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Right arrow Soil Hydrology
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Modeling Soil Water and Solute Transport—Fast, Simplified Numerical Solutions

P. J. Ross*

CSIRO Land and Water, Long Pocket Lab., 120 Meiers Rd., Indooroopilly, Brisbane, QLD 4068, Australia



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Fig. 1. Discretisation of the soil profile into n layers of thickness {Delta}xi with centers at zi, i = 1,2,...,n with water or solute fluxes qi between them.

 


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Fig. 2. Exact water flux from Layer 1 to Layer 2 below compared with that calculated from Eq. [16] with a fixed weighting of w = 0.5 for the gravity component.

 


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Fig. 3. Water fluxes as in Fig. 2 compared with: WS1, flux calculated from Eq. [16] with weighting w for the gravity component calculated from Eq. [17]; WS2, flux calculated by equating fluxes through unsaturated and saturated regions.

 


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Fig. 4. Soil profile and discretisation for the test problem. Soil hydraulic parameters were {theta}S = 0.4, he = -10 cm, {lambda} = 1/3, and KS = 2 cm h-1 for the sandy soil and {theta}S = 0.5, he = -40 cm, {lambda} = 1/9, and KS = 0.2 cm h-1 for the clayey soil, with {eta} = 2/{lambda} + 3. Precipitation was 2.5 cm h-1 for the first 10 h while potential evaporation was constant at 0.05 cm h-1 for the 400 h of the solution.

 


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Fig. 5. Depth of surface ponding for the test problem given by the different methods of solution.

 


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Fig. 6. Evaporation and drainage for the test problem given by the different methods of solution.

 


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Fig. 7. Relative errors in drainage for standard (triangles) and fast (squares) solutions of the test problem as a function of the total number of iterations through the flux calculations. Filled symbols are for 10 soil layers and unfilled are for 20.

 


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Fig. 8. Solutions for solute concentration (arbitrary mass units per cm3 of soil) at 400 h for the test problem with varying numbers of time periods for averaging the water fluxes. There were initially 1000 mass units of solute in the top 10-cm layer.

 


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Fig. 9. Solutions for solute concentration (arbitrary mass units per cm3 of soil) at 400 h for the test problem with varying pairs (ns, nw) of ns solute time steps per nw water time steps with water fluxes averaged over the nw water steps. There were initially 1000 mass units of solute in the top 10-cm layer.

 





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