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1 Spatial Modelling of the Terrestrial Environment - Georeferencial

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Fireline Intensity and Biomass Consumption in Wildland Fires 181<br />

tropical savanna environments, where average intensities <strong>of</strong> c. 8000 kW m −1 have been<br />

noted (Williams et al., 1999). However, <strong>the</strong>se may be best regarded as maximum potential<br />

estimates as <strong>the</strong>y appear to (tacitly) assume complete combustion <strong>of</strong> <strong>the</strong> entire fuel load<br />

and are dependent on <strong>the</strong> accuracy with which <strong>the</strong> rate <strong>of</strong> fire spread is ei<strong>the</strong>r modelled<br />

or measured. Byram (1959) believes that fireline intensities could realistically be expected<br />

to vary from 15 to 100 000 (!) kW m −1 ; <strong>the</strong> primary uncertainties in <strong>the</strong>ir estimation<br />

being <strong>the</strong> rate <strong>of</strong> spread <strong>of</strong> <strong>the</strong> flaming front, followed by <strong>the</strong> fuel consumption and finally<br />

<strong>the</strong> estimation <strong>of</strong> <strong>the</strong> low heat <strong>of</strong> combustion. These huge extremes <strong>of</strong> fireline intensity<br />

described by Byram (1959) have been documented in, for example, wildfires in <strong>the</strong> Canadian<br />

forests (Alexander, 1982) and provide clear evidence as to <strong>the</strong> widely varying nature <strong>of</strong> this<br />

parameter.<br />

Given <strong>the</strong> potential importance <strong>of</strong> accurately estimating fire intensity for a range <strong>of</strong><br />

applications, and <strong>the</strong> inherent difficulties and uncertainties involved with estimating it in<br />

<strong>the</strong> field, <strong>the</strong>re is a pressing need for remote sensing methods for calculating this parameter.<br />

In terms <strong>of</strong> <strong>the</strong> remotely sensed measurement <strong>of</strong> fire-related energy emission and fire<br />

intensity, only <strong>the</strong> fraction <strong>of</strong> <strong>the</strong> liberated energy (I ) that is radiated away from <strong>the</strong> fire<br />

is available to be detected by a remote sensing device. However, if this fraction is known,<br />

because equation (1) relates <strong>the</strong> rate <strong>of</strong> heat release (kW m −1 ) to <strong>the</strong> rate at which biomass is<br />

combusted by <strong>the</strong> fire (kg m −2 × m sec −1 ), <strong>the</strong>re exists <strong>the</strong> possibility <strong>of</strong> estimating <strong>the</strong> rate<br />

at which vegetation is consumed in <strong>the</strong> fire via observations <strong>of</strong> <strong>the</strong> radiant energy produced<br />

(both measures being per unit length <strong>of</strong> <strong>the</strong> fire front in this case). Fur<strong>the</strong>rmore, since it is<br />

expected that such biomass combustion estimates are likely to be strongly correlated to <strong>the</strong><br />

rate at which emissions <strong>of</strong> trace gases and aerosols are produced (Kaufman et al., 1996),<br />

if sufficient radiant energy observations are available and can be integrated over <strong>the</strong> fire’s<br />

lifetime, <strong>the</strong>n in <strong>the</strong>ory <strong>the</strong> total amount <strong>of</strong> radiative energy released can be calculated and<br />

used to estimate <strong>the</strong> total amount <strong>of</strong> biomass consumed.<br />

Perhaps surprisingly, estimation <strong>of</strong> biomass consumption (a first-order fire effect) has not<br />

been a prime concern <strong>of</strong> researchers involved with modelling fire behaviour and dynamics<br />

(Reinhardt et al., 2001), with much more effort placed on developing physical models <strong>of</strong><br />

fire spread and intensity (reviewed by Perry, 1998, and see Perry et al., 1999, for an example).<br />

Initial attempts at measuring fireline intensity using remote sensing were made<br />

via airborne sensors. For example, Budd et al. (1997) modelled head-fire intensity over a<br />

series <strong>of</strong> experimental bushfires in Australian eucalyptus forests using airborne IR imagery<br />

to measure <strong>the</strong> speed <strong>of</strong> fire propagation. They estimated that <strong>the</strong> head-fire intensity (averaged<br />

over 6 minutes) exceeded 1000 kW per metre <strong>of</strong> fire front (kW m −1 ) for most <strong>of</strong> <strong>the</strong><br />

fires when <strong>the</strong>y were at <strong>the</strong>ir most intense, and ranged as high as 3280 kW m −1 . Kaufman<br />

et al. (1998a) used <strong>the</strong> Moderate Resolution Imaging Spectroradiometer (MODIS) Airborne<br />

Simulator to measure <strong>the</strong> rate <strong>of</strong> release <strong>of</strong> <strong>the</strong>rmal energy from spreading cerrado<br />

fires in Brazil, and went on to successfully relate <strong>the</strong> integral <strong>of</strong> this parameter to <strong>the</strong> rate<br />

<strong>of</strong> generation <strong>of</strong> <strong>the</strong> burn scar, which was believed proportional to <strong>the</strong> rate <strong>of</strong> biomass<br />

consumption. The strong relationship between <strong>the</strong>se parameters (r 2 = 0.97, n = 21) supported<br />

<strong>the</strong> idea <strong>of</strong> using such radiative energy measures to directly estimate <strong>the</strong> amount <strong>of</strong><br />

biomass combusted and Kaufman et al. (1998a) found that <strong>the</strong> relationship between FRE<br />

and <strong>the</strong> change in burn scar size was four times stronger than that between simple fire size<br />

and <strong>the</strong> rate <strong>of</strong> change <strong>of</strong> <strong>the</strong> burn scar. This clearly illustrated <strong>the</strong> improvement provided<br />

when <strong>the</strong> actual energy emission from <strong>the</strong> fires was considered.

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