2015
DOI: 10.1016/j.jhydrol.2015.07.032
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Modeling dynamic non-equilibrium water flow observations under various boundary conditions

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Cited by 21 publications
(21 citation statements)
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“…For the finer soils, this effect is even more pronounced and flow equilibrium is hardly reached, even after providing a relatively long time with constant suction (couple of hours). This observation is in contrast to our numerical findings and indicates ''hydraulic non-equilibrium'', i.e., a nonuniqueness of the relation between local water content and local pressure head, as discussed by Diamantopoulos and Durner (2012) and experimentally found in many types of transient flow experiments (Diamantopoulos et al, 2015). The effect of hysteresis can also be observed from the graphs of flow rates.…”
Section: Kusat and Ksatcontrasting
confidence: 99%
“…For the finer soils, this effect is even more pronounced and flow equilibrium is hardly reached, even after providing a relatively long time with constant suction (couple of hours). This observation is in contrast to our numerical findings and indicates ''hydraulic non-equilibrium'', i.e., a nonuniqueness of the relation between local water content and local pressure head, as discussed by Diamantopoulos and Durner (2012) and experimentally found in many types of transient flow experiments (Diamantopoulos et al, 2015). The effect of hysteresis can also be observed from the graphs of flow rates.…”
Section: Kusat and Ksatcontrasting
confidence: 99%
“…This could be done by decoupling both state variables and introducing a term describing the dynamics toward equilibrium while still adhering to the basic concept of the Richards equation (i.e., to link the gradient in soil water potential to the flux by an effective hydraulic conductivity). Such a decoupling was proposed by Ross and Smettem (2000) and extended by Diamantopoulos et al (2015), who separated fast and slow equilibrating pore domains.…”
Section: Challenges At the Pedon Scalementioning
confidence: 91%
“…It has also been defined, by Ross and Smettem (), as a parameter relating the difference ( θ eq − θ ) [ M L − 3 ] between the water content in the equilibrium state and the actual water content to the rate of change in the actual water saturation of a porous medium, ∂θ/∂t [ M L − 3 T − 1 ]. These characterizations of DNE facilitate the description or modeling of pore‐scale dynamic water flows in porous media (Diamantopoulos et al, ). The variations in water content‐capillary pressure functions are mainly manifested in the differences in: capillary pressure at a given water saturation, water saturation at a given capillary pressure under different test conditions, and time lags between corresponding water saturation and capillary pressure values during a drainage or imbibition process.…”
Section: Introductionmentioning
confidence: 99%