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Soil Hydraulic Parameter Upscaling for Steady-State Flow with Root Water Uptake

Jianting Zhu* and Binayak P. Mohanty

Dep. of Biological and Agricultural Engineering, 301B Scoates Hall, Texas A&M Univ., College Station, TX 77843-2117


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Fig. 1. Two different root water uptake distribution functions.

 


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Fig. 2. Influence of dimensionless root zone depth, {delta}*, on the dimensionless flux, qL*, when {tau}* = 1.0: (a) {psi}L* = 0.2; (b) {psi}L* = 5.2.

 


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Fig. 3. Influence of dimensionless transpiration rate, {tau}*, on the dimensionless flux, qL*, when {delta}* = 0.3: (a) {psi}L* = 0.2; (b) {psi}L* = 5.2.

 


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Fig. 4. Influence of {alpha}* on the dimensionless flux, qL*, when {delta}* = 0.3: (a) {psi}L* = 0.2; (b) {psi}L* = 5.2.

 


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Fig. 5. Influence of dimensionless root zone depth {delta}* on the effective coefficient for the {alpha}* field when {tau}* = 1.0 and CV = 1.0: (a) = 1.0, (b) = 6.0, and (c) = 10.0.

 


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Fig. 6. Influence of dimensionless transpiration rate {tau}* on the effective coefficient for the {alpha}* field when {delta}* = 0.3 and CV = 1.0: (a) = 1.0, (b) = 6.0, and (c) = 10.0.

 


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Fig. 7. Influence of on the effective coefficient for the {alpha}* field when {tau}* = 1.0 and {delta}* = 0.3: (a) CV = 0.5 and (b) CV = 1.0.

 


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Fig. 8. Influence of coefficient of variation of the {alpha}* field on the effective coefficient for the {alpha}* field when {tau}* = 1.0 and {delta}* = 0.3: (a) = 1.0, (b) = 6.0, and (c) = 10.0.

 





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