2016
DOI: 10.1002/2015wr018254
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Pore‐scale displacement mechanisms as a source of hysteresis for two‐phase flow in porous media

Abstract: The macroscopic description of the hysteretic behavior of two-phase flow in porous media remains a challenge. It is not obvious how to represent the underlying pore-scale processes at the Darcy-scale in a consistent way. Darcy-scale thermodynamic models do not completely eliminate hysteresis and our findings indicate that the shape of displacement fronts is an additional source of hysteresis that has not been considered before. This is a shortcoming because effective process behavior such as trapping efficienc… Show more

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Cited by 176 publications
(131 citation statements)
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“…The main reason for this is that the information in the P c and k r curves which are often used as the only validation is extremely densely encoded: many aspects of the porous medium and the fluid behavior are lumped into too few parameters to completely characterize the behavior. P c and k r curves are traditionally described as functions of only water saturation, rather than taking all true state variables into account [18,19].…”
Section: Published By the American Physical Society Under The Terms Omentioning
confidence: 99%
See 1 more Smart Citation
“…The main reason for this is that the information in the P c and k r curves which are often used as the only validation is extremely densely encoded: many aspects of the porous medium and the fluid behavior are lumped into too few parameters to completely characterize the behavior. P c and k r curves are traditionally described as functions of only water saturation, rather than taking all true state variables into account [18,19].…”
Section: Published By the American Physical Society Under The Terms Omentioning
confidence: 99%
“…The Euler number is a topological invariant which can be used to characterize the topology of complex shapes and has therefore been used extensively to characterize the nonwetting phase topology in two-phase flow studies [19,21,59]. The Euler number χ of a general nonplanar graph can be defined as χ = v − e with v the number of vertices (in our case, oil-filled pores) and e the number of edges (oil-filled throats) [62].…”
Section: Euler Number Analysismentioning
confidence: 99%
“…To this end, recent advances in pore-scale imaging-based characterization methods (see review [26]) that enable the fast visualization of two-phase flow at pore-scale resolution, most notably microscopy imaging of thin micromodels [18,[27][28][29], X-ray computed tomography [30][31][32][33][34], and confocal microscopy [35,36], have provided valuable insights into 2 Geofluids the interplay of viscous, capillary, gravitational, and inertial forces constituting the complexity of interface dynamics at the pore-scale. For instance, free-energy driven Haines jumps have been confirmed as dominant displacement mechanism for flow at small capillary numbers [29,32].…”
Section: Introductionmentioning
confidence: 99%
“…Some orientation is given by findings of Hincapié and Germann (2010) and Moebius and Or (2012). Promising techniques like time-lapse X-ray or µCT tomography just emerge to be applied (Koestel and Larsbo, 2014;Schlüter et al, 2016). Yet there is consensus that macroporematrix interaction depends on the matric head, the wetting of the macropore wall (Klaus et al, 2013) and is optionally affected 10 by organic coatings which may act hydrophobic (Jarvis, 2007;Rogasik et al, 2014).…”
Section: Macropore-matrix-interactionmentioning
confidence: 99%
“…Pore scale processes (e.g. Moebius and Or, 2012;Shahraeeni and Or, 2012;Snehota et al, 2015;Schlüter et al, 2016) are not resolved here.…”
mentioning
confidence: 99%