Critical velocity in ventilated tunnels in the case of fire plumes and densimetric plumes

Publication date: Available online 17 September 2018

Source: Fire Safety Journal

Author(s): Lei Jiang, Mathieu Creyssels, Antoine Mos, Pietro Salizzoni

Abstract

We focus on the critical velocity in longitudinally ventilated tunnels and on its dependence on the power of the fire source. In particular we aim at identifying the reason for the appearance of the so-called ‘super-critical’ velocity, a ventilation velocity that becomes independent of the heat release rate as this latter becomes large. A critical review of existing literature studies allows us to point out possible explanations for this peculiar phenomenon. Among these, we focus here on effects related to heat fluxes (diffusive and radiative) and to the presence of large (compared to the tunnel height) flames. To enlighten the role of these phenomena, our approach is that of systematically compare the critical velocities as induced, for a given heat release rate, by densimetric plumes and fire plumes. The study is conducted by combining experimental, numerical and theoretical methods. The experiments were performed in a reduced-scale tunnel using densimetric plumes (air/helium mixture and hot air). Numerical simulations were performed with Fire Dynamics Simulator (FDS) and concerned densimetric plumes and fire plumes (propane). These show that the diffusive heat fluxes at the tunnel walls affect only marginally the critical ventilation. Similar conclusions can be drawn for the role of the radiative fluxes. The results also show that plumes arising from small fires can be reliably modelled as buoyant densimetric plumes released at ground level. In these cases the critical velocity increases with the one-third power of the heat release rate. The flow dynamics (and therefore the critical velocity) induced by larger fires is instead different. Notably, the occurrence of large flames (i.e. larger than the tunnel half-height) represent a source of distributed buoyancy, located downwind of the injection of flammable gases. Their presence induces the critical velocity to become almost independent on the heat release rate.

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