TRACE User Guide
TRACE Version 9.6.1
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For scale-resolving simulations, statistics can be computed using the command ComputeStatistics. They are computed as accumulating averages starting at the specified time step and stored in a separate CGNS file. For a generic fluctuating quantities \(\phi\) and \(\psi\), the moments are computed as follows:
\begin{equation} \overline \phi = \frac 1 N \sum_n^N \phi_n, \quad \phi = \overline \phi + \phi' \end{equation}
and Favre average\begin{equation} \tilde \phi = \frac{\overline{\rho \phi}}{\rhobar}, \quad \phi = \tilde \phi + \phi'' \end{equation}
\begin{eqnarray} \overline{\phi' \psi'} &=& \overline{\phi \psi} - \overline \phi \overline \psi \\ \widetilde{\phi'' \psi''} &=& \widetilde{\phi \psi} - \tilde \phi \tilde \psi \end{eqnarray}
The sub-grid stresses are computed based on the Boussinesq assumption (see Original model) and represent the modeled amount of Reynolds stresses. For LES simulations the expression
\begin{equation} \frac{2}{3} \rho^* k^* \delta_{ij} \end{equation}
disappears, because there is no modeled turbulent kinetic energy available (k=0).
Currently the following statistics can be computed.
Moment | CGNS variable name | Symbol | Description |
---|---|---|---|
First | Density | \(\rhobar\) | Reynolds-averaged density |
First | Pressure | \(\overline p\) | Reynolds-averaged pressure |
First | VelocityX/Y/Z | \(\tilde u_i\) | Favre-averaged velocity vector |
Second | ReynoldsStressXX/XY/XZ/YY/YZ/ZZ | \(\uu ij\) | Favre-averaged Reynolds stress tensor |
Second | ReynoldsStressSgsXX/XY/XZ/YY/YZ/ZZ | \(\uu ij_{SGS}\) | Favre-averaged Reynolds stress (SGS) tensor |
Second | PressureStrainXX/XY/XZ/YY/YZ/ZZ | \(\Pi_{ij} = \frac{1}{\rhobar} \overline{p' \left(\parfrac{u_i''}{x_j} + \parfrac{u_j''}{x_i}\right)}\) | Pressure-strain tensor |
Second | TurbulentDissipationXX/XY/XZ/YY/YZ/ZZ | \(\epsilon_{ij} = \frac{2}{\rhobar} \overline{\mu s^*_{kj} \parfrac{u_i''}{x_k} + \mu s^*_{ki} \parfrac{u_j''}{x_k}}\) | Turbulent dissipation tensor |
Third | SkewnessX/Y/Z | \(\frac{\widetilde{u_i''^3}}{\widetilde{u_i''^2}^{3/2}}\) | Normalized Skewness vector |
Fourth | FlatnessX/Y/Z | \(\frac{\widetilde{u_i''^4}}{\widetilde{u_i''^2}^{2}}\) | Normalized Flatness vector |
With the trace-free strain rate tensor
\[ s^*_{ij} = s_{ij} - \frac 1 3 s_{qq}, \quad s_{ij} = \frac 1 2 \left(\parfrac{u_i}{x_j} + \parfrac{u_j}{x_i}\right) \]