Numerical simulations of full-scale enclosure fires in a small compartment with natural roof ventilation
Introduction
In [1], an analysis of an experimental study of full-scale fire tests in a small compartment with a roof opening for natural ventilation is presented. Correlations are presented in [1] of the hot smoke layer thickness and average temperature rise as a function of the total fire heat release rate, roof opening area and fire source area. Three manual calculation methods [2], [3], [4], widely used in the design of smoke and heat exhaust ventilation systems, were evaluated. To that purpose, an estimate had to be made of the total smoke mass flow rate out of the compartment.
The major aim of the present study is to provide insight in the flow phenomena inside the compartment, by means of computational fluid dynamics (CFD) simulations. Therefore, numerical simulation results are presented for all the configurations experimentally studied in [1]. These simulations contain by far more detailed information than the experimental temperature measurements. They provide insight into the entrainment mechanism in the plume, so that the entrainment models of the manual calculation methods [2], [3], [4] can be evaluated.
The NIST code fire dynamics simulator (FDS) [5] is applied. First, it is verified that the mean temperatures and hot smoke layer thickness values, obtained from the CFD simulations, agree well with the experimental data, indicating that the simulation results are reliable. Next, the influence of the thermal wall boundary conditions and the grid sensitivity of the results are investigated.
Finally, two-zone model calculation results are also discussed, by means of the program OZONE [6].
Section snippets
Description of the configurations
Fig. 1 shows the compartment geometry as a ‘Smokeview’ picture. A complete description is provided in [1]. The dimensions are 3.6×3.0×2.3 m with a door opening (0.9×2.0 m) in the middle of the front wall. The two openings in the roof are of size 0.75×1 m each (one opening is covered in Fig. 1). They are centrally positioned around x=1.8 m. The distance between the roof opening centers and the front wall is 1 m. The fire source is positioned in the center of the compartment at 0.3 m height. Two fire
General observations
Fig. 2 shows mean temperature profiles reported as the hot smoke temperature rise with respect to ambient conditions (Ts−Tamb). As in [1], averages are taken over the three thermocouple trees behind the burner. All profile shapes are similar, with a plateau of relatively low temperature below the height z=1.2 m (cold lower layer).
Clearly, the same trends are observed in the simulation results (lines) as in the experiments (symbols). In each figure, the temperatures increase as the fire heat
Conclusions
Numerical simulations have been discussed for large-scale fire tests in a small compartment with a door opening and a ventilation opening in the roof.
CFD simulation results, obtained with FDS, have been presented. The following experimental observations of [1] have been confirmed:
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The hot layer average temperature rise (Ts,av−Tamb) increases almost linearly with the total fire heat release rate , because the total smoke mass flow rate out of the compartment is hardly affected.
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(Ts,av−Tamb)
Acknowledgments
This research was partly financed by Ghent University—UGent, through BOF Project 011/013/04.
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