DNS 1-2 Quantification of Resolution: Difference between revisions
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= Quantification of resolution = | = Quantification of resolution = | ||
==Mesh resolution== | ==Mesh resolution== | ||
Provide wall resolution in wall coordinates, both normally ("y+") and tangentially ("x+", "z+"). | The grid resolution corresponds to uniform <math>\Delta x^+=12.2,\ \Delta z^+=6.3</math> and ranges from <math>\Delta y^+=0.16</math> near the wall (first solution point) to <math>\Delta y^+=4.6</math> at the centre of the channel. The near-wall Kolmogorov length scale, <math>\eta=\left(\bar{\rho}\nu^3/\epsilon\right)^{1/4}</math>, in wall units is <math>\eta^+=1.54</math>. | ||
<!--Provide wall resolution in wall coordinates, both normally ("y+") and tangentially ("x+", "z+"). | |||
Evaluate typical turbulence length scales (Taylor microscale, Kolmogorov) and compare to local | Evaluate typical turbulence length scales (Taylor microscale, Kolmogorov) and compare to local | ||
resolution. In case the case presents homogeneous directions, one could also provide spatial | resolution. In case the case presents homogeneous directions, one could also provide spatial | ||
correlations between the velocity components. If possible provide computed temporal spectra at | correlations between the velocity components. If possible provide computed temporal spectra at | ||
selected locations and relate to spatial resolution e.g. by using Taylor's hypothesis. | selected locations and relate to spatial resolution e.g. by using Taylor's hypothesis.--> | ||
==Solution verification== | ==Solution verification== | ||
The solution accurately captures the near wall and log-law behaviour of averaged streamwise velocity profile as shown in [[lib:DNS_1-2_quantification_#figure2|Fig. 2]]. | |||
<div id="figure2"></div> | |||
{|align="center" | |||
|[[Image:Average_u_logscale.png|400px]] | |||
|- | |||
|'''Figure 2:''' Average streamwise velocity, <math>Re_\tau=180</math>, vs data from Moser et al. (1999) | |||
|} | |||
The turbulent stress profiles agree well with the data from Moser et al. | |||
<div id="figure3"></div> | |||
{|align="center" | |||
|[[Image:Channel_turbulent_stress.png|400px]] | |||
|- | |||
|'''Figure 3:''' Average streamwise velocity, <math>Re_\tau=180</math>, vs data from Moser et al. (1999) | |||
|} | |||
The expected near wall behaviour of turbulent stresses are <math>\widetilde{u^{\prime\prime2}},\widetilde{w^{\prime\prime2}}\sim y^2,\ \widetilde{v^{\prime\prime2}}\sim y^4</math> and <math>\widetilde{u^\prime v^\prime}\sim y^3</math>. These stresses near the wall from the current set of simulations are shown below. | |||
<gallery widths=300px heights=240 mode="packed-hover"> | |||
Image:Near_wall_uu.png|<math>\widetilde{u^{\prime\prime} u^{\prime\prime}}</math> | |||
Image:Near_wall_vv.png|<math>\widetilde{v^{\prime\prime} v^{\prime\prime}}</math> | |||
Image:Near_wall_ww.png|<math>\widetilde{w^{\prime\prime} w^{\prime\prime}}</math> | |||
Image:Near_wall_uv.png|<math>\widetilde{u^{\prime\prime} v^{\prime\prime}}</math> | |||
</gallery> | |||
One way to verify that the DNS are properly resolved is to examine the residuals of the Reynolds- | One way to verify that the DNS are properly resolved is to examine the residuals of the Reynolds- | ||
stress budget equations. These residuals are among the statistical volume data to be provided as | stress budget equations. These residuals are among the statistical volume data to be provided as |
Revision as of 11:59, 7 October 2021
Quantification of resolution
Mesh resolution
The grid resolution corresponds to uniform and ranges from near the wall (first solution point) to at the centre of the channel. The near-wall Kolmogorov length scale, , in wall units is .
Solution verification
The solution accurately captures the near wall and log-law behaviour of averaged streamwise velocity profile as shown in Fig. 2.
Figure 2: Average streamwise velocity, , vs data from Moser et al. (1999) |
The turbulent stress profiles agree well with the data from Moser et al.
Figure 3: Average streamwise velocity, , vs data from Moser et al. (1999) |
The expected near wall behaviour of turbulent stresses are and . These stresses near the wall from the current set of simulations are shown below.
One way to verify that the DNS are properly resolved is to examine the residuals of the Reynolds-
stress budget equations. These residuals are among the statistical volume data to be provided as
described in Statistical Data section.
Contributed by: Lionel Agostini — Imperial College London
© copyright ERCOFTAC 2024