Abstract
In the present study, the prediction accuracy of a dynamic one-equation sub-grid scale model for the large eddy simulation of dispersion around an isolated cubic building is investigated. For this purpose, the localized dynamic \(k_\mathrm{SGS} \)-equation model (LDKM) is employed and the results are compared with the available experimental data and two other classic sub-grid scale models, namely, standard Smagorinsky–Lilly model (SSLM) and dynamic Smagorinsky–Lilly model (DSLM). It is shown that the three SGS models give results in good agreement with experiment. However, near the ground level of the leeward wall, dimensionless time-averaged concentration, \(\langle K\rangle \), profile is not quite similar to the experimental data. It is also demonstrated that the LDKM predicts the values of \(\langle K\rangle \) on the roof, leeward and side walls more acceptably than the SSLM and DSLM. Whereas, the streamwise elongation of time-averaged structures of the plume shape is more over-estimated with the LDKM than with the other two SGS models. In terms of numerical difficulty, the LDKM is found to be stable and computationally reasonable. In addition, it does not suffer from a flow dependent constant such as the Smagorinsky coefficient employed in the SSLM model.
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Abbreviations
- \(\langle \;\rangle \) :
-
Time-averaged value
- c:
-
Concentration
- \(C_D\) :
-
Dynamic coefficient in dynamic Smagorinsky–Lilly model
- \(C_\mu =0.09\) :
-
Constant
- \(C_s\) :
-
Smagorinsky model constant
- \(C_\tau \) :
-
Dynamic coefficient in localized dynamic \(k_\mathrm{SGS} \)-equation model
- CFL:
-
Courant–Friedrichs–Lewy number
- \(D_m\) :
-
Molecular diffusion coefficient
- \(D_\mathrm{SGS}\) :
-
Sub-grid scale turbulent diffusivity
- \(\overline{c}\) :
-
Filtered Concentration
- I:
-
Turbulence intensity
- \(J_j^\mathrm{SGS}\) :
-
SGS scalar flux
- k:
-
Turbulence kinetic energy
- K:
-
Dimensionless concentration
- \(k_\mathrm{SGS} \) :
-
Sub-grid scale turbulence kinetic energy
- \(L_{ij}\) :
-
Leonard stress tensor
- \(Q_x^C =\langle \overline{u} _i \rangle \langle \overline{c} \rangle \) :
-
Convective flux in streamwise direction
- \(Q_x^T =\langle \overline{{u}'} _i \overline{{c}'} \rangle +J_i^\mathrm{SGS}\) :
-
Turbulent flux in streamwise direction
- \(S_{ij}\) :
-
Rate of strain tensor
- \(Sc_\mathrm{SGS}\) :
-
Sub-grid scale turbulent Schmidt number
- \(t^*=t / T, T={H_b } /U_b\) :
-
Dimensionless time
- \(T_{ij} \) :
-
Subtest scale stress tensor
- \({u}',\;{v}'\) and \({w}'\) :
-
Velocity fluctuation components
- \(u_\tau \) :
-
Friction velocity
- \(U_b =3.3\, \mathrm{m/s}\) :
-
Velocity at the building height
- \(U_e =0.63\, \mathrm{m/s}\) :
-
Velocity of effluent
- \(U_\infty =4.5 \, \mathrm{m/s} \) :
-
Free stream velocity (mean velocity at \(y=\delta )\)
- \(y^+\) :
-
Dimensionless wall distance
- \(y_p^+\) :
-
\(y^+\) At the first point from the wall
- \(\kappa =0.41\) :
-
Von Karman constant
- \(\Delta \) :
-
Grid filter width
- \(\widehat{\Delta }\) :
-
Test filter width
- \(\varepsilon \) :
-
Turbulence dissipation rate
- \(\lambda _{uu-z}\) :
-
Integral length scale based on streamwise velocity fluctuation in z direction
- \(\lambda _{vv-z}\) :
-
Integral length scale based on normal velocity fluctuation in z direction
- \(\lambda _{ww-z}\) :
-
Integral length scale based on spanwise velocity fluctuation in z direction
- \(\lambda _{ww-x}\) :
-
Integral length scale based on spanwise velocity fluctuation in x direction
- \(\upsilon _\mathrm{SGS}\) :
-
Sub-grid scale eddy viscosity
- \(\tau _{ij}\) :
-
SGS stress tensor
- \(\xi =x^A-x^B\) :
-
Separation distance between points A and B
- \('\) :
-
Fluctuation component
- C:
-
Convective flux
- T:
-
Turbulent flux
- rms:
-
Root-mean-squared
- SGS:
-
Sub-grid scale
- test:
-
Test filter
- x :
-
Streamwise direction
- y :
-
Normal direction
- z :
-
Spanwise direction
- \(-\) :
-
Filtered
- \(\widehat{a}\) :
-
Test filtered
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Bazdidi-Tehrani, F., Jadidi, M. Large eddy simulation of dispersion around an isolated cubic building: evaluation of localized dynamic \(k_\mathrm{SGS}\)-equation sub-grid scale model. Environ Fluid Mech 14, 565–589 (2014). https://doi.org/10.1007/s10652-013-9316-1
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DOI: https://doi.org/10.1007/s10652-013-9316-1