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22/*! @brief class Source_Diffusion_croisee_echelle_temp_taux_diss_turb
23 *
24 * Terme de diffusion croisee dans l'equation de transport de tau (tau = 1 / omega) ou de omega dans les modeles de turbulence k-tau et k-omega
25 * Cd = sigma_d * alpha * rho *tau * min(grad k, grad tau, 0)
26 *
27 * la phase dont la turbulence est decrite avec le modele k-tau doit etre ecrite en premier dans le bloc phases { } du jeu de donnees
28 * Actuellement k et tau sont necessairement scalaires.
29 * Si cela est amene a evolue pour permettre de la turbulence dans plusieurs phases, il faudra alors revoir cette classe en iterant sur les id_composites des phases turbulentes.
30 * en l'etat, si plusieurs phases sont turbulentes et sont decrites par le modele k-tau, alors elles doivent se suivre dans le bloc phases { } du jeu de donnees
43doublesigma_d_ = 0.; // Kok and Spekreijse (2000) Efficient and accurate implementation of the k-omega turbulence model in the NLR multi-block Navier-Stokes system