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Exponential Distribution Theory and the Interpretation of Splash Detachment and Transport Experiments

A. I. J. M. van Dijk*, A. G. C. A. Meesters and L. A. Bruijnzeel

Faculty of Earth and Life Sciences, Vrije Univ. Amsterdam, De Boelelaan 1085, 1081 HV Amsterdam, The Netherlands



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Fig. 1. The mass of soil splashed beyond a radial distance r from its point source (data from Riezebos and Epema, 1985). Exponential functions are fitted to the data, which represent splash resulting from artificial drops falling from indicated heights.

 


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Fig. 2. One-dimensional distribution of particles splashed from a source strip expressed as a density function of perpendicular distance x {vstrip(x); Eq. [5]} and as a transport function indicating the fraction of detached material splashed beyond distance x {vbeyond(x); Eq. [6]}. All variables have been made dimensionless; dashed lines represent approximate exponential functions. {Lambda} = average splash length.

 


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Fig. 3. Rates of splash transport [q({Delta}X)] onto 10-cm wide strips, placed at increasing distances from a soil tray subjected to artificial rainfall and filled with different soils (approximate median grain size indicated; data from Savat and Poesen, 1981) with Eq. [12c] fitted to the data.

 


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Fig. 4. Illustration of (a) the matrix used to model the distribution of particles splashed from a rectangular area (the meaning of the areas labelled SCREEN and CORNER is explained in the text); (b) a soil tray bordered by a very wide collecting screen having the same length; (c) a soil tray bordered by an infinitely large horizontal collecting screen; and (d) a soil tray bordered by a collector with vertical splash guards on three sides.

 


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Fig. 5. Splash transport onto (a) a wide screen having the same length as a side A, and (b) an infinitely large screen, both placed along a side A of a tray with dimensions A and B, as a function of the dimensionless length of that side, A/{Lambda}, and for a number of different values of the aspect (A/B) of the tray. Splash transport was made dimensionless by expressing it as a fraction of the transport from an infinitely large area of soil.

 


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Fig. 6. Relationship between dimensionless cup radius R/{Lambda} and the amount of soil splashed out of the cup, expressed as a fraction of the total amount of detached sediment (FR).

 


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Fig. 7. Application of the theory for interpreting splash cup data (Eq. [16]) to data collected by Poesen and Torri (1988). The exponential equation proposed by Poesen and Torri (1988) is shown for comparison. mR = cup splash rate, R = radius.

 





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