EGU25-1889, updated on 14 Mar 2025
https://doi.org/10.5194/egusphere-egu25-1889
EGU General Assembly 2025
© Author(s) 2025. This work is distributed under
the Creative Commons Attribution 4.0 License.
Oral | Tuesday, 29 Apr, 09:25–09:35 (CEST)
 
Room 0.96/97
Physics-based simulation of extreme wildfire behavior on sloping terrain
Gilbert Accary1 and Dominique Morvan2
Gilbert Accary and Dominique Morvan
  • 1Lebanese American University, School of Engineering, Industrial and Mechanical Engineering Department, Byblos, Lebanon (gilbert.accary@lau.edu.lb)
  • 2Aix-Marseille University, CNRS, Centrale Marseille, M2P2, Marseille, France (dominique.morvan@univ-amu.fr)

Wildfires pose a significant threat to ecosystems, human lives, and property, especially in regions characterized by variable topography. This work delves into the complexities of wildfire behavior on sloping terrain, where the combined effect of crosswind and slope acting in the same direction substantially influence fire behavior, rate of spread, and fire intensity. Fire regime depends on Byram’s convective number that was modified to account for slope effect according to Eq. 1 (Morvan and Accary 2024), where I is the fire intensity, g is Earth’s gravity, α is the slope angle, ρ and Cp are respectively air density and specific heat at the ambient temperature T0, R is the rate of fire spread and Ue is the effective wind speed that includes the component of buoyancy characteristic-velocity acting in the direction of fire propagation. For steep slopes, this correction results in a convective number that is significantly different from the formulation proposed by Nelson (2015).

           (1)

To test the effectiveness of the proposed Byram’s number expression, Large Eddy Simulations of shrubland fires are carried out using a 3D fully-physical CFD fire simulator (FireStar3D) under various terrain slopes and prevailing crosswind speeds, covering both wind-driven fire regime (NC < 2) and plume-dominated one (NC > 10). Results show that the proposed modification of Byram’s convective number allows a better description of the obtained fire regime. In addition to the numerical simulations, a database consisting of 11 experimental fires carried out in shrublands was used to support the use of the new convective number formula. The heat transfer mechanisms governing fire propagation are described, highlighting in particular the role played by the convective cooling of unburnt vegetation in the case of a plume-dominated fire as the fire draws an adverse air flow in the opposite direction of fire propagation (see Fig. 1).

Furthermore, the development of fire-induced wind and its action on fire behavior is investigated and compared to field data gathered during an experimental shrubland fire on a sloping terrain. Simulations were carried out for three lengths of the ignition line: 30 m (as in the experiment), 90 m, and quasi-infinite fire line simulated using periodic boundary conditions. Results show that fire-induced wind is only significant in the case of a wide fire-front. As the length of the ignition line increases, the interaction between this induced wind and the fire front can change the fire regime from plume-dominated fire to a wind-driven one. 

Fig. 1. Temperature field and streamlines obtained in the vertical median plane of a plume-dominated fire, 90 s after ignition, in the case of 10° slope, an initial crosswind speed of 0.5 m/s, and quasi-infinite fire front. Earth-gravity direction is indicated by an arrow.

How to cite: Accary, G. and Morvan, D.: Physics-based simulation of extreme wildfire behavior on sloping terrain, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-1889, https://doi.org/10.5194/egusphere-egu25-1889, 2025.