This document discusses modeling wildfire behavior and surface-atmosphere interactions. It covers:
1. The challenges of modeling wildfires due to their multi-physics, multi-scale nature and complex interactions between surface fires and atmospheric conditions.
2. The author's PhD research which used data assimilation to reduce uncertainties in regional-scale wildfire spread modeling and multi-physics CFD simulations to study flame-scale processes.
3. The current state-of-the-art in coupled fire-atmosphere modeling including strategies for coupling models, accounting for atmospheric emissions, and offline simulation cases.
1. Towards more accurate predictions of
wildfire behavior
Modeling surface/atmosphere interactions
Mélanie ROCHOUX, Ph.D.
Postdoctoral fellow
Meteorological Research Division
Introductory seminar
13 June 2014
Environnement
Canada
Environment
Canada
2. ①➀ INTRODUCTION: Regional-scale modeling viewpoint
• Fire danger
• Multi-physics multi-scale problem
• Regional-scale modeling viewpoint
➁ Ph.D. RESEARCH: How to address modeling uncertainties?
• Data assimilation at regional scale
• Multi-physics simulation at flame scale
➂ STATE-OF-THE-ART: Fire/atmosphere coupling
• Coupling strategy
• Atmospheric emissions
• Offline simulation case
OUTLINE
Introductory seminar 2
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
4. INTRODUCTION ● ● ●
Fire danger at operational level
Fine fuel moisture
code (FFMC)
Duff moisture
code (DMC)
Drought Code
(DC)
FUEL
MOISTURE
CODES
FIRE WEATHER
OBSERVATION
S
FIRE
BEHAVIOR
INDICES
Air temperature
and humidity,
wind, 24-h rainfall Wind
Air temperature
and humidity, 24-
h rainfall
Air temperature,
24-h rainfall
Initial spread
index (ISI)
Buildup index
(BUI)
Fire weather index (FWI)
4
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
• Canadian Forest Fire Weather Index System
• Fire Weather Index (FWI) ➙ numerical rating of fire potential intensity
• Daily maps of fire weather
• Main limitation ➙ meteorological index
➙ cwfis.cfs.nrcan.gc.ca/home
5. INTRODUCTION ● ● ●
Fire danger at operational level
Fine fuel moisture
code (FFMC)
Duff moisture
code (DMC)
Drought Code
(DC)
FUEL
MOISTURE
CODES
FIRE WEATHER
OBSERVATION
S
FIRE
BEHAVIOR
INDICES
Air temperature
and humidity,
wind, 24-h rainfall Wind
Air temperature
and humidity, 24-
h rainfall
Air temperature,
24-h rainfall
Initial spread
index (ISI)
Buildup index
(BUI)
Fire weather index (FWI)
5
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
• Canadian Forest Fire Weather Index System
• Fire Weather Index (FWI) ➙ numerical rating of fire potential intensity
• Daily maps of fire weather
• Main limitation ➙ meteorological index
DMC: loosely compacted decomposing matter
-nominal depth 7 cm
DC: deep compact organic matter
-nominal depth 18 cm
FFMC: litter and other fine fuels
-nominal depth 1.2 cm
From Chelene Krezek-Hanes,
Great Lakes Forestry Centre,
Canadian Forest Service
➙ cwfis.cfs.nrcan.gc.ca/home
9. ①➀ INTRODUCTION: Regional-scale modeling viewpoint
• Fire danger
• Multi-physics multi-scale problem
• Regional-scale modeling viewpoint
➁ Ph.D. RESEARCH: How to address modeling uncertainties?
• Data assimilation at regional scale
• Multi-physics simulation at flame scale
➂ STATE-OF-THE-ART: Fire/atmosphere coupling
• Coupling strategy
• Atmospheric emissions
• Offline simulation case
OUTLINE
Introductory seminar 9
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
10. PH.D. RESEARCH ● ● ●
Modeling limitations
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
• ISSUE: How to accurately describe wildfire spread?
10
Rochoux M.C., Ph.D.
Ecole Centrale Paris
(2014)
• OBJECTIVE: Quantify and reduce uncertainty in ROS modeling
Data assimilation for
REGIONAL-SCALE wildfire
spread forecast
Environmental conditions
Fire front locationPhysics-based modeling
FLAME-SCALE multi-physics
CFD simulations
11. PH.D. RESEARCH ● ● ●
Data assimilation for regional-scale forecast
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
11
Environmental conditions
Fire front location
• Anisotropy in wildfire spread
➙ complex spatial correlations along the fireline
• Highly non-linear observation operator
➙ complex relationship between ROS model
parameters and model counterparts of
observations
Simulated
front
Observed
front
(x1
, y1
)
(x2
, y2
)
(x3
,y3
)
(x4
, y4
)
(x1
O
,y1
O
)
(x2
O
,y2
O
)
Distance
between fronts
FIREFLY
wildfire spread
simulator
Parameters
Initial condition
Boundary conditions
Comparison
Simulated fronts
Observations
12. PH.D. RESEARCH ● ● ●
Data assimilation for regional-scale forecast
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
12
Environmental conditions
Fire front location
• Parameter estimation
➙ temporal variability of the errors in the ROS
model parameters (mid- to long-term)
➙ reduced-cost approach (Polynomial Chaos)
• State estimation
➙ persistence of the correction of the model initial
condition (short-term)
Simulated front
Observed
front
(x1
, y1
)
(x2
, y2
)
(x3
,y3
)
(x4
, y4
)
(x1
O
,y1
O
)
(x2
O
,y2
O
)
FIREFLY
wildfire spread
simulator
Parameters
Initial condition
Boundary conditions
Comparison
Simulated fronts
Observations
Ensemble Kalman filter
Parameter estimation
State estimation
Analysis
13. PH.D. RESEARCH ● ● ●
Data assimilation for regional-scale forecast
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
13
EnKF analysis of synthetic observations + of fire front
FORECAST
True location
Ensemble members
ANALYSIS True location
Ensemble members
observations
Ensemble generation for state estimation
➙ Anisotropy in wildfire spread
➙ Selection of spatially-distributed biomass
fuel properties and distinct wind conditions
between the ensemble members.
Approach relevant for incomplete
observations due to:
➙ opacity of the thermal plume
➙ limited monitoring
14. PH.D. RESEARCH ● ● ●
Data assimilation for regional-scale forecast
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
14
Controlled grassland fire experiment
x [m]
y [m]
Extraction of the 600 K
iso-temperature at 14-s
time intervals
1min32s50s 1min46s1min04s 1min28s
Time
FRONT
Wind 1m/s
15. PH.D. RESEARCH ● ● ●
Data assimilation for regional-scale forecast
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
15
Controlled grassland fire experiment
state
parameter
state
parameter
state
parameter
• STATE ESTIMATION: non-uniform
correction of the fire front
• PARAMETER ESTIMATION: mean
correction along the fireline
ANALYSIS PERFORMANCE
ANALYSIS
FORECAST
16. ①➀ INTRODUCTION: Regional-scale modeling viewpoint
• Fire danger
• Multi-physics multi-scale problem
• Regional-scale modeling viewpoint
➁ Ph.D. RESEARCH: How to address modeling uncertainties?
• Data assimilation at regional scale
• Multi-physics simulation at flame scale
➂ STATE-OF-THE-ART: Fire/atmosphere coupling
• Coupling strategy
• Atmospheric emissions
• Offline simulation case
OUTLINE
Introductory seminar 16
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
17. ➙ anridea.univ-corse.fr/
➙ OBJECTIVE: develop a
coupled fire-atmosphere
simulation prototype
Biomass thermal
degradation
VEGETATION
SCALES
Combustion
processes
Surface/atmosphe
re interactions
FLAME SCALE
ATMOSPHERIC
SCALES
Atmospheric
dynamics and
emissions
FIRE/ATMOSPHERE MODEL ● ● ●
Coupling strategy 17
INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
18. INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
FIRE/ATMOSPHERE MODEL ● ● ●
Coupling strategy 18
• Lagrangian representation of the subgrid-scale fire front
Atmospheric
model grid size
(∼ 50 m)
VEGETATION
• Terrain data
• Distribution: using
CORINE ESA
database and forest
inventory (BDForêt)
➙ Sensible heat flux
➙ Water vapor flux
➙ Radiant temperature
➙WIND
•Interpolation at the
front markers
•assumed constant
over one model
time step
•1-D boundary
layer model (mid-
grid)
19. INTRODUCTORY SEMINAR May 2014Mélanie ROCHOUX
FIRE/ATMOSPHERE MODEL ● ● ●
Coupling strategy 19
• Introduction of a burning matrix
• Burning ratio Rb = ratio of the burning area over the atmospheric
grid area, ranging from 0 (no fire) to 1 (all burning).
• 1 value of burning ratio per atmospheric model grid box
SURFACE FLUXES REQUIRE:
• Nominal convection heat flux
• Nominal water loading
• Nominal flame temperature Tn (1000 K)
• Soil temperature from the atmospheric model Ts
➙ Sensible heat flux
➙ Water vapor flux
➙ Radiant temperature
FORMULATION OF THE EQUIVALENT RADIANT
TEMPERATURE Te:
Te
4 = (1 - Rb) Ts
4 + Rb Tn
4
20. INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
FIRE/ATMOSPHERE MODEL ● ● ●
Coupling strategy 20
• Limitations in surface wildfire spread modeling
• Physical modeling inaccuracies
➙ Heat transfer to vegetation
➙ Local and steady-state assumption (canyons)
• Absence of modeling for fire/atmosphere interactions
Favone wildfire (30 ha)
FOREFIRE
Coupled
Observed
Two-way fire/atmosphere coupling
FOREFIRE/MESO-NH
21. INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
FIRE/ATMOSPHERE MODEL ● ● ●
Atmospheric chemistry 21
• Emission sources
• Emissions during the biomass thermal degradation
(e.g. soot particles)
• Incomplete combustion
➙ Sensible heat flux
➙ Water vapor flux
➙ Radiant temperature
➙ Gas species emission
• Species emitted in the surface layer (injection model)
and mixed by the turbulence scheme (mainly CO)
• Distinction of flaming and smoldering modes of
combustion in the injection model
• Emission factor database still incomplete, in particular
for Mediterranean ecosystems
22. INTRODUCTORY SEMINAR June 13, 2014Mélanie ROCHOUX
FIRE/ATMOSPHERE MODEL ● ● ●
Atmospheric chemistry 22
• Transport and chemistry in the smoke plume
• No parameterization of the smoke injection height ➙ explicit calculation
• ReLACS chemical kinetic scheme used in MÉSO-NH (no aerosol scheme)
Fire/Surface
➙ Vegetation
➙ Topography
Fire/Atmosphere
➙ Dynamics
➙ Chemistry
Turbulence
Gases
& Aerosols
Wind
Case study : Lançon de Provence
(2005), Strada et al. 2012
23. SOURCES
➙ High-resolution biomass fuel
➙ Combustion
➙ Emission models
ATMOSPHERE
➙ Dynamics of the
smoke plume
➙ Chemistry (aerosols)
➙ Feedbacks on fire
Overview of fire research
OBSERVATIONS
➙ Detection
➙ Monitoring
Hinweis der Redaktion
Qu’est-ce qui fait que de grands feux peuvent se développer ?
Du feu de surface au feu de cimes
Formation d’un panache s’étendant sur plusieurs dizaines voire centaines de km
Difficile de stopper un très grand feu tel les megafires(favorisés par l’occurrence de plus en plus forte d’évènements extrêmes)
Pour éviter que les feux atteignent des dimensions qui les rendent incontrôlables, il faut pouvoir prévoir rapidement où le feu va se propager et ainsi optimiser la stratégie de terrain. Des prévisions fiables de propagation à l’échelle régionale seraient nécessaires, en terme de comportement du feu et aussi de changement de comportement sous l’effet du changement climatique.
the generation of the stochastic ensemble must represent the anisotropy in wildfire spread. This anisotropy was implicitly introduced in the SE ap- proach by selecting spatially-distributed biomass fuel properties and distinct wind conditions between the different members in the ensemble. The SE approach was shown to be successful at retrieving at low computational cost (i.e., with a relatively small number of members in the ensemble) the actual shape of the fire front in cases with strong anisotropic propagation conditions. This approach was also found relevant for observations made with significant errors and/or cases in which the observations are incomplete (e.g., when only a section of the fireline is informed), in order to reconstruct a complete, reliable initial condition for FIREFLY restart.
ISBA est trop "grossier" les données en entrée font des km enrésolution, du coup pas possible et distribution spécifique. Le faireen HR c'est l'objet principal de l'ANR firecaster.
Pour la caractérisation: données terrain (surface/volume... humiditéestimée (= f(humidité de l'air après 1 h pour le vegetal mort))
Pour la distribution spatiale : BDForêt / corine
http://inventaire-forestier.ign.fr/spip/spip.php?rubrique53
Modèle 1D de couche limite, vent mi-maille << approx pourrie etinjustifiable mais meilleure que la fausse hauteur de flamme que l'onpeut diagnostiquer, c'était un des objectifs (trop audacieux) del'étude AVBP/Firestar d'avoir une vue du volume de gaz pour unemeilleure estimation.
Equivalent heat flux (W/m2)
➙ Energy over the hot gaseous column
➙ Multiplication of the nominal convection heat flux by the burning ratio Rb
Water vapor mass flux (kg/m2/s)
➙ Multiplication of the nominal water loading by the burning ratio Rb
Equivalent radiant temperature
➙ Nominal flame temperature Tn (1000 K)
➙ Soil temperature from the atmospheric model Ts
(day temperature at ground level)
➙ Formulation of the radiant temperature Te (K):
Te4 = (1 - Rb) Ts4 + Rb Tn4
- No anthropogenic emissions considered
- No aerosol scheme
- All species are emitted in the first surface level in the model and mixed in the boundary layer by the turbulence scheme. There is no a-priori injection height. A passive tracer (referred to as fire aerosol-like tracer) has been introduced to mimic fire-produced PM10 aerosols. The fire aerosol-like tracer is initialized to zero and has a deposition velocity of 3 cm/s (Seung-Muk et al. 2006); it is only emitted above the fire.
- The simulated smoke plume was trapped within the boundary layer (injection height between 0.9 and 1.2km), a common feature of Mediterranean fires that mostly release emissions into the atmospheric boundary layer.
- The coupled model with simplified assumptions concerning emissions and initialization simulated an sharp increase of O3 precursors near the fire and a subsequent O3 depletion in the fire plume (over 40km) as well as a strong increase of a fire aerosol-like tracer at the proper timing compared to the observations. Production of O3 (over the sea) was simulated several kilometers downwind of the fire as already observed in field campaigns.
ISBA est trop "grossier" les données en entrée font des km enrésolution, du coup pas possible et distribution spécifique. Le faireen HR c'est l'objet principal de l'ANR firecaster.
Pour la caractérisation: données terrain (surface/volume... humiditéestimée (= f(humidité de l'air après 1 h pour le vegetal mort))
Pour la distribution spatiale : BDForêt / corine
http://inventaire-forestier.ign.fr/spip/spip.php?rubrique53
Modèle 1D de couche limite, vent mi-maille << approx pourrie etinjustifiable mais meilleure que la fausse hauteur de flamme que l'onpeut diagnostiquer, c'était un des objectifs (trop audacieux) del'étude AVBP/Firestar d'avoir une vue du volume de gaz pour unemeilleure estimation.
- No anthropogenic emissions considered
- No aerosol scheme
- All species are emitted in the first surface level in the model and mixed in the boundary layer by the turbulence scheme. There is no a-priori injection height. A passive tracer (referred to as fire aerosol-like tracer) has been introduced to mimic fire-produced PM10 aerosols. The fire aerosol-like tracer is initialized to zero and has a deposition velocity of 3 cm/s (Seung-Muk et al. 2006); it is only emitted above the fire.
- The simulated smoke plume was trapped within the boundary layer (injection height between 0.9 and 1.2km), a common feature of Mediterranean fires that mostly release emissions into the atmospheric boundary layer.
- The coupled model with simplified assumptions concerning emissions and initialization simulated an sharp increase of O3 precursors near the fire and a subsequent O3 depletion in the fire plume (over 40km) as well as a strong increase of a fire aerosol-like tracer at the proper timing compared to the observations. Production of O3 (over the sea) was simulated several kilometers downwind of the fire as already observed in field campaigns.