DNS 1-2 Quantification of Resolution: Difference between revisions

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|[[Image:Channel_turbulent_stress.png|400px]]
|[[Image:Channel_turbulent_stress.png|400px]]
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|'''Figure 3:''' Average streamwise velocity, <math>Re_\tau=180</math>,  vs data from Moser et al. (1999)                           
|'''Figure 3:''' Turbulent stress profiles                           
|}
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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.
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">
<gallery widths=250px heights=200 caption="Figure 4: Near wall turbulent stress" mode="packed-hover">
Image:Near_wall_uu.png|<math>\widetilde{u^{\prime\prime} u^{\prime\prime}}</math>
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_vv.png|<math>\widetilde{v^{\prime\prime} v^{\prime\prime}}</math>
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</gallery>
</gallery>


One way to verify that the DNS are properly resolved is to examine the residuals of the Reynolds-
The turbulent kinetic energy budget across the channel is also compared with data from Moser et al. [[lib:DNS_1-2_quantification_#figure5|(Fig. 5)]]. The dashed black line denotes the residual of the budget.
stress budget equations. These residuals are among the statistical volume data to be provided as
<div id="figure5"></div>
described in Statistical Data section.
{|align="center"
|[[Image:Channel_turbulent_energy_budget.png|400px]]
|-
|'''Figure 5:''' Turbulent kinetic energy budget.                            
|}
<br/>
<br/>
----
----
{{ACContribs
{{ACContribs
| authors=Lionel Agostini
| authors=Arun Soman Pillai
| organisation=Imperial College London
| organisation=Imperial College London
}}
}}

Revision as of 12:47, 7 October 2021


Front Page

Description

Computational Details

Quantification of Resolution

Statistical Data

Instantaneous Data

Storage Format

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.

Average u logscale.png
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.

Channel turbulent stress.png
Figure 3: Turbulent stress profiles

The expected near wall behaviour of turbulent stresses are and . These stresses near the wall from the current set of simulations are shown below.

The turbulent kinetic energy budget across the channel is also compared with data from Moser et al. (Fig. 5). The dashed black line denotes the residual of the budget.

Channel turbulent energy budget.png
Figure 5: Turbulent kinetic energy budget.




Contributed by: Arun Soman Pillai — Imperial College London

Front Page

Description

Computational Details

Quantification of Resolution

Statistical Data

Instantaneous Data

Storage Format


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