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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 2 – Land Erodibility ControlsSaleh and Fryrear (1995) identified a number of deficiencies <strong>in</strong> the early studies of moistureeffects on particle mobilization by w<strong>in</strong>d. A particular limitation is that the expressions do notaccount for processes that affect particle entra<strong>in</strong>ment once u * exceeds u *t and the saltationprocess is established. Subsequently, two expressions were developed for abrad<strong>in</strong>g (2.17) andnon-abrad<strong>in</strong>g (2.18) surface conditions where:( TWC / W ') 0.375( TWC / ) 2u ta= +(2.17)*0.205+ 0.182W '( TWC / W ') 0.506( TWC / ) 2u t= +(2.18)*0.305+ 0.222W 'where u *t is the threshold friction velocity under non-abrad<strong>in</strong>g conditions, u *ta is the thresholdfriction velocity under abrad<strong>in</strong>g conditions, TWC is the soil surface threshold water content(the moisture content at which particle entra<strong>in</strong>ment is <strong>in</strong>itiated), and W’ is the gravimetricwater content of the soil. Their results suggest that under abrad<strong>in</strong>g conditions, because of theerosive impact of saltat<strong>in</strong>g particles, less w<strong>in</strong>d energy is required to <strong>in</strong>itiate entra<strong>in</strong>ment.Recent developments <strong>in</strong> quantify<strong>in</strong>g the effects of soil moisture on the process of soilmobilization by w<strong>in</strong>d have comb<strong>in</strong>ed w<strong>in</strong>d tunnel experimentation with conceptual models of<strong>in</strong>ter-particle cohesion. The focus of the research moved from try<strong>in</strong>g to develop regressionequations to quantify<strong>in</strong>g the b<strong>in</strong>d<strong>in</strong>g forces responsible for <strong>in</strong>ter-particle cohesion. McKenna-Neuman and Nickl<strong>in</strong>g (1989) presented a theoretical model for the effect of moisture on u *t .The research developed the notion that <strong>in</strong>ter-particle contacts can be modelled by account<strong>in</strong>gfor capillary forces between particles with angular contact geometries. The basis for themodel, the <strong>in</strong>ter-particle capillary force (F c ) is def<strong>in</strong>ed by:T= G(2.19)PF c2where T is the surface tension of the water, P is the pressure deficiency, and G is a nondimensionalcoefficient. This function was <strong>in</strong>corporated <strong>in</strong>to Bagnold’s (1941) staticthreshold model (Equation 2.5). Two expressions were developed to account for open-packed(Equation 2.20) and closed-packed gra<strong>in</strong>s (Equation 2.21):46

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