An experimental investigation and statistical characterization of intermittent flame ejecting behavior of enclosure fires with an opening

Enclosure fires with an opening are commonly distinguished by two distinct phases namely, internal combustion with no flames ejected out (over-ventilated conditions), and internal combustion extending to external combustion having flames continuously ejected outside (under-ventilated conditions). A transitional phase not previously reported is investigated in this paper with flames being ejected out intermittently with a certain probability. Experiments were carried out in a 0.8 m cubic enclosure for seven different opening geometries. A Liquefied Petroleum Gas (LPG) porous gas burner was used as a fire source with fuel supply rate controlled by a flow meter. The intermittent ejection of flames was recorded by a digital CCD camera. The fraction of the time that the flames are outside the opening is defined as a probability, P. It is found that this probability P increases with the increase in fuel supply rate above a lower critical value (at P = 0) until an upper critical value (at P = 1). These critical lower and upper fuel supply rates or equivalently the corresponding total heat release rates (HRRs), are well correlated using the so called ventilation factor ( A H ) of the enclosure, where A is the area of the opening and H is height with length scales in meter. The ventilation factor ( A H ) is proportional to the rate of air mass inflow for under-ventilated conditions. The values of the lower and upper critical HRR in excess of 1500 A H (kW) (corresponding to heat released inside at under-ventilated conditions) are normalized by a characteristic HRR value applicable for the specific opening geometry. It is proposed that the intermittent ejection of flames is due to the probability of ignition and buoyant turbulent fluctuation of gases ejected from the opening which are affected by both the excess fuel amount and the temperature inside the enclosure which is equal to the temperature of the gases exiting the enclosure. Consequently, a simple mathematical model quantifies the ejection probability P as a function of normalized excess HRR Q ˙ ex ∗ and opening factor parameter A H / A T , where A T is the total exposed surface area of the enclosure. Indeed, the first parameter Q ˙ ex ∗ is related to the excess fuel amount that is ejected outside the enclosure as the conditions change from over-ventilated to under-ventilated, whereas the second parameter A H / A T is related to the heat losses to the wall which together with the heat released inside the encl