />

− ¯ρ<br />

(ũj h s − ũ j˜hs + τ ij<br />

∂x j ∂x j ∂x i<br />

)<br />

ρ V k,j Y k h s,k<br />

− ∂<br />

∂x j<br />

(<br />

N<br />

∑<br />

k=1<br />

+ ¯˙ω T<br />

(2.13)<br />

where h s stands for the sensible enthalpy of the mixture. The quantities (ũ i u j − ũ i ũ j ), (ũ j Y k −<br />

ũ j Ỹ k ) , (ũjh s − ũ j˜hs ), V k,i Y k and ( ¯˙ω k ) are known as the unresolved Reynolds stresses, unresolved<br />

species flux, unresolved enthalpy flux, filtered laminar diffusion fluxes and filtered chemical<br />

reaction rate respectively. These terms, which need to be mo<strong>de</strong>led, are the quantities that account<br />

for the influence of the small structures on the entire physical system. LES system of<br />

equations for reactive flows may vary somehow with respect to Eq. (2.10) - Eq. (2.13) due to<br />

the combustion mo<strong>de</strong>l applied. As an example in the Thickened Flame combustion mo<strong>de</strong>l TF<br />

[11, 17, 74], viscous terms (as for instance the filtered diffusive species flux ¯J j,k and the filtered<br />

heat flux ¯q i ) and notably the filtered chemical reaction rate ¯˙ω k are weighted by several factors<br />

in or<strong>de</strong>r to account for the ‘new’ thickness of the flame.<br />

Large Eddy Simulation has become an important tool for the simulation and post-processing<br />

analysis of turbulent flows. It offers the best promise in the foreseeable future for the estimation<br />

of noise from flows at Reynolds numbers of interest in both open and closed systems. In<br />

aeroacoustics, LES plays an important role in the study of aerodynamical generated noise of<br />

numerous practical cases that range from air jets, high-lift <strong>de</strong>vices or landing gears in an aircraft<br />

to the rear-view mirror of a car or the bla<strong>de</strong>s of a wind turbine [65, 8]. In reactive flows,<br />

LES has been successfully applied to partially premixed and non-premixed open flames [70, 36]

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