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Wind Erosion in Western Queensland Australia

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

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Chapter 5 – Land Erodibility Model Developmentdetect erodible regions <strong>in</strong> arid and semi-arid <strong>Australia</strong> that are consistent with satellite andobservational records of w<strong>in</strong>d erosion activity. However, the model accuracy was affected byits rule-based structure which biased the output toward particular soil texture groups. It didnot account for the dynamic nature of soil surface conditions. In addition to this, the modelformulation was restrictive such that AUSLEM could not capture the full range of theerodibility cont<strong>in</strong>uum (Figure 2.11). The monthly temporal resolution of <strong>in</strong>puts confoundedthis issue and suppressed the model sensitivity to short-term (e.g. daily) ra<strong>in</strong>fall events thatare an important driver of land erodibility dynamics. A new scheme is therefore requiredwhich can capture high temporal resolution changes <strong>in</strong> land erodibility and through the fullrange of the land erodibility cont<strong>in</strong>uum described <strong>in</strong> Chapter 2.Computation of u *t forms the basis of the particle emission schemes <strong>in</strong> many process basedw<strong>in</strong>d erosion models (Hagen, 1991; Marticorena and Bergametti, 1995; Shao et al., 1996;Gregory et al., 2004). As u *t is <strong>in</strong>dependent of but determ<strong>in</strong>es the w<strong>in</strong>d velocity at whichparticle entra<strong>in</strong>ment occurs it can be physically related to erosion controls. However,modell<strong>in</strong>g land susceptibility to w<strong>in</strong>d erosion us<strong>in</strong>g a physical parameterisation of u *t iscomputationally <strong>in</strong>tensive and requires cont<strong>in</strong>ual measurement of variables that are difficultto quantify, e.g. frontal area effects of vegetation and soil particle size distribution (Shao,2000). The lack of suitable spatial data required as <strong>in</strong>put to the models has also been alimit<strong>in</strong>g factor to their application (Raupach and Lu, 2004).Land erodibility to w<strong>in</strong>d is a concept and cannot be directly measured <strong>in</strong> the field. It can,however, be <strong>in</strong>ferred through either u *t , or measurements of w<strong>in</strong>d erosion rates under avariety of conditions for some reference w<strong>in</strong>d velocity. Empirical functions relat<strong>in</strong>g erosionrates (i.e. streamwise sediment flux <strong>in</strong> gm -1 s -1 ) to surface conditions have been used <strong>in</strong> thedevelopment of field scale w<strong>in</strong>d erosion models with applications <strong>in</strong> North America andAfrica (Woodruff and Siddoway, 1965; Fryrear et al., 1998; Visser et al., 2005; Chapter 3). Ifderived under standard measurement conditions (i.e. w<strong>in</strong>d tunnel dimensions, w<strong>in</strong>d speeds,etc.) simple empirical expressions can be comb<strong>in</strong>ed to model the land erodibility cont<strong>in</strong>uum.A benefit of this approach is that a model can be developed us<strong>in</strong>g functions for which spatialdata tend to be readily available as <strong>in</strong>puts. Further, calibration of the models to improveperformance can be achieved without violat<strong>in</strong>g assumptions <strong>in</strong>herent to physicalparameterisations of u *t . Caveats of us<strong>in</strong>g empirical soil loss functions to def<strong>in</strong>e w<strong>in</strong>d erosionrates and land erodibility are that they must exist relative to some reference w<strong>in</strong>d speed at135

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