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Published online 27 May 2008
Published in Vadose Zone J 7:782-797 (2008)
DOI: 10.2136/vzj2007.0074
© 2008 Soil Science Society of America
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Modeling Nonequilibrium Flow and Transport Processes Using HYDRUS

Jirka Simuneka,* and Martinus Th. van Genuchtenb

a Dep. of Environmental Sciences, Univ. of California, Riverside, CA 92521
b USDA-ARS, U.S. Salinity Lab., 450 West Big Springs Rd., Riverside, CA 92507


Figure 1
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FIG. 1. Conceptual physical nonequilibrium models for water flow and solute transport. In the plots, {theta} is the water content, {theta}mo and {theta}im in (b) and (c) are water contents of the mobile and immobile flow regions, respectively; {theta}M and {theta}F in (d) are water contents of the matrix and macropore (fracture) regions, respectively, and {theta}M,mo, {theta}M,im, and {theta}F in (e) are water contents of the mobile and immobile flow regions of the matrix domain, and in the macropore (fracture) domain, respectively; c are concentrations of corresponding regions, with subscripts having the same meaning as for water contents, while S is the total solute content of the liquid phase.

 

Figure 2
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FIG. 2. Conceptual physical nonequilibrium models for water flow and solute transport.

 

Figure 3
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FIG. 3. Conceptual chemical nonequilibrium models for reactive solute transport. In the plots, {theta} is the water content, {theta}mo and {theta}im in (d) are water contents of the mobile and immobile flow regions, respectively; {theta}M and {theta}F in (e) are water contents of the matrix and macropore (fracture) regions, respectively; c are concentrations of the corresponding regions, se are sorbed concentrations in equilibrium with the liquid concentrations of the corresponding regions, and sk are kinetically sorbed solute concentrations of the corresponding regions.

 

Figure 4
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FIG. 4. Breakthrough curves calculated using the Uniform Transport Model for a 10-cm-long soil column and the following parameters: q = 5 cm d–1, {theta} = 0.5, and {rho}b = 1.5 g cm–3; on the left, Kd = 1 cm3 g–1 and {lambda} = 0.1, 1, and 10 cm; and on the right, {lambda} = 1 cm and Kd = 0, 1, and 3 cm3 g–1.

 

Figure 5
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FIG. 5. Breakthrough curves calculated using the Mobile–Immobile Water Model for a 10-cm-long soil column and the following parameters: q = 3 cm d–1, {theta} = 0.5, {lambda}mo = 1 cm, Kd = 1 cm3 g–1, {rho}b = 1.5 g cm–3. On the left: fmo = 0.6, {theta}mo = 0.3, {theta}im = 0.2, and {omega}mim = 0.1, 0.5, 10 d–1. On the right: {omega}mim = 0.5 d–1 and (a) fmo = 0.4, {theta}mo = 0.2, {theta}im = 0.3; (b) fmo = 0.6, {theta}mo = 0.3, {theta}im = 0.2; and (c) fmo = 0.8, {theta}mo = 0.4, {theta}im = 0.1.

 

Figure 6
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FIG. 6. Breakthrough curves calculated using the Dual-Permeability Model for a 10-cm-long soil column and the following parameters: qm = 3 cm d–1, qf = 30 cm d–1, {theta} = {theta}m = {theta}f = 0.5, w = 0.1, {lambda}m = {lambda}f = 1 cm, Kdm = Kdf = 1 cm3 g–1, {rho}b = 1.5 g cm–3, and {omega}dp = 0, 0.1, and 0.5 d–1. Matrix, fracture, and total breakthrough curves are represented by thin, medium, and thick lines, respectively.

 

Figure 7
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FIG. 7. Breakthrough curves calculated using the Dual-Permeability Model with MIM for a 10-cm-long soil column and the following parameters: qm = 3 cm d–1, qf = 30 cm d–1, {theta} = {theta}m = {theta}f = 0.5, w = 0.1, {lambda}m = {lambda}f = 1 cm, Kdm = Kdf = 1 cm3 g–1, {rho}b = 1.5 g cm–3, {omega}dp = 0.1 d–1, {omega}dpm = 0.1 d–1, {theta}im,m (thim) = 0.0, 0.1, 0.3, and 0.4, and fm = 1, 0.8, 0.4, and 0.2, respectively. Matrix, fracture, and total breakthrough curves are represented by thin, medium, and thick lines, respectively.

 

Figure 8
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FIG. 8. Breakthrough curves calculated using the One Kinetic Site Model for a 10-cm-long soil column and the following parameters: q = 5 cm d–1, {theta} = 0.5, {lambda} = 1 cm, Kd = 1 cm3 g–1, {rho}b = 1.5 g cm–3, and {alpha}k = 0.1, 0.5, and 10 d–1.

 

Figure 9
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FIG. 9. Breakthrough curves calculated using the Two-Site Kinetic Model for a 10-cm-long soil column and the following parameters: q = 5 cm d–1, {theta} = 0.5, {lambda} = 1 cm, Kd = 1 cm3 g–1, and {rho}b = 1.5 g cm–3; on the left, fe = 0.4 and {alpha}k = 0.1, 0.5, and 10 d–1; and on the right, {alpha}k = 0.5 d–1 and fe = 0.1, 0.4, and 0.8.

 

Figure 10
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FIG. 10. Breakthrough curves calculated using the Two Kinetic Sites Model for a 10-cm-long soil column and the following parameters: solute pulse duration = 10 d, q = 5 cm d–1, {theta} = 0.5, {lambda} = 1 cm, Kd = 1 cm3 g–1, {rho}b = 1.5 g cm–3, ka1 = 1.5 d–1, kd1 = 0.5 d–1, and ka2 = 0.0, 0.3, and 3.0 d–1 with kd2 = 0.0, 0.1, and 1.0 d–1, respectively.

 

Figure 11
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FIG. 11. Breakthrough curves calculated using the Dual-Porosity Model with One Kinetic Site for a 10-cm-long soil column and the following parameters: solute pulse duration = 10 d, q = 3 cm d–1, {theta} = 0.5, {theta}mo = 0.3, {theta}im = 0.2, {lambda}mo = 1 cm, Kd = 1 cm3 g–1, {rho}b = 1.5 g cm–3, fmo = 0.6, {alpha} = 0.1 d–1; on the left, fem = 0.4 and {alpha}ch = 0.1, 0.5, and 10 d–1 ; and on the right, {alpha}ch = 0.1 d–1 and fem = 1.0, 0.7, 0.4, and 0.1.

 

Figure 12
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FIG. 12. Breakthrough curves calculated using the Dual-Permeability Model with Two-Site Sorption for a 10-cm-long soil column and the following parameters: solute pulse duration = 10 d, qm = 3 cm d–1, qf = 30 cm d–1, {theta} = {theta}m = {theta}f = 0.5, w = 0.1, {lambda}m = {lambda}f = 1 cm, Kdm = Kdf = 1 cm3 g–1, {rho}b = 1.5 g cm–3, {omega}dp = 0.1 d–1, {alpha}ch,m = {alpha}ch,f = 0.1 d–1, and ff = fm = 1, 0.7, and 0.4. Matrix, fracture, and total breakthrough curves are represented by thin, medium, and thick lines, respectively.

 





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