UFR 1-07 Evaluation: Difference between revisions

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be an adequate estimate for engineering purposes, although the axial
be an adequate estimate for engineering purposes, although the axial
velocity in this case was overpredicted by nearly a factor of two.  
velocity in this case was overpredicted by nearly a factor of two.  
[[Image:UFR1-07_fig11.png|center]
<center>'''Figure 11 '''&nbsp;Boundary conditions for the O&lsquo;Hern&nbsp;''et al.''&nbsp;[[UFR_1-07_References#4|[4]]] experiments.</center>





Revision as of 19:05, 12 July 2010


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Unsteady Near-Field Plumes

Underlying Flow Regime 1-07


Comparison of DesJardin et al. [1] CFD Calculations with Experiments

Figure 11 shows a snapshot of the flow field predicted by the CFD model of DesJardin et al. [1]. With the coarse grid, the plume puffing frequency was found to be approximately 1.8 Hz, much higher than the frequency measured in the experiments of 1.37 Hz. The predictions improved as the grid was refined, with the fine grid producing a frequency of 1.5 Hz. A similar frequency was obtained with or without an SGS model. DesJardin et al. [1] also presented results from a simulation with no SGS model and a very coarse mesh (220k nodes in total and only 30 cells across the source diameter). This produced a puffing frequency of 1.7 Hz, which they considered to be an adequate estimate for engineering purposes, although the axial velocity in this case was overpredicted by nearly a factor of two.


[[Image:UFR1-07_fig11.png|center]

Figure 11  Boundary conditions for the O‘Hern et al. [4] experiments.


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Contributed by: Simon Gant — UK Health & Safety Laboratory

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