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Wind Erosion in Western Queensland Australia

Modelling Land Susceptibility to Wind Erosion in Western ... - Ninti One

Modelling Land Susceptibility to Wind Erosion in Western ... - Ninti One

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Chapter 3 – Modell<strong>in</strong>g Land Erodibility ReviewWEELS computes w<strong>in</strong>d erosion as hourly assessments (thr -1 ). The model can be used to maperosion risk <strong>in</strong> terms of the duration of erosive conditions and correspond<strong>in</strong>g maximumsediment transport rate. Simulated monthly and annual time series of w<strong>in</strong>d erosion conditionswere compared with data from test sites <strong>in</strong> England and Germany (Böhner et al., 2003).Spatial and temporal patterns of modelled w<strong>in</strong>d erosion were found to be <strong>in</strong> agreement withobservations of w<strong>in</strong>d erosion. However, no quantitative assessments of the modelperformance have been published.3.3.2 <strong>W<strong>in</strong>d</strong> <strong>Erosion</strong> Assessment Model (WEAM)The <strong>W<strong>in</strong>d</strong> <strong>Erosion</strong> Assessment Model (WEAM) was the first <strong>in</strong>tegrated model developed <strong>in</strong><strong>Australia</strong> to quantify w<strong>in</strong>d erosion rates (Shao et al., 1994). The model was designed tooperate at a moderate spatial resolution and predict dust emissions from the Murray-Darl<strong>in</strong>gBas<strong>in</strong> <strong>in</strong> south-eastern <strong>Australia</strong>. WEAM comb<strong>in</strong>ed current theories on the effects of climate,soil, vegetation and land use on w<strong>in</strong>d erosion.WEAM quantifies land erodibility through the threshold friction velocity, with erosionoccurr<strong>in</strong>g when u * > u *t . The model computes streamwise sediment flux (Q) and vertical dustflux (F). It uses the saltation model of Owen (1964), a sand transport equation, to compute Q,which is adjusted us<strong>in</strong>g soil particle size distributions. The w<strong>in</strong>d shear velocity (u * ) isdeterm<strong>in</strong>ed from climatic conditions and the surface roughness height (Shao et al., 1996). Thethreshold friction velocity is calculated as a function of soil particle size, frontal area <strong>in</strong>dex ofsurface roughness elements, soil moisture, and the hardness of the surface crust:( d ,w,c)ut( ds,0,0,0)( ) H ( w) M ( s)*u* t s, = (3.20)Rwhere u *t (d s , 0, 0, 0) was approximated from the model of Greeley and Iversen (1985), R(λ) isthe ratio the bare threshold velocity over the covered (rough) threshold velocity, H(w) is theratio of the threshold velocity of the wet surface over the threshold velocity of the dry surfaceand, M(s) is a mobility coefficient describ<strong>in</strong>g the <strong>in</strong>fluence of the state of soil aggregation andcrust<strong>in</strong>g, and the chemical b<strong>in</strong>d<strong>in</strong>g strength which ma<strong>in</strong>ta<strong>in</strong>s this state.83

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