Study of wood self-extinguishment with a double sliding cone calorimeter

The aim of the present work was to improve the study of wood self-extinguishment under cone calorimeter thanks to a dedicated experimental setup. A cone calorimeter was modified into a double sliding cone calorimeter in vertical orientation for studying samples extinguishment. With this new setup, the external heat flux can be quickly switched from a high to a low value seeking for the heat flux leading to the sample extinguishment. Samples were first submitted to different heat fluxes (60, 82.5 and 93.5 kW.m2) leading to auto-ignition. After different exposure times (6, 9, 15 and 18 min), the heat flux was suddenly reduced to a lower value (between 38.5 and 60 kW.m2) by sliding from one cone to the other one. All in all, 206 tests were performed varying heat fluxes and exposure time. This large number of test made it possible to carry out a statistic study and to deduce a critical Mass Loss rate and a critical heat flux for self-extinguishment. The critical heat flux for selfextinguishment varied from 44 to 51 kW.m 2 depending on the heat flux that was used to ignite the sample. These critical heat fluxes were found weakly dependent on the time during which the sample was exposed to the high flux. Time-to-extinguishment was between 40 s and 100 s. Mass Loss Rate Per Unit Area (MLRPUA) for which self-extinguishment occur was found to be equal to 3.95 g.m 2s 1 and this value is almost independent on experiment parameters (exposure time and heat flux).

Automated summary

The aim of this study was to improve the understanding of wood self-extinguishment using a modified cone calorimeter setup. By conducting 206 tests with varying heat flux and exposure time, critical heat flux and time-to-extinguishment were determined. The critical heat flux for self-extinguishment was found to be dependent on the ignition heat flux, while the time-to-extinguishment ranged from 40 to 100 seconds. The Mass Loss Rate Per Unit Area for self-extinguishment was consistent at 3.95 g.m2s1 regardless of experimental parameters.